Stephen Dicker

Bursting Bubbles and Bilayers

This paper discusses various interactions between ultrasound, phospholipid monolayer-coated gas bubbles, phospholipid bilayer vesicles, and cells. The paper begins with a review of microbubble physics models, developed to describe microbubble dynamic behavior in the presence of ultrasound, and follows this with a discussion of how such models can be used to predict inertial cavitation profiles. Predicted sensitivities of inertial cavitation to changes in the values of membrane properties, including surface tension, surface dilatational viscosity, and area expansion modulus, indicate that area expansion modulus exerts the greatest relative influence on inertial cavitation. Accordingly, the theoretical dependence of area expansion modulus on chemical composition - in particular, poly (ethylene glyclol) (PEG) - is reviewed, and predictions of inertial cavitation for different PEG molecular weights and compositions are compared with experiment. Noteworthy is the predicted dependence, or lack thereof, of inertial cavitation on PEG molecular weight and mole fraction. Specifically, inertial cavitation is predicted to be independent of PEG molecular weight and mole fraction in the so-called mushroom regime. In the “brush” regime, however, inertial cavitation is predicted to increase with PEG mole fraction but to decrease (to the inverse 3/5 power) with PEG molecular weight. While excellent agreement between experiment and theory can be achieved, it is shown that the calculated inertial cavitation profiles depend strongly on the criterion used to predict inertial cavitation. This is followed by a discussion of nesting microbubbles inside the aqueous core of microcapsules and how this significantly increases the inertial cavitation threshold. Nesting thus offers a means for avoiding unwanted inertial cavitation and cell death during imaging and other applications such as sonoporation. A review of putative sonoporation mechanisms is then presented, including those involving microbubbles to deliver cargo into a cell, and those - not necessarily involving microubbles - to release cargo from a phospholipid vesicle (or reverse sonoporation). It is shown that the rate of (reverse) sonoporation from liposomes correlates with phospholipid bilayer phase behavior, liquid-disordered phases giving appreciably faster release than liquid-ordered phases. Moreover, liquid-disordered phases exhibit evidence of two release mechanisms, which are described well mathematically by enhanced diffusion (possibly via dilation of membrane phospholipids) and irreversible membrane disruption, whereas liquid-ordered phases are described by a single mechanism, which has yet to be positively identified. The ability to tune release kinetics with bilayer composition makes reverse sonoporation of phospholipid vesicles a promising methodology for controlled drug delivery. Moreover, nesting of microbubbles inside vesicles constitutes a truly “theranostic” vehicle, one that can be used for both long-lasting, safe imaging and for controlled drug delivery.

Determination of microbubble cavitation threshold pressure as function of shell chemistry

AbstractThe sensitivity of inertial cavitation threshold to changes in shell viscosity and elasticity makes shell chemistry (here, polyethylene glycol (PEG) molecular weight and composition) a potential tuning parameter for microbubble based ultrasound contrast and drug delivery applications. It is anticipated that microbubble shell chemistry can be used to adjust the inertial cavitation threshold so as to either avoid or achieve cavitation at a given operating pressure. Here such ideas are tested by measuring the inertial cavitation threshold for populations of phospholipid shelled microbubbles suspended in aqueous media, and this method is used to quantify the influence of shell chemistry on the inertial cavitation threshold. The experimental cavitation data are fitted with a modification of the Herring equation, using shell viscosity and elasticity as the tuning parameters. It is concluded that the design and synthesis of microbubbles with a prescribed inertial cavitation threshold is feasible using PE...

Influence of shell composition on the resonance frequency of microbubble contrast agents.

The effect of variations in microbubble shell composition on microbubble resonance frequency is revealed through experiment. These variations are achieved by altering the mole fraction and molecular weight of functionalized polyethylene glycol (PEG) in the microbubble phospholipid monolayer shell and measuring the microbubble resonance frequency. The resonance frequency is measured via a chirp pulse and identified as the frequency at which the pressure amplitude loss of the ultrasound wave is the greatest as a result of passing through a population of microbubbles. For the shell compositions used herein, we find that PEG molecular weight has little to no influence on resonance frequency at an overall PEG mole fraction (0.01) corresponding to a mushroom regime and influences the resonance frequency markedly at overall PEG mole fractions (0.050-0.100) corresponding to a brush regime. Specifically, the measured resonance frequency was found to be 8.4, 4.9, 3.3 and 1.4 MHz at PEG molecular weights of 1000, 2000, 3000 and 5000 g/mol, respectively, at an overall PEG mole fraction of 0.075. At an overall PEG mole fraction of just 0.01, on the other hand, resonance frequency exhibited no systematic variation, with values ranging from 5.7 to 4.9 MHz. Experimental results were analyzed using the Sarkar bubble dynamics model. With the dilatational viscosity held constant (10(-8) N·s/m) and the elastic modulus used as a fitting parameter, model fits to the pressure amplitude loss data resulted in elastic modulus values of 2.2, 2.4, 1.6 and 1.8 N/m for PEG molecular weights of 1000, 2000, 3000 and 5000 g/mol, respectively, at an overall PEG mole fraction of 0.010 and 4.2, 1.4, 0.5 and 0.0 N/m, respectively, at an overall PEG mole fraction of 0.075. These results are consistent with theory, which predicts that the elastic modulus is constant in the mushroom regime and decreases with PEG molecular weight to the inverse 3/5 power in the brush regime. Additionally, these results are consistent with inertial cavitation studies, which revealed that increasing PEG molecular weight has little to no effect on inethe rtial cavitation threshold in the mushroom regime, but that increasing PEG molecular weight decreases inertial cavitation markedly in the brush regime. We conclude that the design and synthesis of microbubbles with a prescribed resonance frequency is attainable by tuning PEG composition and molecular weight.

