TY - JOUR
T1 - Dynamic shear stress in parallel-plate flow chambers
AU - Bacabac, R.G.
AU - Smit, T.H.
AU - Cowin, S.C.
AU - van Loon, J.J.W.A.
AU - Nieuwstadt, F.T.M.
AU - Heethaar, R.
AU - Klein-Nulend, J.
PY - 2005/1
Y1 - 2005/1
N2 - An in vitro model using a parallel-plate fluid flow chamber is supposed to simulate in vivo fluid shear stresses on various cell types exposed to dynamic fluid flow in their physiological environment. The metabolic response of cells in vitro is associated with the wall shear stress. However, parallel-plate flow chambers have not been characterized for dynamic fluid flow experiments. We use a dimensionless ratio h/λv, in determining the exact magnitude of the dynamic wall shear stress, with its oscillating components scaled by a shear factor T. It is shown that, in order to expose cells to predictable levels of dynamic fluid shear stress, two conditions have to be met: (1) h/λv<2, where h is the distance between the plates and λv is the viscous penetration depth; and (2) f0<fc/m, where the critical frequency fc is the upper threshold for this flow regime, m is the highest harmonic mode of the flow, and f0 is the fundamental frequency of fluid flow.
AB - An in vitro model using a parallel-plate fluid flow chamber is supposed to simulate in vivo fluid shear stresses on various cell types exposed to dynamic fluid flow in their physiological environment. The metabolic response of cells in vitro is associated with the wall shear stress. However, parallel-plate flow chambers have not been characterized for dynamic fluid flow experiments. We use a dimensionless ratio h/λv, in determining the exact magnitude of the dynamic wall shear stress, with its oscillating components scaled by a shear factor T. It is shown that, in order to expose cells to predictable levels of dynamic fluid shear stress, two conditions have to be met: (1) h/λv<2, where h is the distance between the plates and λv is the viscous penetration depth; and (2) f0<fc/m, where the critical frequency fc is the upper threshold for this flow regime, m is the highest harmonic mode of the flow, and f0 is the fundamental frequency of fluid flow.
U2 - 10.1016/j.jbiomech.2004.03.020
DO - 10.1016/j.jbiomech.2004.03.020
M3 - Article
SN - 0021-9290
VL - 38
SP - 159
EP - 167
JO - Journal of Biomechanics
JF - Journal of Biomechanics
IS - 1
ER -