Contrast Ultrasound Imaging

Even though ultrasound remains the safest and the most popular (one in every three imaging in the world) means of imaging, its utility is limited due to poor contrast. 20% of the 17 million echocardiography performed in the United States in 2000 were suboptimal, i.e. did not provide definitive diagnosis for coronary heart disease. Microbubbles intravenously injected into patients’ body can enhance the contrast of ultrasound images. A good contrast agent will enable reliable imaging of abnormal blood flows leading to early diagnosis of heart disease, as well as those of the kidney, liver and brain. They can also deliver drugs to tageted tissues. Current methods of contrast agent design and its use in drug delivery are empirical.

In collaboration with Professor Flemming Forsberg (Thomas Jefferson Medical School) we perform in vitro experiments and develop theoretical models to offer a unique and clear pathway for a rigorous methodology to customize contrast agent design for specific tasks and applications. It will be a useful tool to agent developers (e.g. GE Health Care) and scanner manufacturers (e.g. GE or Phillips). Contrast bubbles are stabilized by a thin encapsulating layer ( ~ 4-10nm) of surface active material, such as protein, lipid or surfactant. The encapsulation plays a critical role in the performance of these agents. In 2003 we first proposed and developed interfacial rheological models for the encapsulation, which has since become popular with the contrast agent reserach community. The encapsulation is treated as an interface having zero thickness and an intrinsic surface rheology (surface viscosity and elasticity). The rationale for our model vis-à-vis ones with a thick layer is the anisotropy and inhomogeneity (in thickness direction) in the molecular structure of the encapsulation. Our hypothesis is that a model, if it retains the essential physics, will offer applicability over a wide range of acoustic excitations. We adopted a two-prongted approach of determination and validation. After we determine the model parameters from one set of experiments, we proceed to validate the model using a different set of experiments. The model is validated by comparing its prediction against the scattered nonlinear (sub- and super-harmonic) response measured at higher amplitudes. We have succesfully applied this approach to model commercialy available agents such as Optison® (Mallinckrodt, St Loius, MO) and Definity® (Bristol Meyer-Squibb Imaging, N. Billerica, MA). Our current focus has been further model development, applicatiosn to newer agents and developing underlying physics of other applications such as subharmonic aided noninvasive pressure estimation (SHAPE).

Related Publication

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

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  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

  • Paul S, Nahire R, Mallik S, Sarkar K 2014 “Encapsulated microbubbles and echogenic liposomes for contrast ultrasound imaging and targeted drug delivery,” Computational Mechanics, 53,413-435.

    Micron- to nanometer-sized ultrasound agents,like encapsulated microbubbles and echogenic liposomes,are being developed for diagnostic imaging and ultra-sound mediated drug/gene delivery. This review providesan overview of the current state of the art of the mathe-matical models of the acoustic behavior of ultrasound con-trast microbubbles. We also present a review of the in vitroexperimental characterization of the acoustic properties ofmicrobubble based contrast agents undertaken in our lab-oratory. The hierarchical two-pronged approach of model-ing contrast agents we developed is demonstrated for a lipidcoated (SonazoidTM)and a polymer shelled (polyD-L-lactic acid) contrast microbubbles. The acoustic and drugrelease properties of the newly developed echogenic lipo-somes are discussed for their use as simultaneous imagingand drug/gene delivery agents. Although echogenicity is con-clusively demonstrated in experiments, its physical mecha-nisms remain uncertain. Addressing questions raised herewill accelerate further development and eventual clinicalapproval of these novel technologies.

  • Nahire R, Halder M, Paul S, Margoum A, Ambre AH, Katti KS, Gange KN, Srivastava D K, Sarkar K, Mallik S 2014 “pH-Triggered Echogenicity and Contents Release from Liposomes,” Molecular Pharamaceutics, 11, 4059-4068.

    Liposomes are representative lipid nanoparticles widelyused for delivering anticancer drugs, DNA fragments, or siRNA to cancercells. Upon targeting, various internal and external triggers have been usedto increase the rate for contents release from the liposomes. Among theinternal triggers, decreased pH within the cellular lysosomes has beensuccessfully used to enhance the rate for releasing contents. However,imparting pH sensitivity to liposomes requires the synthesis of specializedlipids with structures that are substantially modified at a reduced pH.Herein, we report an alternative strategy to render liposomes pH sensitiveby encapsulating a precursor which generates gas bubblesin situinresponse to acidic pH. The disturbance created by the escaping gasbubbles leads to the rapid release of the encapsulated contents from theliposomes. Atomic force microscopic studies indicate that the liposomalstructure is destroyed at a reduced pH. The gas bubbles also render theliposomes echogenic, allowing ultrasound imaging. To demonstrate the applicability of this strategy, we have successfully targeteddoxorubicin-encapsulated liposomes to the pancreatic ductal carcinoma cells that overexpress the folate receptor on the surface.In response to the decreased pH in the lysosomes, the encapsulated anticancer drug is efficiently released. Contents releasedfrom these liposomes are further enhanced by the application of continuous wave ultrasound (1 MHz), resulting in substantiallyreduced viability for the pancreatic cancer cells (14%).

  • Nahire R, Halder M, Paul S, Margoum A, Ambre AH, Katti KS, Gange KN, Srivastava D K, Sarkar K, Mallik S 2013 “Polymer Coated Echogenic Lipid Nanoparticles with dual release triggers,” Biomacromolecules, 14, 841-853.

    Although lipid nanoparticles are promising drugdelivery vehicles, passive release of encapsulated contents atthe target site is often slow. Herein, we report contents releasefrom targeted, polymer-coated, echogenic lipid nanoparticles inthe cell cytoplasm by redox trigger and simultaneouslyenhanced by diagnostic frequency ultrasound. The lipidnanoparticles were polymerized on the external leaflet usinga disulfide cross-linker. In the presence of cytosolicconcentrations of glutathione, the lipid nanoparticles released76% of encapsulated contents. Plasma concentrations ofglutathione failed to releasethe encapsulated contents.Application of 3 MHz ultrasound for 2 min simultaneouslywith the reducing agent enhanced the release to 96%. Folicacid conjugated, doxorubicin-loaded nanoparticles showed enhanced uptake and higher cytotoxicity in cancer cells overexpressingthe folate receptor (compared to the control). With further developments, these lipid nanoparticles have the potential to be usedas multimodal nanocarriers for simultaneous targeted drug delivery and ultrasound imaging.

  • Nahire R, Hossain R, Patel R, Paul S, Ambre AH, Meghnani V, Layek B, Katti KS, Gange KN, Leclarc E, Srivastava D K, Sarkar K, Mallik S 2014 “Multifunctional polymersomes for cytosolic delivery of gemcitabine and doxorubicin to cancer cells,” Biomaterials, 35, 6482-6497.

    Although liposomes are widely used as carriers of drugs and imaging agents, they suffer from a lack ofstability and the slow release of the encapsulated contents at the targeted site. Polymersomes (vesicles ofamphiphilic polymers) are considerably more stable compared to liposomes; however, they alsodemonstrate a slow release for the encapsulated contents, limiting their efficacy as a drug-delivery tool.As a solution, we prepared and characterized echogenic polymersomes, which are programmed torelease the encapsulated drugs rapidly when incubated with cytosolic concentrations of glutathione.These vesicles encapsulated air bubbles inside and efficiently reflected diagnostic-frequency ultrasound.Folate-targeted polymersomes showed an enhanced uptake by breast and pancreatic-cancer cells in amonolayer as well as in three-dimensional spheroid cultures. Polymersomes encapsulated with theanticancer drugs gemcitabine and doxorubicin showed significant cytotoxicity to these cells. Withfurther improvements, these vesicles hold the promise to serve as multifunctional nanocarriers, offeringa triggered release as well as diagnostic ultrasound imaging.

  • Kumar KN, Sarkar K 2015 “Effects of ambient hydrostatic pressure on the material properties of the encapsulation of an ultrasound contrast microbubble,” Journal of the Acoustical Society of America, 138, 624-634.

    Ultrasound contrast microbubbles experience widely varying ambient blood pressure in differentorgans, which can also change due to diseases. Pressure change can alter the material properties ofthe encapsulation of these microbubbles. Here the characteristic rheological parameters of contrastagent Definity are determined by varying the ambient pressure (in a physiologically relevant range0–200 mm Hg). Four different interfacial rheological models are used to characterize the microbub-bles. Effects of gas diffusion under excess ambient pressure are investigated in detail accountingfor size decrease of contrast microbubbles. Definity contrast agent show a change in their interfacialdilatational viscosity (3.6108Ns/m at 0 mm Hg to 4.45108Ns/m at 200 mm Hg) and inter-facial dilatational elasticity (0.86 N/m at 0 mm Hg to 1.06 N/m at 200 mm Hg) with ambient pres-sure increase. The increase results from material consolidation, similar to such enhancement inbulk properties under pressure. The model that accounts for enhancement in material propertieswith increasing ambient pressure matches with experimentally measured subharmonic response asa function of ambient pressure, while assuming constant material parameters does not.

  • Lang X, Porter T, Sarkar K 2015 “Interpreting attenuation at different excitation amplitudes to estimate strain-dependent interfacial rheological properties of lipid-coated monodisperse microbubbles,” Journal of the Acoustical Society of America, 138, 3994-4003.

    Broadband attenuation of ultrasound measured at different excitation pressures being differentraises a serious theoretical concern, because the underlying assumption of linear and independentpropagation of different frequency components nominally requires attenuation to be independent ofexcitation. Here, this issue is investigated by examining ultrasound attenuation through a monodis-perse lipid-coated microbubble suspension measured at four different acoustic excitation ampli-tudes. The attenuation data are used to determine interfacial rheological properties (surface tension,surface dilatational elasticity, and surface dilatational viscosity) of the encapsulation according tothree different models. Although different models result in similar rheological properties, attenua-tion measured at different excitation levels (4–110 kPa) leads to different values for them; the dila-tation elasticity (0.56 to 0.18 N/m) and viscosity (2.4108to 1.52108Ns/m) both decreasewith increasing pressure. Numerically simulating the scattered response, nonlinear energy transferbetween frequencies are shown to be negligible, thereby demonstrating the linearity in propagationand validating the attenuation analysis. There is a second concern to the characterization arisingfrom shell properties being dependent on excitation amplitude, which is not a proper constitutivevariable. It is resolved by arriving at a strain-dependent rheology for the encapsulation. The limita-tions of the underlying analysis are discussed.

  • Kumar KN, Sarkar K 2016 “Interfacial rheological properties of contrast microbubble Targestar P as a function of ambient pressure,” Ultrasound in Medicine and Biology, 42, 1010-1017.

    In this Technical Note, we determine the interfacial rheological parameters of the encapsulation of thecontrast agent Targestar P using ultrasound attenuation. The characteristic parameters are obtained according totwo interfacial rheological models. The properties—surface dilatational elasticity (0.09 ± 0.01 N/m) and surfacedilatational viscosity (8 ± 0.1E–9 N$s/m)—are found to be of similar magnitude for both models. Contrast micro-bubbles experience different ambient pressure in different organs. We also measure these parameters as functionsof ambient pressure using attenuation measured at different overpressures (0, 100 and 200 mm Hg). For each valueof ambient hydrostatic pressure, we determine the rheological properties, accounting for changes in the size dis-tribution caused by the pressure change. We discuss different models of size distribution change under overpres-sure: pure adiabatic compression or gas exchange with surrounding medium. The dilatational surface elasticityand viscosity are found to increase with increasing ambient pressure.

  • Kumar KN, Mallik S, Sarkar K, 2017 “Role of freeze-drying in the presence of mannitol on the echogenicity of echogenic liposomes,” Journal of the Acoustical Society of America, 142, 3670-3676.

    Echogenic liposomes (ELIPs) are an excellent candidate for ultrasound activated therapeutics andimaging. Although multiple experiments have established their echogenicity, the underlying mech-anism has remained unknown. However, freeze-drying in the presence of mannitol during ELIPpreparation has proved critical to ensuring echogenicity. Here, the role of this key component in thepreparation protocol was investigated by measuring scattering from freshly prepared freeze-driedaqueous solution of mannitol—and a number of other excipients commonly used in lyophiliza-tion—directly dispersed in water without any lipids in the experiment. Mannitol, meso-erythritol,glycine, and glucose that form a highly porous crystalline phase upon freeze-drying generated bub-bles resulting in strong echoes during their dissolution. On the other hand, sucrose, trehalose, andxylitol, which become glassy while freeze-dried, did not. Freeze-dried mannitol and other crystal-line substances, if thawed before being introduced into the scattering volume, did not produce echo-genicity, as they lost their crystallinity in the thawed state. The echogenicity disappeared in adegassed environment. Higher amounts of sugar in the original aqueous solution before freeze-drying resulted in higher echogenicity because of the stronger supersaturation and crystallinity. Thebubbles created by the freeze-dried mannitol in the ELIP formulation play a critical role in makingELIPs echogenic.

  • Xia L, Karandish F, Kumar KN, Froberg J, Kulkarni P, Gange KN, Choi Y, Mallik S, Sarkar K 2017 “Acoustic characterization of echogenic polymersomes prepared from amphiphilic block copolymers,” Ultrasound in Medicine and Biology, 44, 447-457.

    Polymersomes are a class of artificial vesicles prepared from amphiphilic polymers. Like lipid vesicles(liposomes), they too can encapsulate hydrophilic and hydrophobic drug molecules in the aqueous core and thehydrophobic bilayer respectively, but are more stable than liposomes. Although echogenic liposomes have beenwidely investigated for simultaneous ultrasound imaging and controlled drug delivery, the potential of thepolymersomes remains unexplored. We prepared two different echogenic polymersomes from the amphiphilic co-polymers polyethylene glycol–poly-DL-lactic acid (PEG-PLA) and polyethylene glycol–poly-L-lactic acid (PEG-PLLA), incorporating multiple freeze-dry cycles in the synthesis protocol to ensure their echogenicity. We investigatedacoustic behavior with potential applications in biomedical imaging. We characterized the polymeric vesicles acous-tically with three different excitation frequencies of 2.25, 5 and 10 MHz at 500 kPa. The polymersomes exhibitedstrong echogenicity at all three excitation frequencies (about 50- and 25-dB enhancements in fundamental andsubharmonic, respectively, at 5-MHz excitation from 20g/mL polymers in solution). Unlike echogenic lipo-somes, they emitted strong subharmonic responses. The scattering results indicated their potential as contrastagents, which was also confirmed by clinical ultrasound imaging.

  • Aliabouzar M, Kumar KN, Sarkar K, 2018 “Acoustic vaporization threshold of lipid coated perfluoropentane droplets,” Journal of the Acoustical Society of America, 143, 2001-2012.

    Phase shift droplets vaporizable by acoustic stimulation offer the advantages of producing micro-bubbles as contrast agentsin situas well as higher stability and the possibility of achieving smallersizes. Here, the acoustic droplet vaporization (ADV) threshold of a suspension of droplets with aperfluoropentane (PFP) core (diameter 400–3000 nm) is acoustically measured as a function of theexcitation frequency in a tubeless setup at room temperature. The changes in scattered responses—fundamental, sub-, and second harmonic—are investigated, a quantitative criterion is used to deter-mine the ADV phenomenon, and findings are discussed. The average threshold obtained using threedifferent scattered components increases with frequency—1.0560.28 MPa at 2.25 MHz,1.8960.57 MPa at 5 MHz, and 2.3460.014 MPa at 10 MHz. The scattered response from vapor-ized droplets was also found to qualitatively match with that from an independently prepared lipid-coated microbubble suspension in magnitude as well as trends above the determined ADV thresh-old value.

  • Aliabouzar M, Kumar KN, Sarkar K, 2018 “Acoustic vaporization threshold of lipid coated perfluoropentane droplets,” Journal of the Acoustical Society of America, 143, 2001-2012.

    Phase shift droplets vaporizable by acoustic stimulation offer the advantages of producing micro-bubbles as contrast agentsin situas well as higher stability and the possibility of achieving smallersizes. Here, the acoustic droplet vaporization (ADV) threshold of a suspension of droplets with aperfluoropentane (PFP) core (diameter 400–3000 nm) is acoustically measured as a function of theexcitation frequency in a tubeless setup at room temperature. The changes in scattered responses—fundamental, sub-, and second harmonic—are investigated, a quantitative criterion is used to deter-mine the ADV phenomenon, and findings are discussed. The average threshold obtained using threedifferent scattered components increases with frequency—1.0560.28 MPa at 2.25 MHz,1.8960.57 MPa at 5 MHz, and 2.3460.014 MPa at 10 MHz. The scattered response from vapor-ized droplets was also found to qualitatively match with that from an independently prepared lipid-coated microbubble suspension in magnitude as well as trends above the determined ADV thresh-old value.

  • Kulkarni P, Haldar MK, Karandish F, Confeld M, Hossain R, Borowicz P, Gange KN, Xia L, Sarkar K, Mallik S 2018 “Tissue-penetrating, hypoxia-responsive echogenic polymersomes for drug delivery to solid tumors,” Chemistry A European Journal, 24, 12490-12494.

    Hypoxia in solid tumors facilitates the progres-sion of the disease, develops resistance to chemo and radiotherapy, and contributes to relapse. Due to the lack of tumor penetration, most of the reported drug carriers are unable to reach the hypoxic niches of the solid tumors. We have developed tissue-penetrating, hypoxia-responsive echogenic polymersomes to deliver anti cancer drugs to solid tumors. The polymersomes are composed of a hy-poxia-responsive azobenzene conjugated and a tissue penetrating peptide functionalized polylactic acid-polyethylene glycol polymer. The drug-encapsulated, hypoxia-responsive polymersomes substantially decreased the viability of pancreatic cancer cells in spheroidal cultures. Under normoxic conditions, polymersomes were echogenic at diagnostic ultrasound frequencies but lose the echogenicity under hypoxia. In vivo imaging studies with xenograft mouse model further confirmed the ability of the polymersomes to target, penetrate, and deliver the encapsulated contents in hypoxic pancreatic tumor tissues.

  • Karandish F, Haldar MK, Xia L, Gange KN, Feng L, You S, Choi Y, Sarkar K, Mallik S  2018 “Nucleus-targeted, echogenic polymersomes for delivering a cancer stemness inhibitor to pancreatic cancer cells,” Biomacromolecules, 19,4122-4132.

    Chemotherapeutic agents for treating cancers show considerable sideeffects, toxicity, and drug resistance. To mitigate the problems, we designed nucleus-targeted, echogenic, stimuli-responsive polymeric vesicles (polymersomes) to transport andsubsequently release the encapsulated anticancer drugs within the nuclei of pancreaticcancer cells. We synthesized an alkyne-dexamethasone derivative and conjugated it to N3−polyethylene glycol (PEG)−polylactic acid (PLA) copolymer employing the Cu2+catalyzed“Click”reaction. We prepared polymersomes from the dexamethasone−PEG−PLA conjugate along with a synthesized stimuli-responsive polymer PEG−S−S−PLA. Thedexamethasone group dilates the nuclear pore complexes and transports the vesicles to thenuclei. We designed the polymersomes to release the encapsulated drugs in the presence ofa high concentration of reducing agents in the nuclei of pancreatic cancer cells. Weobserved that the nucleus-targeted, stimuli-responsive polymersomes released 70% ofencapsulated contents in the nucleus-mimicking environment in 80 min. We encapsulatedthe cancer stemness inhibitor BBI608 in the vesicles and observed that the BBI608encapsulated polymersomes reduced the viability of the BxPC3 cells to 43% in three-dimensional spheroid cultures. Thepolymersomes were prepared following a special protocol so that they scatter ultrasound, allowing imaging by a medicalultrasound scanner. Therefore, these echogenic, targeted, stimuli-responsive, and drug-encapsulated polymersomes have thepotential for trackable, targeted carrier of chemotherapeutic drugs to cancer cell nuclei.

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

  • Nahire R, Halder M, Paul S, Margoum A, Ambre AH, Katti KS, Gange KN, Srivastava D K, Sarkar K, Mallik S 2014 “pH-Triggered Echogenicity and Contents Release from Liposomes,” Molecular Pharamaceutics, 11, 4059-4068.

    Liposomes are representative lipid nanoparticles widelyused for delivering anticancer drugs, DNA fragments, or siRNA to cancercells. Upon targeting, various internal and external triggers have been usedto increase the rate for contents release from the liposomes. Among theinternal triggers, decreased pH within the cellular lysosomes has beensuccessfully used to enhance the rate for releasing contents. However,imparting pH sensitivity to liposomes requires the synthesis of specializedlipids with structures that are substantially modified at a reduced pH.Herein, we report an alternative strategy to render liposomes pH sensitiveby encapsulating a precursor which generates gas bubblesin situinresponse to acidic pH. The disturbance created by the escaping gasbubbles leads to the rapid release of the encapsulated contents from theliposomes. Atomic force microscopic studies indicate that the liposomalstructure is destroyed at a reduced pH. The gas bubbles also render theliposomes echogenic, allowing ultrasound imaging. To demonstrate the applicability of this strategy, we have successfully targeteddoxorubicin-encapsulated liposomes to the pancreatic ductal carcinoma cells that overexpress the folate receptor on the surface.In response to the decreased pH in the lysosomes, the encapsulated anticancer drug is efficiently released. Contents releasedfrom these liposomes are further enhanced by the application of continuous wave ultrasound (1 MHz), resulting in substantiallyreduced viability for the pancreatic cancer cells (14%).

  • Paul S, Nahire R, Mallik S, Sarkar K 2014 “Encapsulated microbubbles and echogenic liposomes for contrast ultrasound imaging and targeted drug delivery,” Computational Mechanics, 53,413-435.

    Micron- to nanometer-sized ultrasound agents,like encapsulated microbubbles and echogenic liposomes,are being developed for diagnostic imaging and ultra-sound mediated drug/gene delivery. This review providesan overview of the current state of the art of the mathe-matical models of the acoustic behavior of ultrasound con-trast microbubbles. We also present a review of the in vitroexperimental characterization of the acoustic properties ofmicrobubble based contrast agents undertaken in our lab-oratory. The hierarchical two-pronged approach of model-ing contrast agents we developed is demonstrated for a lipidcoated (SonazoidTM)and a polymer shelled (polyD-L-lactic acid) contrast microbubbles. The acoustic and drugrelease properties of the newly developed echogenic lipo-somes are discussed for their use as simultaneous imagingand drug/gene delivery agents. Although echogenicity is con-clusively demonstrated in experiments, its physical mecha-nisms remain uncertain. Addressing questions raised herewill accelerate further development and eventual clinicalapproval of these novel technologies.

