Extracting non-linear viscoelastic material properties from violently-collapsing cavitation bubbles
Introduction
Cavitation is a common phenomenon found in many biological and engineering systems, from the prey-stunning capacity of the snapping shrimp to cavitation erosion on metallic pumps and propellers, to cavitation induced cell and tissue damage [1], [2], [3], [4], [5], [6]. When harnessed carefully, focused, energy-driven cavitation can be a very beneficial tool in a wide array of surgical, medical, and materials applications including: tissue phantom, laser surgery, lithotripsy, DNA injection and more recently, high to ultra-high strain-rates soft material characterization [7], [8], [9], [10], [11], [12], [13], [14], [15].
In particular, laser-based Inertial Microcavitation Rheometry (IMR), a new technique we recently developed, can provide a robust experimental approach for characterizing highly compliant materials at large strains (up to 1000% strain) and ultra-high strain-rates () [15]. Here, a single isolated spherical bubble is induced within a viscoelastic medium through a spatially-focused, pulsed laser [16] while real-time, ultra high-speed videography is employed for recording the subsequent bubble expansion–collapse cycles. Due to the dependency of the bubble dynamics on the mechanical properties of the surrounding medium, the viscoelastic properties of the material can be determined by analyzing the temporal evolution of the bubble radius within a relevant framework of associated governing equations of inertial cavitation [15], [17], [18], [19], [20], [21].
While at small to moderate material stretches (e.g., 1 6) the material surrounding the cavitating bubble remains primarily viscoelastic, higher stretch ratios can introduce a new host of additional physical phenomena. These include, but are not limited to, significant strain stiffening and inelastic material effects (e.g., material damage, plasticity, combustion, etc.) as the local, material Mach number exceeds , a condition of violent collapse.
The natural occurrence and physics of violent bubble collapse have been extensively discussed within the fluid mechanics community [7], [22], [23], [24], while here we extend this notion and definition to observations in solid, albeit highly compliant, materials. While it is generally understood that violent collapses bear significant changes in the material’s compressibility and stability of the contracting bubble and surrounding material, direct experimental evidence thereof still remains sparse.
Here by employing ultra-high speed imaging of up to 2 million frames per second, we provide direct experimental evidence that significant inelastic effects can occur during the collapse process in a model system of soft and stiff polyacrylamide (PA) hydrogels with nominal equilibrium shear moduli ranging from a few hundred to a few thousand pascals. By closely tracking native, inherent material features, we find a significant departure in the motion of our fiducial material markers from viscoelastic behavior at a critical collapse Mach number of around 0.08, consistent with the notion of a violent collapse. Yet, we find that as long as the temporal sampling frequency is high enough, i.e., greater than one million frames per second, the non-linear viscoelastic material properties can still be uniquely determined from just the first collapse regime until close to the bubble collapse point.
Furthermore, we show that through the incorporation of an explicit, higher order strain stiffening term in the constitutive response of the surrounding material, the accuracy in the estimated material parameters can be improved while also recovering the quasi-statically determined equilibrium shear modulus.
In sum, this paper provides a new approach for accurately deducing non-linear viscoelastic material properties from violently collapsing cavitation bubbles while providing direct experimental evidence of significant inelastic behavior during and after the initial bubble collapse.
Section snippets
Experimental setup
In our experiments, single cavitation bubbles were generated in polyacrylamide (PA) hydrogels (protocols are summarized in Supplementary Material Section S1) through a single 6 ns pulse from an adjustable 1–25 mJ Q-switched Nd:YAG Minilite II (Continuum, Milpitas, CA) laser platform frequency-doubled to 532 nm [15], [16]. Laser pulses were spatially expanded to fill the back aperture of a Nikon Plan Fluor 20/0.5 NA imaging objective and were aligned through the back camera port of a Nikon
Results and discussions
For each PA hydrogel, ten individual tests were conducted yielding average maximum and equilibrium radii of , and for soft PA, and , and for stiff PA, respectively. All resultant bubble radii vs. time curves are normalized in terms of the material stretch ratio, (Fig. 3(a); Table 1). Representative radial stretch ratio () versus time () curves for each of our soft and stiff PA samples are shown in Fig. 3(a) featuring average maximum
Conclusions
In this paper, we extend our previously developed inertial microcavitation rheometry (IMR) technique to successfully characterize the strain stiffening behavior of soft materials experiencing large material stretches and violent bubble collapse, a condition, featuring significant changes in the material physics upon first collapse. By tracking the displacement motion of naturally-occurring, native material features in the vicinity of the laser-induced cavitation bubble, we identify a critical
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgments
We gratefully acknowledge the funding support from the Office of Naval Research, United States (Dr. Timothy Bentley) under grants N000141612872 and N000141712058. We thank Dr. Jonathan Estrada and Prof. David Henann for their helpful discussions.
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