Coupled Horizontal Spring Mass Oscillator: Difference between revisions
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Mark.bernet (talk | contribs) (New page: =Coupled Oscillator Spring Mass Oscillator: State Space = ==Problem Statement== Two 4 Kg Weights are suspended between two walls. They are connected by a spring between them with a spring...) |
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===Things we know=== |
===Things we know=== |
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<math>m_1 = |
<math>m_1 = 5 kg \frac{}{}</math> |
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<math>m_2 = |
<math>m_2 = 5 kg \frac{}{}</math> |
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<math>k_1 = 50 Nm \frac{}{}</math> |
<math>k_1 = 50 Nm \frac{}{}</math> |
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<math>k_3 = 50 Nm \frac{}{}</math> |
<math>k_3 = 50 Nm \frac{}{}</math> |
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<math>\text {So now that we have are problem we need to start setting up the equations we need to solve it.}\,</math> |
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<math>\dot{x_1}=\dot{x_1}</math> |
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<math>\ddot{x_1}+\frac{k_1+k_2}{m_1}{x_1}-\frac{k_2}{m_1}{x_2}=0</math> |
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<math>\dot{x_2}=\dot{x_2}</math> |
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<math>\ddot{x_2}+\frac{k_3+k_2}{m_2}{x_2}-\frac{k_2}{m_2}{x_1}=0</math> |
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<math>\text {Now we take these equations and put them in a state space model.}\,</math> |
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<math>\begin{bmatrix} \dot{x_1} \\\ddot{x_1} \\\dot{x_2} \\\ddot{x_2}\end{bmatrix}\, |
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</math> |
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= |
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<math>\begin{bmatrix}0&1&0&0 \\\frac{(k_1+k_2)}{m_1}&0&\frac{-k_1}{m_1}&0 \\0&0&0&1 \\\frac{-k_1}{m_2}&0&\frac{(k_1+k_2)}{m_2}&0 |
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\end{bmatrix} |
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\begin{bmatrix}x_1 \\\dot{x}_1 \\x_2 \\\dot{x}_2 |
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\end{bmatrix} |
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+ |
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\begin{bmatrix}0\end{bmatrix} |
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</math> |
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<math>\text {Now we make the appropriate numerical substitutions.}\,</math> |
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<math>\begin{bmatrix} \dot{x_1} \\\ddot{x_1} \\\dot{x_2} \\\ddot{x_2}\end{bmatrix}\, |
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</math> |
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= |
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<math>\begin{bmatrix}0&1&0&0 \\\frac{150}{5}&0&\frac{-50}{5}&0 \\0&0&0&1 \\\frac{-50}{5}&0&\frac{150}{5}&0 \end{bmatrix} |
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\begin{bmatrix}x_1 \\\dot{x}_1 \\x_2 \\\dot{x}_2\end{bmatrix} |
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+ |
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\begin{bmatrix}0\end{bmatrix} |
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</math> |
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<math>\begin{bmatrix} \dot{x_1} \\\ddot{x_1} \\\dot{x_2} \\\ddot{x_2}\end{bmatrix}\, |
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= |
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\begin{bmatrix}0&1&0&0 \\30&0&-10&0 \\0&0&0&1 \\-10&0&30&0\end{bmatrix} |
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\begin{bmatrix}x_1 \\\dot{x}_1 \\x_2 \\\dot{x}_2\end{bmatrix} |
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+ |
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\begin{bmatrix}0\end{bmatrix} |
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</math> |
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<math>\text {So using Maple I was able to obtain the eigenvalues and eigenvectors.}\,</math> |
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<math>\text {Eigenvalues.}\,</math> |
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<math>\lambda_1=2\sqrt{10}\,</math> |
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<math>\lambda_2=-2\sqrt{10}\,</math> |
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<math>\lambda_3=2\sqrt{5}\,</math> |
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<math>\lambda_4=-2\sqrt{5}\,</math> |
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<math>\text {Eigenvectors.}\,</math> |
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<math>\ {K_1=}\,</math><math>\begin{bmatrix}-1 \\-2\sqrt(10) \\1 \\2\sqrt(10)\end{bmatrix}\, |
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</math>,<math>\ {K_2=}\,</math><math>\begin{bmatrix}-1 \\2\sqrt(10) \\1 \\-2\sqrt(10)\end{bmatrix}\, |
