4.5 Article

Accelerated sequences of 4D flow MRI using GRAPPA and compressed sensing: A comparison against conventional MRI and computational fluid dynamics

期刊

MAGNETIC RESONANCE IN MEDICINE
卷 88, 期 6, 页码 2432-2446

出版社

WILEY
DOI: 10.1002/mrm.29404

关键词

4D flow; compressed sensing; computational fluid dynamics (CFD); flow phantom

资金

  1. GENCI-CINES [A0080307194, A0100307194]
  2. MESO@LR-Platform - University of Montpellie
  3. Spin Up

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This study evaluated hemodynamic markers obtained by accelerated GRAPPA and compressed sensing 4D flow MRI sequences under complex flow conditions. The results showed similar hemodynamic patterns between MRI and computational fluid dynamics simulations, with larger discrepancies near the boundary walls. MRI scans tended to overestimate velocity profiles and peak velocities, but showed good agreement for flow rates. Computational fluid dynamics simulations are a useful tool to assess these differences, but are sensitive to modeling parameters.
Purpose To evaluate hemodynamic markers obtained by accelerated GRAPPA (R = 2, 3, 4) and compressed sensing (R = 7.6) 4D flow MRI sequences under complex flow conditions. Methods The accelerated 4D flow MRI scans were performed on a pulsatile flow phantom, along with a nonaccelerated fully sampled k-space acquisition. Computational fluid dynamics simulations based on the experimentally measured flow fields were conducted for additional comparison. Voxel-wise comparisons (Bland-Altman analysis, L2$$ {L}_2 $$-norm metric), as well as nonderived quantities (velocity profiles, flow rates, and peak velocities), were used to compare the velocity fields obtained from the different modalities. Results 4D flow acquisitions and computational fluid dynamics depicted similar hemodynamic patterns. Voxel-wise comparisons between the MRI scans highlighted larger discrepancies at the voxels located near the phantom's boundary walls. A trend for all MR scans to overestimate velocity profiles and peak velocities as compared to computational fluid dynamics was noticed in regions associated with high velocity or acceleration. However, good agreement for the flow rates was observed, and eddy-current correction appeared essential for consistency of the flow rates measurements with respect to the principle of mass conservation. Conclusion GRAPPA (R = 2, 3) and highly accelerated compressed sensing showed good agreement with the fully sampled acquisition. Yet, all 4D flow MRI scans were hampered by artifacts inherent to the phase-contrast acquisition procedure. Computational fluid dynamics simulations are an interesting tool to assess these differences but are sensitive to modeling parameters.

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