Research Commentary |
From the Department of Physics, Oakland University, Rochester, Mich.
Correspondence to Brad Roth, Department of Physics, Oakland University, 190 SEB, Rochester, MI 48309. E-mail roth{at}oakland.edu
AbstractRecently, Spach et al
(Circ Res. 1998;83:11441164) measured the
transmembrane action potential 150 to 200 µm below the tissue
surface during longitudinal and transverse propagation. They found that
"during longitudinal propagation there was initial slowing of
Vm [action potential] foot that resulted in deviations
from a simple exponential... " (p 1144). They attributed this
behavior to the effects of capillaries on propagation. The purpose of
this commentary is to show that the perfusing bath plays an important
role in determining the time course of the action potential foot, even
when the transmembrane potential is measured 150 µm below the
tissue surface. Using numerical simulations based on the bidomain
model, we find that the action potential foot for transverse
propagation is nearly exponential (
foot=314 µs). For
longitudinal propagation, the action potential foot is not exponential
because of an initial slowing (best-fit
foot=483 µs).
We conclude that the perfusing bath must be taken into account when
interpreting data showing differences in the shape of the action
potential foot with propagation direction, even if the transmembrane
potential is measured 150 µm below the tissue surface. The full
text of this article is available at http://www.circresaha.org.
Key Words: bidomain action potential foot perfusing bath anisotropy
This article has been cited by other articles:
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M. L. Trew, B. J. Caldwell, G. B. Sands, D. A. Hooks, D. C.-S. Tai, T. M. Austin, I. J. LeGrice, A. J. Pullan, and B. H. Smaill Cardiac electrophysiology and tissue structure: bridging the scale gap with a joint measurement and modelling paradigm Exp Physiol, March 1, 2006; 91(2): 355 - 370. [Abstract] [Full Text] [PDF] |
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