Ux y x y our physical intuition suggests that the

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Unformatted text preview: ximated by P = −2 1 0 · 0 1 −2 1 · 0 0 1 −2 · · ··· ··· ··· ··· ··· n2 P u, 0 0 · · −2 . Finally, the coefficient (T /ρ(x)) can be represented by the diagonal matrix 0 0 ··· 0 T /ρ(x1 ) 0 T /ρ(x2 ) 0 ··· 0 . 0 0 T /ρ(x3 ) · · · · Q= · · · ··· · 0 0 · · · · T /ρ(xn−1 ) Putting all this together, we find that our wave equation with variable mass density is approximated by a second order homogeneous linear system of ordinary differential equations d2 u = Au, dt2 where A = n2 QP. The eigenvalues of low absolute value are approximated by the eigenvalues of A, while the eigenfunctions representing the lowest frequency modes of oscillation are approximated eigenvectors corresponding to the lowest eigenvalues of A. For example, we could ask the question: What is the shape of the lowest mode of oscillation in the case where ρ(x) = 1/(x + .1)? To answer this question, 113 we could utilize the following Mathematica program (which is quite similar to the one presented in...
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This document was uploaded on 01/12/2014.

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