Laplace transforms: Critically Damped Motion: Difference between revisions

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<math>\text {it through the Laplace Transform.}\,</math>
<math>\text {it through the Laplace Transform.}\,</math>


<math>\mathcal{L}\frac{d^2x}{dt^2}+8\frac{dx}{dt}+16x</math><br /><br />
<math>\mathcal{L}[\frac{d^2x}{dt^2}+8\frac{dx}{dt}+16x]</math><br /><br />


<math>\text {And we get the equation (after some substitution and simplification)}.\,</math>
<math>\text {And we get the equation (after some substitution and simplification)}.\,</math>
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<math>\text {Now that we have completed the Laplace Transform}\,</math>
<math>\text {Now that we have completed the Laplace Transform}\,</math>
<math>\text {and solved for X(s) we must so an inverse Laplace Transform. }\,</math>
<math>\text {and solved for X(s) we must so an inverse Laplace Transform. }\,</math>

<math>\mathcal{L}^{-1}[-\frac{3}{(s+4)^2}]</math><br /><br />

<math>\text {and we get}\,</math>

<math>\mathbf {x}(t)=-3te^{-4t}</math><br /><br />

<math>\text {So there you have it the equation of a Critically Damped spring mass system.}\,</math>

Revision as of 18:09, 22 October 2009

Using the Laplace Transform to solve a spring mass system that is critically damped

Problem Statement

An 8 pound weight is attached to a spring with a spring constant k of 4 lb/ft. The spring is stretched 2 ft and rests at its equilibrium position. It is then released from rest with an initial upward velocity of 3 ft/s. The system contains a damping force of 2 times the initial velocity.

Solution

Things we know

Solving the problem