Matsumoto T, Hayashi K
Department of Mechatronics and Precision Engineering, Faculty of Engineering, Tohoku University, Sendai, Japan.
J Biomech Eng. 1996 Feb;118(1):62-73. doi: 10.1115/1.2795947.
The effects of hypertension on the stress and strain distributions through the wall thickness were studied in the rat thoracic aorta. Goldblatt hypertension was induced by constricting the left renal artery for 8 weeks. Static pressure-diameter-axial force relations were determined on excised tubular segments. The segments were then sliced into thin ring specimens. Circumferential strain distributions were determined from the cross-sectional shape of the ring specimens observed before and after releasing residual stresses by radial cutting. Stress distributions were calculated using a logarithmic type of strain energy density function. The wall thickness at the systolic blood pressure, P(sys) significantly correlated with P(sys). The mean stress and strain developed by P(sys) in the circumferential direction were not significantly different between the hypertensive and control aortas, while those in the axial direction were significantly smaller in the hypertensive aorta than in the control. The opening angles of the stress free ring specimens correlated well with P(sys). The stress concentration factor in the circumferential direction was almost constant and independent of P(sys) although the stress distributions were not uniform through the wall thickness. Histological observation showed that the wall thickening caused by hypertension is mainly due to the hypertrophy of the lamellar units of the media, especially in the subintimal layer where the stress increase developed by hypertension is larger than in the other layers. These results indicate that: (a) the aortic wall adapts itself to the mechanical field by changing not only the wall dimensions but also the residual stresses, (b) this adaptation is primarily related to the circumferential stress but not to the axial stress, and (c) the aortic smooth muscle cells seem to change their morphology in response to the mechanical stress.
在大鼠胸主动脉中研究了高血压对整个壁厚上应力和应变分布的影响。通过结扎左肾动脉8周诱导产生Goldblatt高血压。在切除的管状节段上测定静态压力-直径-轴向力关系。然后将这些节段切成薄环标本。通过观察径向切割释放残余应力前后环标本的横截面形状来确定周向应变分布。使用对数型应变能密度函数计算应力分布。收缩压P(sys)时的壁厚与P(sys)显著相关。高血压主动脉和对照主动脉在周向由P(sys)产生的平均应力和应变无显著差异,而在轴向,高血压主动脉中的平均应力和应变显著小于对照主动脉。无应力环标本的开口角度与P(sys)密切相关。尽管应力分布在整个壁厚上不均匀,但周向应力集中系数几乎恒定且与P(sys)无关。组织学观察表明,高血压引起的壁厚增厚主要是由于中膜板层单元肥大,尤其是在内皮下层,高血压在此处产生的应力增加大于其他层。这些结果表明:(a)主动脉壁不仅通过改变壁尺寸而且通过改变残余应力来适应机械场;(b)这种适应主要与周向应力有关,而与轴向应力无关;(c)主动脉平滑肌细胞似乎会响应机械应力而改变其形态。