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Validation of Motion-Robust Liver Diffusion MRI in Multi-Stiffness Pulsatile Motion Phantoms
Srijyotsna Volety1,2, James Rice2,3, Ali Pirasteh1,2, Alejandro Roldan-Alzate2,3, and Diego Hernando1,2
1Medical Physics, University of Wisconsin - Madison, Madison, WI, United States, 2Radiology, University of Wisconsin - Madison, Madison, WI, United States, 3Mechanical Engineering, University of Wisconsin - Madison, Madison, WI, United States

Synopsis

Keywords: Simulation/Validation, Contrast Mechanisms

Motivation: Quantitative diffusion MRI is a proposed marker for assessment of liver fibrosis. However, poor reproducibility and lack of highly controlled validation of liver ADC mapping precludes its clinical utilization.

Goal(s): Introduce hydrogel liver models with pulsatile motion and varying stiffness. These enable controlled validation of ADC accuracy and reproducibility across DWI acquisition parameters and physiological-mimicking motion.

Approach: Conventional monopolar (MONO) and motion-robust M1-optimized diffusion waveforms (MODI) were used to acquire DWI of three hydrogel liver models.

Results: MODI-DWI resulted in less biased DWI and ADC maps than MONO-DWI in areas of motion. A significant inverse relationship was observed between ADC and phantom stiffness.

Impact: Quantitative diffusion MRI may enable assessment of liver fibrosis. However, the relationship between diffusion parameters and stiffness requires controlled evaluation. The proposed phantom-based approach may help validate and optimize diffusion MRI of the liver and other abdominal organs.

Introduction

Liver fibrosis is the consequence of chronic liver injury. End-stage liver fibrosis is the primary cause of liver-disease related deaths.1-2 Magnetic Resonance Elastography (MRE) is validated for non-invasive estimation of liver stiffness, an indirect measurement of fibrosis.3-4 However, MRE requires additional hardware, has limited sensitivity in detecting early-stages of fibrosis, and cannot differentiate fibrosis from concurrent liver inflammation.5-6

The apparent diffusion coefficient (ADC) obtained through diffusion weighted imaging (DWI) is a proposed marker for liver fibrosis. However, DWI of the liver is limited by several technical challenges, including the sensitivity of DWI to physiological motion, low signal-to-noise (SNR), and non-uniform acquisition parameters across studies.7-9 M1-optimized diffusion imaging (MODI) gradient waveforms enable robustness to pulsatile motion of the liver and have previously been reported to improve accuracy of ADC compared to conventional monopolar gradient waveforms (MONO).10 Furthermore, MODI-DWI paired with low-resolution imaging has previously shown improved accuracy of ADC for evaluation of diffuse liver disease.11 Despite early validation of low-resolution MODI-DWI in vivo, highly controlled evaluation of diffusion acquisition parameters has yet to be conducted. Hence, the purpose of this work is to validate motion-robust liver DWI across acquisition parameters and stiffness in a highly controlled liver model with pulsatile motion.

Methods

Motion Phantom:
An anthropomorphic hydrogel liver model surrounds a pulsating tube with bifurcation, while being surrounded by rigid plastic walls. This setup mimics the cardiovascular-induced compressive tissue motion in the liver. The liver model was placed into the scanner bore and water was pumped through the system (Figure 1). Water was pumped at four flow velocities (0,0.5,1.0,1.5 L/min) to introduce deformation of the tube and adjacent hydrogel liver model. Three hydrogel liver models were fabricated with varying hydrogel compositions to create differing shear stiffness, quantified via MRE.

Image Acquisition:
DW images were acquired at 3.0T (Signa Premier, GE Healthcare) using an anterior array coil (Air Coil, GE Healthcare) and a posterior embedded table coil. Three hydrogel liver models were scanned using MONO and MODI diffusion gradient waveforms. MONO images were acquired with three orthogonal diffusion directions at two b-value pairs (b = [50,500] and b = [50,800] s/mm2, NEX = [2,4]). As usual in MONO, M1 increased substantially with b-value. MODI images were acquired with the same b-values, repetitions, diffusion directions, and a fixed M1 motion moment (0.628 s/mm) for all b-values. For each type of DW acquisition, two different spatial resolutions were acquired (2.8x2.8x6 & 6x6x6 mm3).

Analysis:
For each DWI acquisition, ADC maps were generated in MATLAB (R2020a) and subsequently analyzed in Horos (v3.3.6). ROIs were drawn on the averaged b = 50 s/mm2 images. ROIs were copied onto the corresponding ADC maps for measurement. Student’s t-tests evaluated the relationship between stiffness and ADC across the hydrogel liver models, and the differences in ADC across acquisition parameters.