Coencapsulation of lipid microbubbles within polymer microcapsules for contrast applications

In this work, the authors examine the acoustic response generated by the coencapsulation of phospholipid shelled microbubbles within the aqueous core of polymer microcapsules and its feasibility as an ultrasound contrast agent. The addition of the polymer shell provides the added benefit of approximately doubling the inertial cavitation threshold of the microbubbles contained within. The feasibility of the utilisation of the coencapsulated contrast agent as a drug delivery vehicle is also discussed. It is concluded that the coencapsulated contrast agent provides contrast similar to that of unencapsulated microbubbles, both in acoustic response and image intensity of contrast to tissue.

Controlling cavitation for controlled release

We present a novel, long-lived ultrasound contrast vehicle with triggered drug release capability. The vehicle comprises shell-stabilized microbubbles encapsulated within the aqueous core of a vesicle-like microcapsule. Encapsulating microbubbles enhances their longevity as ultrasound contrast agents by shielding the microbubbles from dissolution in a bulk aqueous phase. Moreover, co-encapsulation of microbubbles with a drug offers a simple mechanism for controlled drug release; ultrasound-induced cavitation of the microbubbles within microcapsules causes leakage of the inner contents from the microcapsules into the surrounding medium. By controlling the extent of microbubble cavitation one can control when - and at what rate - the microcapsule releases drug. Here we describe construction of the vehicle, how one can tune the microbubble cavitation threshold via changes in microbubble shell elasticity, and how ultrasound-induced leakage varies with microcapsule shell type and composition. We show results for different microcapsule shell materials, including self-assembled bilayers of phospholipids (liposomes) and di-block copolymers (polymersomes) and a non-self-assembled, macromolecular polymer, using the fluorescent dye calcein as a drug mimic.

Influence of nesting shell size on brightness longevity and resistance to ultrasound-induced dissolution during enhanced B-mode contrast imaging.

This study aims to bridge the gap between transport mechanisms of an improved ultrasound contrast agent (UCA) and its resulting behavior in a clinical imaging study. Phospholipid-shelled microbubbles nested within the aqueous core of a polymer microcapsule are examined for their use and feasibility as an improved UCA. The nested formulation provides contrast comparable to traditional formulations, specifically an SF6 microbubble coated by a DSPC PEG-3000 monolayer, with the advantage that contrast persists at least nine times longer in a mock clinical, in vitro setting. The effectiveness of the sample was measured using a contrast ratio in units of decibels (dB) which compares the brightness of the nested microbubbles to a reference value of a phantom tissue mimic. During a 40min imaging study, six nesting formulations with average outer capsule diameters of 1.95, 2.53, 5.55, 9.95, 14.95, and 20.51μm reached final contrast ratio values of 0.25, 2.35, 3.68, 4.51, 5.93, and 8.00dB, respectively. The starting contrast ratio in each case was approximately 8dB and accounts for the brightness attributed to the nesting shell. As compared with empty microcapsules (no microbubbles nested within), enhancement of the initial contrast ratio increased systematically with decreasing microcapsule size. The time required to reach a steady state in the temporal contrast ratio profile also varied with microcapsule diameter and was found to be 420s for each of the four smallest shell diameters and 210s and 150s, respectively, for the largest two shell diameters. All nested formulations were longer-lived and gave higher final contrast ratios than a control sample comprising un-nested, but otherwise equivalent, microbubbles. Specifically, the contrast ratio of the un-nested microbubbles decreased to a negative value after 4min of continuous ultrasound exposure with complete disappearance of the microbubbles after 15min whereas all nested formulations maintained positive contrast ratio values for the duration of the 40min trial. The results are consistent with two distinct stages of gas transport: in the first stage, passive diffusion occurs under ambient conditions across the microbubble monolayer within the first few minutes after formulation until the aqueous interior of the microcapsule is saturated with gas; in the second stage ultrasound drives additional gas dissolution even further due to pressure modulation. It is important to understand the chemistry and transport mechanisms of this contrast agent under the influence of ultrasound to attain better perspicacity for enhanced applications in imaging. Results from this study will facilitate future preclinical studies and clinical applications of nested microbubbles for therapeutic and diagnostic imaging.