  • Nahire R, Halder M, Paul S, Margoum A, Ambre AH, Katti KS, Gange KN, Srivastava D K, Sarkar K, Mallik S 2013 “Polymer Coated Echogenic Lipid Nanoparticles with dual release triggers,” Biomacromolecules, 14, 841-853.

    Although lipid nanoparticles are promising drugdelivery vehicles, passive release of encapsulated contents atthe target site is often slow. Herein, we report contents releasefrom targeted, polymer-coated, echogenic lipid nanoparticles inthe cell cytoplasm by redox trigger and simultaneouslyenhanced by diagnostic frequency ultrasound. The lipidnanoparticles were polymerized on the external leaflet usinga disulfide cross-linker. In the presence of cytosolicconcentrations of glutathione, the lipid nanoparticles released76% of encapsulated contents. Plasma concentrations ofglutathione failed to releasethe encapsulated contents.Application of 3 MHz ultrasound for 2 min simultaneouslywith the reducing agent enhanced the release to 96%. Folicacid conjugated, doxorubicin-loaded nanoparticles showed enhanced uptake and higher cytotoxicity in cancer cells overexpressingthe folate receptor (compared to the control). With further developments, these lipid nanoparticles have the potential to be usedas multimodal nanocarriers for simultaneous targeted drug delivery and ultrasound imaging.

  • Nahire R, Hossain R, Patel R, Paul S, Ambre AH, Meghnani V, Layek B, Katti KS, Gange KN, Leclarc E, Srivastava D K, Sarkar K, Mallik S 2014 “Multifunctional polymersomes for cytosolic delivery of gemcitabine and doxorubicin to cancer cells,” Biomaterials, 35, 6482-6497.

    Although liposomes are widely used as carriers of drugs and imaging agents, they suffer from a lack ofstability and the slow release of the encapsulated contents at the targeted site. Polymersomes (vesicles ofamphiphilic polymers) are considerably more stable compared to liposomes; however, they alsodemonstrate a slow release for the encapsulated contents, limiting their efficacy as a drug-delivery tool.As a solution, we prepared and characterized echogenic polymersomes, which are programmed torelease the encapsulated drugs rapidly when incubated with cytosolic concentrations of glutathione.These vesicles encapsulated air bubbles inside and efficiently reflected diagnostic-frequency ultrasound.Folate-targeted polymersomes showed an enhanced uptake by breast and pancreatic-cancer cells in amonolayer as well as in three-dimensional spheroid cultures. Polymersomes encapsulated with theanticancer drugs gemcitabine and doxorubicin showed significant cytotoxicity to these cells. Withfurther improvements, these vesicles hold the promise to serve as multifunctional nanocarriers, offeringa triggered release as well as diagnostic ultrasound imaging.

  • Kumar KN, Sarkar K 2015 “Effects of ambient hydrostatic pressure on the material properties of the encapsulation of an ultrasound contrast microbubble,” Journal of the Acoustical Society of America, 138, 624-634.

    Ultrasound contrast microbubbles experience widely varying ambient blood pressure in differentorgans, which can also change due to diseases. Pressure change can alter the material properties ofthe encapsulation of these microbubbles. Here the characteristic rheological parameters of contrastagent Definity are determined by varying the ambient pressure (in a physiologically relevant range0–200 mm Hg). Four different interfacial rheological models are used to characterize the microbub-bles. Effects of gas diffusion under excess ambient pressure are investigated in detail accountingfor size decrease of contrast microbubbles. Definity contrast agent show a change in their interfacialdilatational viscosity (3.6108Ns/m at 0 mm Hg to 4.45108Ns/m at 200 mm Hg) and inter-facial dilatational elasticity (0.86 N/m at 0 mm Hg to 1.06 N/m at 200 mm Hg) with ambient pres-sure increase. The increase results from material consolidation, similar to such enhancement inbulk properties under pressure. The model that accounts for enhancement in material propertieswith increasing ambient pressure matches with experimentally measured subharmonic response asa function of ambient pressure, while assuming constant material parameters does not.

  • Lang X, Porter T, Sarkar K 2015 “Interpreting attenuation at different excitation amplitudes to estimate strain-dependent interfacial rheological properties of lipid-coated monodisperse microbubbles,” Journal of the Acoustical Society of America, 138, 3994-4003.

    Broadband attenuation of ultrasound measured at different excitation pressures being differentraises a serious theoretical concern, because the underlying assumption of linear and independentpropagation of different frequency components nominally requires attenuation to be independent ofexcitation. Here, this issue is investigated by examining ultrasound attenuation through a monodis-perse lipid-coated microbubble suspension measured at four different acoustic excitation ampli-tudes. The attenuation data are used to determine interfacial rheological properties (surface tension,surface dilatational elasticity, and surface dilatational viscosity) of the encapsulation according tothree different models. Although different models result in similar rheological properties, attenua-tion measured at different excitation levels (4–110 kPa) leads to different values for them; the dila-tation elasticity (0.56 to 0.18 N/m) and viscosity (2.4108to 1.52108Ns/m) both decreasewith increasing pressure. Numerically simulating the scattered response, nonlinear energy transferbetween frequencies are shown to be negligible, thereby demonstrating the linearity in propagationand validating the attenuation analysis. There is a second concern to the characterization arisingfrom shell properties being dependent on excitation amplitude, which is not a proper constitutivevariable. It is resolved by arriving at a strain-dependent rheology for the encapsulation. The limita-tions of the underlying analysis are discussed.

  • Kumar KN, Sarkar K 2016 “Interfacial rheological properties of contrast microbubble Targestar P as a function of ambient pressure,” Ultrasound in Medicine and Biology, 42, 1010-1017.

    In this Technical Note, we determine the interfacial rheological parameters of the encapsulation of thecontrast agent Targestar P using ultrasound attenuation. The characteristic parameters are obtained according totwo interfacial rheological models. The properties—surface dilatational elasticity (0.09 ± 0.01 N/m) and surfacedilatational viscosity (8 ± 0.1E–9 N$s/m)—are found to be of similar magnitude for both models. Contrast micro-bubbles experience different ambient pressure in different organs. We also measure these parameters as functionsof ambient pressure using attenuation measured at different overpressures (0, 100 and 200 mm Hg). For each valueof ambient hydrostatic pressure, we determine the rheological properties, accounting for changes in the size dis-tribution caused by the pressure change. We discuss different models of size distribution change under overpres-sure: pure adiabatic compression or gas exchange with surrounding medium. The dilatational surface elasticityand viscosity are found to increase with increasing ambient pressure.

  • Kumar KN, Mallik S, Sarkar K, 2017 “Role of freeze-drying in the presence of mannitol on the echogenicity of echogenic liposomes,” Journal of the Acoustical Society of America, 142, 3670-3676.

    Echogenic liposomes (ELIPs) are an excellent candidate for ultrasound activated therapeutics andimaging. Although multiple experiments have established their echogenicity, the underlying mech-anism has remained unknown. However, freeze-drying in the presence of mannitol during ELIPpreparation has proved critical to ensuring echogenicity. Here, the role of this key component in thepreparation protocol was investigated by measuring scattering from freshly prepared freeze-driedaqueous solution of mannitol—and a number of other excipients commonly used in lyophiliza-tion—directly dispersed in water without any lipids in the experiment. Mannitol, meso-erythritol,glycine, and glucose that form a highly porous crystalline phase upon freeze-drying generated bub-bles resulting in strong echoes during their dissolution. On the other hand, sucrose, trehalose, andxylitol, which become glassy while freeze-dried, did not. Freeze-dried mannitol and other crystal-line substances, if thawed before being introduced into the scattering volume, did not produce echo-genicity, as they lost their crystallinity in the thawed state. The echogenicity disappeared in adegassed environment. Higher amounts of sugar in the original aqueous solution before freeze-drying resulted in higher echogenicity because of the stronger supersaturation and crystallinity. Thebubbles created by the freeze-dried mannitol in the ELIP formulation play a critical role in makingELIPs echogenic.

  • Xia L, Karandish F, Kumar KN, Froberg J, Kulkarni P, Gange KN, Choi Y, Mallik S, Sarkar K 2017 “Acoustic characterization of echogenic polymersomes prepared from amphiphilic block copolymers,” Ultrasound in Medicine and Biology, 44, 447-457.

    Polymersomes are a class of artificial vesicles prepared from amphiphilic polymers. Like lipid vesicles(liposomes), they too can encapsulate hydrophilic and hydrophobic drug molecules in the aqueous core and thehydrophobic bilayer respectively, but are more stable than liposomes. Although echogenic liposomes have beenwidely investigated for simultaneous ultrasound imaging and controlled drug delivery, the potential of thepolymersomes remains unexplored. We prepared two different echogenic polymersomes from the amphiphilic co-polymers polyethylene glycol–poly-DL-lactic acid (PEG-PLA) and polyethylene glycol–poly-L-lactic acid (PEG-PLLA), incorporating multiple freeze-dry cycles in the synthesis protocol to ensure their echogenicity. We investigatedacoustic behavior with potential applications in biomedical imaging. We characterized the polymeric vesicles acous-tically with three different excitation frequencies of 2.25, 5 and 10 MHz at 500 kPa. The polymersomes exhibitedstrong echogenicity at all three excitation frequencies (about 50- and 25-dB enhancements in fundamental andsubharmonic, respectively, at 5-MHz excitation from 20g/mL polymers in solution). Unlike echogenic lipo-somes, they emitted strong subharmonic responses. The scattering results indicated their potential as contrastagents, which was also confirmed by clinical ultrasound imaging.

  • Aliabouzar M, Kumar KN, Sarkar K, 2018 “Acoustic vaporization threshold of lipid coated perfluoropentane droplets,” Journal of the Acoustical Society of America, 143, 2001-2012.

    Phase shift droplets vaporizable by acoustic stimulation offer the advantages of producing micro-bubbles as contrast agentsin situas well as higher stability and the possibility of achieving smallersizes. Here, the acoustic droplet vaporization (ADV) threshold of a suspension of droplets with aperfluoropentane (PFP) core (diameter 400–3000 nm) is acoustically measured as a function of theexcitation frequency in a tubeless setup at room temperature. The changes in scattered responses—fundamental, sub-, and second harmonic—are investigated, a quantitative criterion is used to deter-mine the ADV phenomenon, and findings are discussed. The average threshold obtained using threedifferent scattered components increases with frequency—1.0560.28 MPa at 2.25 MHz,1.8960.57 MPa at 5 MHz, and 2.3460.014 MPa at 10 MHz. The scattered response from vapor-ized droplets was also found to qualitatively match with that from an independently prepared lipid-coated microbubble suspension in magnitude as well as trends above the determined ADV thresh-old value.

  • Kulkarni P, Haldar MK, Karandish F, Confeld M, Hossain R, Borowicz P, Gange KN, Xia L, Sarkar K, Mallik S 2018 “Tissue-penetrating, hypoxia-responsive echogenic polymersomes for drug delivery to solid tumors,” Chemistry A European Journal, 24, 12490-12494.

    Hypoxia in solid tumors facilitates the progres-sion of the disease, develops resistance to chemo and radiotherapy, and contributes to relapse. Due to the lack of tumor penetration, most of the reported drug carriers are unable to reach the hypoxic niches of the solid tumors. We have developed tissue-penetrating, hypoxia-responsive echogenic polymersomes to deliver anti cancer drugs to solid tumors. The polymersomes are composed of a hy-poxia-responsive azobenzene conjugated and a tissue penetrating peptide functionalized polylactic acid-polyethylene glycol polymer. The drug-encapsulated, hypoxia-responsive polymersomes substantially decreased the viability of pancreatic cancer cells in spheroidal cultures. Under normoxic conditions, polymersomes were echogenic at diagnostic ultrasound frequencies but lose the echogenicity under hypoxia. In vivo imaging studies with xenograft mouse model further confirmed the ability of the polymersomes to target, penetrate, and deliver the encapsulated contents in hypoxic pancreatic tumor tissues.

  • Karandish F, Haldar MK, Xia L, Gange KN, Feng L, You S, Choi Y, Sarkar K, Mallik S  2018 “Nucleus-targeted, echogenic polymersomes for delivering a cancer stemness inhibitor to pancreatic cancer cells,” Biomacromolecules, 19,4122-4132.

    Chemotherapeutic agents for treating cancers show considerable sideeffects, toxicity, and drug resistance. To mitigate the problems, we designed nucleus-targeted, echogenic, stimuli-responsive polymeric vesicles (polymersomes) to transport andsubsequently release the encapsulated anticancer drugs within the nuclei of pancreaticcancer cells. We synthesized an alkyne-dexamethasone derivative and conjugated it to N3−polyethylene glycol (PEG)−polylactic acid (PLA) copolymer employing the Cu2+catalyzed“Click”reaction. We prepared polymersomes from the dexamethasone−PEG−PLA conjugate along with a synthesized stimuli-responsive polymer PEG−S−S−PLA. Thedexamethasone group dilates the nuclear pore complexes and transports the vesicles to thenuclei. We designed the polymersomes to release the encapsulated drugs in the presence ofa high concentration of reducing agents in the nuclei of pancreatic cancer cells. Weobserved that the nucleus-targeted, stimuli-responsive polymersomes released 70% ofencapsulated contents in the nucleus-mimicking environment in 80 min. We encapsulatedthe cancer stemness inhibitor BBI608 in the vesicles and observed that the BBI608encapsulated polymersomes reduced the viability of the BxPC3 cells to 43% in three-dimensional spheroid cultures. Thepolymersomes were prepared following a special protocol so that they scatter ultrasound, allowing imaging by a medicalultrasound scanner. Therefore, these echogenic, targeted, stimuli-responsive, and drug-encapsulated polymersomes have thepotential for trackable, targeted carrier of chemotherapeutic drugs to cancer cell nuclei.

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Aliabouzar M, Kumar KN, Sarkar K, 2018 “Acoustic vaporization threshold of lipid coated perfluoropentane droplets,” Journal of the Acoustical Society of America, 143, 2001-2012.

    Phase shift droplets vaporizable by acoustic stimulation offer the advantages of producing micro-bubbles as contrast agentsin situas well as higher stability and the possibility of achieving smallersizes. Here, the acoustic droplet vaporization (ADV) threshold of a suspension of droplets with aperfluoropentane (PFP) core (diameter 400–3000 nm) is acoustically measured as a function of theexcitation frequency in a tubeless setup at room temperature. The changes in scattered responses—fundamental, sub-, and second harmonic—are investigated, a quantitative criterion is used to deter-mine the ADV phenomenon, and findings are discussed. The average threshold obtained using threedifferent scattered components increases with frequency—1.0560.28 MPa at 2.25 MHz,1.8960.57 MPa at 5 MHz, and 2.3460.014 MPa at 10 MHz. The scattered response from vapor-ized droplets was also found to qualitatively match with that from an independently prepared lipid-coated microbubble suspension in magnitude as well as trends above the determined ADV thresh-old value.

  • Karandish F, Haldar MK, Xia L, Gange KN, Feng L, You S, Choi Y, Sarkar K, Mallik S  2018 “Nucleus-targeted, echogenic polymersomes for delivering a cancer stemness inhibitor to pancreatic cancer cells,” Biomacromolecules, 19,4122-4132.

    Chemotherapeutic agents for treating cancers show considerable sideeffects, toxicity, and drug resistance. To mitigate the problems, we designed nucleus-targeted, echogenic, stimuli-responsive polymeric vesicles (polymersomes) to transport andsubsequently release the encapsulated anticancer drugs within the nuclei of pancreaticcancer cells. We synthesized an alkyne-dexamethasone derivative and conjugated it to N3−polyethylene glycol (PEG)−polylactic acid (PLA) copolymer employing the Cu2+catalyzed“Click”reaction. We prepared polymersomes from the dexamethasone−PEG−PLA conjugate along with a synthesized stimuli-responsive polymer PEG−S−S−PLA. Thedexamethasone group dilates the nuclear pore complexes and transports the vesicles to thenuclei. We designed the polymersomes to release the encapsulated drugs in the presence ofa high concentration of reducing agents in the nuclei of pancreatic cancer cells. Weobserved that the nucleus-targeted, stimuli-responsive polymersomes released 70% ofencapsulated contents in the nucleus-mimicking environment in 80 min. We encapsulatedthe cancer stemness inhibitor BBI608 in the vesicles and observed that the BBI608encapsulated polymersomes reduced the viability of the BxPC3 cells to 43% in three-dimensional spheroid cultures. Thepolymersomes were prepared following a special protocol so that they scatter ultrasound, allowing imaging by a medicalultrasound scanner. Therefore, these echogenic, targeted, stimuli-responsive, and drug-encapsulated polymersomes have thepotential for trackable, targeted carrier of chemotherapeutic drugs to cancer cell nuclei.

  • Kulkarni P, Haldar MK, Karandish F, Confeld M, Hossain R, Borowicz P, Gange KN, Xia L, Sarkar K, Mallik S 2018 “Tissue-penetrating, hypoxia-responsive echogenic polymersomes for drug delivery to solid tumors,” Chemistry A European Journal, 24, 12490-12494.

    Hypoxia in solid tumors facilitates the progres-sion of the disease, develops resistance to chemo and radiotherapy, and contributes to relapse. Due to the lack of tumor penetration, most of the reported drug carriers are unable to reach the hypoxic niches of the solid tumors. We have developed tissue-penetrating, hypoxia-responsive echogenic polymersomes to deliver anti cancer drugs to solid tumors. The polymersomes are composed of a hy-poxia-responsive azobenzene conjugated and a tissue penetrating peptide functionalized polylactic acid-polyethylene glycol polymer. The drug-encapsulated, hypoxia-responsive polymersomes substantially decreased the viability of pancreatic cancer cells in spheroidal cultures. Under normoxic conditions, polymersomes were echogenic at diagnostic ultrasound frequencies but lose the echogenicity under hypoxia. In vivo imaging studies with xenograft mouse model further confirmed the ability of the polymersomes to target, penetrate, and deliver the encapsulated contents in hypoxic pancreatic tumor tissues.

  • Kulkarni P, Haldar MK, Karandish F, Confeld M, Hossain R, Borowicz P, Gange KN, Xia L, Sarkar K, Mallik S 2018 “Tissue-penetrating, hypoxia-responsive echogenic polymersomes for drug delivery to solid tumors,” Chemistry A European Journal, 24, 12490-12494.

    Hypoxia in solid tumors facilitates the progres-sion of the disease, develops resistance to chemo and radiotherapy, and contributes to relapse. Due to the lack of tumor penetration, most of the reported drug carriers are unable to reach the hypoxic niches of the solid tumors. We have developed tissue-penetrating, hypoxia-responsive echogenic polymersomes to deliver anti cancer drugs to solid tumors. The polymersomes are composed of a hy-poxia-responsive azobenzene conjugated and a tissue penetrating peptide functionalized polylactic acid-polyethylene glycol polymer. The drug-encapsulated, hypoxia-responsive polymersomes substantially decreased the viability of pancreatic cancer cells in spheroidal cultures. Under normoxic conditions, polymersomes were echogenic at diagnostic ultrasound frequencies but lose the echogenicity under hypoxia. In vivo imaging studies with xenograft mouse model further confirmed the ability of the polymersomes to target, penetrate, and deliver the encapsulated contents in hypoxic pancreatic tumor tissues.

  • Kumar KN, Mallik S, Sarkar K, 2017 “Role of freeze-drying in the presence of mannitol on the echogenicity of echogenic liposomes,” Journal of the Acoustical Society of America, 142, 3670-3676.

    Echogenic liposomes (ELIPs) are an excellent candidate for ultrasound activated therapeutics andimaging. Although multiple experiments have established their echogenicity, the underlying mech-anism has remained unknown. However, freeze-drying in the presence of mannitol during ELIPpreparation has proved critical to ensuring echogenicity. Here, the role of this key component in thepreparation protocol was investigated by measuring scattering from freshly prepared freeze-driedaqueous solution of mannitol—and a number of other excipients commonly used in lyophiliza-tion—directly dispersed in water without any lipids in the experiment. Mannitol, meso-erythritol,glycine, and glucose that form a highly porous crystalline phase upon freeze-drying generated bub-bles resulting in strong echoes during their dissolution. On the other hand, sucrose, trehalose, andxylitol, which become glassy while freeze-dried, did not. Freeze-dried mannitol and other crystal-line substances, if thawed before being introduced into the scattering volume, did not produce echo-genicity, as they lost their crystallinity in the thawed state. The echogenicity disappeared in adegassed environment. Higher amounts of sugar in the original aqueous solution before freeze-drying resulted in higher echogenicity because of the stronger supersaturation and crystallinity. Thebubbles created by the freeze-dried mannitol in the ELIP formulation play a critical role in makingELIPs echogenic.

  • Xia L, Karandish F, Kumar KN, Froberg J, Kulkarni P, Gange KN, Choi Y, Mallik S, Sarkar K 2017 “Acoustic characterization of echogenic polymersomes prepared from amphiphilic block copolymers,” Ultrasound in Medicine and Biology, 44, 447-457.

    Polymersomes are a class of artificial vesicles prepared from amphiphilic polymers. Like lipid vesicles(liposomes), they too can encapsulate hydrophilic and hydrophobic drug molecules in the aqueous core and thehydrophobic bilayer respectively, but are more stable than liposomes. Although echogenic liposomes have beenwidely investigated for simultaneous ultrasound imaging and controlled drug delivery, the potential of thepolymersomes remains unexplored. We prepared two different echogenic polymersomes from the amphiphilic co-polymers polyethylene glycol–poly-DL-lactic acid (PEG-PLA) and polyethylene glycol–poly-L-lactic acid (PEG-PLLA), incorporating multiple freeze-dry cycles in the synthesis protocol to ensure their echogenicity. We investigatedacoustic behavior with potential applications in biomedical imaging. We characterized the polymeric vesicles acous-tically with three different excitation frequencies of 2.25, 5 and 10 MHz at 500 kPa. The polymersomes exhibitedstrong echogenicity at all three excitation frequencies (about 50- and 25-dB enhancements in fundamental andsubharmonic, respectively, at 5-MHz excitation from 20g/mL polymers in solution). Unlike echogenic lipo-somes, they emitted strong subharmonic responses. The scattering results indicated their potential as contrastagents, which was also confirmed by clinical ultrasound imaging.