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</math>,<math>\ {K_3=}\,</math><math>\begin{bmatrix}1 \\2\sqrt(5) \\1 \\2\sqrt(5)\end{bmatrix}\, |
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</math>,<math>\ {K_4=}\,</math><math>\begin{bmatrix}1 \\-2\sqrt(5) \\1 \\-2\sqrt(5)\end{bmatrix}\, |
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</math> |
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<math>\text {So then the answer is...}\,</math> |
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<math>\ x=c_1</math><math>\begin{bmatrix}-1 \\-2\sqrt(10) \\1 \\2\sqrt(10)\end{bmatrix}\,</math><math>e^{2\sqrt{10}}+ c_2</math><math>\begin{bmatrix}-1 \\2\sqrt(10) \\1 \\-2\sqrt(10)\end{bmatrix}\,</math><math>e^{2*-2\sqrt{10}}+ c_3</math><math>\begin{bmatrix}1 \\2\sqrt(5) \\1 \\2\sqrt(5)\end{bmatrix}\,</math><math>e^{3*2\sqrt{5}}+ c_4</math><math>\begin{bmatrix}1 \\-2\sqrt(5) \\1 \\-2\sqrt(5)\end{bmatrix}\,</math><math>e^{4*-2\sqrt{5}}\,</math> |
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==Solve with the Matrix exponential== |
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<math>\text {So first we need to know what the matrix exponential equation looks like.}\,</math> |
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<math>\text {it is...}\,</math> |
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<math>\tilde{x}=e^{\tilde{A}t}\tilde{x(0)}\,</math> |
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<math>\text {Where A is a matrix}\,</math> |
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<math>\text {Also }\,</math> |
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<math>\tilde{z}=\tilde{T}\tilde{x}\,</math> |
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<math>\tilde{x}=\tilde{T}^{-1}\tilde{z}\,</math> |
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<math>\text {Where }\,</math> |
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<math>\tilde{T}^{-1}=\,</math><math>\begin{bmatrix}-1&-1&1&1 \\-2\sqrt(10)&2\sqrt(10)&2\sqrt(5)&-2\sqrt(5) \\1&1&1&1 \\2\sqrt(10)&-2\sqrt(10)&2\sqrt(5)&-2\sqrt(5)\end{bmatrix}\, |
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</math> |
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<math>\text {I converted the T matrix to decimal form for make it easier to write up on here }\,</math> |
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<math>\tilde{T}=\,</math></math><math>\begin{bmatrix}-.25&-.039528&.25&.039528 \\-.25&.039528&.25&-.039528 \\.25&.055902&.25&.055902 \\.25&-.055902&.25&-.055902\end{bmatrix}\, |
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</math> |
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<math>\text {and}\,</math> |
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<math>\hat{A}=\,</math><math>\begin{bmatrix}e^{\lambda_1t}&0&0&0 \\0&e^{\lambda_2t}&0&0 \\0&0&e^{\lambda_3t}&0 \\0&0&0&e^{\lambda_4t}\end{bmatrix}\, |
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</math> |
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<math>e^{\hat{A}t}=\,</math><math>\begin{bmatrix}e^{2\sqrt{10}t}&0&0&0 \\0&e^{-2\sqrt{10}t}&0&0 \\0&0&e^{2\sqrt{5}t}&0 \\0&0&0&e^{-2\sqrt{5}t}\end{bmatrix}\, |
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</math> |
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<math>\text {Then the next step is}\,</math> |
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<math>\tilde{z}=e^{\hat{A}t}\tilde{z}(0)\,</math> |
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<math>\text {So that implies}\,</math> |
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<math>\tilde{x}=\tilde{T}^{-1}e^{\hat{A}t}\tilde{z}(0)\,</math><math>=\tilde{T}^{-1}e^{\hat{A}t}\tilde{T}^{-1}\tilde{x}(0)\,</math> |
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<math>\text {Now Simply substitute back in and we have the answer. }\,</math> |
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<math>\tilde{x}=\,</math><math>\begin{bmatrix}-1&-1&1&1 \\-2\sqrt(10)&2\sqrt(10)&2\sqrt(5)&-2\sqrt(5) \\1&1&1&1 \\2\sqrt(10)&-2\sqrt(10)&2\sqrt(5)&-2\sqrt(5)\end{bmatrix}\begin{bmatrix}e^{2\sqrt{10}t}&0&0&0 \\0&e^{-2\sqrt{10}t}&0&0 \\0&0&e^{2\sqrt{5}t}&0 \\0&0&0&e^{-2\sqrt{5}t}\end{bmatrix}</math><math>\begin{bmatrix}-.25&-.039528&.25&.039528 \\-.25&.039528&.25&-.039528 \\.25&.055902&.25&.055902 \\.25&-.055902&.25&-.055902\end{bmatrix}\tilde{x}(0)\,</math> |
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---- |
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Created By: Mark Bernet |
Latest revision as of 19:32, 9 December 2009
Coupled Oscillator Spring Mass Oscillator: State Space
Problem Statement
Two 4 Kg Weights are suspended between two walls. They are connected by a spring between them with a spring constant k2. They are connected to the walls by two springs k1 and k3 with k1=k3. m1 is a distance x1 form m2 and m2 is x2 from the wall.
Solution
Things we know
=
=
,,,
Solve with the Matrix exponential
</math>
Created By: Mark Bernet