Wall shear stress calculations based on 3D cine phase contrast MRI and computational fluid dynamics: a comparison study in healthy carotid arteries

被引:64
作者
Cibis, Merih [1 ]
Potters, Wouter V. [2 ]
Gijsen, Frank J. H. [1 ]
Marquering, Henk [2 ,3 ]
VanBavel, Ed [3 ]
van der Steen, Antonius F. W. [1 ,4 ]
Nederveen, Aart J. [2 ]
Wentzel, Jolanda J. [1 ]
机构
[1] Erasmus MC, Dept Biomed Engn, Rotterdam, Netherlands
[2] Univ Amsterdam, Acad Med Ctr, Dept Radiol, NL-1105 AZ Amsterdam, Netherlands
[3] Univ Amsterdam, Acad Med Ctr, Dept Biomed Engn & Phys, NL-1105 AZ Amsterdam, Netherlands
[4] Delft Univ Technol, Dept Imaging Sci & Technol, Delft, Netherlands
关键词
shear stress; carotid arteries; phase contrast MRI; CFD; BLOOD-FLOW; IN-VIVO; ATHEROSCLEROSIS; RESPONSES; VECTORS; VITRO; AORTA;
D O I
10.1002/nbm.3126
中图分类号
Q6 [生物物理学];
学科分类号
071011 ;
摘要
Wall shear stress (WSS) is involved in many pathophysiological processes related to cardiovascular diseases, and knowledge of WSS may provide vital information on disease progression. WSS is generally quantified with computational fluid dynamics (CFD), but can also be calculated using phase contrast MRI (PC-MRI) measurements. In this study, our objectives were to calculate WSS on the entire luminal surface of human carotid arteries using PC-MRI velocities (WSSMRI) and to compare it with WSS based on CFD (WSSCFD). Six healthy volunteers were scanned with a 3 T MRI scanner. WSSCFD was calculated using a generalized flow waveform with a mean flow equal to the mean measured flow. WSSMRI was calculated by estimating the velocity gradient along the inward normal of each mesh node on the luminal surface. Furthermore, WSS was calculated for a down-sampled CFD velocity field mimicking the MRI resolution (WSSCFDlowres). To ensure minimum temporal variation, WSS was analyzed only at diastole. The patterns of WSSCFD and WSSMRI were compared by quantifying the overlap between low, medium and high WSS tertiles. Finally, WSS directions were compared by calculating the angles between the WSSCFD and WSSMRI vectors. WSSMRI magnitude was found to be lower than WSSCFD (0.62 +/- 0.18 Pa versus 0.88 +/- 0.30 Pa, p< 0.01) but closer to WSS(CFD)lowres (0.56 +/- 0.18 Pa, p< 0.01). WSSMRI patterns matched well with those of WSSCFD. The overlap area was 68.7 +/- 4.4% in low and 69.0 +/- 8.9% in high WSS tertiles. The angles between WSSMRI and WSSCFD vectors were small in the high WSS tertiles (20.3 +/- 8.2 degrees), but larger in the low WSS tertiles (65.6 +/- 17.4 degrees). In conclusion, although WSSMRI magnitudewas lower than WSSCFD, the spatial WSS patterns at diastole, which are more relevant to the vascular biology, were similar. PC-MRI-based WSS has potential to be used in the clinic to indicate regions of low and high WSS and the direction of WSS, especially in regions of high WSS. Copyright (C) 2014 John Wiley & Sons, Ltd.
引用
收藏
页码:826 / 834
页数:9
相关论文
共 34 条
[1]   An image-based modeling framework for patient-specific computational hemodynamics [J].
Antiga, Luca ;
Piccinelli, Marina ;
Botti, Lorenzo ;
Ene-Iordache, Bogdan ;
Remuzzi, Andrea ;
Steinman, David A. .
MEDICAL & BIOLOGICAL ENGINEERING & COMPUTING, 2008, 46 (11) :1097-1112
[2]   Phase-Contrast Magnetic Resonance Imaging Measurements in Intracranial Aneurysms In Vivo of Flow Patterns, Velocity Fields, and Wall Shear Stress: Comparison with Computational Fluid Dynamics [J].
Boussel, Loic ;
Rayz, Vitaliy ;
Martin, Alastair ;
Acevedo-Bolton, Gabriel ;
Lawton, Michael T. ;
Higashida, Randall ;
Smith, Wade S. ;
Young, William L. ;
Saloner, David .
MAGNETIC RESONANCE IN MEDICINE, 2009, 61 (02) :409-417
[3]   Role of hemodynamic shear stress in cardiovascular disease [J].
Cecchi, Emanuele ;
Giglioli, Cristina ;
Valente, Serafina ;
Lazzeri, Chiara ;
Gensini, Gian Franco ;
Abbate, Rosanna ;
Mannini, Lucia .
ATHEROSCLEROSIS, 2011, 214 (02) :249-256
[4]   Endothelial cell responses to atheroprone flow are driven by two separate flow components: low time-average shear stress and fluid flow reversal [J].
Conway, Daniel E. ;
Williams, Marcie R. ;
Eskin, Suzanne G. ;
McIntire, Larry V. .
AMERICAN JOURNAL OF PHYSIOLOGY-HEART AND CIRCULATORY PHYSIOLOGY, 2010, 298 (02) :H367-H374
[5]   Three-Dimensional Analysis of Segmental Wall Shear Stress in the Aorta by Flow-Sensitive Four-Dimensional-MRI [J].
Frydrychowicz, Alex ;
Stalder, Aurelien F. ;
Russe, Maximilian F. ;
Bock, Jelena ;
Bauer, Simon ;
Harloff, Andreas ;
Berger, Alexander ;
Langer, Mathias ;
Hennig, Juergen ;
Markl, Michael .
JOURNAL OF MAGNETIC RESONANCE IMAGING, 2009, 30 (01) :77-84
[6]  
Giese Daniel., 2014, Journal of Cardiovascular Magnetic Resonance, V16, pW29
[7]   Wall shear stress distribution at the carotid bifurcation: influence of eversion carotid endarterectomy [J].
Harloff, A. ;
Berg, S. ;
Barker, A. J. ;
Schoellhorn, J. ;
Schumacher, M. ;
Weiller, C. ;
Markl, M. .
EUROPEAN RADIOLOGY, 2013, 23 (12) :3361-3369
[8]   Comparison of hemodynamics of intracranial aneurysms between MR fluid dynamics using 3D cine phase-contrast MRI and MR-based computational fluid dynamics [J].
Isoda, Haruo ;
Ohkura, Yasuhide ;
Kosugi, Takashi ;
Hirano, Masaya ;
Alley, Marcus T. ;
Bammer, Roland ;
Pelc, Norbert J. ;
Namba, Hiroki ;
Sakahara, Harumi .
NEURORADIOLOGY, 2010, 52 (10) :913-920
[9]   MRI measurement of wall shear stress vectors in bifurcation models and comparison with CFD predictions [J].
Köhler, U ;
Marshall, I ;
Robertson, MB ;
Long, Q ;
Xu, XY ;
Hoskins, PR .
JOURNAL OF MAGNETIC RESONANCE IMAGING, 2001, 14 (05) :563-573
[10]   Geometry of the carotid bifurcation predicts its exposure to disturbed flow [J].
Lee, Sang-Wook ;
Antiga, Luca ;
Spence, J. David ;
Steinman, David A. .
STROKE, 2008, 39 (08) :2341-2347