  • Kumar KN, Sarkar K 2016 “Interfacial rheological properties of contrast microbubble Targestar P as a function of ambient pressure,” Ultrasound in Medicine and Biology, 42, 1010-1017.

    In this Technical Note, we determine the interfacial rheological parameters of the encapsulation of thecontrast agent Targestar P using ultrasound attenuation. The characteristic parameters are obtained according totwo interfacial rheological models. The properties—surface dilatational elasticity (0.09 ± 0.01 N/m) and surfacedilatational viscosity (8 ± 0.1E–9 N$s/m)—are found to be of similar magnitude for both models. Contrast micro-bubbles experience different ambient pressure in different organs. We also measure these parameters as functionsof ambient pressure using attenuation measured at different overpressures (0, 100 and 200 mm Hg). For each valueof ambient hydrostatic pressure, we determine the rheological properties, accounting for changes in the size dis-tribution caused by the pressure change. We discuss different models of size distribution change under overpres-sure: pure adiabatic compression or gas exchange with surrounding medium. The dilatational surface elasticityand viscosity are found to increase with increasing ambient pressure.

  • Kumar KN, Sarkar K 2015 “Effects of ambient hydrostatic pressure on the material properties of the encapsulation of an ultrasound contrast microbubble,” Journal of the Acoustical Society of America, 138, 624-634.

    Ultrasound contrast microbubbles experience widely varying ambient blood pressure in differentorgans, which can also change due to diseases. Pressure change can alter the material properties ofthe encapsulation of these microbubbles. Here the characteristic rheological parameters of contrastagent Definity are determined by varying the ambient pressure (in a physiologically relevant range0–200 mm Hg). Four different interfacial rheological models are used to characterize the microbub-bles. Effects of gas diffusion under excess ambient pressure are investigated in detail accountingfor size decrease of contrast microbubbles. Definity contrast agent show a change in their interfacialdilatational viscosity (3.6108Ns/m at 0 mm Hg to 4.45108Ns/m at 200 mm Hg) and inter-facial dilatational elasticity (0.86 N/m at 0 mm Hg to 1.06 N/m at 200 mm Hg) with ambient pres-sure increase. The increase results from material consolidation, similar to such enhancement inbulk properties under pressure. The model that accounts for enhancement in material propertieswith increasing ambient pressure matches with experimentally measured subharmonic response asa function of ambient pressure, while assuming constant material parameters does not.

  • Kumar KN, Sarkar K 2016 “Interfacial rheological properties of contrast microbubble Targestar P as a function of ambient pressure,” Ultrasound in Medicine and Biology, 42, 1010-1017.

    In this Technical Note, we determine the interfacial rheological parameters of the encapsulation of thecontrast agent Targestar P using ultrasound attenuation. The characteristic parameters are obtained according totwo interfacial rheological models. The properties—surface dilatational elasticity (0.09 ± 0.01 N/m) and surfacedilatational viscosity (8 ± 0.1E–9 N$s/m)—are found to be of similar magnitude for both models. Contrast micro-bubbles experience different ambient pressure in different organs. We also measure these parameters as functionsof ambient pressure using attenuation measured at different overpressures (0, 100 and 200 mm Hg). For each valueof ambient hydrostatic pressure, we determine the rheological properties, accounting for changes in the size dis-tribution caused by the pressure change. We discuss different models of size distribution change under overpres-sure: pure adiabatic compression or gas exchange with surrounding medium. The dilatational surface elasticityand viscosity are found to increase with increasing ambient pressure.

  • Kumar KN, Sarkar K 2015 “Effects of ambient hydrostatic pressure on the material properties of the encapsulation of an ultrasound contrast microbubble,” Journal of the Acoustical Society of America, 138, 624-634.

    Ultrasound contrast microbubbles experience widely varying ambient blood pressure in differentorgans, which can also change due to diseases. Pressure change can alter the material properties ofthe encapsulation of these microbubbles. Here the characteristic rheological parameters of contrastagent Definity are determined by varying the ambient pressure (in a physiologically relevant range0–200 mm Hg). Four different interfacial rheological models are used to characterize the microbub-bles. Effects of gas diffusion under excess ambient pressure are investigated in detail accountingfor size decrease of contrast microbubbles. Definity contrast agent show a change in their interfacialdilatational viscosity (3.6108Ns/m at 0 mm Hg to 4.45108Ns/m at 200 mm Hg) and inter-facial dilatational elasticity (0.86 N/m at 0 mm Hg to 1.06 N/m at 200 mm Hg) with ambient pres-sure increase. The increase results from material consolidation, similar to such enhancement inbulk properties under pressure. The model that accounts for enhancement in material propertieswith increasing ambient pressure matches with experimentally measured subharmonic response asa function of ambient pressure, while assuming constant material parameters does not.

  • Kumar KN, Sarkar K 2016 “Interfacial rheological properties of contrast microbubble Targestar P as a function of ambient pressure,” Ultrasound in Medicine and Biology, 42, 1010-1017.

    In this Technical Note, we determine the interfacial rheological parameters of the encapsulation of thecontrast agent Targestar P using ultrasound attenuation. The characteristic parameters are obtained according totwo interfacial rheological models. The properties—surface dilatational elasticity (0.09 ± 0.01 N/m) and surfacedilatational viscosity (8 ± 0.1E–9 N$s/m)—are found to be of similar magnitude for both models. Contrast micro-bubbles experience different ambient pressure in different organs. We also measure these parameters as functionsof ambient pressure using attenuation measured at different overpressures (0, 100 and 200 mm Hg). For each valueof ambient hydrostatic pressure, we determine the rheological properties, accounting for changes in the size dis-tribution caused by the pressure change. We discuss different models of size distribution change under overpres-sure: pure adiabatic compression or gas exchange with surrounding medium. The dilatational surface elasticityand viscosity are found to increase with increasing ambient pressure.

  • Kumar KN, Sarkar K 2015 “Effects of ambient hydrostatic pressure on the material properties of the encapsulation of an ultrasound contrast microbubble,” Journal of the Acoustical Society of America, 138, 624-634.

    Ultrasound contrast microbubbles experience widely varying ambient blood pressure in differentorgans, which can also change due to diseases. Pressure change can alter the material properties ofthe encapsulation of these microbubbles. Here the characteristic rheological parameters of contrastagent Definity are determined by varying the ambient pressure (in a physiologically relevant range0–200 mm Hg). Four different interfacial rheological models are used to characterize the microbub-bles. Effects of gas diffusion under excess ambient pressure are investigated in detail accountingfor size decrease of contrast microbubbles. Definity contrast agent show a change in their interfacialdilatational viscosity (3.6108Ns/m at 0 mm Hg to 4.45108Ns/m at 200 mm Hg) and inter-facial dilatational elasticity (0.86 N/m at 0 mm Hg to 1.06 N/m at 200 mm Hg) with ambient pres-sure increase. The increase results from material consolidation, similar to such enhancement inbulk properties under pressure. The model that accounts for enhancement in material propertieswith increasing ambient pressure matches with experimentally measured subharmonic response asa function of ambient pressure, while assuming constant material parameters does not.

  • Kumar KN, Sarkar K 2015 “Effects of ambient hydrostatic pressure on the material properties of the encapsulation of an ultrasound contrast microbubble,” Journal of the Acoustical Society of America, 138, 624-634.

    Ultrasound contrast microbubbles experience widely varying ambient blood pressure in differentorgans, which can also change due to diseases. Pressure change can alter the material properties ofthe encapsulation of these microbubbles. Here the characteristic rheological parameters of contrastagent Definity are determined by varying the ambient pressure (in a physiologically relevant range0–200 mm Hg). Four different interfacial rheological models are used to characterize the microbub-bles. Effects of gas diffusion under excess ambient pressure are investigated in detail accountingfor size decrease of contrast microbubbles. Definity contrast agent show a change in their interfacialdilatational viscosity (3.6108Ns/m at 0 mm Hg to 4.45108Ns/m at 200 mm Hg) and inter-facial dilatational elasticity (0.86 N/m at 0 mm Hg to 1.06 N/m at 200 mm Hg) with ambient pres-sure increase. The increase results from material consolidation, similar to such enhancement inbulk properties under pressure. The model that accounts for enhancement in material propertieswith increasing ambient pressure matches with experimentally measured subharmonic response asa function of ambient pressure, while assuming constant material parameters does not.

  • Lang X, Porter T, Sarkar K 2015 “Interpreting attenuation at different excitation amplitudes to estimate strain-dependent interfacial rheological properties of lipid-coated monodisperse microbubbles,” Journal of the Acoustical Society of America, 138, 3994-4003.

    Broadband attenuation of ultrasound measured at different excitation pressures being differentraises a serious theoretical concern, because the underlying assumption of linear and independentpropagation of different frequency components nominally requires attenuation to be independent ofexcitation. Here, this issue is investigated by examining ultrasound attenuation through a monodis-perse lipid-coated microbubble suspension measured at four different acoustic excitation ampli-tudes. The attenuation data are used to determine interfacial rheological properties (surface tension,surface dilatational elasticity, and surface dilatational viscosity) of the encapsulation according tothree different models. Although different models result in similar rheological properties, attenua-tion measured at different excitation levels (4–110 kPa) leads to different values for them; the dila-tation elasticity (0.56 to 0.18 N/m) and viscosity (2.4108to 1.52108Ns/m) both decreasewith increasing pressure. Numerically simulating the scattered response, nonlinear energy transferbetween frequencies are shown to be negligible, thereby demonstrating the linearity in propagationand validating the attenuation analysis. There is a second concern to the characterization arisingfrom shell properties being dependent on excitation amplitude, which is not a proper constitutivevariable. It is resolved by arriving at a strain-dependent rheology for the encapsulation. The limita-tions of the underlying analysis are discussed.

  • Kulkarni P, Haldar MK, Karandish F, Confeld M, Hossain R, Borowicz P, Gange KN, Xia L, Sarkar K, Mallik S 2018 “Tissue-penetrating, hypoxia-responsive echogenic polymersomes for drug delivery to solid tumors,” Chemistry A European Journal, 24, 12490-12494.

    Hypoxia in solid tumors facilitates the progres-sion of the disease, develops resistance to chemo and radiotherapy, and contributes to relapse. Due to the lack of tumor penetration, most of the reported drug carriers are unable to reach the hypoxic niches of the solid tumors. We have developed tissue-penetrating, hypoxia-responsive echogenic polymersomes to deliver anti cancer drugs to solid tumors. The polymersomes are composed of a hy-poxia-responsive azobenzene conjugated and a tissue penetrating peptide functionalized polylactic acid-polyethylene glycol polymer. The drug-encapsulated, hypoxia-responsive polymersomes substantially decreased the viability of pancreatic cancer cells in spheroidal cultures. Under normoxic conditions, polymersomes were echogenic at diagnostic ultrasound frequencies but lose the echogenicity under hypoxia. In vivo imaging studies with xenograft mouse model further confirmed the ability of the polymersomes to target, penetrate, and deliver the encapsulated contents in hypoxic pancreatic tumor tissues.

  • Nahire R, Halder M, Paul S, Margoum A, Ambre AH, Katti KS, Gange KN, Srivastava D K, Sarkar K, Mallik S 2014 “pH-Triggered Echogenicity and Contents Release from Liposomes,” Molecular Pharamaceutics, 11, 4059-4068.

    Liposomes are representative lipid nanoparticles widelyused for delivering anticancer drugs, DNA fragments, or siRNA to cancercells. Upon targeting, various internal and external triggers have been usedto increase the rate for contents release from the liposomes. Among theinternal triggers, decreased pH within the cellular lysosomes has beensuccessfully used to enhance the rate for releasing contents. However,imparting pH sensitivity to liposomes requires the synthesis of specializedlipids with structures that are substantially modified at a reduced pH.Herein, we report an alternative strategy to render liposomes pH sensitiveby encapsulating a precursor which generates gas bubblesin situinresponse to acidic pH. The disturbance created by the escaping gasbubbles leads to the rapid release of the encapsulated contents from theliposomes. Atomic force microscopic studies indicate that the liposomalstructure is destroyed at a reduced pH. The gas bubbles also render theliposomes echogenic, allowing ultrasound imaging. To demonstrate the applicability of this strategy, we have successfully targeteddoxorubicin-encapsulated liposomes to the pancreatic ductal carcinoma cells that overexpress the folate receptor on the surface.In response to the decreased pH in the lysosomes, the encapsulated anticancer drug is efficiently released. Contents releasedfrom these liposomes are further enhanced by the application of continuous wave ultrasound (1 MHz), resulting in substantiallyreduced viability for the pancreatic cancer cells (14%).

  • Nahire R, Hossain R, Patel R, Paul S, Ambre AH, Meghnani V, Layek B, Katti KS, Gange KN, Leclarc E, Srivastava D K, Sarkar K, Mallik S 2014 “Multifunctional polymersomes for cytosolic delivery of gemcitabine and doxorubicin to cancer cells,” Biomaterials, 35, 6482-6497.

    Although liposomes are widely used as carriers of drugs and imaging agents, they suffer from a lack ofstability and the slow release of the encapsulated contents at the targeted site. Polymersomes (vesicles ofamphiphilic polymers) are considerably more stable compared to liposomes; however, they alsodemonstrate a slow release for the encapsulated contents, limiting their efficacy as a drug-delivery tool.As a solution, we prepared and characterized echogenic polymersomes, which are programmed torelease the encapsulated drugs rapidly when incubated with cytosolic concentrations of glutathione.These vesicles encapsulated air bubbles inside and efficiently reflected diagnostic-frequency ultrasound.Folate-targeted polymersomes showed an enhanced uptake by breast and pancreatic-cancer cells in amonolayer as well as in three-dimensional spheroid cultures. Polymersomes encapsulated with theanticancer drugs gemcitabine and doxorubicin showed significant cytotoxicity to these cells. Withfurther improvements, these vesicles hold the promise to serve as multifunctional nanocarriers, offeringa triggered release as well as diagnostic ultrasound imaging.

  • Paul S, Nahire R, Mallik S, Sarkar K 2014 “Encapsulated microbubbles and echogenic liposomes for contrast ultrasound imaging and targeted drug delivery,” Computational Mechanics, 53,413-435.

    Micron- to nanometer-sized ultrasound agents,like encapsulated microbubbles and echogenic liposomes,are being developed for diagnostic imaging and ultra-sound mediated drug/gene delivery. This review providesan overview of the current state of the art of the mathe-matical models of the acoustic behavior of ultrasound con-trast microbubbles. We also present a review of the in vitroexperimental characterization of the acoustic properties ofmicrobubble based contrast agents undertaken in our lab-oratory. The hierarchical two-pronged approach of model-ing contrast agents we developed is demonstrated for a lipidcoated (SonazoidTM)and a polymer shelled (polyD-L-lactic acid) contrast microbubbles. The acoustic and drugrelease properties of the newly developed echogenic lipo-somes are discussed for their use as simultaneous imagingand drug/gene delivery agents. Although echogenicity is con-clusively demonstrated in experiments, its physical mecha-nisms remain uncertain. Addressing questions raised herewill accelerate further development and eventual clinicalapproval of these novel technologies.

  • Nahire R, Halder M, Paul S, Margoum A, Ambre AH, Katti KS, Gange KN, Srivastava D K, Sarkar K, Mallik S 2013 “Polymer Coated Echogenic Lipid Nanoparticles with dual release triggers,” Biomacromolecules, 14, 841-853.

    Although lipid nanoparticles are promising drugdelivery vehicles, passive release of encapsulated contents atthe target site is often slow. Herein, we report contents releasefrom targeted, polymer-coated, echogenic lipid nanoparticles inthe cell cytoplasm by redox trigger and simultaneouslyenhanced by diagnostic frequency ultrasound. The lipidnanoparticles were polymerized on the external leaflet usinga disulfide cross-linker. In the presence of cytosolicconcentrations of glutathione, the lipid nanoparticles released76% of encapsulated contents. Plasma concentrations ofglutathione failed to releasethe encapsulated contents.Application of 3 MHz ultrasound for 2 min simultaneouslywith the reducing agent enhanced the release to 96%. Folicacid conjugated, doxorubicin-loaded nanoparticles showed enhanced uptake and higher cytotoxicity in cancer cells overexpressingthe folate receptor (compared to the control). With further developments, these lipid nanoparticles have the potential to be usedas multimodal nanocarriers for simultaneous targeted drug delivery and ultrasound imaging.

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

  • Aliabouzar M, Kumar KN, Sarkar K, 2018 “Acoustic vaporization threshold of lipid coated perfluoropentane droplets,” Journal of the Acoustical Society of America, 143, 2001-2012.

    Phase shift droplets vaporizable by acoustic stimulation offer the advantages of producing micro-bubbles as contrast agentsin situas well as higher stability and the possibility of achieving smallersizes. Here, the acoustic droplet vaporization (ADV) threshold of a suspension of droplets with aperfluoropentane (PFP) core (diameter 400–3000 nm) is acoustically measured as a function of theexcitation frequency in a tubeless setup at room temperature. The changes in scattered responses—fundamental, sub-, and second harmonic—are investigated, a quantitative criterion is used to deter-mine the ADV phenomenon, and findings are discussed. The average threshold obtained using threedifferent scattered components increases with frequency—1.0560.28 MPa at 2.25 MHz,1.8960.57 MPa at 5 MHz, and 2.3460.014 MPa at 10 MHz. The scattered response from vapor-ized droplets was also found to qualitatively match with that from an independently prepared lipid-coated microbubble suspension in magnitude as well as trends above the determined ADV thresh-old value.

  • Kulkarni P, Haldar MK, Karandish F, Confeld M, Hossain R, Borowicz P, Gange KN, Xia L, Sarkar K, Mallik S 2018 “Tissue-penetrating, hypoxia-responsive echogenic polymersomes for drug delivery to solid tumors,” Chemistry A European Journal, 24, 12490-12494.

    Hypoxia in solid tumors facilitates the progres-sion of the disease, develops resistance to chemo and radiotherapy, and contributes to relapse. Due to the lack of tumor penetration, most of the reported drug carriers are unable to reach the hypoxic niches of the solid tumors. We have developed tissue-penetrating, hypoxia-responsive echogenic polymersomes to deliver anti cancer drugs to solid tumors. The polymersomes are composed of a hy-poxia-responsive azobenzene conjugated and a tissue penetrating peptide functionalized polylactic acid-polyethylene glycol polymer. The drug-encapsulated, hypoxia-responsive polymersomes substantially decreased the viability of pancreatic cancer cells in spheroidal cultures. Under normoxic conditions, polymersomes were echogenic at diagnostic ultrasound frequencies but lose the echogenicity under hypoxia. In vivo imaging studies with xenograft mouse model further confirmed the ability of the polymersomes to target, penetrate, and deliver the encapsulated contents in hypoxic pancreatic tumor tissues.

  • Karandish F, Haldar MK, Xia L, Gange KN, Feng L, You S, Choi Y, Sarkar K, Mallik S  2018 “Nucleus-targeted, echogenic polymersomes for delivering a cancer stemness inhibitor to pancreatic cancer cells,” Biomacromolecules, 19,4122-4132.

    Chemotherapeutic agents for treating cancers show considerable sideeffects, toxicity, and drug resistance. To mitigate the problems, we designed nucleus-targeted, echogenic, stimuli-responsive polymeric vesicles (polymersomes) to transport andsubsequently release the encapsulated anticancer drugs within the nuclei of pancreaticcancer cells. We synthesized an alkyne-dexamethasone derivative and conjugated it to N3−polyethylene glycol (PEG)−polylactic acid (PLA) copolymer employing the Cu2+catalyzed“Click”reaction. We prepared polymersomes from the dexamethasone−PEG−PLA conjugate along with a synthesized stimuli-responsive polymer PEG−S−S−PLA. Thedexamethasone group dilates the nuclear pore complexes and transports the vesicles to thenuclei. We designed the polymersomes to release the encapsulated drugs in the presence ofa high concentration of reducing agents in the nuclei of pancreatic cancer cells. Weobserved that the nucleus-targeted, stimuli-responsive polymersomes released 70% ofencapsulated contents in the nucleus-mimicking environment in 80 min. We encapsulatedthe cancer stemness inhibitor BBI608 in the vesicles and observed that the BBI608encapsulated polymersomes reduced the viability of the BxPC3 cells to 43% in three-dimensional spheroid cultures. Thepolymersomes were prepared following a special protocol so that they scatter ultrasound, allowing imaging by a medicalultrasound scanner. Therefore, these echogenic, targeted, stimuli-responsive, and drug-encapsulated polymersomes have thepotential for trackable, targeted carrier of chemotherapeutic drugs to cancer cell nuclei.

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Aliabouzar M, Kumar KN, Sarkar K, 2018 “Acoustic vaporization threshold of lipid coated perfluoropentane droplets,” Journal of the Acoustical Society of America, 143, 2001-2012.

    Phase shift droplets vaporizable by acoustic stimulation offer the advantages of producing micro-bubbles as contrast agentsin situas well as higher stability and the possibility of achieving smallersizes. Here, the acoustic droplet vaporization (ADV) threshold of a suspension of droplets with aperfluoropentane (PFP) core (diameter 400–3000 nm) is acoustically measured as a function of theexcitation frequency in a tubeless setup at room temperature. The changes in scattered responses—fundamental, sub-, and second harmonic—are investigated, a quantitative criterion is used to deter-mine the ADV phenomenon, and findings are discussed. The average threshold obtained using threedifferent scattered components increases with frequency—1.0560.28 MPa at 2.25 MHz,1.8960.57 MPa at 5 MHz, and 2.3460.014 MPa at 10 MHz. The scattered response from vapor-ized droplets was also found to qualitatively match with that from an independently prepared lipid-coated microbubble suspension in magnitude as well as trends above the determined ADV thresh-old value.