Nesting microbubbles: influence on acoustic activity and image brightness

In the following study, gas filled microbubbles encapsulated in a polymer shell were characterised for use as contrast agents, as compared to commercially available contrast agents such as Definity microbubbles. The lifetime of these nested microparticles was also explored. It was found that even with changing the contrast agent due to the enclosure in a polymer shell, the acoustic response using Definity microbubbles and nested microparticles can be matched by simply varying the starting concentrations, and there is no change in their behaviour as a contrast agent. The results also indicate the ability of the nested microparticles to provide contrast steadily for up to 1·5 h.

Microcapsules: Reverse Sonoporation and Long-lasting, Safe Contrast

We present a novel vehicle designed to serve the dual roles of enhanced ultrasound contrast and ultrasound-triggered drug delivery. The vehicle is comprised of a microcapsule that is filled with water in whose aqueous core a population of freely floating, phospholipid-coated microbubbles is suspended. At ultrasound intensities below the inertial cavitation threshold of the microbubbles, the microbubbles provide enhanced ultrasound contrast. The measured contrast is comparable in strength with SonoVue®. Encapsulation of microbubbles within microcapsules putatively eliminates – or at least significantly slows – dissolution of gas in the bulk aqueous medium, thereby avoiding disappearance of microbubbles that would otherwise occur due to pressure-induced gas diffusion across the surfactant monolayer coating the microbubble-water interface. Results suggest that our vehicle might provide longer lasting contrast in a clinical setting. We demonstrate that encapsulation of the microbubbles within microcapsules causes at least a doubling of the ultrasound intensity necessary to induce inertial cavitation. Moreover, no cell death was observed when cells were insonified in the presence of microbubble-containing microcapsules, whereas appreciable cell death occurs with unencapsulated microbubbles. These results point toward a potential safety benefit during ultrasound contrast imaging by using encapsulated microbubbles. Studies are underway to investigate the feasibility of ultrasound-triggered release of drug from the microcapsules, owing to inertial- or stable-cavitation, or both. Whereas leakage from polymeric microcapsule shells, such as poly(lactic acid), seemingly requires shell rupture and is exceedingly difficult to achieve, leakage across a lipid bilayer microcapsule shells appears feasible. Leakage across a bilayer shell has the additional benefit that the leakage mechanism can be tuned via phase behavior (liquid-ordered versus liquid-disordered) and cavitation mechanism (stable versus inertial).

Inertial cavitation threshold of nested microbubbles.

Cavitation of ultrasound contrast agents (UCAs) promotes both beneficial and detrimental bioeffects in vivo (Radhakrishnan et al., 2013) [1]. The ability to determine the inertial cavitation threshold of UCA microbubbles has potential application in contrast imaging, development of therapeutic agents, and evaluation of localized effects on the body (Ammi et al., 2006) [2]. This study evaluates a novel UCA and its inertial cavitation behavior as determined by a home built cavitation detection system. Two 2.25 MHz transducers are placed at a 90° angle to one another where one transducer is driven by a high voltage pulser and the other transducer receives the signal from the oscillating microbubble. The sample chamber is placed in the overlap of the focal region of the two transducers where the microbubbles are exposed to a pulser signal consisting of 600 pulse trains per experiment at a pulse repetition frequency of 5 Hz where each train has four pulses of four cycles. The formulation being analyzed is comprised of an SF6 microbubble coated by a DSPC PEG-3000 monolayer nested within a poly-lactic acid (PLA) spherical shell. The effect of varying shell diameters and microbubble concentration on cavitation threshold profile for peak negative pressures ranging from 50 kPa to 2 MPa are presented and discussed in this paper. The nesting shell decreases inertial cavitation events from 97.96% for an un-nested microbubble to 19.09% for the same microbubbles nested within a 2.53 μm shell. As shell diameter decreases, the percentage of inertially cavitating microbubbles also decreases. For nesting formulations with average outer capsule diameters of 20.52, 14.95, 9.95, 5.55, 2.53, and 1.95 μm, the percentage of sample destroyed at 1 MPa was 51.02, 38.94, 33.25, 25.27, 19.09, and 5.37% respectively.

Size distribution of microbubbles as a function of shell composition.

The effect of modifying the shell composition of a population of microbubbles on their size demonstrated through experiment. Specifically, these variations include altering both the mole fraction and molecular weight of functionalized polymer, polyethylene glycol (PEG) in the microbubble phospholipid monolayer shell (1-15 mol% PEG, and 1000-5000 g/mole, respectively). The size distribution is measured with an unbiased image segmentation program written in MATLAB which identifies and sizes bubbles from micrographs. For a population of microbubbles with a shell composition of 5 mol% PEG2000, the mean diameter is 1.42 μm with a variance of 0.244 μm. For the remainder of the shell compositions studied herein, we find that the size distributions do not show a statistically significant correlation to either PEG molecular weight or mole fraction. All the measured distributions are nearly Gaussian in shape and have a monomodal peak.