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In graph theory, the resistance distance between two vertices of a simple connected graph, G, is equal to the resistance between two equivalent points on an electrical network, constructed so as to correspond to G, with each edge being replaced by a 1 ohm resistance. It is a metric on graphs.
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On a graph G, the resistance distance Ωi,j between two vertices vi and vj is defined as
\Omega_{i,j}:=\Gamma_{i,i}+\Gamma_{j,j}-\Gamma_{i,j}-\Gamma_{j,i}\,
where Γ is the Moore-Penrose inverse of the Laplacian matrix of G.
If i=j then
For an undirected graph
\Omega_{i,j}=\Omega_{j,i}=\Gamma_{i,i}+\Gamma_{j,j}-2\Gamma_{i,j}\,
For any N-vertex simple connected graph G = (V, E) and arbitrary NXN matrix M:
From this generalized sum rule a number of relationships can be derived depending on the choice of M. Two of note are;
where the are the non-zero eigenvalues of the Laplacian matrix.
For a simple connected graph G = (V, E), the resistance distance between two vertices may by expressed as a function of the set of spanning trees, T, of G as follows:
\Omega_{i,j}=\begin{cases} \frac{\left | \{t:t \in T, e_{i,j} \subseteq T\} \right \vert}{\left | T \right \vert}, & (i,j) \in E\\ \frac{\left | T^\'-T \right \vert}{\left | T \right \vert}, &(i,j) \not \in E \end{cases}
where T\' is the set of spanning trees for the graph .
In classical mechanics, resistance distance is defined as the distance from the resistance (on a lever) to the fulcrum.
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