  • Kulkarni P, Haldar MK, Karandish F, Confeld M, Hossain R, Borowicz P, Gange KN, Xia L, Sarkar K, Mallik S 2018 “Tissue-penetrating, hypoxia-responsive echogenic polymersomes for drug delivery to solid tumors,” Chemistry A European Journal, 24, 12490-12494.

    Hypoxia in solid tumors facilitates the progres-sion of the disease, develops resistance to chemo and radiotherapy, and contributes to relapse. Due to the lack of tumor penetration, most of the reported drug carriers are unable to reach the hypoxic niches of the solid tumors. We have developed tissue-penetrating, hypoxia-responsive echogenic polymersomes to deliver anti cancer drugs to solid tumors. The polymersomes are composed of a hy-poxia-responsive azobenzene conjugated and a tissue penetrating peptide functionalized polylactic acid-polyethylene glycol polymer. The drug-encapsulated, hypoxia-responsive polymersomes substantially decreased the viability of pancreatic cancer cells in spheroidal cultures. Under normoxic conditions, polymersomes were echogenic at diagnostic ultrasound frequencies but lose the echogenicity under hypoxia. In vivo imaging studies with xenograft mouse model further confirmed the ability of the polymersomes to target, penetrate, and deliver the encapsulated contents in hypoxic pancreatic tumor tissues.

  • Karandish F, Haldar MK, Xia L, Gange KN, Feng L, You S, Choi Y, Sarkar K, Mallik S  2018 “Nucleus-targeted, echogenic polymersomes for delivering a cancer stemness inhibitor to pancreatic cancer cells,” Biomacromolecules, 19,4122-4132.

    Chemotherapeutic agents for treating cancers show considerable sideeffects, toxicity, and drug resistance. To mitigate the problems, we designed nucleus-targeted, echogenic, stimuli-responsive polymeric vesicles (polymersomes) to transport andsubsequently release the encapsulated anticancer drugs within the nuclei of pancreaticcancer cells. We synthesized an alkyne-dexamethasone derivative and conjugated it to N3−polyethylene glycol (PEG)−polylactic acid (PLA) copolymer employing the Cu2+catalyzed“Click”reaction. We prepared polymersomes from the dexamethasone−PEG−PLA conjugate along with a synthesized stimuli-responsive polymer PEG−S−S−PLA. Thedexamethasone group dilates the nuclear pore complexes and transports the vesicles to thenuclei. We designed the polymersomes to release the encapsulated drugs in the presence ofa high concentration of reducing agents in the nuclei of pancreatic cancer cells. Weobserved that the nucleus-targeted, stimuli-responsive polymersomes released 70% ofencapsulated contents in the nucleus-mimicking environment in 80 min. We encapsulatedthe cancer stemness inhibitor BBI608 in the vesicles and observed that the BBI608encapsulated polymersomes reduced the viability of the BxPC3 cells to 43% in three-dimensional spheroid cultures. Thepolymersomes were prepared following a special protocol so that they scatter ultrasound, allowing imaging by a medicalultrasound scanner. Therefore, these echogenic, targeted, stimuli-responsive, and drug-encapsulated polymersomes have thepotential for trackable, targeted carrier of chemotherapeutic drugs to cancer cell nuclei.

  • Kumar KN, Mallik S, Sarkar K, 2017 “Role of freeze-drying in the presence of mannitol on the echogenicity of echogenic liposomes,” Journal of the Acoustical Society of America, 142, 3670-3676.

    Echogenic liposomes (ELIPs) are an excellent candidate for ultrasound activated therapeutics andimaging. Although multiple experiments have established their echogenicity, the underlying mech-anism has remained unknown. However, freeze-drying in the presence of mannitol during ELIPpreparation has proved critical to ensuring echogenicity. Here, the role of this key component in thepreparation protocol was investigated by measuring scattering from freshly prepared freeze-driedaqueous solution of mannitol—and a number of other excipients commonly used in lyophiliza-tion—directly dispersed in water without any lipids in the experiment. Mannitol, meso-erythritol,glycine, and glucose that form a highly porous crystalline phase upon freeze-drying generated bub-bles resulting in strong echoes during their dissolution. On the other hand, sucrose, trehalose, andxylitol, which become glassy while freeze-dried, did not. Freeze-dried mannitol and other crystal-line substances, if thawed before being introduced into the scattering volume, did not produce echo-genicity, as they lost their crystallinity in the thawed state. The echogenicity disappeared in adegassed environment. Higher amounts of sugar in the original aqueous solution before freeze-drying resulted in higher echogenicity because of the stronger supersaturation and crystallinity. Thebubbles created by the freeze-dried mannitol in the ELIP formulation play a critical role in makingELIPs echogenic.

  • Xia L, Karandish F, Kumar KN, Froberg J, Kulkarni P, Gange KN, Choi Y, Mallik S, Sarkar K 2017 “Acoustic characterization of echogenic polymersomes prepared from amphiphilic block copolymers,” Ultrasound in Medicine and Biology, 44, 447-457.

    Polymersomes are a class of artificial vesicles prepared from amphiphilic polymers. Like lipid vesicles(liposomes), they too can encapsulate hydrophilic and hydrophobic drug molecules in the aqueous core and thehydrophobic bilayer respectively, but are more stable than liposomes. Although echogenic liposomes have beenwidely investigated for simultaneous ultrasound imaging and controlled drug delivery, the potential of thepolymersomes remains unexplored. We prepared two different echogenic polymersomes from the amphiphilic co-polymers polyethylene glycol–poly-DL-lactic acid (PEG-PLA) and polyethylene glycol–poly-L-lactic acid (PEG-PLLA), incorporating multiple freeze-dry cycles in the synthesis protocol to ensure their echogenicity. We investigatedacoustic behavior with potential applications in biomedical imaging. We characterized the polymeric vesicles acous-tically with three different excitation frequencies of 2.25, 5 and 10 MHz at 500 kPa. The polymersomes exhibitedstrong echogenicity at all three excitation frequencies (about 50- and 25-dB enhancements in fundamental andsubharmonic, respectively, at 5-MHz excitation from 20g/mL polymers in solution). Unlike echogenic lipo-somes, they emitted strong subharmonic responses. The scattering results indicated their potential as contrastagents, which was also confirmed by clinical ultrasound imaging.

  • Kumar KN, Sarkar K 2016 “Interfacial rheological properties of contrast microbubble Targestar P as a function of ambient pressure,” Ultrasound in Medicine and Biology, 42, 1010-1017.

    In this Technical Note, we determine the interfacial rheological parameters of the encapsulation of thecontrast agent Targestar P using ultrasound attenuation. The characteristic parameters are obtained according totwo interfacial rheological models. The properties—surface dilatational elasticity (0.09 ± 0.01 N/m) and surfacedilatational viscosity (8 ± 0.1E–9 N$s/m)—are found to be of similar magnitude for both models. Contrast micro-bubbles experience different ambient pressure in different organs. We also measure these parameters as functionsof ambient pressure using attenuation measured at different overpressures (0, 100 and 200 mm Hg). For each valueof ambient hydrostatic pressure, we determine the rheological properties, accounting for changes in the size dis-tribution caused by the pressure change. We discuss different models of size distribution change under overpres-sure: pure adiabatic compression or gas exchange with surrounding medium. The dilatational surface elasticityand viscosity are found to increase with increasing ambient pressure.

  • Kumar KN, Sarkar K 2015 “Effects of ambient hydrostatic pressure on the material properties of the encapsulation of an ultrasound contrast microbubble,” Journal of the Acoustical Society of America, 138, 624-634.

    Ultrasound contrast microbubbles experience widely varying ambient blood pressure in differentorgans, which can also change due to diseases. Pressure change can alter the material properties ofthe encapsulation of these microbubbles. Here the characteristic rheological parameters of contrastagent Definity are determined by varying the ambient pressure (in a physiologically relevant range0–200 mm Hg). Four different interfacial rheological models are used to characterize the microbub-bles. Effects of gas diffusion under excess ambient pressure are investigated in detail accountingfor size decrease of contrast microbubbles. Definity contrast agent show a change in their interfacialdilatational viscosity (3.6108Ns/m at 0 mm Hg to 4.45108Ns/m at 200 mm Hg) and inter-facial dilatational elasticity (0.86 N/m at 0 mm Hg to 1.06 N/m at 200 mm Hg) with ambient pres-sure increase. The increase results from material consolidation, similar to such enhancement inbulk properties under pressure. The model that accounts for enhancement in material propertieswith increasing ambient pressure matches with experimentally measured subharmonic response asa function of ambient pressure, while assuming constant material parameters does not.

  • Lang X, Porter T, Sarkar K 2015 “Interpreting attenuation at different excitation amplitudes to estimate strain-dependent interfacial rheological properties of lipid-coated monodisperse microbubbles,” Journal of the Acoustical Society of America, 138, 3994-4003.

    Broadband attenuation of ultrasound measured at different excitation pressures being differentraises a serious theoretical concern, because the underlying assumption of linear and independentpropagation of different frequency components nominally requires attenuation to be independent ofexcitation. Here, this issue is investigated by examining ultrasound attenuation through a monodis-perse lipid-coated microbubble suspension measured at four different acoustic excitation ampli-tudes. The attenuation data are used to determine interfacial rheological properties (surface tension,surface dilatational elasticity, and surface dilatational viscosity) of the encapsulation according tothree different models. Although different models result in similar rheological properties, attenua-tion measured at different excitation levels (4–110 kPa) leads to different values for them; the dila-tation elasticity (0.56 to 0.18 N/m) and viscosity (2.4108to 1.52108Ns/m) both decreasewith increasing pressure. Numerically simulating the scattered response, nonlinear energy transferbetween frequencies are shown to be negligible, thereby demonstrating the linearity in propagationand validating the attenuation analysis. There is a second concern to the characterization arisingfrom shell properties being dependent on excitation amplitude, which is not a proper constitutivevariable. It is resolved by arriving at a strain-dependent rheology for the encapsulation. The limita-tions of the underlying analysis are discussed.

  • Nahire R, Halder M, Paul S, Margoum A, Ambre AH, Katti KS, Gange KN, Srivastava D K, Sarkar K, Mallik S 2014 “pH-Triggered Echogenicity and Contents Release from Liposomes,” Molecular Pharamaceutics, 11, 4059-4068.

    Liposomes are representative lipid nanoparticles widelyused for delivering anticancer drugs, DNA fragments, or siRNA to cancercells. Upon targeting, various internal and external triggers have been usedto increase the rate for contents release from the liposomes. Among theinternal triggers, decreased pH within the cellular lysosomes has beensuccessfully used to enhance the rate for releasing contents. However,imparting pH sensitivity to liposomes requires the synthesis of specializedlipids with structures that are substantially modified at a reduced pH.Herein, we report an alternative strategy to render liposomes pH sensitiveby encapsulating a precursor which generates gas bubblesin situinresponse to acidic pH. The disturbance created by the escaping gasbubbles leads to the rapid release of the encapsulated contents from theliposomes. Atomic force microscopic studies indicate that the liposomalstructure is destroyed at a reduced pH. The gas bubbles also render theliposomes echogenic, allowing ultrasound imaging. To demonstrate the applicability of this strategy, we have successfully targeteddoxorubicin-encapsulated liposomes to the pancreatic ductal carcinoma cells that overexpress the folate receptor on the surface.In response to the decreased pH in the lysosomes, the encapsulated anticancer drug is efficiently released. Contents releasedfrom these liposomes are further enhanced by the application of continuous wave ultrasound (1 MHz), resulting in substantiallyreduced viability for the pancreatic cancer cells (14%).

  • Paul S, Nahire R, Mallik S, Sarkar K 2014 “Encapsulated microbubbles and echogenic liposomes for contrast ultrasound imaging and targeted drug delivery,” Computational Mechanics, 53,413-435.

    Micron- to nanometer-sized ultrasound agents,like encapsulated microbubbles and echogenic liposomes,are being developed for diagnostic imaging and ultra-sound mediated drug/gene delivery. This review providesan overview of the current state of the art of the mathe-matical models of the acoustic behavior of ultrasound con-trast microbubbles. We also present a review of the in vitroexperimental characterization of the acoustic properties ofmicrobubble based contrast agents undertaken in our lab-oratory. The hierarchical two-pronged approach of model-ing contrast agents we developed is demonstrated for a lipidcoated (SonazoidTM)and a polymer shelled (polyD-L-lactic acid) contrast microbubbles. The acoustic and drugrelease properties of the newly developed echogenic lipo-somes are discussed for their use as simultaneous imagingand drug/gene delivery agents. Although echogenicity is con-clusively demonstrated in experiments, its physical mecha-nisms remain uncertain. Addressing questions raised herewill accelerate further development and eventual clinicalapproval of these novel technologies.

  • Nahire R, Hossain R, Patel R, Paul S, Ambre AH, Meghnani V, Layek B, Katti KS, Gange KN, Leclarc E, Srivastava D K, Sarkar K, Mallik S 2014 “Multifunctional polymersomes for cytosolic delivery of gemcitabine and doxorubicin to cancer cells,” Biomaterials, 35, 6482-6497.

    Although liposomes are widely used as carriers of drugs and imaging agents, they suffer from a lack ofstability and the slow release of the encapsulated contents at the targeted site. Polymersomes (vesicles ofamphiphilic polymers) are considerably more stable compared to liposomes; however, they alsodemonstrate a slow release for the encapsulated contents, limiting their efficacy as a drug-delivery tool.As a solution, we prepared and characterized echogenic polymersomes, which are programmed torelease the encapsulated drugs rapidly when incubated with cytosolic concentrations of glutathione.These vesicles encapsulated air bubbles inside and efficiently reflected diagnostic-frequency ultrasound.Folate-targeted polymersomes showed an enhanced uptake by breast and pancreatic-cancer cells in amonolayer as well as in three-dimensional spheroid cultures. Polymersomes encapsulated with theanticancer drugs gemcitabine and doxorubicin showed significant cytotoxicity to these cells. Withfurther improvements, these vesicles hold the promise to serve as multifunctional nanocarriers, offeringa triggered release as well as diagnostic ultrasound imaging.

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

  • Karandish F, Haldar MK, Xia L, Gange KN, Feng L, You S, Choi Y, Sarkar K, Mallik S  2018 “Nucleus-targeted, echogenic polymersomes for delivering a cancer stemness inhibitor to pancreatic cancer cells,” Biomacromolecules, 19,4122-4132.

    Chemotherapeutic agents for treating cancers show considerable sideeffects, toxicity, and drug resistance. To mitigate the problems, we designed nucleus-targeted, echogenic, stimuli-responsive polymeric vesicles (polymersomes) to transport andsubsequently release the encapsulated anticancer drugs within the nuclei of pancreaticcancer cells. We synthesized an alkyne-dexamethasone derivative and conjugated it to N3−polyethylene glycol (PEG)−polylactic acid (PLA) copolymer employing the Cu2+catalyzed“Click”reaction. We prepared polymersomes from the dexamethasone−PEG−PLA conjugate along with a synthesized stimuli-responsive polymer PEG−S−S−PLA. Thedexamethasone group dilates the nuclear pore complexes and transports the vesicles to thenuclei. We designed the polymersomes to release the encapsulated drugs in the presence ofa high concentration of reducing agents in the nuclei of pancreatic cancer cells. Weobserved that the nucleus-targeted, stimuli-responsive polymersomes released 70% ofencapsulated contents in the nucleus-mimicking environment in 80 min. We encapsulatedthe cancer stemness inhibitor BBI608 in the vesicles and observed that the BBI608encapsulated polymersomes reduced the viability of the BxPC3 cells to 43% in three-dimensional spheroid cultures. Thepolymersomes were prepared following a special protocol so that they scatter ultrasound, allowing imaging by a medicalultrasound scanner. Therefore, these echogenic, targeted, stimuli-responsive, and drug-encapsulated polymersomes have thepotential for trackable, targeted carrier of chemotherapeutic drugs to cancer cell nuclei.

  • Nahire R, Halder M, Paul S, Margoum A, Ambre AH, Katti KS, Gange KN, Srivastava D K, Sarkar K, Mallik S 2013 “Polymer Coated Echogenic Lipid Nanoparticles with dual release triggers,” Biomacromolecules, 14, 841-853.

    Although lipid nanoparticles are promising drugdelivery vehicles, passive release of encapsulated contents atthe target site is often slow. Herein, we report contents releasefrom targeted, polymer-coated, echogenic lipid nanoparticles inthe cell cytoplasm by redox trigger and simultaneouslyenhanced by diagnostic frequency ultrasound. The lipidnanoparticles were polymerized on the external leaflet usinga disulfide cross-linker. In the presence of cytosolicconcentrations of glutathione, the lipid nanoparticles released76% of encapsulated contents. Plasma concentrations ofglutathione failed to releasethe encapsulated contents.Application of 3 MHz ultrasound for 2 min simultaneouslywith the reducing agent enhanced the release to 96%. Folicacid conjugated, doxorubicin-loaded nanoparticles showed enhanced uptake and higher cytotoxicity in cancer cells overexpressingthe folate receptor (compared to the control). With further developments, these lipid nanoparticles have the potential to be usedas multimodal nanocarriers for simultaneous targeted drug delivery and ultrasound imaging.

  • Mobadersany N, Sarkar K 2019 “Acoustic microstreaming near a plane wall due to a pulsating free or coated bubble: velocity, vorticity and closed streamlines,” Journal of Fluid Mechanics, 875 781-806.

    Acoustic microstreaming due to an oscillating microbubble, either coated or free, is analytically investigated. The detailed flow field is obtained and the closed streamlines of the ring vortex generated by microstreaming are plotted in both Eulerian and Lagrangian descriptions. Analytical expressions are found for the ring vortex showing that its length depends only on the separation of the microbubble from the wall
    and the dependence is linear. The circulation as a scalar measure of the vortex is computed quantitatively identifying its spatial location. The functional dependence of circulation on bubble separation and coating parameters is shown to be similar to that of the shear stress.

  • Mobadersany N, Sarkar K 2019 “Acoustic microstreaming near a plane wall due to a pulsating free or coated bubble: velocity, vorticity and closed streamlines,” Journal of Fluid Mechanics, 875 781-806.

    Acoustic microstreaming due to an oscillating microbubble, either coated or free, is analytically investigated. The detailed flow field is obtained and the closed streamlines of the ring vortex generated by microstreaming are plotted in both Eulerian and Lagrangian descriptions. Analytical expressions are found for the ring vortex showing that its length depends only on the separation of the microbubble from the wall
    and the dependence is linear. The circulation as a scalar measure of the vortex is computed quantitatively identifying its spatial location. The functional dependence of circulation on bubble separation and coating parameters is shown to be similar to that of the shear stress.

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Kulkarni P, Haldar MK, Karandish F, Confeld M, Hossain R, Borowicz P, Gange KN, Xia L, Sarkar K, Mallik S 2018 “Tissue-penetrating, hypoxia-responsive echogenic polymersomes for drug delivery to solid tumors,” Chemistry A European Journal, 24, 12490-12494.

    Hypoxia in solid tumors facilitates the progres-sion of the disease, develops resistance to chemo and radiotherapy, and contributes to relapse. Due to the lack of tumor penetration, most of the reported drug carriers are unable to reach the hypoxic niches of the solid tumors. We have developed tissue-penetrating, hypoxia-responsive echogenic polymersomes to deliver anti cancer drugs to solid tumors. The polymersomes are composed of a hy-poxia-responsive azobenzene conjugated and a tissue penetrating peptide functionalized polylactic acid-polyethylene glycol polymer. The drug-encapsulated, hypoxia-responsive polymersomes substantially decreased the viability of pancreatic cancer cells in spheroidal cultures. Under normoxic conditions, polymersomes were echogenic at diagnostic ultrasound frequencies but lose the echogenicity under hypoxia. In vivo imaging studies with xenograft mouse model further confirmed the ability of the polymersomes to target, penetrate, and deliver the encapsulated contents in hypoxic pancreatic tumor tissues.

  • Aliabouzar M, Kumar KN, Sarkar K, 2018 “Acoustic vaporization threshold of lipid coated perfluoropentane droplets,” Journal of the Acoustical Society of America, 143, 2001-2012.

    Phase shift droplets vaporizable by acoustic stimulation offer the advantages of producing micro-bubbles as contrast agentsin situas well as higher stability and the possibility of achieving smallersizes. Here, the acoustic droplet vaporization (ADV) threshold of a suspension of droplets with aperfluoropentane (PFP) core (diameter 400–3000 nm) is acoustically measured as a function of theexcitation frequency in a tubeless setup at room temperature. The changes in scattered responses—fundamental, sub-, and second harmonic—are investigated, a quantitative criterion is used to deter-mine the ADV phenomenon, and findings are discussed. The average threshold obtained using threedifferent scattered components increases with frequency—1.0560.28 MPa at 2.25 MHz,1.8960.57 MPa at 5 MHz, and 2.3460.014 MPa at 10 MHz. The scattered response from vapor-ized droplets was also found to qualitatively match with that from an independently prepared lipid-coated microbubble suspension in magnitude as well as trends above the determined ADV thresh-old value.

  • Aliabouzar M, Kumar KN, Sarkar K, 2018 “Acoustic vaporization threshold of lipid coated perfluoropentane droplets,” Journal of the Acoustical Society of America, 143, 2001-2012.

    Phase shift droplets vaporizable by acoustic stimulation offer the advantages of producing micro-bubbles as contrast agentsin situas well as higher stability and the possibility of achieving smallersizes. Here, the acoustic droplet vaporization (ADV) threshold of a suspension of droplets with aperfluoropentane (PFP) core (diameter 400–3000 nm) is acoustically measured as a function of theexcitation frequency in a tubeless setup at room temperature. The changes in scattered responses—fundamental, sub-, and second harmonic—are investigated, a quantitative criterion is used to deter-mine the ADV phenomenon, and findings are discussed. The average threshold obtained using threedifferent scattered components increases with frequency—1.0560.28 MPa at 2.25 MHz,1.8960.57 MPa at 5 MHz, and 2.3460.014 MPa at 10 MHz. The scattered response from vapor-ized droplets was also found to qualitatively match with that from an independently prepared lipid-coated microbubble suspension in magnitude as well as trends above the determined ADV thresh-old value.

