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Comparative analysis of indentation and magnetic resonance elastography for measuring viscoelastic properties
Yu Chen1, Suhao Qiu1, Zhao He1, Fuhua Yan2, Ruokun Li2, and Yuan Feng1
1Institute for Medical Imaging Technology, School of Biomedical Engineering, Shanghai Jiao Tog University, Shanghai, China, 2Department of Radiology, Ruijin Hospital, Shanghai Jiao Tong University School of Medicine, Shanghai, China

Synopsis

Comparing viscoelastic properties of soft tissues measured in vivo and ex vivo are of interests for basic science and clinical translation. Magnetic resonance elastography (MRE) and indentation are two commonly used techniques for measurement of tissue viscoelasticity. In this study, we used a gelatin phantom to compare measurements by MRE and indentation. Using 2nd-order Prony series, frequency response measured from indentation was estimated. We observed apparent frequency-dependent behaviors from MRE in the range of 50-100 Hz, but not from indentation. Results implied that MRE and indentation measures at different frequency ranges.

Introduction

Viscoelastic properties of soft tissue were traditional measured using indentation or rotational rheometry.1,2 Magnetic resonance elastography (MRE), as a non-invasive method, is clinically used for in vivo measurement of viscoelasticity.3,4 Many comparative studies were conducted between rheometry and MRE for in vivo measurement verification. 5-7 However, few studies have compared measurement between MRE and indentation. In this study, we used 2nd-order Prony series to analyze the frequency response of a gelatin phantom based on indentation test. The results were compared with that from a multi-frequency tests of MRE.

Methods

Gelatin phantoms mimicking soft tissues were measured using a ramp-hold indentation protocol (Figure 1a).8 Viscoelastic properties were estimated by fitting the relaxation curve using 2nd-order Prony series:
$$ G(t) = C_0 + C_1·e^{-\frac{t}{\tau_{1}}} + C_2·e^{-\frac{t}{\tau_{2}}}, $$
where and are viscoelastic parameters.
A custom-built magnetic resonance elastography (MRE) system was used for measuring the dynamic moduli of the phantom 9. The experiments were performed on a 3T MRI scanner (uMR 790, United Imaging Healthcare, Shanghai, China). (Figure 1b). The measured frequencies ranged from 50 to 100 Hz with a 10Hz step. A spin echo-EPI sequence was used for imaging, with TR/TE=1000/48 ms,FOV=300x300 mm2, a matrix size of 127x127, and a slice thickness of 5 mm. Dynamic shear modulus measured from MRE were estimated by both local frequency estimation (LFE) and direction inversion (DI).
To analyze the frequency response of the model estimated from indentation, we convert the 2nd-order Prony series into a 5-parameter Maxwell model (Figure 2). The model parameters were determined based on the physical interpretation of the Prony series:
$$ E_1 = 3C_0, E_2 = 3C_1, E_3 = 3C_{2}, $$
$$ F_2 = 3\tau_{1}C_1, F_3 = 3\tau_{2}C_{2}. $$
If incompressibility was assumed, the dynamic shear modulus can be determined by . For a 2nd-order linear viscoelastic model 10,
$$ E(i\omega) = \frac{-q_{2}\omega^{2} + iq_{1}\omega + q_{0}}{-p_{2}\omega^{2} + ip_{1}\omega + 1} $$
where and were linear viscoelastic model parameters.
Therefore, by comparing the Laplacian transformation of the constitutive equation of the 5-parameter model with the analytical dynamic shear modulus, the linear viscoelastic model parameters and can be determined:
$$ q_2 = 3\tau_{1}\tau_{2}(C_0 + C_1 + C_2), q_1 = 3C_0\tau_1 + 3C_0\tau_2 + 3C_1\tau_1 + 3C_2\tau_2, $$
$$ q_0 = 3C_{0}, p_2 = \tau_{1}·\tau_{2}, p_1 = \tau_{1} + \tau_{2}. $$

Results and Discussion

The typical ramp-hold relaxation curve from the indentation tests is shown in Figure 3a. The Wave propagation images from the MRE tests with 6 different actuation frequencies are shown in Figure 3b. A quantitative comparison of viscoelastic properties is shown in Figure 4. In the frequency range of 50-100 Hz, the result of MRE showed an apparent frequency-dependent behavior. The measured shear moduli increased with the vibration frequency increased. However, in the same frequency range, no such behavior was observed based on the indentation test. The differences in the frequency response between the MRE and indentation tests indicated the considerable influences of boundary conditions and loading conditions. Since the calculation of shear modulus in indentation test was based on , the different frequency responses of shear modulus between MRE and indentation implied that the Poisson’s ratio could be frequency-dependent, too.

Conclusion

In this study, we analyzed and compared the viscoelastic parameters estimated from indentation and MRE. Both Indentation and MRE tests were used to measure the dynamic responses of viscoelastic soft tissues. The former is more prone to capture the low-frequency range response, while the latter is better for describing the response at a relatively higher frequency range. The results could provide helpful information for the ex vivo and in vivo measurements of soft tissues.

Acknowledgements

Funding support from grant 31870941 from National Natural Science Foundation of China (NSFC) and grant 1944190700 from Shanghai Science and Technology Committee (STCSM) are acknowledged. We thank the technical support from Jiayu Zhu, Xiaomao Gong, Cong Zhang, Xiaodong Zhou, and Qiang He from United Imaging Healthcare, Shanghai.

References

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Figures

Figure 1. Viscoelastic properties of the gel phantom measured by (a) indentation and (b) MRE.

Figure 2. A Maxwell model for the 2nd-order Prony series, which contains 3 springs ($$$ E_1, E_2, E_3 $$$) and 2 dashpots ($$$ F_2, F_3 $$$).

Figure 3. (a) The experimental and fitted ramp and relaxation curves from indentation tests. (b) Wave propagation images of MRE from 6 different actuation frequencies.

Figure 4. Comparisons of the shear moduli of the gel phantom based on indentation and MRE measurements.

Proc. Intl. Soc. Mag. Reson. Med. 29 (2021)
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