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We also know what T equals and we can solve it for our case |
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'''We also know what T equals and we can solve it for our case''' |
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:<math>T^{-1}=[k_1|k_2|k_3|k_4]\,</math> |
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:<math>T^{-1}=[k_1|k_2|k_3|k_4]\,</math> |
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:<math>T^{-1}=\begin{bmatrix} |
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:<math>T^{-1}=\begin{bmatrix} |
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\end{bmatrix}</math> |
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\end{bmatrix}</math> |
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Taking the inverse of this we can solve for T |
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'''Taking the inverse of this we can solve for T''' |
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:<math>T=\begin{bmatrix} |
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:<math>T=\begin{bmatrix} |
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0 & 0 & 0 & 0 \\ |
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0 & 0 & 0 & 0 \\ |
Revision as of 14:05, 10 December 2009
Problem Statement
Write up on the Wiki a solution of a coupled oscillator problem like the coupled pendulum. Use State Space methods. Describe the eigenmodes and eigenvectors of the system.
Initial Conditions:
Equations for M_1
Equations for M_2
Additional Equations
State Equations
=
With the numbers...
=
Eigen Values
Once you have your equations of equilibrium in matrix form you can plug them into MATLAB which will give you the eigen values automatically.
- Given
We now have
From this we get
Eigen Vectors
Using the equation above and the same given conditions we can plug everything into MATLAB and get the eigen vectors which we will denote as .
Matrix Exponential
We now use matrix exponentials to solve the same problem.
So from the above equation we get this to prove the matrix exponetial works.
We also know what T equals and we can solve it for our case
Taking the inverse of this we can solve for T