  • Karandish F, Haldar MK, Xia L, Gange KN, Feng L, You S, Choi Y, Sarkar K, Mallik S  2018 “Nucleus-targeted, echogenic polymersomes for delivering a cancer stemness inhibitor to pancreatic cancer cells,” Biomacromolecules, 19,4122-4132.

    Chemotherapeutic agents for treating cancers show considerable sideeffects, toxicity, and drug resistance. To mitigate the problems, we designed nucleus-targeted, echogenic, stimuli-responsive polymeric vesicles (polymersomes) to transport andsubsequently release the encapsulated anticancer drugs within the nuclei of pancreaticcancer cells. We synthesized an alkyne-dexamethasone derivative and conjugated it to N3−polyethylene glycol (PEG)−polylactic acid (PLA) copolymer employing the Cu2+catalyzed“Click”reaction. We prepared polymersomes from the dexamethasone−PEG−PLA conjugate along with a synthesized stimuli-responsive polymer PEG−S−S−PLA. Thedexamethasone group dilates the nuclear pore complexes and transports the vesicles to thenuclei. We designed the polymersomes to release the encapsulated drugs in the presence ofa high concentration of reducing agents in the nuclei of pancreatic cancer cells. Weobserved that the nucleus-targeted, stimuli-responsive polymersomes released 70% ofencapsulated contents in the nucleus-mimicking environment in 80 min. We encapsulatedthe cancer stemness inhibitor BBI608 in the vesicles and observed that the BBI608encapsulated polymersomes reduced the viability of the BxPC3 cells to 43% in three-dimensional spheroid cultures. Thepolymersomes were prepared following a special protocol so that they scatter ultrasound, allowing imaging by a medicalultrasound scanner. Therefore, these echogenic, targeted, stimuli-responsive, and drug-encapsulated polymersomes have thepotential for trackable, targeted carrier of chemotherapeutic drugs to cancer cell nuclei.

  • Xia L, Karandish F, Kumar KN, Froberg J, Kulkarni P, Gange KN, Choi Y, Mallik S, Sarkar K 2017 “Acoustic characterization of echogenic polymersomes prepared from amphiphilic block copolymers,” Ultrasound in Medicine and Biology, 44, 447-457.

    Polymersomes are a class of artificial vesicles prepared from amphiphilic polymers. Like lipid vesicles(liposomes), they too can encapsulate hydrophilic and hydrophobic drug molecules in the aqueous core and thehydrophobic bilayer respectively, but are more stable than liposomes. Although echogenic liposomes have beenwidely investigated for simultaneous ultrasound imaging and controlled drug delivery, the potential of thepolymersomes remains unexplored. We prepared two different echogenic polymersomes from the amphiphilic co-polymers polyethylene glycol–poly-DL-lactic acid (PEG-PLA) and polyethylene glycol–poly-L-lactic acid (PEG-PLLA), incorporating multiple freeze-dry cycles in the synthesis protocol to ensure their echogenicity. We investigatedacoustic behavior with potential applications in biomedical imaging. We characterized the polymeric vesicles acous-tically with three different excitation frequencies of 2.25, 5 and 10 MHz at 500 kPa. The polymersomes exhibitedstrong echogenicity at all three excitation frequencies (about 50- and 25-dB enhancements in fundamental andsubharmonic, respectively, at 5-MHz excitation from 20g/mL polymers in solution). Unlike echogenic lipo-somes, they emitted strong subharmonic responses. The scattering results indicated their potential as contrastagents, which was also confirmed by clinical ultrasound imaging.

  • Kumar KN, Mallik S, Sarkar K, 2017 “Role of freeze-drying in the presence of mannitol on the echogenicity of echogenic liposomes,” Journal of the Acoustical Society of America, 142, 3670-3676.

    Echogenic liposomes (ELIPs) are an excellent candidate for ultrasound activated therapeutics andimaging. Although multiple experiments have established their echogenicity, the underlying mech-anism has remained unknown. However, freeze-drying in the presence of mannitol during ELIPpreparation has proved critical to ensuring echogenicity. Here, the role of this key component in thepreparation protocol was investigated by measuring scattering from freshly prepared freeze-driedaqueous solution of mannitol—and a number of other excipients commonly used in lyophiliza-tion—directly dispersed in water without any lipids in the experiment. Mannitol, meso-erythritol,glycine, and glucose that form a highly porous crystalline phase upon freeze-drying generated bub-bles resulting in strong echoes during their dissolution. On the other hand, sucrose, trehalose, andxylitol, which become glassy while freeze-dried, did not. Freeze-dried mannitol and other crystal-line substances, if thawed before being introduced into the scattering volume, did not produce echo-genicity, as they lost their crystallinity in the thawed state. The echogenicity disappeared in adegassed environment. Higher amounts of sugar in the original aqueous solution before freeze-drying resulted in higher echogenicity because of the stronger supersaturation and crystallinity. Thebubbles created by the freeze-dried mannitol in the ELIP formulation play a critical role in makingELIPs echogenic.

  • Kumar KN, Sarkar K 2016 “Interfacial rheological properties of contrast microbubble Targestar P as a function of ambient pressure,” Ultrasound in Medicine and Biology, 42, 1010-1017.

    In this Technical Note, we determine the interfacial rheological parameters of the encapsulation of thecontrast agent Targestar P using ultrasound attenuation. The characteristic parameters are obtained according totwo interfacial rheological models. The properties—surface dilatational elasticity (0.09 ± 0.01 N/m) and surfacedilatational viscosity (8 ± 0.1E–9 N$s/m)—are found to be of similar magnitude for both models. Contrast micro-bubbles experience different ambient pressure in different organs. We also measure these parameters as functionsof ambient pressure using attenuation measured at different overpressures (0, 100 and 200 mm Hg). For each valueof ambient hydrostatic pressure, we determine the rheological properties, accounting for changes in the size dis-tribution caused by the pressure change. We discuss different models of size distribution change under overpres-sure: pure adiabatic compression or gas exchange with surrounding medium. The dilatational surface elasticityand viscosity are found to increase with increasing ambient pressure.

  • Kumar KN, Sarkar K 2015 “Effects of ambient hydrostatic pressure on the material properties of the encapsulation of an ultrasound contrast microbubble,” Journal of the Acoustical Society of America, 138, 624-634.

    Ultrasound contrast microbubbles experience widely varying ambient blood pressure in differentorgans, which can also change due to diseases. Pressure change can alter the material properties ofthe encapsulation of these microbubbles. Here the characteristic rheological parameters of contrastagent Definity are determined by varying the ambient pressure (in a physiologically relevant range0–200 mm Hg). Four different interfacial rheological models are used to characterize the microbub-bles. Effects of gas diffusion under excess ambient pressure are investigated in detail accountingfor size decrease of contrast microbubbles. Definity contrast agent show a change in their interfacialdilatational viscosity (3.6108Ns/m at 0 mm Hg to 4.45108Ns/m at 200 mm Hg) and inter-facial dilatational elasticity (0.86 N/m at 0 mm Hg to 1.06 N/m at 200 mm Hg) with ambient pres-sure increase. The increase results from material consolidation, similar to such enhancement inbulk properties under pressure. The model that accounts for enhancement in material propertieswith increasing ambient pressure matches with experimentally measured subharmonic response asa function of ambient pressure, while assuming constant material parameters does not.

  • Lang X, Porter T, Sarkar K 2015 “Interpreting attenuation at different excitation amplitudes to estimate strain-dependent interfacial rheological properties of lipid-coated monodisperse microbubbles,” Journal of the Acoustical Society of America, 138, 3994-4003.

    Broadband attenuation of ultrasound measured at different excitation pressures being differentraises a serious theoretical concern, because the underlying assumption of linear and independentpropagation of different frequency components nominally requires attenuation to be independent ofexcitation. Here, this issue is investigated by examining ultrasound attenuation through a monodis-perse lipid-coated microbubble suspension measured at four different acoustic excitation ampli-tudes. The attenuation data are used to determine interfacial rheological properties (surface tension,surface dilatational elasticity, and surface dilatational viscosity) of the encapsulation according tothree different models. Although different models result in similar rheological properties, attenua-tion measured at different excitation levels (4–110 kPa) leads to different values for them; the dila-tation elasticity (0.56 to 0.18 N/m) and viscosity (2.4108to 1.52108Ns/m) both decreasewith increasing pressure. Numerically simulating the scattered response, nonlinear energy transferbetween frequencies are shown to be negligible, thereby demonstrating the linearity in propagationand validating the attenuation analysis. There is a second concern to the characterization arisingfrom shell properties being dependent on excitation amplitude, which is not a proper constitutivevariable. It is resolved by arriving at a strain-dependent rheology for the encapsulation. The limita-tions of the underlying analysis are discussed.

  • Nahire R, Hossain R, Patel R, Paul S, Ambre AH, Meghnani V, Layek B, Katti KS, Gange KN, Leclarc E, Srivastava D K, Sarkar K, Mallik S 2014 “Multifunctional polymersomes for cytosolic delivery of gemcitabine and doxorubicin to cancer cells,” Biomaterials, 35, 6482-6497.

    Although liposomes are widely used as carriers of drugs and imaging agents, they suffer from a lack ofstability and the slow release of the encapsulated contents at the targeted site. Polymersomes (vesicles ofamphiphilic polymers) are considerably more stable compared to liposomes; however, they alsodemonstrate a slow release for the encapsulated contents, limiting their efficacy as a drug-delivery tool.As a solution, we prepared and characterized echogenic polymersomes, which are programmed torelease the encapsulated drugs rapidly when incubated with cytosolic concentrations of glutathione.These vesicles encapsulated air bubbles inside and efficiently reflected diagnostic-frequency ultrasound.Folate-targeted polymersomes showed an enhanced uptake by breast and pancreatic-cancer cells in amonolayer as well as in three-dimensional spheroid cultures. Polymersomes encapsulated with theanticancer drugs gemcitabine and doxorubicin showed significant cytotoxicity to these cells. Withfurther improvements, these vesicles hold the promise to serve as multifunctional nanocarriers, offeringa triggered release as well as diagnostic ultrasound imaging.

  • Nahire R, Halder M, Paul S, Margoum A, Ambre AH, Katti KS, Gange KN, Srivastava D K, Sarkar K, Mallik S 2014 “pH-Triggered Echogenicity and Contents Release from Liposomes,” Molecular Pharamaceutics, 11, 4059-4068.

    Liposomes are representative lipid nanoparticles widelyused for delivering anticancer drugs, DNA fragments, or siRNA to cancercells. Upon targeting, various internal and external triggers have been usedto increase the rate for contents release from the liposomes. Among theinternal triggers, decreased pH within the cellular lysosomes has beensuccessfully used to enhance the rate for releasing contents. However,imparting pH sensitivity to liposomes requires the synthesis of specializedlipids with structures that are substantially modified at a reduced pH.Herein, we report an alternative strategy to render liposomes pH sensitiveby encapsulating a precursor which generates gas bubblesin situinresponse to acidic pH. The disturbance created by the escaping gasbubbles leads to the rapid release of the encapsulated contents from theliposomes. Atomic force microscopic studies indicate that the liposomalstructure is destroyed at a reduced pH. The gas bubbles also render theliposomes echogenic, allowing ultrasound imaging. To demonstrate the applicability of this strategy, we have successfully targeteddoxorubicin-encapsulated liposomes to the pancreatic ductal carcinoma cells that overexpress the folate receptor on the surface.In response to the decreased pH in the lysosomes, the encapsulated anticancer drug is efficiently released. Contents releasedfrom these liposomes are further enhanced by the application of continuous wave ultrasound (1 MHz), resulting in substantiallyreduced viability for the pancreatic cancer cells (14%).

  • Paul S, Nahire R, Mallik S, Sarkar K 2014 “Encapsulated microbubbles and echogenic liposomes for contrast ultrasound imaging and targeted drug delivery,” Computational Mechanics, 53,413-435.

    Micron- to nanometer-sized ultrasound agents,like encapsulated microbubbles and echogenic liposomes,are being developed for diagnostic imaging and ultra-sound mediated drug/gene delivery. This review providesan overview of the current state of the art of the mathe-matical models of the acoustic behavior of ultrasound con-trast microbubbles. We also present a review of the in vitroexperimental characterization of the acoustic properties ofmicrobubble based contrast agents undertaken in our lab-oratory. The hierarchical two-pronged approach of model-ing contrast agents we developed is demonstrated for a lipidcoated (SonazoidTM)and a polymer shelled (polyD-L-lactic acid) contrast microbubbles. The acoustic and drugrelease properties of the newly developed echogenic lipo-somes are discussed for their use as simultaneous imagingand drug/gene delivery agents. Although echogenicity is con-clusively demonstrated in experiments, its physical mecha-nisms remain uncertain. Addressing questions raised herewill accelerate further development and eventual clinicalapproval of these novel technologies.

  • Nahire R, Halder M, Paul S, Margoum A, Ambre AH, Katti KS, Gange KN, Srivastava D K, Sarkar K, Mallik S 2013 “Polymer Coated Echogenic Lipid Nanoparticles with dual release triggers,” Biomacromolecules, 14, 841-853.

    Although lipid nanoparticles are promising drugdelivery vehicles, passive release of encapsulated contents atthe target site is often slow. Herein, we report contents releasefrom targeted, polymer-coated, echogenic lipid nanoparticles inthe cell cytoplasm by redox trigger and simultaneouslyenhanced by diagnostic frequency ultrasound. The lipidnanoparticles were polymerized on the external leaflet usinga disulfide cross-linker. In the presence of cytosolicconcentrations of glutathione, the lipid nanoparticles released76% of encapsulated contents. Plasma concentrations ofglutathione failed to releasethe encapsulated contents.Application of 3 MHz ultrasound for 2 min simultaneouslywith the reducing agent enhanced the release to 96%. Folicacid conjugated, doxorubicin-loaded nanoparticles showed enhanced uptake and higher cytotoxicity in cancer cells overexpressingthe folate receptor (compared to the control). With further developments, these lipid nanoparticles have the potential to be usedas multimodal nanocarriers for simultaneous targeted drug delivery and ultrasound imaging.

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

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  • Duraiswami R, Sarkar K, Chahine GL 1998 "Efficient 2D and 3D electrical impedance tomography using dual reciprocity boundary element techniques," Engineering Analysis with Boundary Elements, 22, 13-31.

    This paper presents applications of boundary element methods to electrical impe- dance tomography. An algorithm for imaging the interior of a domain that consists of regions of constant conductivity is developed, that makes use of a simpler parametrization of the shapes of the regions to achieve efficiency. Numerical results from tests of this algorithm on synthetic data are presented, and show that the method is quite promising.

  • Duraiswami R, Sarkar K, Chahine GL 1998 "Efficient 2D and 3D electrical impedance tomography using dual reciprocity boundary element techniques," Engineering Analysis with Boundary Elements, 22, 13-31.

    This paper presents applications of boundary element methods to electrical impe- dance tomography. An algorithm for imaging the interior of a domain that consists of regions of constant conductivity is developed, that makes use of a simpler parametrization of the shapes of the regions to achieve efficiency. Numerical results from tests of this algorithm on synthetic data are presented, and show that the method is quite promising.

  • Duraiswami R, Sarkar K, Chahine GL 1998 "Efficient 2D and 3D electrical impedance tomography using dual reciprocity boundary element techniques," Engineering Analysis with Boundary Elements, 22, 13-31.

    This paper presents applications of boundary element methods to electrical impe- dance tomography. An algorithm for imaging the interior of a domain that consists of regions of constant conductivity is developed, that makes use of a simpler parametrization of the shapes of the regions to achieve efficiency. Numerical results from tests of this algorithm on synthetic data are presented, and show that the method is quite promising.

  • Duraiswami R, Sarkar K, Chahine GL 1998 "Efficient 2D and 3D electrical impedance tomography using dual reciprocity boundary element techniques," Engineering Analysis with Boundary Elements, 22, 13-31.

    This paper presents applications of boundary element methods to electrical impe- dance tomography. An algorithm for imaging the interior of a domain that consists of regions of constant conductivity is developed, that makes use of a simpler parametrization of the shapes of the regions to achieve efficiency. Numerical results from tests of this algorithm on synthetic data are presented, and show that the method is quite promising.

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Aliabouzar M, Kumar KN, Sarkar K, 2018 “Acoustic vaporization threshold of lipid coated perfluoropentane droplets,” Journal of the Acoustical Society of America, 143, 2001-2012.

    Phase shift droplets vaporizable by acoustic stimulation offer the advantages of producing micro-bubbles as contrast agentsin situas well as higher stability and the possibility of achieving smallersizes. Here, the acoustic droplet vaporization (ADV) threshold of a suspension of droplets with aperfluoropentane (PFP) core (diameter 400–3000 nm) is acoustically measured as a function of theexcitation frequency in a tubeless setup at room temperature. The changes in scattered responses—fundamental, sub-, and second harmonic—are investigated, a quantitative criterion is used to deter-mine the ADV phenomenon, and findings are discussed. The average threshold obtained using threedifferent scattered components increases with frequency—1.0560.28 MPa at 2.25 MHz,1.8960.57 MPa at 5 MHz, and 2.3460.014 MPa at 10 MHz. The scattered response from vapor-ized droplets was also found to qualitatively match with that from an independently prepared lipid-coated microbubble suspension in magnitude as well as trends above the determined ADV thresh-old value.

  • Kulkarni P, Haldar MK, Karandish F, Confeld M, Hossain R, Borowicz P, Gange KN, Xia L, Sarkar K, Mallik S 2018 “Tissue-penetrating, hypoxia-responsive echogenic polymersomes for drug delivery to solid tumors,” Chemistry A European Journal, 24, 12490-12494.

    Hypoxia in solid tumors facilitates the progres-sion of the disease, develops resistance to chemo and radiotherapy, and contributes to relapse. Due to the lack of tumor penetration, most of the reported drug carriers are unable to reach the hypoxic niches of the solid tumors. We have developed tissue-penetrating, hypoxia-responsive echogenic polymersomes to deliver anti cancer drugs to solid tumors. The polymersomes are composed of a hy-poxia-responsive azobenzene conjugated and a tissue penetrating peptide functionalized polylactic acid-polyethylene glycol polymer. The drug-encapsulated, hypoxia-responsive polymersomes substantially decreased the viability of pancreatic cancer cells in spheroidal cultures. Under normoxic conditions, polymersomes were echogenic at diagnostic ultrasound frequencies but lose the echogenicity under hypoxia. In vivo imaging studies with xenograft mouse model further confirmed the ability of the polymersomes to target, penetrate, and deliver the encapsulated contents in hypoxic pancreatic tumor tissues.

  • Karandish F, Haldar MK, Xia L, Gange KN, Feng L, You S, Choi Y, Sarkar K, Mallik S  2018 “Nucleus-targeted, echogenic polymersomes for delivering a cancer stemness inhibitor to pancreatic cancer cells,” Biomacromolecules, 19,4122-4132.

    Chemotherapeutic agents for treating cancers show considerable sideeffects, toxicity, and drug resistance. To mitigate the problems, we designed nucleus-targeted, echogenic, stimuli-responsive polymeric vesicles (polymersomes) to transport andsubsequently release the encapsulated anticancer drugs within the nuclei of pancreaticcancer cells. We synthesized an alkyne-dexamethasone derivative and conjugated it to N3−polyethylene glycol (PEG)−polylactic acid (PLA) copolymer employing the Cu2+catalyzed“Click”reaction. We prepared polymersomes from the dexamethasone−PEG−PLA conjugate along with a synthesized stimuli-responsive polymer PEG−S−S−PLA. Thedexamethasone group dilates the nuclear pore complexes and transports the vesicles to thenuclei. We designed the polymersomes to release the encapsulated drugs in the presence ofa high concentration of reducing agents in the nuclei of pancreatic cancer cells. Weobserved that the nucleus-targeted, stimuli-responsive polymersomes released 70% ofencapsulated contents in the nucleus-mimicking environment in 80 min. We encapsulatedthe cancer stemness inhibitor BBI608 in the vesicles and observed that the BBI608encapsulated polymersomes reduced the viability of the BxPC3 cells to 43% in three-dimensional spheroid cultures. Thepolymersomes were prepared following a special protocol so that they scatter ultrasound, allowing imaging by a medicalultrasound scanner. Therefore, these echogenic, targeted, stimuli-responsive, and drug-encapsulated polymersomes have thepotential for trackable, targeted carrier of chemotherapeutic drugs to cancer cell nuclei.

  • Lang X, Porter T, Sarkar K 2015 “Interpreting attenuation at different excitation amplitudes to estimate strain-dependent interfacial rheological properties of lipid-coated monodisperse microbubbles,” Journal of the Acoustical Society of America, 138, 3994-4003.

    Broadband attenuation of ultrasound measured at different excitation pressures being differentraises a serious theoretical concern, because the underlying assumption of linear and independentpropagation of different frequency components nominally requires attenuation to be independent ofexcitation. Here, this issue is investigated by examining ultrasound attenuation through a monodis-perse lipid-coated microbubble suspension measured at four different acoustic excitation ampli-tudes. The attenuation data are used to determine interfacial rheological properties (surface tension,surface dilatational elasticity, and surface dilatational viscosity) of the encapsulation according tothree different models. Although different models result in similar rheological properties, attenua-tion measured at different excitation levels (4–110 kPa) leads to different values for them; the dila-tation elasticity (0.56 to 0.18 N/m) and viscosity (2.4108to 1.52108Ns/m) both decreasewith increasing pressure. Numerically simulating the scattered response, nonlinear energy transferbetween frequencies are shown to be negligible, thereby demonstrating the linearity in propagationand validating the attenuation analysis. There is a second concern to the characterization arisingfrom shell properties being dependent on excitation amplitude, which is not a proper constitutivevariable. It is resolved by arriving at a strain-dependent rheology for the encapsulation. The limita-tions of the underlying analysis are discussed.

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Mobadersany N, Sarkar K 2019 “Acoustic microstreaming near a plane wall due to a pulsating free or coated bubble: velocity, vorticity and closed streamlines,” Journal of Fluid Mechanics, 875 781-806.

