In: The Influence of Shear Stress on Restenosis (Humana Press eBooks)
Chapter In A Book 2007 English
Authors
AT
Attila Thury
JW
Jolanda J. Wentzel
FG
Frank Gijsen
Abstract
1 min read
Wall shear stress (WSS) is the (tangential) drag force acting on the luminal wall, induced by blood flow, normalized to wall area. As WSS is defined as force/area, its dimension equals that of pressure, i.e., N/m2 or Pa. An older, frequently used unit for shear stress, i.e., dyne/cm2 relates to Pa according to 1 Pa = 10 dyne/cm2. WSS on the endothelium (Fig. 1) can be calculated from the local shear rate (s−1) times blood viscosity (μ) (Pa/s). Shear rate is the spatial blood velocity gradient ([m/s]/m). Especially near the vessel wall, generally large velocity gradients between adjacent fluid layers exist and the shear stress is at its highest value. In a simple straight tube the Hagen-Poiseuille formula (WSS = 4μQ/πR3, with μ viscosity, R tube radius and Q flow) can be applied for steady laminar viscous flow. A normal WSS range of 0.68 ± 0.2 Pa was derived from Doppler based velocity measurements in angiographically normal coronary
Attila Thury, Glenn Van Langenhove, Stéphane Carlier, Mariano Albertal, Ken Kozuma, Evelyn Regar, George Sianos, Jolanda J. Wentzel, Rob Krams, Cornelis J. Slager, Jan J. Piek, Patrick W. Serruys
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