Series

Polynomial eigenvalue — the series

2 essays on one idea, from the one that introduces it to the one that assumes the rest.
  1. 00.0939569-2-1.24498-0.4899610.2650581.020081.7751real partimaginary parttwo routes, one spectrumeigenvalues16rows8complex16against the closed form2.1·10⁻¹⁵n rows and 2n eigenvaluesso the eigenvectors are not a basis

    A matrix that depends on its own eigenvalue

    A damped structure does not produce Ax = λx. It produces (λ²M + λC + K)x = 0, where the matrix whose null vector is wanted is a function of the number being solved for — so there is nothing to factorise, an n × n problem has 2n answers, and the eigenvectors cannot be a basis.

    part 1 · polynomial
  2. finite eigenvalues (degree of det Q)13at infinity (2n − degree)1at infinity, by the rank of M12n, if M were nonsingular14a degree, not a decisiondegree of det Q13at infinity1by the rank of M1singular-value gap∞the count is a degreeand the other route is a judgement

    One mass removed, and one eigenvalue gone

    A coordinate with no inertia reads like a coordinate that has been deleted, and a chain of eight masses with one of them removed would then be a chain of seven, with fourteen eigenvalues. It has fifteen. The massless coordinate is still there, still carrying a damper, and it contributes a first-order equation rather than none.

    part 2 · polynomial

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