Kinouchi Y, Yamaguchi H, Tenforde T S
Department of Electrical and Electronic Engineering, University of Tokushima, Japan.
Bioelectromagnetics. 1996;17(1):21-32. doi: 10.1002/(SICI)1521-186X(1996)17:1<21::AID-BEM3>3.0.CO;2-8.
The flow of blood in the presence of a magnetic field gives rise to induced voltages in the major arteries of the central circulatory system. Under certain simplifying conditions, such as the assumption that the length of major arteries (e.g., the aorta) is infinite and that the vessel walls are not electrically conductive, the distribution of induced voltages and currents within these blood vessels can be calculated with reasonable precision. However, the propagation of magnetically induced voltages and currents from the aorta into neighboring tissue structures such as the sinuatrial node of the heart has not been previously determined by any experimental or theoretical technique. In the analysis presented in this paper, a solution of the complete Navier-Stokes equation was obtained by the finite element technique for blood flow through the ascending and descending aortic vessels in the presence of a uniform static magnetic field. Spatial distributions of the magnetically induced voltage and current were obtained for the aortic vessel and surrounding tissues under the assumption that the wall of the aorta is electrically conductive. Results are presented for the calculated values of magnetically induced voltages and current densities in the aorta and surrounding tissue structures, including the sinuatrial node, and for their field-strength dependence. In addition, an analysis is presented of magnetohydrodynamic interactions that lead to a small reduction of blood volume flow at high field levels above approximately 10 tesla (T). Quantitative results are presented on the offsetting effects of oppositely directed blood flows in the ascending and descending aortic segments, and a quantitative estimate is made of the effects of assuming an infinite vs. a finite length of the aortic vessel in calculating the magnetically induced voltage and current density distribution in tissue.
在存在磁场的情况下,血液流动会在中央循环系统的主要动脉中产生感应电压。在某些简化条件下,例如假设主要动脉(如主动脉)的长度是无限的,且血管壁不导电,就可以较为精确地计算出这些血管内感应电压和电流的分布。然而,此前尚未通过任何实验或理论技术确定从主动脉磁诱导的电压和电流向诸如心脏窦房结等邻近组织结构的传播情况。在本文所呈现的分析中,采用有限元技术求解了完整的纳维 - 斯托克斯方程,以研究在均匀静磁场存在的情况下血液流经升主动脉和降主动脉血管的情况。在假设主动脉壁导电的情况下,得出了主动脉血管及其周围组织的磁诱导电压和电流的空间分布。给出了主动脉及周围组织结构(包括窦房结)中磁诱导电压和电流密度的计算值及其对场强的依赖性结果。此外,还分析了磁流体动力学相互作用,这种相互作用会导致在高于约10特斯拉(T)的高场强下血液体积流量略有减少。给出了升主动脉段和降主动脉段中相反方向血流的抵消效应的定量结果,并对在计算组织中磁诱导电压和电流密度分布时假设主动脉血管为无限长与有限长的影响进行了定量估计。