Possibly silly linear algebra question

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The discussion revolves around solving a generalized circuit using 4x4 tensor matrices, focusing on simplifying the problem by setting common nodes to zero current. A proposed method involves deleting a specific equation and variable from the system, resulting in a smaller system that can be solved using Gaussian elimination. This approach allows for the calculation of all variables except the deleted one, which is assumed to be zero. Participants confirm that this method effectively addresses the original query. The conversation highlights a matrix-level solution to a complex circuit problem without relying on algebraic methods.
sokrates
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This is NOT homework.

I am trying to solve a generalized circuit ( each node is a 4-component generalization) and matrices are 4x4 tensors.

And I am trying to write them down -- making common nodes "zero" current, ending up with a matrix as in what's shown in the link:


http://imgur.com/xAgNPMD

Is there a non-algebraic, clean matrix-level way of solving the problem I describe there?

If the answer is not obvious please let me know. :)
 
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We can delete the i:th-equation and the variable xi (corresponding to the matrix obtained from A by deleting row i and column j), obtaining a system with n-1 equations and n-1 unknowns, which can be solved by e.g. Gaussian elimination. This gives us values of all variables except xi, which is assumed to be 0. With these values, yi can now be calculated.
 
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Yes - you are right.This was exactly what I was looking for.
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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