Vessel distensibility and flow distribution in vascular trees

Journal of Mathematical Biology - Tập 44 - Trang 360-374 - 2002
Gary S. Krenz1, Christopher A. Dawson2
1Department of Mathematics, Statistics, and Computer Science, Marquette University, PO 1881, Milwaukee, WI 53201-1881, USA (e-mail: [email protected]). Research Service, Zablocki Veterans Affairs Medical Center, Milwaukee, WI 53295, USA, , US
2Department of Biomedical Engineering, Marquette University, Milwaukee, WI 53201-1881, USA. Research Service, Zablocki Veterans Affairs Medical Center, Milwaukee, WI 53295, USA. Department of Physiology, Medical College of Wisconsin, Milwaukee, WI 53226, USA, , US

Tóm tắt

 In a class of model vascular trees having distensible blood vessels, we prove that flow partitioning throughout the tree remains constant, independent of the nonzero driving flow (or nonzero inlet to terminal outlet pressure difference). Underlying assumptions are: (1) every vessel in the tree exhibits the same distensibility relationship given by $D/D_0 = f(P)$ where $D$ is the diameter which results from distending pressure $P$ and $D_0$ is the diameter of the individual vessel at zero pressure (each vessel may have its own individual $D_0$). The choice of $f(P)$ includes distensibilities often used in vessel biomechanics modeling, e.g., $f(P) = 1 + \alpha P$ or $f(P) = b + (1-b) \exp(-c P)$, as well as $f(P)$ which exhibit autoregulatory behavior. (2) Every terminal vessel in the tree is subjected to the same terminal outlet pressure. (3) Bernoulli effects are ignored. (4) Flow is nonpulsatile. (5) Blood viscosity within any individual vessel is constant. The results imply that for a vascular tree consistent with assumptions 2–5, the flow distribution calculations based on a rigid geometry, e.g., $D=D_0$, also gives the flow distribution when assuming the common distensibility relationships.