- #1
skrat
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- 8
Homework Statement
It's not really a homework so I will try to be as clear as possible. Hopefully, somebody will understand me and be able to help.
I used Euler-Bernoulli theory to analyze the dynamics of a free-free beam (for the problem it is not important to understand what it is). If one discreticizes a beam into ##n=5## equal parts (as in the picture)
than each NODE has two variables (the deflection and the angle of rotation). Declaring a vector ##\vec d## of variables simplifies the writing a bit $$\vec d=(W_1,\Phi_1,W_2,\Phi_2,W_3,\Phi_3,W_4,\Phi_4,W_5,\Phi_5,W_6,\Phi_6)^\intercal.$$
Now let's assume we have the global stiffness (##\ K##) and mass (##\ M##) matrices. The equation we have to solve than is $$\ M \ddot{ \vec d}+\ K\vec d=\vec 0$$
Assuming the system will respond harmonically (in that case ##\ddot{ \vec d}=-\omega_0^2\vec d##) the equation of motion rewrites into $$(K-\omega_0^2\ M)\vec d=\vec 0$$ or even better (assuming ##\ M## is reversible $$(\ M^{-1}\ K-\omega_0^2)\vec d=0$$
Now this is an eigenproblem now. Eigenvalues are frequencies of corresponding modes (eigenvectors).
Homework Equations
The Attempt at a Solution
Ok...
Solving that eigensystem is really not a problem, so let's assume I have the eigenvalues and eigenvectors.
Now let's say I would like to visualize the displacement (so every odd component of a vector ##\vec d##). How do I do that? Would it make sense to simply multiply an eigenvector by vector ##(1,0,1,0,1,0,1,0,1,0,1,0)## to simply ignore the angles or is that completely wrong?