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Measuring the Hyperelastic Response of Porcine Liver Tissues In-Vitro Using Controlled Cavitation Rheology

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Abstract

Background

Measuring the mechanical properties of soft biological tissues in-vitro by using conventional methods (e.g. tension, compression, or indentation) is prone to external testing and sample preparation factors. For example, sample slippage affects the measurement accuracy of mechanical properties of soft biological tissues. In addition, samples have to go through a complex cutting process to be prepared in specific shapes, which increases the post-mortem time spent before testing.

Objective

The purpose of this study is to investigate the capability of a new technique to measure the mechanics of soft biological tissues without experiencing the conventional challenges. It measures the mechanical behavior of soft materials by introducing and expanding spherical cavity deformations within materials’ internal structure while generating two stresses simultaneously, radial and hoop stresses.

Methods

Two porcine livers were tested. The experimental data were used to calibrate the material parameters of three hyperelastic models, namely: Yeoh, Arruda-Boyce, and Ogden. Numerical simulations were performed to validate the material parameters. Also, Computed Tomography (CT) imaging technology was used to verify the configuration of the cavity deformations.

Results

The outcome of the numerical simulations showed that hyperelastic models were able to predict the material response to cavity loading. In addition, CT imaging confirmed the spherical configuration of the applied deformations.

Conclusions

From the experimental results, numerical simulations and the CT imaging, it can be concluded that the cavity expansion test is capable of measuring the mechanics of soft biological tissues without experiencing the difficulties encountered in conventional techniques.

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Correspondence to A. Al-Mayah.

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Appendix 1

Appendix 1

The definition of R is very critical to determine the deformation term in the circumferential direction, λ. In this work, R was estimated to be 1.42 mm; this radius is derived from an initial volume which is expressed as

$$ Vi={V}_{n-b}+{V}_p $$
(24)

Where Vn-b is the volume of the balloon region which is 2.837 mm3, The dimensions of this region are described in Fig. 2 of the main manuscript; Vp is the volume that is introduced into the balloon before the tissues start to resist the cavity expansion, which is 9.177 mm3 as indicated by the pressure sensor data in Fig.7, see [72] for more details about the mechanism of injecting fluids into soft biological tissues. When the needle was inserted inside the tissues, it created a channel along the needle’s shaft. This channel made the tissues loose resulting into a negligible resistance against initially introduced volumes. A FE simulation was conducted for a process similar to that of a flat punch indentation test to calculate the measured initial volume (Vi) numerically. It was found that the magnitude of the volume induced due to a displacement equal to the thickness of the needle-balloon region was around 12 mm3, similar to the experimental Vi. This indicates that the insertion of the needle created a cut that allows the tissues to displace during initial volumes of inflation before resisting expansion.

Although, CT images have shown that the inflated balloon was nearly spherical in the injected volumes, the initial volume of the balloon has a cylindrical configuration. However, the stretch ratio (λ) can be calculated based on the volumetric ratio. Therefore, the exact geometry of the cavity does not affect the stretch (λ) calculation. The initial cylindrical volume can be represented by an equivalent spherical volume by using the concept of Equivalent-Volume Diameter (EVD) which was adopted in this study to define the initial radius, see [73] for more details about EVD. The EVD is based on equating irregular-shaped volumes to an equivalent sphere volume with a diameter of

$$ {\mathrm{D}}_{\mathrm{e}}=\sqrt[3]{\frac{6\ast {\mathrm{V}}_{\mathrm{i}}}{\pi }} $$
(25)

R is then calculated as \( \frac{{\mathrm{D}}_{\mathrm{e}}}{2} \)

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Nafo, W., Al-Mayah, A. Measuring the Hyperelastic Response of Porcine Liver Tissues In-Vitro Using Controlled Cavitation Rheology. Exp Mech 61, 445–458 (2021). https://doi.org/10.1007/s11340-020-00674-6

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