Pulsatile CFD was performed for three cardiac cycles (Schirmer and Malek 2007a) with a 500 timestep pulsatile velocity waveform that was derived from waveforms described in healthy human subjects by Ford et al. (Holdsworth et al. 1999). Validation of the computational approach used in this study has been previously reported (Schirmer and Malek 2007a, b, 2008). Postprocessing was performed using Ensight software (Ver. 8, CEI, Apex, NC). Statistical analysis of

mean values was Inhibitors,research,lifescience,medical performed using Student’s t-tests and statistical significance was assumed for P < 0.05 (SAS, Cary, NC). Results Changes of the flow pattern in CS Starting with laminar flow in the common carotid (CCA), a considerable distortion of the flow pattern was seen in all eight cases (Fig. 2A). The average Reynolds number in the stenosis was 114 ± 30, the maximum 162. Three modes of flow alteration Inhibitors,research,lifescience,medical were discerned as a function of the geometry of the stenosis: in axisymmetric stenosis of the ICA (cases 1 and 7) recirculation and secondary flow patterns was seen downstream from the stenosis in the poststenotic dilatation of the vessel. The jet of accelerated blood in the center of the vessel downstream of the stenosis evolves into increased twisting and curling of the flow, characterized by the pseudoscalar quantity helicity (Fig. 1B, cases 1 and 7). In cases where the stenosis was close to

the carotid bulb or just downstream to the bifurcation (cases 3–5 and 8), recirculation Inhibitors,research,lifescience,medical developed both upstream and downstream to the stenosis. Significant Inhibitors,research,lifescience,medical twisting of the flow with increased helicity, however, could only be demonstrated on orthogonal cutplanes through the stenosis itself (panel b) and in the poststenotic segment of the flow (see insert panel a in Fig. 1C, cases 1–2 and 6–7). Inhibitors,research,lifescience,medical The increase in helicity is characterized by the development of a division of the pathlines into a right-handed and left-handed twisting component of the

flow. One case with an elongated and flattened stenosis twisted around itself (case 6) had only small areas of recirculation, but increased helicity along the length of the stenotic vessel segment (Fig. 1C, case 6). The two corkscrew components of the flow merge further downstream upon restoration of a laminar flow condition Isotretinoin (Fig. 1B, case 2, distal ICA). Figure 1 (A) Pathlines color coded for the time-averaged velocity magnitude. (B) Examples of pathlines, color coded for the helicity density. (C) Helicity density on orthogonal cutplanes that correspond to a prestenotic RGFP966 purchase cutplane a (see schematic), a cutplane at … Figure 2 (A–C) Three example (case 3, 5, and 6) detailing the temporal evolution of the instantaneous wall shear stress (WSS) vectors at the stenosis and poststenotic region (PSR) during the cardiac cycle (reds points on pulse wave). Regions of antegrade … WSS in carotid stenosis The WSS magnitude, averaged over the course of the cardiac cycle, was computed and exhibited a visible increase in the area of the stenosis (Fig.