Maxwell J A, Anliker M
Biophys J. 1968 Aug;8(8):920-50. doi: 10.1016/S0006-3495(68)86529-4.
Theoretical and experimental evidence suggests that the dissipation of high frequency pressure waves in blood vessels is caused primarily by the viscoelastic behavior of the vessel wall. In this theoretical analysis the vessels are considered as fluid-filled circular cylindrical shells whose walls have isotropic and homogeneous viscoelastic properties and are subjected to an initial axial stretch and a transmural pressure. If the wall material is incompressible and behaves as a Voigt solid in shear, the results predict a decrease in wave amplitude per wavelength which is essentially independent of frequency over a wide range. This finding is in qualitative agreement with recent experiments on anesthetized dogs. A parametric study also shows a great sensitivity of the dissipation to changes in transmural pressure and axial stretch. Axisymmetric waves are only mildly dispersive, while all nonaxisymmetric waves are highly dispersive and exhibit much stronger damping per wavelength at low frequencies than do axisymmetric waves.
理论和实验证据表明,血管中高频压力波的耗散主要是由血管壁的粘弹性行为引起的。在该理论分析中,血管被视为充满流体的圆柱壳,其壁具有各向同性和均匀的粘弹性特性,并承受初始轴向拉伸和跨壁压力。如果壁材料不可压缩且在剪切时表现为沃伊特固体,则结果预测每波长的波幅减小,这在很宽的频率范围内基本与频率无关。这一发现与最近在麻醉犬身上进行的实验定性一致。参数研究还表明,耗散对跨壁压力和轴向拉伸的变化非常敏感。轴对称波只是轻微色散,而所有非轴对称波都是高度色散的,并且在低频下每波长的阻尼比轴对称波要强得多。