Abstract

In this paper we study Current Density Impedance Imaging (CDII) on Electrical Networks. The inverse problem is to determine the conductivity matrix of an electrical network from the prescribed knowledge of the magnitude of the induced current along the edges coupled with the imposed voltage or injected current on the boundary nodes. This problem leads to a weighted $ l^1 $ minimization problem for the corresponding voltage potential. We also investigate the problem of determining the transition probabilities of random walks on graphs from the prescribed expected net number of times the walker passes along the edges of the graph. Convergent numerical algorithms for solving such problems are also presented. Our results can be utilized in the design of electrical networks when certain current flow on the network is desired as well as the design of random walk models on graphs when the expected net number of the times the walker passes along the edges is prescribed. We also show that a mass preserving flow $ J = (J_{ij}) $ on a network can be uniquely recovered from the knowledge of $ |J| = (|J_{ij}|) $ and the flux of the flow on the boundary nodes, where $ J_{ij} $ is the flow from node $ i $ to node $ j $ and $ J_{ij} = -J_{ji} $, and discuss its potential application in cryptography.

Highlights

  • Let G = (V, E) be a simple, undirected, weighted graph with n vertices

  • We will assume that Jij = 0 if the vertices i and j are not connected by an edge, and that Jii = 0

  • The inverse problem we investigate here translates to intriguing questions in various contexts where a random walk model on graphs is utilized

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Summary

Introduction

In this paper we are interested in the inverse problem of determining the conductivity matrix of an electrical network from the knowledge of the induced current along the edges of the network and Dirichlet or Neumann boundary conditions. We study the inverse problem of determining the conductivity matrix σ = (σij)n×n from the knowledge of its induced current J = (Jij)n×n on E and the imposed voltage potential f on ∂V (Dirichlet boundary conditions).

Results
Conclusion

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