Cederbaum's theorem[1] defines hypothetical analog electrical networks which will automatically produce a solution to the minimum s–t cut problem. Alternatively, simulation of such a network will also produce a solution to the minimum s–t cut problem. This article gives basic definitions, a statement of the theorem and a proof of the theorem. The presentation in this article closely follows the presentation of the theorem in the original publication.
Definitions in this article are consistent in all respects with those given in a discussion of the maximum-flow minimum-cut theorem.
Cederbaum's theorem applies to a particular type of directed graph: . V is the set of nodes.
E
E=(a,b)\inV x V
s\inV
t\inV
Flow,, is a positive quantity associated with each edge in the graph. Flow is constrained by the weight of the associated edge and by the conservation of flow at each vertex as described here.
Current is defined as a map for each edge pair to the real numbers, . Current maps from the voltage to a range that is determined by the weights of the respective forward and reverse edges. Each edge pair is the tuple consisting of the forward and reverse edges for a given pair of vertices. The current in the forward and reverse directions between a pair of nodes are the additive inverses of one another: . Current is conserved at each interior node in the network. The net current at the
s
t
s
s
Ns
Iin=
\sum | |
b\inNs |
isb
Voltage is defined as a mapping from the set of edge pairs to real numbers, . Voltage is directly analogous to electrical voltage in an electrical network. The voltage in the forward and reverse directions between a pair of nodes are the additive inverses of one another: . The input voltage is the sum of the voltages over a set of edges,
Pab
s
t
Vin=
\sum | |
(a,b)\inPab |
vab
An s–t cut is a partition of the graph into two parts each containing one of either
s
t
S\cupT=V
s\inS
t\inT
(S,T)
S
T
XC=\{(a,b)\inE\mida\inS,b\inT\}
An electrical network is a model that is derived from a flow graph. Each resistive element in the electrical network corresponds to an edge pair in the flow graph. The positive and negative terminals of the electrical network are the nodes corresponding to the
s
t
infty
A resistive element in the context of this theorem is a component of the electrical network that corresponds to an edge pair in the flow graph.
The
iv
(i) Current and voltage are continuous function with respect to one another.
(ii) Current and voltage are non-decreasing functions with respect to one another.
(iii) The range of the current is limited by the weights of the forward and reverse edges corresponding to the resistive element. The current range may be inclusive or exclusive of the endpoints. The domain of the voltage is exclusive of the maximum and minimum currents:
The limit of the current between the input terminals of the electrical network as the input voltage, approaches
infty
\lim | |
Vin → infty |
(Iin)=
min | |
XC |
\sum | |
(a,b)\inXC |
wab.
Claim 1 Current at any resistive element in the electrical network in either direction is always less than or equal to the maximum flow at the corresponding edge in the graph. Therefore, the maximum current through the electrical network is less than the weight of the minimum cut of the flow graph:
\lim | |
Vin → infty |
(Iin)\leq
min | |
XC |
\sum | |
(a,b)\inXC |
wab.
Claim 2 As the input voltage
Vin
X'C
\existsX'C \forall (a,b)\inX'C
\lim | |
Vin → infty |
(vab)=infty
This implies that:
\lim | |
Vin → infty |
(Iin)=
\sum | |
(a,b)\inX'C |
wab \geq
min | |
XC |
\sum | |
(a,b)\inXC |
wab.
Given claims 1 and 2 above:
\lim | |
Vin → infty |
(Iin)=
min | |
XC |
\sum | |
(a,b)\inXC |
wab.
The existence and uniqueness of a solution to the equations of an electrical network composed of monotone resistive elements was established by Duffin.[2]
Cederbaum's maximum flow theorem is the basis for the Simcut algorithm.[3] [4]