Simulation of propagation along a cylindrical bundle of cardiac tissue. II. Results of simulation
For pt.I see ibid., vol.37, no.9, p.850-60 (1990). Nonlinear membrane kinetics are introduced into the bidomain membrane and equal anisotropy ratios are assumed, permitting the transmembrane potential to be computed and its behavior examined at different depths in the bundle and for different values...
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Published in | IEEE transactions on biomedical engineering Vol. 37; no. 9; pp. 861 - 875 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
New York, NY
IEEE
01.09.1990
Institute of Electrical and Electronics Engineers |
Subjects | |
Online Access | Get full text |
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Summary: | For pt.I see ibid., vol.37, no.9, p.850-60 (1990). Nonlinear membrane kinetics are introduced into the bidomain membrane and equal anisotropy ratios are assumed, permitting the transmembrane potential to be computed and its behavior examined at different depths in the bundle and for different values of conductivity and bundle diameters. In contrast with single-fiber models, the bundle model reveals that the shape of the action potential is influenced by tissue resistivities. In addition, the steady-state activation wavefront through the cross section perpendicular to the long axis of the bundle is not planar and propagates with a velocity that lies between that of a single fiber in an unbounded volume and a single-fiber in a restricted extracellular space. In general, the bundle model is shown to be significantly better than the classical single fiber model in describing the behavior of real cardiac tissue.< > |
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Bibliography: | ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 ObjectType-Article-1 ObjectType-Feature-2 |
ISSN: | 0018-9294 1558-2531 |
DOI: | 10.1109/10.58597 |