    Acoustic microstreaming due to an oscillating microbubble, either coated or free, is analytically investigated. The detailed flow field is obtained and the closed streamlines of the ring vortex generated by microstreaming are plotted in both Eulerian and Lagrangian descriptions. Analytical expressions are found for the ring vortex showing that its length depends only on the separation of the microbubble from the wall
    and the dependence is linear. The circulation as a scalar measure of the vortex is computed quantitatively identifying its spatial location. The functional dependence of circulation on bubble separation and coating parameters is shown to be similar to that of the shear stress.

  • Aliabouzar M, Kumar KN, Sarkar K, 2018 “Acoustic vaporization threshold of lipid coated perfluoropentane droplets,” Journal of the Acoustical Society of America, 143, 2001-2012.

    Phase shift droplets vaporizable by acoustic stimulation offer the advantages of producing micro-bubbles as contrast agentsin situas well as higher stability and the possibility of achieving smallersizes. Here, the acoustic droplet vaporization (ADV) threshold of a suspension of droplets with aperfluoropentane (PFP) core (diameter 400–3000 nm) is acoustically measured as a function of theexcitation frequency in a tubeless setup at room temperature. The changes in scattered responses—fundamental, sub-, and second harmonic—are investigated, a quantitative criterion is used to deter-mine the ADV phenomenon, and findings are discussed. The average threshold obtained using threedifferent scattered components increases with frequency—1.0560.28 MPa at 2.25 MHz,1.8960.57 MPa at 5 MHz, and 2.3460.014 MPa at 10 MHz. The scattered response from vapor-ized droplets was also found to qualitatively match with that from an independently prepared lipid-coated microbubble suspension in magnitude as well as trends above the determined ADV thresh-old value.

  • Kulkarni P, Haldar MK, Karandish F, Confeld M, Hossain R, Borowicz P, Gange KN, Xia L, Sarkar K, Mallik S 2018 “Tissue-penetrating, hypoxia-responsive echogenic polymersomes for drug delivery to solid tumors,” Chemistry A European Journal, 24, 12490-12494.

    Hypoxia in solid tumors facilitates the progres-sion of the disease, develops resistance to chemo and radiotherapy, and contributes to relapse. Due to the lack of tumor penetration, most of the reported drug carriers are unable to reach the hypoxic niches of the solid tumors. We have developed tissue-penetrating, hypoxia-responsive echogenic polymersomes to deliver anti cancer drugs to solid tumors. The polymersomes are composed of a hy-poxia-responsive azobenzene conjugated and a tissue penetrating peptide functionalized polylactic acid-polyethylene glycol polymer. The drug-encapsulated, hypoxia-responsive polymersomes substantially decreased the viability of pancreatic cancer cells in spheroidal cultures. Under normoxic conditions, polymersomes were echogenic at diagnostic ultrasound frequencies but lose the echogenicity under hypoxia. In vivo imaging studies with xenograft mouse model further confirmed the ability of the polymersomes to target, penetrate, and deliver the encapsulated contents in hypoxic pancreatic tumor tissues.

  • Karandish F, Haldar MK, Xia L, Gange KN, Feng L, You S, Choi Y, Sarkar K, Mallik S  2018 “Nucleus-targeted, echogenic polymersomes for delivering a cancer stemness inhibitor to pancreatic cancer cells,” Biomacromolecules, 19,4122-4132.

    Chemotherapeutic agents for treating cancers show considerable sideeffects, toxicity, and drug resistance. To mitigate the problems, we designed nucleus-targeted, echogenic, stimuli-responsive polymeric vesicles (polymersomes) to transport andsubsequently release the encapsulated anticancer drugs within the nuclei of pancreaticcancer cells. We synthesized an alkyne-dexamethasone derivative and conjugated it to N3−polyethylene glycol (PEG)−polylactic acid (PLA) copolymer employing the Cu2+catalyzed“Click”reaction. We prepared polymersomes from the dexamethasone−PEG−PLA conjugate along with a synthesized stimuli-responsive polymer PEG−S−S−PLA. Thedexamethasone group dilates the nuclear pore complexes and transports the vesicles to thenuclei. We designed the polymersomes to release the encapsulated drugs in the presence ofa high concentration of reducing agents in the nuclei of pancreatic cancer cells. Weobserved that the nucleus-targeted, stimuli-responsive polymersomes released 70% ofencapsulated contents in the nucleus-mimicking environment in 80 min. We encapsulatedthe cancer stemness inhibitor BBI608 in the vesicles and observed that the BBI608encapsulated polymersomes reduced the viability of the BxPC3 cells to 43% in three-dimensional spheroid cultures. Thepolymersomes were prepared following a special protocol so that they scatter ultrasound, allowing imaging by a medicalultrasound scanner. Therefore, these echogenic, targeted, stimuli-responsive, and drug-encapsulated polymersomes have thepotential for trackable, targeted carrier of chemotherapeutic drugs to cancer cell nuclei.

  • Kumar KN, Mallik S, Sarkar K, 2017 “Role of freeze-drying in the presence of mannitol on the echogenicity of echogenic liposomes,” Journal of the Acoustical Society of America, 142, 3670-3676.

    Echogenic liposomes (ELIPs) are an excellent candidate for ultrasound activated therapeutics andimaging. Although multiple experiments have established their echogenicity, the underlying mech-anism has remained unknown. However, freeze-drying in the presence of mannitol during ELIPpreparation has proved critical to ensuring echogenicity. Here, the role of this key component in thepreparation protocol was investigated by measuring scattering from freshly prepared freeze-driedaqueous solution of mannitol—and a number of other excipients commonly used in lyophiliza-tion—directly dispersed in water without any lipids in the experiment. Mannitol, meso-erythritol,glycine, and glucose that form a highly porous crystalline phase upon freeze-drying generated bub-bles resulting in strong echoes during their dissolution. On the other hand, sucrose, trehalose, andxylitol, which become glassy while freeze-dried, did not. Freeze-dried mannitol and other crystal-line substances, if thawed before being introduced into the scattering volume, did not produce echo-genicity, as they lost their crystallinity in the thawed state. The echogenicity disappeared in adegassed environment. Higher amounts of sugar in the original aqueous solution before freeze-drying resulted in higher echogenicity because of the stronger supersaturation and crystallinity. Thebubbles created by the freeze-dried mannitol in the ELIP formulation play a critical role in makingELIPs echogenic.

  • Xia L, Karandish F, Kumar KN, Froberg J, Kulkarni P, Gange KN, Choi Y, Mallik S, Sarkar K 2017 “Acoustic characterization of echogenic polymersomes prepared from amphiphilic block copolymers,” Ultrasound in Medicine and Biology, 44, 447-457.

    Polymersomes are a class of artificial vesicles prepared from amphiphilic polymers. Like lipid vesicles(liposomes), they too can encapsulate hydrophilic and hydrophobic drug molecules in the aqueous core and thehydrophobic bilayer respectively, but are more stable than liposomes. Although echogenic liposomes have beenwidely investigated for simultaneous ultrasound imaging and controlled drug delivery, the potential of thepolymersomes remains unexplored. We prepared two different echogenic polymersomes from the amphiphilic co-polymers polyethylene glycol–poly-DL-lactic acid (PEG-PLA) and polyethylene glycol–poly-L-lactic acid (PEG-PLLA), incorporating multiple freeze-dry cycles in the synthesis protocol to ensure their echogenicity. We investigatedacoustic behavior with potential applications in biomedical imaging. We characterized the polymeric vesicles acous-tically with three different excitation frequencies of 2.25, 5 and 10 MHz at 500 kPa. The polymersomes exhibitedstrong echogenicity at all three excitation frequencies (about 50- and 25-dB enhancements in fundamental andsubharmonic, respectively, at 5-MHz excitation from 20g/mL polymers in solution). Unlike echogenic lipo-somes, they emitted strong subharmonic responses. The scattering results indicated their potential as contrastagents, which was also confirmed by clinical ultrasound imaging.

  • Kumar KN, Sarkar K 2016 “Interfacial rheological properties of contrast microbubble Targestar P as a function of ambient pressure,” Ultrasound in Medicine and Biology, 42, 1010-1017.

    In this Technical Note, we determine the interfacial rheological parameters of the encapsulation of thecontrast agent Targestar P using ultrasound attenuation. The characteristic parameters are obtained according totwo interfacial rheological models. The properties—surface dilatational elasticity (0.09 ± 0.01 N/m) and surfacedilatational viscosity (8 ± 0.1E–9 N$s/m)—are found to be of similar magnitude for both models. Contrast micro-bubbles experience different ambient pressure in different organs. We also measure these parameters as functionsof ambient pressure using attenuation measured at different overpressures (0, 100 and 200 mm Hg). For each valueof ambient hydrostatic pressure, we determine the rheological properties, accounting for changes in the size dis-tribution caused by the pressure change. We discuss different models of size distribution change under overpres-sure: pure adiabatic compression or gas exchange with surrounding medium. The dilatational surface elasticityand viscosity are found to increase with increasing ambient pressure.

  • Lang X, Porter T, Sarkar K 2015 “Interpreting attenuation at different excitation amplitudes to estimate strain-dependent interfacial rheological properties of lipid-coated monodisperse microbubbles,” Journal of the Acoustical Society of America, 138, 3994-4003.

    Broadband attenuation of ultrasound measured at different excitation pressures being differentraises a serious theoretical concern, because the underlying assumption of linear and independentpropagation of different frequency components nominally requires attenuation to be independent ofexcitation. Here, this issue is investigated by examining ultrasound attenuation through a monodis-perse lipid-coated microbubble suspension measured at four different acoustic excitation ampli-tudes. The attenuation data are used to determine interfacial rheological properties (surface tension,surface dilatational elasticity, and surface dilatational viscosity) of the encapsulation according tothree different models. Although different models result in similar rheological properties, attenua-tion measured at different excitation levels (4–110 kPa) leads to different values for them; the dila-tation elasticity (0.56 to 0.18 N/m) and viscosity (2.4108to 1.52108Ns/m) both decreasewith increasing pressure. Numerically simulating the scattered response, nonlinear energy transferbetween frequencies are shown to be negligible, thereby demonstrating the linearity in propagationand validating the attenuation analysis. There is a second concern to the characterization arisingfrom shell properties being dependent on excitation amplitude, which is not a proper constitutivevariable. It is resolved by arriving at a strain-dependent rheology for the encapsulation. The limita-tions of the underlying analysis are discussed.

  • Kumar KN, Sarkar K 2015 “Effects of ambient hydrostatic pressure on the material properties of the encapsulation of an ultrasound contrast microbubble,” Journal of the Acoustical Society of America, 138, 624-634.

    Ultrasound contrast microbubbles experience widely varying ambient blood pressure in differentorgans, which can also change due to diseases. Pressure change can alter the material properties ofthe encapsulation of these microbubbles. Here the characteristic rheological parameters of contrastagent Definity are determined by varying the ambient pressure (in a physiologically relevant range0–200 mm Hg). Four different interfacial rheological models are used to characterize the microbub-bles. Effects of gas diffusion under excess ambient pressure are investigated in detail accountingfor size decrease of contrast microbubbles. Definity contrast agent show a change in their interfacialdilatational viscosity (3.6108Ns/m at 0 mm Hg to 4.45108Ns/m at 200 mm Hg) and inter-facial dilatational elasticity (0.86 N/m at 0 mm Hg to 1.06 N/m at 200 mm Hg) with ambient pres-sure increase. The increase results from material consolidation, similar to such enhancement inbulk properties under pressure. The model that accounts for enhancement in material propertieswith increasing ambient pressure matches with experimentally measured subharmonic response asa function of ambient pressure, while assuming constant material parameters does not.

  • Nahire R, Hossain R, Patel R, Paul S, Ambre AH, Meghnani V, Layek B, Katti KS, Gange KN, Leclarc E, Srivastava D K, Sarkar K, Mallik S 2014 “Multifunctional polymersomes for cytosolic delivery of gemcitabine and doxorubicin to cancer cells,” Biomaterials, 35, 6482-6497.

    Although liposomes are widely used as carriers of drugs and imaging agents, they suffer from a lack ofstability and the slow release of the encapsulated contents at the targeted site. Polymersomes (vesicles ofamphiphilic polymers) are considerably more stable compared to liposomes; however, they alsodemonstrate a slow release for the encapsulated contents, limiting their efficacy as a drug-delivery tool.As a solution, we prepared and characterized echogenic polymersomes, which are programmed torelease the encapsulated drugs rapidly when incubated with cytosolic concentrations of glutathione.These vesicles encapsulated air bubbles inside and efficiently reflected diagnostic-frequency ultrasound.Folate-targeted polymersomes showed an enhanced uptake by breast and pancreatic-cancer cells in amonolayer as well as in three-dimensional spheroid cultures. Polymersomes encapsulated with theanticancer drugs gemcitabine and doxorubicin showed significant cytotoxicity to these cells. Withfurther improvements, these vesicles hold the promise to serve as multifunctional nanocarriers, offeringa triggered release as well as diagnostic ultrasound imaging.

  • Nahire R, Halder M, Paul S, Margoum A, Ambre AH, Katti KS, Gange KN, Srivastava D K, Sarkar K, Mallik S 2014 “pH-Triggered Echogenicity and Contents Release from Liposomes,” Molecular Pharamaceutics, 11, 4059-4068.

    Liposomes are representative lipid nanoparticles widelyused for delivering anticancer drugs, DNA fragments, or siRNA to cancercells. Upon targeting, various internal and external triggers have been usedto increase the rate for contents release from the liposomes. Among theinternal triggers, decreased pH within the cellular lysosomes has beensuccessfully used to enhance the rate for releasing contents. However,imparting pH sensitivity to liposomes requires the synthesis of specializedlipids with structures that are substantially modified at a reduced pH.Herein, we report an alternative strategy to render liposomes pH sensitiveby encapsulating a precursor which generates gas bubblesin situinresponse to acidic pH. The disturbance created by the escaping gasbubbles leads to the rapid release of the encapsulated contents from theliposomes. Atomic force microscopic studies indicate that the liposomalstructure is destroyed at a reduced pH. The gas bubbles also render theliposomes echogenic, allowing ultrasound imaging. To demonstrate the applicability of this strategy, we have successfully targeteddoxorubicin-encapsulated liposomes to the pancreatic ductal carcinoma cells that overexpress the folate receptor on the surface.In response to the decreased pH in the lysosomes, the encapsulated anticancer drug is efficiently released. Contents releasedfrom these liposomes are further enhanced by the application of continuous wave ultrasound (1 MHz), resulting in substantiallyreduced viability for the pancreatic cancer cells (14%).

  • Paul S, Nahire R, Mallik S, Sarkar K 2014 “Encapsulated microbubbles and echogenic liposomes for contrast ultrasound imaging and targeted drug delivery,” Computational Mechanics, 53,413-435.

    Micron- to nanometer-sized ultrasound agents,like encapsulated microbubbles and echogenic liposomes,are being developed for diagnostic imaging and ultra-sound mediated drug/gene delivery. This review providesan overview of the current state of the art of the mathe-matical models of the acoustic behavior of ultrasound con-trast microbubbles. We also present a review of the in vitroexperimental characterization of the acoustic properties ofmicrobubble based contrast agents undertaken in our lab-oratory. The hierarchical two-pronged approach of model-ing contrast agents we developed is demonstrated for a lipidcoated (SonazoidTM)and a polymer shelled (polyD-L-lactic acid) contrast microbubbles. The acoustic and drugrelease properties of the newly developed echogenic lipo-somes are discussed for their use as simultaneous imagingand drug/gene delivery agents. Although echogenicity is con-clusively demonstrated in experiments, its physical mecha-nisms remain uncertain. Addressing questions raised herewill accelerate further development and eventual clinicalapproval of these novel technologies.

  • Nahire R, Halder M, Paul S, Margoum A, Ambre AH, Katti KS, Gange KN, Srivastava D K, Sarkar K, Mallik S 2013 “Polymer Coated Echogenic Lipid Nanoparticles with dual release triggers,” Biomacromolecules, 14, 841-853.

    Although lipid nanoparticles are promising drugdelivery vehicles, passive release of encapsulated contents atthe target site is often slow. Herein, we report contents releasefrom targeted, polymer-coated, echogenic lipid nanoparticles inthe cell cytoplasm by redox trigger and simultaneouslyenhanced by diagnostic frequency ultrasound. The lipidnanoparticles were polymerized on the external leaflet usinga disulfide cross-linker. In the presence of cytosolicconcentrations of glutathione, the lipid nanoparticles released76% of encapsulated contents. Plasma concentrations ofglutathione failed to releasethe encapsulated contents.Application of 3 MHz ultrasound for 2 min simultaneouslywith the reducing agent enhanced the release to 96%. Folicacid conjugated, doxorubicin-loaded nanoparticles showed enhanced uptake and higher cytotoxicity in cancer cells overexpressingthe folate receptor (compared to the control). With further developments, these lipid nanoparticles have the potential to be usedas multimodal nanocarriers for simultaneous targeted drug delivery and ultrasound imaging.

  • Mukherjee S, Sarkar K 2013 “Effects of matrix viscoelasticity on the lateral migration of a deformable drop in a wall-bounded shear,” Journal of Fluid Mechanics, 727, 318-345.

    The dynamics of a drop deforming, orienting and moving in a shear flow of aviscoelastic liquid near a wall is numerically investigated using a front-tracking finite-difference method and a semi-analytic theory. The viscoelasticity is modelled usingthe modified FENE-CR constitutive equation. In a Newtonian system, deformation in adrop breaks the reversal symmetry of the system resulting in a migration away fromthe wall. This study shows that the matrix elasticity reduces the migration velocity, thereduction scaling approximately linearly with viscoelasticity (product of the Deborah number De and the ratio of polymer viscosity to total viscosity β). Similar to a Newtonian system, for small Deborah numbers, the dynamics quickly reaches a quasi-steady state where deformation, inclination, as well as migration and slip velocitiesbecome independent of the initial drop–wall separation. They all approximately scaleinversely with the square of the instantaneous separation except for deformation whichscales inversely with the cube of separation. The deformation shows a non-monotonicvariation with increasing viscoelasticity similar to the case of a drop in an unboundedshear and is found to influence little the change in migration. Two competing effectsdue to matrix viscoelasticity on drop migration are identified. The first stems fromthe reduced inclination angle of the drop with increasing viscoelasticity that tries toenhance migration velocity. However, it is overcome by the second effect inhibitingmigration that results from the normal stress differences from the curved streamlinesaround the drop; they are more curved on the side away from the wall comparedwith those in the gap between the wall and the drop, an effect that is also presentfor a rigid particle. A perturbative theory of migration is developed for small ratioof the drop size to its separation from the wall that clearly shows the migrationto be caused by the image stresslet field due to the drop in presence of the wall. The theory delineates the two competing viscoelastic effects, their relative magnitudes, and predicts migration that matches well with the simulation. Using the simulationresults and the stresslet theory, we develop an algebraic expression for the quasi-steadymigration velocity as a function of Ca, De and β. The transient dynamics of themigrating drop is seen to be governed by the finite time needed for development of theviscoelastic stresses. For larger capillary numbers, in both Newtonian and viscoelasticmatrices, a viscous drop fails to reach a quasi-steady state independent of initialdrop–wall separation. Matrix viscoelasticity tends to prevent drop breakup. Drops that† Email address for correspondence: sarkar@gwu.edu

     

     

  • Duraiswami R, Sarkar K, Chahine GL 1998 "Efficient 2D and 3D electrical impedance tomography using dual reciprocity boundary element techniques," Engineering Analysis with Boundary Elements, 22, 13-31.

    This paper presents applications of boundary element methods to electrical impe- dance tomography. An algorithm for imaging the interior of a domain that consists of regions of constant conductivity is developed, that makes use of a simpler parametrization of the shapes of the regions to achieve efficiency. Numerical results from tests of this algorithm on synthetic data are presented, and show that the method is quite promising.

  • Chatterjee D, Sarkar K 2003 “A Newtonian rheological model for the interface of microbubble contrast agents,” Ultrasound in Medicine and Biology, 29, 1749-1757.

    A quantitative model of the dynamics of an encapsulated microbubble contrast agent will be avaluable tool in contrast ultrasound (US). Such a model must have predictive ability for widely varyingfrequencies and pressure amplitudes. We have developed a new model for contrast agents, and successfullyinvestigated its applicability for a wide range of operating parameters. The encapsulation is modeled as acomplex interface of an infinitesimal thickness. A Newtonian rheology with surface viscosities and interfacialtension is assumed for the interface, and a modified Rayleigh–Plesset equation is derived. The rheologicalparameters (surface tension and surface dilatational viscosity) for a number of contrast agents (Albunex,Optisonand Quantison) are determined by matching the linearized model dynamics with experimentallyobtained attenuation data. The model behavior for Optison(surface tension 0.9 N/m and surface dilatationalviscosity 0.08 msP) was investigated in detail. Specifically, we have carried out a detailed interrogation of themodel, fitted in the linear regime, for its nonlinear prediction. In contrast to existing models, the new model isfound to capture the characteristic subharmonic emission of Optisonobserved by Shi et al. (1999). A detailedparametric study of the bubble behavior was executed using the ratio of scattering to attenuation (STAR). Itshows that the encapsulation drastically reduces the influence of resonance frequency on scattering cross-section,suggesting possible means of improvement in imaging at off-resonant frequencies. The predictive capability of thepresent model indicates that it can be used for characterizing different agents and designing new ones.

  • Sarkar K, Shi WT, Chatterjee D, Forsberg F 2005 “Characterization of ultrasound contrast microbubbles using in vitro experiments and viscous and viscoelastic interface models for encapsulation,” Journal of the Acoustical Society of America, 118, 539-550.

    Zero-thickness interface models are developed to describe the encapsulation of microbubblecontrast agents. Two different rheological models of the interface, Newtonianviscousandviscoelastic, with rheological parameters such as surface tension, surface dilatational viscosity, andsurface dilatational elasticity are presented to characterize the encapsulation. The models are appliedto characterize a widely used microbubble based ultrasound contrast agent. Attenuation ofultrasound passing through a solution of contrast agent is measured. The model parameters for thecontrast agent are determined by matching the linearized model dynamics with measuredattenuation data. The models are investigated for its ability to match with other experiments.Specifically, model predictions are compared with scattered fundamental and subharmonicresponses. Experiments and model prediction results are discussed along with thoseobtained using an existing modelChurch, J. Acoust. Soc. Am.97, 15101995and Hoffet al.,J. Acoust. Soc. Am.107, 22722000of contrast agents.

