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Possible Resolution: Resistive inhomogeneities via gap junctions, fiber geometry and rotation, etc.

Suppose that $ \sigma_i = \sigma_i(x)$, $\sigma_e = \sigma_e(x)$. Then the bidomain model (in 1D) reduces to

\begin{displaymath}
\chi (C_m{\partial\phi \over \partial \tau} + I_m ) =
{\part...
...\over\partial x}\left({\sigma_i\over \sigma_e+\sigma_i}\right)
\end{displaymath}

and in steady state:



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