Fall 2009/JonathanS: Difference between revisions
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Now we can take the Laplace Transform to change the second order differential equation, from the t domain, into a simple linear equation, from the s domain, that's much easier to work with |
Now we can take the Laplace Transform to change the second order differential equation, from the t domain, into a simple linear equation, from the s domain, that's much easier to work with |
||
:<math>\mathcal{L}\{{\mathrm{d}^2\theta\over \mathrm{d}t^2}+{19.62}\theta\}=s^2F(s)-sf(0)-f^{ '}(0)+{19.62}\theta=0</math> |
:<math>\mathcal{L}\{{\mathrm{d}^2\theta\over \mathrm{d}t^2}+{19.62}\theta\}=s^2F(s)-sf(0)-f^{ '}(0)+{19.62}\theta=0</math> |
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:<math>\Rightarrow</math> <math> |
:<math>\Rightarrow</math> <math> s^2\theta(s)-s\theta(0)-\theta^{ '}(0)+{19.62}\theta=0 \,</math> |
Revision as of 13:50, 22 October 2009
Problem
A simple pendulum with a length L = 0.5m is pulled back and released from an initial angle . Find it's location at t = 3s.
Solution
Assuming no damping and a small angle(), the equation for the motion of a simple pendulum can be written as
Substituting values we get
Remember the identities
Now we can take the Laplace Transform to change the second order differential equation, from the t domain, into a simple linear equation, from the s domain, that's much easier to work with