Results

Figures 2-3 show ADC maps across flow rates and stiffness, from MONO-DWI and MODI-DWI, respectively. MONO suffered from large ADC bias at higher flow rates and in liver models with low stiffness. MODI suffered from localized ADC bias at the highest flow rate (1.5 L/min) in the lowest stiffness liver model, and minimal ADC bias in other models.

Figure 4 plots MONO and MODI ADC versus phantom stiffness in the absence of flow. Each liver model exhibited different ADCs at baseline, dependent on the stiffness of the hydrogel. As stiffness increased, the ADC decreased (P = <0.01) for both MONO and MODI.

Figure 5 displays ADC values for all MONO and MODI DWI acquisitions across flow rates. MONO exhibited consistent ADC measurements at higher stiffness but suffered from large motion-induced ADC bias in the lowest stiffness hydrogel liver model. This trend was observed across b-value and resolution. MODI ADC measurements were consistent across all hydrogel liver models regardless of DW acquisition parameters.

Discussion

We validated motion-robust liver diffusion techniques in pulsatile motion phantoms with varying stiffness. We demonstrated that MODI ADC measurements in our liver model have an inverse relationship with MRE stiffness, a reduction in motion-induced ADC bias exists at higher stiffness, and improved motion-robustness using M1-optimized acquisitions. These highly controlled phantom results are well aligned with previously reported in vivo measurements.12-16

Limitations of this study include the reliance of a pulsatile flow approach to induce compressive motion in the liver model, as the fluid used does not accurately mimic quantitative properties of blood.

Overall, our phantom validation approach with highly controlled compressive motion and stiffness may prove useful in development and validation of motion-robust DWI for assessment of liver fibrosis in vivo.

Acknowledgements

The authors acknowledge support from the NIH (R01 EB030497), from the University of Wisconsin-Madison Office of the Vice Chancellor for Research and Graduate Education with funding from the Wisconsin Alumni Research Foundation, as well as from the UW Departments of Radiology, Medical Physics, Mechanical Engineering. Also, GE Healthcare provides research support to the University of Wisconsin-Madison.

Research reported in this publication was supported by the National Cancer Institute of the National Institutes of Health under Award Number T32CA009206. The content is solely the responsibility of the authors and does not necessarily represent the official views of the National Institutes of Health.

References

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8. Kwee TC, Takahara T, Niwa T,et al. Influence of cardiac motion on diffusion-weighted magnetic resonance imaging of the liver. Magnetic Resonance Materials in Physics, Biology and Medicine, 2009, 22(5), 319-325.
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Figures

Figure 1: an anthropomorphic, in-vitro, MRI compatible hydrogel model of the liver. Setup in MRI room with a pulsatile flow circuit. Water is pumped through the system to induce pulsation from the inner tube, leading to compressive motion of the hydrogel model. T2-weighted images display appearance of phantom in three orthogonal planes.


Figure 2: demonstrates ADC maps from MONO-DWI across flow rates and stiffness. MONO suffered from large ADC bias (yellow arrows) at higher flow rates and in liver models with low stiffness (4%). There is slight ADC bias in the 6% hydrogel phantom near the vessel edge, and none in the 8%.

Figure 3: demonstrates ADC maps from MODI-DWI across flow rates and stiffness. MODI suffered from localized ADC bias at the highest flow rate (1.5 L/min) in the lowest stiffness liver model (4%, yellow arrow). Minimal ADC bias was visualized in other hydrogel models.

Figure 4: plots MONO and MODI ADC versus phantom stiffness in the absence of flow. Each liver model exhibited different ADCs at baseline, dependent on the stiffness of the hydrogel. Hydrogel compositions of 4%, 6%, and 8% corresponded to stiffness of 1.6 kPa, 4.9 kPa, and 10.7 kPa, respectively. As stiffness increased, the ADC decreased (P = <0.01) for both MONO and MODI. Mean ADC and Standard Deviation are also reported in a table for all DWI acquisitions across b-values and resolutions.

Figure 5: displays ADC values for all MONO and MODI DWI acquisitions across flow rates. Both MONO and MODI exhibited consistent ADC measurements at higher stiffness. MODI remained consistent in the lowest stiffness phantom, while MONO exhibited large motion-induced ADC bias.

Proc. Intl. Soc. Mag. Reson. Med. 32 (2024)
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DOI: https://doi.org/10.58530/2024/2590