Random walks and the effective resistance sum rules
In this paper, using the intimate relations between random walks and electrical networks, we first prove the following effective resistance local sum rules: c i Ω i j + ∑ k ∈ Γ ( i ) c i k ( Ω i k − Ω j k ) = 2 , where Ω i j is the effective resistance between vertices i and j , c i k is the conduct...
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Published in: | Discrete Applied Mathematics Vol. 158; no. 15; pp. 1691 - 1700 |
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Main Author: | |
Format: | Journal Article |
Language: | English |
Published: |
Kidlington
Elsevier B.V
06-08-2010
Elsevier |
Subjects: | |
Online Access: | Get full text |
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Summary: | In this paper, using the intimate relations between random walks and electrical networks, we first prove the following effective resistance local sum rules:
c
i
Ω
i
j
+
∑
k
∈
Γ
(
i
)
c
i
k
(
Ω
i
k
−
Ω
j
k
)
=
2
,
where
Ω
i
j
is the effective resistance between vertices
i
and
j
,
c
i
k
is the conductance of the edge,
Γ
(
i
)
is the neighbor set of
i
, and
c
i
=
∑
k
∈
Γ
(
i
)
c
i
k
. Then we show that from the above rules we can deduce many other local sum rules, including the well-known Foster’s
k
-th formula. Finally, using the above local sum rules, for several kinds of electrical networks, we give the explicit expressions for the effective resistance between two arbitrary vertices. |
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Bibliography: | ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
ISSN: | 0166-218X 1872-6771 |
DOI: | 10.1016/j.dam.2010.05.020 |