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	<title>Paving matroid - Revision history</title>
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		<title>en&gt;Luismanu: /* d-Partitions */</title>
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		<updated>2014-01-22T05:13:11Z</updated>

		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;d-Partitions&lt;/span&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{unreferenced|date=October 2013}}&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;monodomain model&amp;#039;&amp;#039;&amp;#039; is a reduction of the [[bidomain model]] of the electrical propagation in myocardial tissue.&lt;br /&gt;
The reduction comes from assuming that the intra- and extracellular domains have equal anisotropy ratios.&lt;br /&gt;
Although not as physiologically accurate as the [[Bidomain|bidomain model]], it is still adequate in some cases, and has reduced complexity.&lt;br /&gt;
&lt;br /&gt;
==Formulation==&lt;br /&gt;
The monodomain model can be formulated as follows&lt;br /&gt;
: &amp;lt;math&amp;gt;&lt;br /&gt;
\frac{\lambda}{1+\lambda} \nabla \cdot \left(\mathbf\Sigma_i \nabla v \right) = \chi \left( C_m \frac{\partial v}{\partial t} + I_\text{ion} \right)&lt;br /&gt;
,&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\mathbf\Sigma_i&amp;lt;/math&amp;gt; is the intracellular conductivity tensor, &amp;lt;math&amp;gt;v&amp;lt;/math&amp;gt; is the transmembrane potential, &amp;lt;math&amp;gt;I_\text{ion}&amp;lt;/math&amp;gt; is the transmembrane ionic current per unit area, &amp;lt;math&amp;gt;C_m&amp;lt;/math&amp;gt; is the membrane conductivity per unit area, &amp;lt;math&amp;gt;\lambda&amp;lt;/math&amp;gt; is the intra- to extracellular conductivity ratio, and &amp;lt;math&amp;gt;\chi&amp;lt;/math&amp;gt; is the membrane surface to volume ratio.&lt;br /&gt;
&lt;br /&gt;
==Derivation==&lt;br /&gt;
The [[Bidomain|bidomain model]] model can be written as&lt;br /&gt;
: &amp;lt;math&amp;gt;&lt;br /&gt;
\begin{alignat}{2}&lt;br /&gt;
\nabla \cdot \left(\mathbf\Sigma_i \nabla v \right) + \nabla \cdot \left(\mathbf\Sigma_i \nabla v_e \right) &amp;amp; = \chi \left( C_m \frac{\partial v}{\partial t} + I_\text{ion} \right) \\&lt;br /&gt;
\nabla \cdot \left( \mathbf\Sigma_i \nabla v \right) + \nabla \cdot \left( \left( \mathbf\Sigma_i + \mathbf\Sigma_e \right) \nabla v_e \right) &amp;amp; = 0&lt;br /&gt;
\end{alignat}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Assuming equal anisotropy ratios, i.e. &amp;lt;math&amp;gt;\mathbf\Sigma_e = \lambda\mathbf\Sigma_i&amp;lt;/math&amp;gt;, the second equation can be written&lt;br /&gt;
: &amp;lt;math&amp;gt;&lt;br /&gt;
\nabla \cdot \left(\mathbf\Sigma_i\nabla v_e\right) = -\frac{1}{1+\lambda}\nabla\cdot\left(\mathbf\Sigma_i\nabla v\right) &lt;br /&gt;
.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Inserting this into the first bidomain equation gives&lt;br /&gt;
: &amp;lt;math&amp;gt;&lt;br /&gt;
\frac{\lambda}{1+\lambda} \nabla \cdot \left(\mathbf\Sigma_i \nabla v \right) = \chi \left( C_m \frac{\partial v}{\partial t} + I_\text{ion} \right)&lt;br /&gt;
.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Cardiac electrophysiology]]&lt;br /&gt;
{{Applied-math-stub}}&lt;/div&gt;</summary>
		<author><name>en&gt;Luismanu</name></author>
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