Construction of the nodal conductance matrix of a planar resistive grid and derivation of the analytical expressions of its eigenvalues and eigenvectors using the Kronecker product and sum
V. Tavşanoglu · 2016
This paper considers the task of constructing an (M×A+1)-node rectangular planar resistive grid as: first forming two (M×A+1)-node planar sub-grids; one made up of M of (N+1)-node horizontal, and the other of N of (M+1)-node vertical linear resistive grids, then joining their corresponding nodes. By doing so it is sho wn that the nodal conductance matrices GHand GVof the two sub-grids can be expressed as the Kronecker products GH= IM⊗ GN, GV= GM⊗ In, and G of the resultant planar grid as the Kronecker sum G = GN⊕ GM, where GMand IMare, respectively, the nodal conductance matrix of a linear resistive grid and the identity matrix, both of size M. Moreover, since the analytical expression s for the eigenvalues and eigenvectors of GM- which is a symmetric tridiagonal matrix - are well known, this approach enables the derivation of the analytical expressions of the eigenvalues and eigenvectors of GH, GVand G in terms of those of GMand GN, thereby drastically simplifying their computation and rendering the use of any matrix-inversion-based method unnecessary in the solution of nodal equations of very large grids.