Each supplied eigenvector gives relative displacements at in a standing wave. Insert zero at to describe the whole sampled string. A real normal mode is : its shape stays fixed while its amplitude oscillates.
These semidiscrete fixed-string normal modes are samples of , with in the order listed. More precisely, their interior vectors are , which have unit Euclidean norm and form an orthonormal basis of . Their eigenvalues and angular frequencies obey
Thus larger absolute value of a negative eigenvalue means faster oscillation, rather than faster decay. The numerical angular frequencies approximate the continuous fixed-string values ; the finite difference spatial approximation changes them. Only three independent interior normal modes exist on this grid, and any interior displacement or initial velocity vector can be expanded in this orthonormal basis.
Figure 1.
Three fixed-string normal modes and conservative four-box transport
. The left panels show the supplied unit eigenvectors with zero endpoints; smooth sine curves guide the eye through the samples. The right panel is an original directed graph of the numerical transport matrix in Question 6: every arrow from j to i is labelled by Aij. It is not a reproduction of source Figure 6. Details.

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