  • Chatterjee D, Sarkar K, Jain P, Schreppler N 2005 “On the suitability of broadband attenuation measurement for characterizing contrast microbubbles,” Ultrasound in Medicine and Biology, 31,781-786.

    Broadband attenuation measurement has been widely used for characterizing ultrasound contrastagents. Chen et al. (2002) recently suggested that broadband attenuation data depend on the center frequency ofthe broadband excitation pulse and, therefore, that they are not a reliable measure of the bubble behavior. Weinvestigated the suitability of measurement of broadband attenuation as a characterizing tool using the contrastagent Definity®as a test case. Analyzing the attenuation data obtained with three broadband unfocusedtransducers with different center frequencies (2.25, 3.5 and 5 MHz), we found that attenuation is independent ofthe transducer used and matches in the overlap regions of any two transducers. Attenuation does not depend onexcitation pressure amplitude as long as the excitation amplitude remains below a critical value (0.26 MPa),indicating that the measurement of broadband attenuation below critical excitation can, indeed, be used forcharacterization. Furthermore, the linear relationship of attenuation with concentrations of Definity®is alsoinvestigated.

  • Katiyar A, Sarkar K, Jain P, 2009 “Effects of encapsulation elasticity on the stability of an encapsulated microbubble,” Journal of Colloid and Interface Science, 336, 519-525.

    A model for gas transport from an encapsulated microbubble into the surrounding medium is developedand investigated incorporating the effects of encapsulation elasticity. Encapsulation elasticity stabilizesmicrobubbles against dissolution and explains the long shelf life of microbubble contrast agent. We con-sider air bubbles as well as bubbles containing perfluorocarbon gas. Analytical conditions between satu-ration level, surface tension and interfacial dilatational elasticity are determined for attaining non-zeroequilibrium radius for these microbubbles. Numerical solution of the equation verifies the stability ofthe equilibrium radii. In an undersaturated medium all encapsulated bubbles dissolve. In a saturatedmedium, an encapsulated bubble is found to achieve a long-time stable radius when interfacial dilata-tional elasticity is larger than equilibrium surface tension. For bubbles with interfacial dilatational elas-ticity smaller than the equilibrium surface tension, stable bubble of non-zero radius can be achieved onlywhen the saturation level is greater than a critical value. Even if they initially contain a gas other than air,bubbles that reach a stable radius finally become air bubbles. The model is applied to an octafluoropro-pane filled lipid-coated 2.5lm bubble, which displayed a transient swelling due to air intake beforereaching an equilibrium size. Effects of elasticity, shell permeability, initial mole fraction, initial radiusand saturation level are investigated and discussed. Shell permeability and mole fraction do not affectthe final equilibrium radius of the microbubble but affect the time scale and the transient dynamics. Sim-ilarly, the ratio of equilibrium radius to initial radius remains unaffected by the variation in initial radius.

  • Sarkar K, Katiyar A, Jain P 2009 “Growth and dissolution of an encapsulated contrast microbubble: effects of encapsulation permeability,” Ultrasound in Medicine and Biology, 35, 1385-1396.

    Gas diffusion from an encapsulated microbubble is modeled using an explicit linear relation for gaspermeation through the encapsulation. Both the cases of single gas (air) and multiple gases (perfluorocarbon insidethe bubble and air dissolved in surrounding liquid) are considered. An analytical expression for the dissolutiontime for an encapsulated air bubble is obtained; it showed that for small permeability the dissolution time increaseslinearly with decreasing permeability. A perfluorocarbon-filled contrast microbubble such as DefinityÒwas pre-dicted to experience a transient growth because of air infusion before it dissolves in conformity with previousexperimental findings. The growth phase occurs only for bubbles with a critical value of initial mole fraction ofperfluorocarbon relative to air. With empirically obtained property values, the dissolution time of a 2.5-microndiameter (same as that of Definity), lipid-coated octafluoropropane bubble, with surface tension 25 mN/m, is pre-dicted to be 42 min in an air-saturated medium. The properties such as shell permeability, surface tension andrelative mole fraction of octafluoropropane are varied to investigate their effects on the time scales of bubblegrowth and dissolution, including their asymptotic scalings where appropriate. The dissolution dynamics scaleswith permeability, in that when the time is nondimensioanlized with permeability, curves for different permeabil-ities collapse on a single curve. Investigation of bubbles filled with other gases (nonoctafluoropropane perfluoro-carbon and sulfur hexafluoride) indicates longer dissolution time because of lower solubility and lowerdiffusivity for larger gas molecules. For such micron-size encapsulated bubbles, lifetime of hours is possibleonly at extremely low surface tension (,1 mN/m) or at extreme oversaturation.(E-mail:sarkar@udel.edu)Ó2009 World Federation for Ultrasound in Medicine & Biology.

  • Katiyar A, Sarkar K, 2010 “Stability Analysis of an Encapsulated Microbubble against Gas Diffusion,” Journal of Colloid and Interface Science, 343, 42-47.

    Linear stability analysis is performed for a mathematical model of diffusion of gases from an encapsulatedmicrobubble. It is an Epstein–Plesset model modified to account for encapsulation elasticity and finite gaspermeability. Although bubbles, containing gases other than air, are considered, the final stable bubble, ifany, contains only air, and stability is achieved only when the surrounding medium is saturated or over-saturated with air. In absence of encapsulation elasticity, only a neutral stability is achieved for zero sur-face tension, the other solution being unstable. For an elastic encapsulation, different equilibriumsolutions are obtained depending on the saturation level and whether the surface tension is smaller orhigher than the elasticity. For an elastic encapsulation, elasticity can stabilize the bubble. However,imposing a non-negativity condition on the effective surface tension (consisting of reference surface ten-sion and the elastic stress) leads to an equilibrium radius which is only neutrally stable. If the encapsu-lation can support a net compressive stress, it achieves actual stability. The linear stability results areconsistent with our recent numerical findings. Physical mechanisms for the stability or instability of var-ious equilibriums are provided.

  • Paul S, Katiyar A, Sarkar K, Chatterjee D, Shi WT, Forsberg F 2010 “Material characterization of the encapsulation of an ultrasound contrast microbubble and its subharmonic response: Strain-softening interfacial elasticity model,” Journal of the Acoustical Society of America, 127, 3846-3857.

    Two nonlinear interfacial elasticity models—interfacial elasticity decreasing linearly andexponentially with area fraction—are developed for the encapsulation of contrast microbubbles. Thestrain softeningdecreasing elasticityresults from the decreasing association between theconstitutive molecules of the encapsulation. The models are used to find the characteristic propertiessurface tension, interfacial elasticity, interfacial viscosity and nonlinear elasticity parametersfor acommercial contrast agent. Properties are found using the ultrasound attenuation measured througha suspension of contrast agent. Dynamics of the resulting models are simulated, compared withother existing models and discussed. Imposing non-negativity on the effective surface tensiontheencapsulation experiences no net compressive stressshows “compression-only” behavior. Theexponential and the quadraticlinearly varying elasticitymodels result in similar behaviors. Thevalidity of the models is investigated by comparing their predictions of the scattered nonlinearresponse for the contrast agent at higher excitations against experimental measurement. All modelspredict well the scattered fundamental response. The nonlinear strain softening included in theproposed elastic models of the encapsulation improves their ability to predict subharmonic response.They predict the threshold excitation for the initiation of subharmonic response and its subsequentsaturation.

  • Katiyar A, Sarkar K 2011 “Excitation threshold for subharmonic generation from contrast microbubbles,” Journal of the Acoustical Society of America, 130, 3137-3147.

    Six models of contrast microbubbles are investigated to determine the excitation threshold for sub-harmonic generation. The models are applied to a commercial contrast agent; its characteristic pa-rameters according to each model are determined using experimentally measured ultrasoundattenuation. In contrast to the classical perturbative result, the minimum threshold for subharmonicgeneration is not always predicted at excitation with twice the resonance frequency; instead itoccurs over a range of frequencies from resonance to twice the resonance frequency. The quantita-tive variation of the threshold with frequency depends on the model and the bubble radius. All mod-els are transformed into a common interfacial rheological form, where the encapsulation isrepresented by two radius dependent surface properties—effective surface tension and surface dila-tational viscosity. Variation of the effective surface tension with radius, specifically having anupper limit (resulting from strain softening or rupture of the encapsulation during expansion), playsa critical role. Without the upper limit, the predicted threshold is extremely large, especially nearthe resonance frequency. Having a lower limit on surface tension (e.g., zero surface tension in thebuckled state) increases the threshold value at twice the resonance frequency, in some cases shiftingthe minimum threshold toward resonance.

  • Katiyar A, Sarkar K, Forsberg F 2011 “Modeling subharmonic response from contrast microbubbles as a function of ambient static pressure,” Journal of the Acoustical Society of America, 129, 2325-2335.

    Variation of subharmonic response from contrast microbubbles with ambient pressure is numericallyinvestigated for non-invasive monitoring of organ-level blood pressure. Previously, several contrastmicrobubbles bothin vitroandin vivoregistered approximately linear (5–15 dB) subharmonicresponse reduction with 188 mm Hg change in ambient pressure. In contrast, simulated subharmonicresponse from a single microbubble is seen here to either increase or decrease with ambient pressure.This is shown using the code BUBBLESIM for encapsulated microbubbles, and then the underlyingdynamics is investigated using a free bubble model. The ratio of the excitation frequency to the natu-ral frequency of the bubble is the determining parameter—increasing ambient pressure increases nat-ural frequency thereby changing this ratio. For frequency ratio below a lower critical value,increasing ambient pressure monotonically decreases subharmonic response. Above an upper criticalvalue of the same ratio, increasing ambient pressure increases subharmonic response; in between, thesubharmonic variation is non-monotonic. The precise values of frequency ratio for these three differ-ent trends depend on bubble radius and excitation amplitude. The modeled increase or decrease ofsubharmonic with ambient pressure, when one happens, is approximately linear only for certain rangeof excitation levels. Possible reasons for discrepancies between model and previous experiments arediscussed.

  • Katiyar A, Sarkar K 2012 “Effects of encapsulation damping on excitation threshold for subharmonic generation from contrast microbubbles,” Journal of the Acoustical Society of America, 132, 3576-3585.

    A recent study [Katiyar and Sarkar (2011). J. Acoust. Soc. Am.130, 3137–3147] showed that incontrast to the analytical result for free bubbles, the minimum threshold for subharmonic generationfor contrast microbubbles does not necessarily occur at twice the resonance frequency. Hereincreased damping—either due to the small radius or the encapsulation—is shown to shift the mini-mum threshold away from twice the resonance frequency. Free bubbles as well as four modelsof the contrast agent encapsulation are investigated varying the surface dilatational viscosity.Encapsulation properties are determined using measured attenuation data for a commercial contrastagent. For sufficiently small damping, models predict two minima for the threshold curve—one attwice the resonance frequency being lower than the other at resonance frequency—in accord withthe classical analytical result. However, increased damping damps the bubble response more attwice the resonance than at resonance, leading to a flattening of the threshold curve and a gradualshift of the absolute minimum from twice the resonance frequency toward the resonance frequency.The deviation from the classical result stems from the fact that the perturbation analysis employedto obtain it assumes small damping, not always applicable for contrast microbubbles.

  • Paul S, Russakow D, Rodger T, Sarkar K, Cochran M, Wheatley M 2013 “Determination of the interfacial rheological properties of a Poly(DL-Lactic Acid)-encapsulated contrast agent using in vitro attenuation and scattering,” Ultrasound in Medicine and Biology

    The stabilizing encapsulation of a microbubble-based ultrasound contrast agent (UCA) critically affectsits acoustic properties. Polymers, which behave differently from materials commonly used (i.e.,lipids or proteins)for monolayer encapsulation, have the potential for better stability and improved control of encapsulation prop-erties. Air-filled microbubbles coated with poly(DL-lactic acid) (PLA) are characterized here usingin vitroacousticexperiments and several models of encapsulation. The interfacial rheological properties of the encapsulation aredetermined according to each model using attenuation of ultrasound through a suspension of microbubbles.Then the model predictions are compared with scattered non-linear (sub- and second harmonic) responses. Forthis microbubble population (average diameter, 1.9mm), the peak in attenuation measurement indicatesa weighted-average resonance frequency of 2.5–3 MHz, which, in contrast to other encapsulated microbubbles,is lower than the resonance frequency of a free bubble of similar size (diameter, 1.9mm). This apparently contra-dictory result stems from the extremely low surface dilational elasticity (around 0.01–0.07 N/m) and the reducedsurface tension of the poly(DL-lactic acid) encapsulation, as well as the polydispersity of the bubble population. Allmodels considered here are shown to behave similarly even in the non-linear regime because of the low surface dila-tional elasticity value. Pressure-dependent scattering measurements at two different excitation frequencies (2.25and 3 MHz) revealed strongly non-linear behavior with 25–30 dB and 5–20 dB enhancements in fundamentaland second-harmonic responses, respectively, for a contrast agent concentration of 1.33mg/mL in the suspension.Sub-harmonic responses are registered above a relatively low generation threshold of 100–150 kPa, with up to 20dB enhancement beyond that pressure. Numerical predictions from all models show good agreement with theexperimentally measured fundamental response, but not with the experimental second-harmonic response. Thecharacteristic features of sub-harmonic responses and the steady response beyond the threshold are matchedwell by model predictions. However, prediction of the threshold value depends on estimated properties and sizedistribution. The variation in size distribution from sample to sample leads to variation in estimates of encapsula-tion properties: the lowest estimated value for surface dilational viscosity better predicts the sub-harmonicthreshold.

  • Kumar KN, Sarkar K 2015 “Effects of ambient hydrostatic pressure on the material properties of the encapsulation of an ultrasound contrast microbubble,” Journal of the Acoustical Society of America, 138, 624-634.

    Ultrasound contrast microbubbles experience widely varying ambient blood pressure in differentorgans, which can also change due to diseases. Pressure change can alter the material properties ofthe encapsulation of these microbubbles. Here the characteristic rheological parameters of contrastagent Definity are determined by varying the ambient pressure (in a physiologically relevant range0–200 mm Hg). Four different interfacial rheological models are used to characterize the microbub-bles. Effects of gas diffusion under excess ambient pressure are investigated in detail accountingfor size decrease of contrast microbubbles. Definity contrast agent show a change in their interfacialdilatational viscosity (3.6108Ns/m at 0 mm Hg to 4.45108Ns/m at 200 mm Hg) and inter-facial dilatational elasticity (0.86 N/m at 0 mm Hg to 1.06 N/m at 200 mm Hg) with ambient pres-sure increase. The increase results from material consolidation, similar to such enhancement inbulk properties under pressure. The model that accounts for enhancement in material propertieswith increasing ambient pressure matches with experimentally measured subharmonic response asa function of ambient pressure, while assuming constant material parameters does not.

  • Lang X, Porter T, Sarkar K 2015 “Interpreting attenuation at different excitation amplitudes to estimate strain-dependent interfacial rheological properties of lipid-coated monodisperse microbubbles,” Journal of the Acoustical Society of America, 138, 3994-4003.

    Broadband attenuation of ultrasound measured at different excitation pressures being differentraises a serious theoretical concern, because the underlying assumption of linear and independentpropagation of different frequency components nominally requires attenuation to be independent ofexcitation. Here, this issue is investigated by examining ultrasound attenuation through a monodis-perse lipid-coated microbubble suspension measured at four different acoustic excitation ampli-tudes. The attenuation data are used to determine interfacial rheological properties (surface tension,surface dilatational elasticity, and surface dilatational viscosity) of the encapsulation according tothree different models. Although different models result in similar rheological properties, attenua-tion measured at different excitation levels (4–110 kPa) leads to different values for them; the dila-tation elasticity (0.56 to 0.18 N/m) and viscosity (2.4108to 1.52108Ns/m) both decreasewith increasing pressure. Numerically simulating the scattered response, nonlinear energy transferbetween frequencies are shown to be negligible, thereby demonstrating the linearity in propagationand validating the attenuation analysis. There is a second concern to the characterization arisingfrom shell properties being dependent on excitation amplitude, which is not a proper constitutivevariable. It is resolved by arriving at a strain-dependent rheology for the encapsulation. The limita-tions of the underlying analysis are discussed.

  • Kumar KN, Sarkar K 2016 “Interfacial rheological properties of contrast microbubble Targestar P as a function of ambient pressure,” Ultrasound in Medicine and Biology, 42, 1010-1017.

    In this Technical Note, we determine the interfacial rheological parameters of the encapsulation of thecontrast agent Targestar P using ultrasound attenuation. The characteristic parameters are obtained according totwo interfacial rheological models. The properties—surface dilatational elasticity (0.09 ± 0.01 N/m) and surfacedilatational viscosity (8 ± 0.1E–9 N$s/m)—are found to be of similar magnitude for both models. Contrast micro-bubbles experience different ambient pressure in different organs. We also measure these parameters as functionsof ambient pressure using attenuation measured at different overpressures (0, 100 and 200 mm Hg). For each valueof ambient hydrostatic pressure, we determine the rheological properties, accounting for changes in the size dis-tribution caused by the pressure change. We discuss different models of size distribution change under overpres-sure: pure adiabatic compression or gas exchange with surrounding medium. The dilatational surface elasticityand viscosity are found to increase with increasing ambient pressure.

  • Xia L, Karandish F, Kumar KN, Froberg J, Kulkarni P, Gange KN, Choi Y, Mallik S, Sarkar K 2017 “Acoustic characterization of echogenic polymersomes prepared from amphiphilic block copolymers,” Ultrasound in Medicine and Biology, 44, 447-457.

    Polymersomes are a class of artificial vesicles prepared from amphiphilic polymers. Like lipid vesicles(liposomes), they too can encapsulate hydrophilic and hydrophobic drug molecules in the aqueous core and thehydrophobic bilayer respectively, but are more stable than liposomes. Although echogenic liposomes have beenwidely investigated for simultaneous ultrasound imaging and controlled drug delivery, the potential of thepolymersomes remains unexplored. We prepared two different echogenic polymersomes from the amphiphilic co-polymers polyethylene glycol–poly-DL-lactic acid (PEG-PLA) and polyethylene glycol–poly-L-lactic acid (PEG-PLLA), incorporating multiple freeze-dry cycles in the synthesis protocol to ensure their echogenicity. We investigatedacoustic behavior with potential applications in biomedical imaging. We characterized the polymeric vesicles acous-tically with three different excitation frequencies of 2.25, 5 and 10 MHz at 500 kPa. The polymersomes exhibitedstrong echogenicity at all three excitation frequencies (about 50- and 25-dB enhancements in fundamental andsubharmonic, respectively, at 5-MHz excitation from 20g/mL polymers in solution). Unlike echogenic lipo-somes, they emitted strong subharmonic responses. The scattering results indicated their potential as contrastagents, which was also confirmed by clinical ultrasound imaging.

  • Karandish F, Haldar MK, Xia L, Gange KN, Feng L, You S, Choi Y, Sarkar K, Mallik S  2018 “Nucleus-targeted, echogenic polymersomes for delivering a cancer stemness inhibitor to pancreatic cancer cells,” Biomacromolecules, 19,4122-4132.

    Chemotherapeutic agents for treating cancers show considerable sideeffects, toxicity, and drug resistance. To mitigate the problems, we designed nucleus-targeted, echogenic, stimuli-responsive polymeric vesicles (polymersomes) to transport andsubsequently release the encapsulated anticancer drugs within the nuclei of pancreaticcancer cells. We synthesized an alkyne-dexamethasone derivative and conjugated it to N3−polyethylene glycol (PEG)−polylactic acid (PLA) copolymer employing the Cu2+catalyzed“Click”reaction. We prepared polymersomes from the dexamethasone−PEG−PLA conjugate along with a synthesized stimuli-responsive polymer PEG−S−S−PLA. Thedexamethasone group dilates the nuclear pore complexes and transports the vesicles to thenuclei. We designed the polymersomes to release the encapsulated drugs in the presence ofa high concentration of reducing agents in the nuclei of pancreatic cancer cells. Weobserved that the nucleus-targeted, stimuli-responsive polymersomes released 70% ofencapsulated contents in the nucleus-mimicking environment in 80 min. We encapsulatedthe cancer stemness inhibitor BBI608 in the vesicles and observed that the BBI608encapsulated polymersomes reduced the viability of the BxPC3 cells to 43% in three-dimensional spheroid cultures. Thepolymersomes were prepared following a special protocol so that they scatter ultrasound, allowing imaging by a medicalultrasound scanner. Therefore, these echogenic, targeted, stimuli-responsive, and drug-encapsulated polymersomes have thepotential for trackable, targeted carrier of chemotherapeutic drugs to cancer cell nuclei.

  • Kulkarni P, Haldar MK, Karandish F, Confeld M, Hossain R, Borowicz P, Gange KN, Xia L, Sarkar K, Mallik S 2018 “Tissue-penetrating, hypoxia-responsive echogenic polymersomes for drug delivery to solid tumors,” Chemistry A European Journal, 24, 12490-12494.

    Hypoxia in solid tumors facilitates the progres-sion of the disease, develops resistance to chemo and radiotherapy, and contributes to relapse. Due to the lack of tumor penetration, most of the reported drug carriers are unable to reach the hypoxic niches of the solid tumors. We have developed tissue-penetrating, hypoxia-responsive echogenic polymersomes to deliver anti cancer drugs to solid tumors. The polymersomes are composed of a hy-poxia-responsive azobenzene conjugated and a tissue penetrating peptide functionalized polylactic acid-polyethylene glycol polymer. The drug-encapsulated, hypoxia-responsive polymersomes substantially decreased the viability of pancreatic cancer cells in spheroidal cultures. Under normoxic conditions, polymersomes were echogenic at diagnostic ultrasound frequencies but lose the echogenicity under hypoxia. In vivo imaging studies with xenograft mouse model further confirmed the ability of the polymersomes to target, penetrate, and deliver the encapsulated contents in hypoxic pancreatic tumor tissues.

