Coupled Oscillator: Coupled Mass-Spring System with Damping: Difference between revisions

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<math> \ddot{x}_1= - \frac{2b_1}{m_1} \dot{x}_1 - \frac{k_1}{m_1}l_1 - \frac{k_1}{m_1}x_1 + \frac{k_2}{m_2}l_1 + \frac{k_2}{m_2}x_2 + g </math>
<math> \ddot{x}_1= - \frac{2b_1}{m_1} \dot{x}_1 - \frac{k_1}{m_1}x_1 + \frac{k_2}{m_2}x_2 1 \frac{k_2}{m_2}x_1 + g </math>


and
and


<math> \ddot{x}_2= - \frac{2b_2}{m_2} \dot{x}_2 - \frac{k_2}{m_2}l_2 - \frac{k_2}{m_2}x_2 + g </math>
<math> \ddot{x}_2= - \frac{2b_2}{m_2} \dot{x}_2 - \frac{k_2}{m_2}x_2 + \frac{k_2}{m_2}x_1 + g </math>


==State Space Equation==
==State Space Equation==

Revision as of 11:27, 3 December 2009

Problem Statement

For the below system set up a set of state variable equations, and then solve using Laplace transformations. Assume all motion takes place in the vertical directions.

Fig. 1

Initial Values

For the upper mass:

And for the lower mass:

Find the Force Equations

First we need to sum forces in the y-direction for each block.

For mass 1:


For mass 2:


So if we put the equations above into the correct form we have:


and

State Space Equation

The general form for the state equation is as shown below:



Where denotes a matrix and denotes a vector.


If we let , , , and be the state variables, then



We don't need to include gravity here if we allow are initial conditions for the spring be zero with gravity accounted for.