  • Aliabouzar M, Kumar KN, Sarkar K, 2018 “Acoustic vaporization threshold of lipid coated perfluoropentane droplets,” Journal of the Acoustical Society of America, 143, 2001-2012.

    Phase shift droplets vaporizable by acoustic stimulation offer the advantages of producing micro-bubbles as contrast agentsin situas well as higher stability and the possibility of achieving smallersizes. Here, the acoustic droplet vaporization (ADV) threshold of a suspension of droplets with aperfluoropentane (PFP) core (diameter 400–3000 nm) is acoustically measured as a function of theexcitation frequency in a tubeless setup at room temperature. The changes in scattered responses—fundamental, sub-, and second harmonic—are investigated, a quantitative criterion is used to deter-mine the ADV phenomenon, and findings are discussed. The average threshold obtained using threedifferent scattered components increases with frequency—1.0560.28 MPa at 2.25 MHz,1.8960.57 MPa at 5 MHz, and 2.3460.014 MPa at 10 MHz. The scattered response from vapor-ized droplets was also found to qualitatively match with that from an independently prepared lipid-coated microbubble suspension in magnitude as well as trends above the determined ADV thresh-old value.

  • Mobadersany N, Sarkar K 2019 “Acoustic microstreaming near a plane wall due to a pulsating free or coated bubble: velocity, vorticity and closed streamlines,” Journal of Fluid Mechanics, 875 781-806.

    Acoustic microstreaming due to an oscillating microbubble, either coated or free, is analytically investigated. The detailed flow field is obtained and the closed streamlines of the ring vortex generated by microstreaming are plotted in both Eulerian and Lagrangian descriptions. Analytical expressions are found for the ring vortex showing that its length depends only on the separation of the microbubble from the wall
    and the dependence is linear. The circulation as a scalar measure of the vortex is computed quantitatively identifying its spatial location. The functional dependence of circulation on bubble separation and coating parameters is shown to be similar to that of the shear stress.

  • Aliabouzar M, Kumar KN, Sarkar K, 2019 “Effects of droplet size and perfluorocarbon boiling point on the frequency dependence of acoustic vaporization threshold,” Journal of the Acoustical Society of America, 145, 1105-1106.

    Phase shift liquid perfluorocarbon (PFC) droplets vaporizable by ultrasound into echogenicmicrobubble above a threshold pressure, termed acoustic droplet vaporization (ADV), are usedfor therapeutic and diagnostic applications. This study systematically investigated the effect ofexcitation frequency (2.25, 10, and 15 MHz) on the ADV and inertial cavitation (IC) thresholds oflipid-coated PFC droplets of three different liquid cores—perfluoropentane (PFP), perfluorohexane(PFH), and perfluorooctyl bromide (PFOB)—and of two different sizes—average diameters smallerthan 3lm and larger than 10lm—in a tubeless setup. This study found that the ADV thresholdincreases with frequency for the lowest boiling point liquid, PFP, for both large and small sizedroplets. For higher boiling point liquids, PFH and PFOB, this study did not detect vaporization forsmall size droplets at the excitation levels (maximum 4 MPa peak negative) studied here. The largePFOB droplets experienced ADV only at the highest excitation frequency 15 MHz. For large PFHdroplets, ADV threshold decreases with frequency that could possibly be due to the superharmonicfocusing being a significant effect at larger sizes and the higher excitation pressures. ADV thresh-olds at all the frequencies studied here occurred at lower rarefactional pressures than IC thresholdsindicating that phase transition precedes inertial cavitation.

  • Osborn J, Pullan JE, Froberg J, Shreffler J, Gange KN, Molden T, Choi Y, Brooks A, Mallik S, Sarkar K 2020 "Echogenic exosomes as ultrasound contrast agents" Nanoscale Advances, 2, 3411-3422

    Exosomes are naturally secreted extracellular bilayer vesicles (diameter 40–130 nm), which have recently been found to play a critical role in cell-to-cell communication and biomolecule delivery. Their unique characteristics—stability, permeability, biocompatibility and low immunogenicity—have made them a prime candidate for use in delivering cancer therapeutics and other natural products. Here we present the first ever report of echogenic exosomes, which combine the benefits of the acoustic responsiveness of traditional microbubbles with the non-immunogenic and small-size morphology of exosomes. Microbubbles, although effective as ultrasound contrast agents, are restricted to intravascular usage due to their large size. In the current study, we have rendered bovine milk-derived exosomes echogenic by freeze drying them in the presence of mannitol. Ultrasound imaging and direct measurement of linear and nonlinear scattered responses were used to investigate the echogenicity and stability of the prepared exosomes. A commercial scanner registered enhancement (28.9% at 40 MHz) in the brightness of ultrasound images in presence of echogenic exosomes at 5 mg mL1 . The exosomes also showed significant linear and nonlinear scattered responses—11 dB enhancement in fundamental, 8.5 dB in subharmonic and 3.5 dB in second harmonic all at 40 mg mL1 concentration. Echogenic exosomes injected into the tail vein of mice and the synovial fluid of rats resulted in significantly higher brightness— as much as 300%—of the ultrasound images, showing their promise in a variety of in vivo applications. The echogenic exosomes, with their large-scale extractability from bovine milk, lack of toxicity and minimal immunogenic response, successfully served as ultrasound contrast agents in this study and offer an exciting possibility to act as an effective ultrasound responsive drug delivery system.

  • Hoeve WV, Serrano MV, Winkel L, Forsberg F, Dave JK, Sarkar K, Wessner CE, Eisenbrey JR 2022, "Improved Sensitivity of Ultrasound-Based Subharmonic Aided Pressure Estimation Using Monodisperse Microbubbles" Journal of Ultrasound in Medicine, 41, 1781-1789

    Subharmonic aided pressure estimation (SHAPE) has been shown effective for noninvasively measuring hydrostatic fluid pressures in a variety of clinical applications. The objective of this study was to explore potential improvements in SHAPE sensitivity using monodisperse mirobubbles.

  • Hoeve WV, Serrano MV, Winkel L, Forsberg F, Dave JK, Sarkar K, Wessner CE, Eisenbrey JR 2022, "Improved Sensitivity of Ultrasound-Based Subharmonic Aided Pressure Estimation Using Monodisperse Microbubbles" Journal of Ultrasound in Medicine, 41, 1781-1789

    Subharmonic aided pressure estimation (SHAPE) has been shown effective for noninvasively measuring hydrostatic fluid pressures in a variety of clinical applications. The objective of this study was to explore potential improvements in SHAPE sensitivity using monodisperse mirobubbles.

  • Azami RH, Aliabouzar M, Osborn J, Kumar KN, Forsberg F, Eisenbrey JR, Mallik S, Sarkar K 2022, "Material properties, dissolution and time evolution of PEGylated lipid-shelled microbubbles: effects of the polyethylene glycol hydrophilic chain configurations" Ultrasound in Medicine and Biology, 48(9), 1720-1732

    Polyethylene glycol (PEG) is often added to the lipid coating of a contrast microbubble to prevent coalescence and improve circulation. At high surface density, PEG chains are known to undergo a transition from a mushroom configuration to an extended brush configuration. We investigated the effects of PEG chain configuration on attenuation and dissolution of microbubbles by varying the molar ratio of the PEGylated lipid in the shell with three (0%, 2% and 5%) in the mushroom configuration and two (10% and 20%) in the brush configuration. We measured attenuation through the bubble suspensions and used it to obtain the characteristic rheological properties of their shells according to two interfacial rheological models. The interfacial elasticity was found to be significantly lower in the brush regime (»0.6 N/m) than in the mushroom regime (»1.3 N/m), but similar in value within each regime. The dissolution behavior of microbubbles under acoustic excitation inside an air-saturated medium was studied by measuring the time-dependent attenuation. Total attenuation recorded a transient increase because of growth resulting from air influx and an eventual decrease caused by dissolution. Microbubble shell composition with varying PEG concentrations had significant effects on dissolution dynamics

  • Azami RH, Forsberg F, Eisenbrey JR, Sarkar K 2023, "Ambient Pressure Sensitivity of the Subharmonic Response of Coated Microbubbles: Effects of Acoustic Excitation Parameters" Ultrasound in Medicine and Biology, 49, 1550-1560

    Objective: The sensitivity of the acoustic response of microbubbles, specifically a strong correlation between their subharmonic response and the ambient pressure, has motivated development of a non-invasive subharmonicaided pressure estimation (SHAPE) method. However, this correlation has previously been found to vary depending on the microbubble type, the acoustic excitation and the hydrostatic pressure range. In this study, the ambient pressure sensitivity of microbubble response was investigated. Methods: The fundamental, subharmonic, second harmonic and ultraharmonic responses from an in-house lipidcoated microbubble were measured for excitations with peak negative pressures (PNPs) of 50−700 kPa and frequencies of 2, 3 and 4 MHz in the ambient overpressure range 0−25 kPa (0−187 mmHg) in an in vitro setup. Results: The subharmonic response typically has three stages—occurrence, growth and saturation—with increasing excitation PNP. We find distinct decreasing and increasing variations of the subharmonic signal with overpressure that are closely related to the threshold of subharmonic generation in a lipid-shelled microbubble. Above the excitation threshold, that is, in the growth-saturation phase, subharmonic signals decreased linearly with slopes as high as −0.56 dB/kPa with ambient pressure increase; below the threshold excitation (at atmospheric pressure), increasing overpressure triggers subharmonic generation, indicating a lowering of subharmonic threshold, and therefore leads to an increase in subharmonic with overpressure, the maximum enhancement being ∼11 dB for 15 kPa overpressure at 2 MHz and 100 kPa PNP. Conclusion: This study indicates the possible development of novel and improved SHAPE methodologies

  • Azami RH, Forsberg F, Eisenbrey JR, Sarkar K 2024, "Acoustic response and ambient pressure sensitivity characterization of SonoVue for noninvasive pressure estimation" The Journal of the Acoustical Society of America, 155(4), 2636-2645

    Subharmonic aided pressure estimation (SHAPE) is a noninvasive pressure measurement technique based on the pressure dependent subharmonic signal from contrast microbubbles. Here, SonoVue microbubble with a sulfur hexafluoride (SF6) core, was investigated for use in SHAPE. The study uses excitations of 25–700 kPa peak negative pressure (PNP) and 3 MHz frequency over eight pressurization cycles between atmospheric pressure and overpressures, ranging from 0 to 25 kPa (0 to 186 mm Hg). The SonoVue subharmonic response was characterized into two types. Unlike other microbubbles, SonoVue showed significant subharmonic signals at low excitations (PNPs, 25–400 kPa), denoted here as type I subharmonic. It linearly decreased with increasing overpressure (–0.52 dB/kPa at 100 kPa PNP). However, over multiple pressurization-depressurization cycles, type I subharmonic changed; its value at atmospheric pressure decreased over multiple cycles, and at later cycles, it recorded an increase in amplitude with overpressure (highest, þ13 dB at 50 kPa PNP and 10 kPa overpressure). The subharmonic at higher excitations (PNP > 400 kPa), denoted here as type II subharmonic, showed a consistent decrease with the ambient pressure increase with strongest sensitivity of –0.4 dB/kPa at 500 kPa PNP

  • Azami RH, Yapar M, Halder S, Forsberg F, Eisenbrey JR, Sarkar K 2025, "Effects of Different Gas Cores on the Ambient Pressure Sensitivity of the Subharmonic Response of SonoVue" Ultrasound in Medicine and Biology, 51, 373-380

    Objective: Subharmonic Aided Pressure Estimation (SHAPE) is a noninvasive technique for estimating organ-level blood pressure using the strong correlation between the subharmonic signal and ambient pressure. The compressible gas core of microbubbles enables them to generate linear and nonlinear acoustic responses when exposed to ultrasound. Here, the sulfur hexafluoride (SF6) gas core of SonoVue (known as Lumason in the United States), a clinical contrast agent, was exchanged with a perfluorobutane (PFB) core to investigate its effect on the SHAPE response. Methods: Excitations of 25−700 kPa peak negative pressure (PNP) and 3 MHz transmission frequency were used to study in vitro the effects of overpressure changes ranging from 5 to 25 kPa (37−186 mm Hg). Results: Unlike SonoVue with SF6, at low PNPs (<400 kPa), SonoVue with a PFB gas core exhibited no subharmonic at the atmospheric pressure, but during pressurization, a stable subharmonic response (maximum of 25 dB at 100 kPa PNP and 20 kPa Overpressure) appeared. SonoVue with a PFB gas core showed an increase in subharmonics with overpressure at high PNPs (>400 kPa), which was not observed before in normal SonoVue or other lipid microbubbles. With negligible size distribution difference between these two microbubbles, these effects on subharmonic generation are likely due to the gas core, casting new light on the mechanism by which ambient overpressure affects subharmonic. Conclusion: This study may inform future SHAPE technique developments.

  • Sarkar K 2025, "Dynamics of bubbles and ultrasound: Diagnostic imaging to blood pressure monitoring and tissue engineering" Physical Review Fluids, 10, 030501

    Coated microbubbles in conjunction with ultrasound have emerged as an important biomedical tool for diagnostic imaging and therapeutics. Here, I offer my perspective based on research spanning over two decades, highlighting the underlying physics of linear and nonlinear bubble dynamics. I will describe our effort at mathematical modeling of contrast microbubble behaviors, specifically our adoption of an interfacial rheological model for the stabilizing shell and a hierarchical approach of model building and improvement using attenuation and scattering experiments. I will describe our collaborative effort at using the sensitivity of the acoustic response of microbubbles to ambient hydrostatic pressure for a subharmonic aided pressure estimation (SHAPE) method for noninvasive organlevel blood pressure monitoring. Other collaborative projects demonstrated microbubbles together with low-intensity pulsed ultrasound (LIPUS) to be an effective tool in tissue engineering, growing bone and cartilage from human mesenchymal stem cells in a 3D printed tissue engineering scaffold. We have theoretically investigated various underlying mechanisms for such bioeffects of ultrasound-insonated microbubbles, specifically microstreaming at low acoustic excitations and cavitating jet formation at high excitations for shelled microbubbles. Finally, I briefly describe my computational research on viscous and viscoelastic emulsions and suspensions of drops, vesicles, and biological cells.

  • Halder S, Yapar M, Sarkar K 2025, "Analyzing size and shell stability of lipid-coated microbubbles over a fixed time span" The Journal of the Acoustical Society of America, 157(4_Supplement), A261

    Microbubbles are gas-filled contrast increasing agents used in ultrasound imaging, typically ranging from 1 to 10 μm in size. They are encapsulated by a protective shell to improve stability and prevent coalescence. Ensuring a stable size distribution and reliable performance over time is becoming increasingly important for their effectiveness. In this study, we explore the long-term stability and acoustic performance of our homemade microbubbles. These microbubbles are created using a mechanical agitation method, with a gas core of perfluorobutane (C4F10) and a shell made from a lipid mixture of DPPC and DPPE-PEG-2000 in a 9:1 ratio. We measure the size distribution, scattering, and attenuation of these microbubbles at regular intervals over 4 weeks. Additionally, we analyze the bubble shell properties by using the size and attenuation data. This research provides insights into the lifespan and stability of polydisperse microbubbles over expanded periods, highlighting their potential as efficient ultrasound contrast agents.

  • Halder S, Yapar M, Sarkar K 2025, "Analyzing size and shell stability of lipid-coated microbubbles over a fixed time span" The Journal of the Acoustical Society of America, 157(4_Supplement), A261

    Microbubbles are gas-filled contrast increasing agents used in ultrasound imaging, typically ranging from 1 to 10 μm in size. They are encapsulated by a protective shell to improve stability and prevent coalescence. Ensuring a stable size distribution and reliable performance over time is becoming increasingly important for their effectiveness. In this study, we explore the long-term stability and acoustic performance of our homemade microbubbles. These microbubbles are created using a mechanical agitation method, with a gas core of perfluorobutane (C4F10) and a shell made from a lipid mixture of DPPC and DPPE-PEG-2000 in a 9:1 ratio. We measure the size distribution, scattering, and attenuation of these microbubbles at regular intervals over 4 weeks. Additionally, we analyze the bubble shell properties by using the size and attenuation data. This research provides insights into the lifespan and stability of polydisperse microbubbles over expanded periods, highlighting their potential as efficient ultrasound contrast agents.

  • Halder S, Yapar M, Sarkar K 2025, "Analyzing size and shell stability of lipid-coated microbubbles over a fixed time span" The Journal of the Acoustical Society of America, 157(4_Supplement), A261

    Microbubbles are gas-filled contrast increasing agents used in ultrasound imaging, typically ranging from 1 to 10 μm in size. They are encapsulated by a protective shell to improve stability and prevent coalescence. Ensuring a stable size distribution and reliable performance over time is becoming increasingly important for their effectiveness. In this study, we explore the long-term stability and acoustic performance of our homemade microbubbles. These microbubbles are created using a mechanical agitation method, with a gas core of perfluorobutane (C4F10) and a shell made from a lipid mixture of DPPC and DPPE-PEG-2000 in a 9:1 ratio. We measure the size distribution, scattering, and attenuation of these microbubbles at regular intervals over 4 weeks. Additionally, we analyze the bubble shell properties by using the size and attenuation data. This research provides insights into the lifespan and stability of polydisperse microbubbles over expanded periods, highlighting their potential as efficient ultrasound contrast agents.

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  • Halder S, Yapar M, Sarkar K 2025, "Analyzing size and shell stability of lipid-coated microbubbles over a fixed time span" The Journal of the Acoustical Society of America, 157(4_Supplement), A261

    Microbubbles are gas-filled contrast increasing agents used in ultrasound imaging, typically ranging from 1 to 10 μm in size. They are encapsulated by a protective shell to improve stability and prevent coalescence. Ensuring a stable size distribution and reliable performance over time is becoming increasingly important for their effectiveness. In this study, we explore the long-term stability and acoustic performance of our homemade microbubbles. These microbubbles are created using a mechanical agitation method, with a gas core of perfluorobutane (C4F10) and a shell made from a lipid mixture of DPPC and DPPE-PEG-2000 in a 9:1 ratio. We measure the size distribution, scattering, and attenuation of these microbubbles at regular intervals over 4 weeks. Additionally, we analyze the bubble shell properties by using the size and attenuation data. This research provides insights into the lifespan and stability of polydisperse microbubbles over expanded periods, highlighting their potential as efficient ultrasound contrast agents.

  • Halder S, Yapar M, Sarkar K 2025, "Analyzing size and shell stability of lipid-coated microbubbles over a fixed time span" The Journal of the Acoustical Society of America, 157(4_Supplement), A261

    Microbubbles are gas-filled contrast increasing agents used in ultrasound imaging, typically ranging from 1 to 10 μm in size. They are encapsulated by a protective shell to improve stability and prevent coalescence. Ensuring a stable size distribution and reliable performance over time is becoming increasingly important for their effectiveness. In this study, we explore the long-term stability and acoustic performance of our homemade microbubbles. These microbubbles are created using a mechanical agitation method, with a gas core of perfluorobutane (C4F10) and a shell made from a lipid mixture of DPPC and DPPE-PEG-2000 in a 9:1 ratio. We measure the size distribution, scattering, and attenuation of these microbubbles at regular intervals over 4 weeks. Additionally, we analyze the bubble shell properties by using the size and attenuation data. This research provides insights into the lifespan and stability of polydisperse microbubbles over expanded periods, highlighting their potential as efficient ultrasound contrast agents.

  • Halder S, Yapar M, Sarkar K 2025, "Analyzing size and shell stability of lipid-coated microbubbles over a fixed time span" The Journal of the Acoustical Society of America, 157(4_Supplement), A261

    Microbubbles are gas-filled contrast increasing agents used in ultrasound imaging, typically ranging from 1 to 10 μm in size. They are encapsulated by a protective shell to improve stability and prevent coalescence. Ensuring a stable size distribution and reliable performance over time is becoming increasingly important for their effectiveness. In this study, we explore the long-term stability and acoustic performance of our homemade microbubbles. These microbubbles are created using a mechanical agitation method, with a gas core of perfluorobutane (C4F10) and a shell made from a lipid mixture of DPPC and DPPE-PEG-2000 in a 9:1 ratio. We measure the size distribution, scattering, and attenuation of these microbubbles at regular intervals over 4 weeks. Additionally, we analyze the bubble shell properties by using the size and attenuation data. This research provides insights into the lifespan and stability of polydisperse microbubbles over expanded periods, highlighting their potential as efficient ultrasound contrast agents.

  • Azami RH, Aliabouzar M, Osborn J, Kumar KN, Forsberg F, Eisenbrey JR, Mallik S, Sarkar K 2022, "Material properties, dissolution and time evolution of PEGylated lipid-shelled microbubbles: effects of the polyethylene glycol hydrophilic chain configurations" Ultrasound in Medicine and Biology, 48(9), 1720-1732

    Polyethylene glycol (PEG) is often added to the lipid coating of a contrast microbubble to prevent coalescence and improve circulation. At high surface density, PEG chains are known to undergo a transition from a mushroom configuration to an extended brush configuration. We investigated the effects of PEG chain configuration on attenuation and dissolution of microbubbles by varying the molar ratio of the PEGylated lipid in the shell with three (0%, 2% and 5%) in the mushroom configuration and two (10% and 20%) in the brush configuration. We measured attenuation through the bubble suspensions and used it to obtain the characteristic rheological properties of their shells according to two interfacial rheological models. The interfacial elasticity was found to be significantly lower in the brush regime (»0.6 N/m) than in the mushroom regime (»1.3 N/m), but similar in value within each regime. The dissolution behavior of microbubbles under acoustic excitation inside an air-saturated medium was studied by measuring the time-dependent attenuation. Total attenuation recorded a transient increase because of growth resulting from air influx and an eventual decrease caused by dissolution. Microbubble shell composition with varying PEG concentrations had significant effects on dissolution dynamics

People Involved

Abhilash Reddy Malipeddi
Alumni

PHD Student Abhilash started his Ph.D. in Fall 2013 and graduated in Fall 2021. He worked on computational methods

Lang Xia
Alumni

PHD student Lang Xia is a Ph.D. student (2012 - 2017 expected) in the Department of Mechanical & Aerospace Engi

Nima Mobadersany
Alumni

PHD Student Nima received his M.Sc. degree in Mechanical engineering from University of Tabriz, Iran. He joined our

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