Fall 2009/JonathanS: Difference between revisions

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== Solution ==
== Solution ==


Assuming no damping and a small angle(<math>\theta < 15^o</math>), the equation for the motion of a simple pendulum can be written as:
Assuming no damping and a small angle(<math>\theta < 15^o</math>), the equation for the motion of a simple pendulum can be written as
:<math>{\mathrm{d}^2\theta\over \mathrm{d}t^2}+{g\over \ell}\theta=0.</math>
:<math>{\mathrm{d}^2\theta\over \mathrm{d}t^2}+{g\over \ell}\theta=0.</math>


We can then use the Laplace Transform to convert from the '''time(t)''' domain into the '''s''' domain.


Substituting values we get
Given
:<math>\mathcal{L}\{f(t)\}=F(s)</math>
:<math>{\mathrm{d}^2\theta\over \mathrm{d}t^2}+{9.81\over 0.5}\theta=0.</math>
:<math>\Rightarrow{\mathrm{d}^2\theta\over \mathrm{d}t^2}+{19.62}\theta=0.</math>



:<math>{\mathrm{d}^2\theta\over \mathrm{d}t^2}=f^{ ''}(t)</math>
Remember the identities
:<math>\mathcal{L}\{f(t)\}=F(s)=\int_0^{\infty} e^{-st} f(t) \,dt. </math>


:<math>\mathcal{L}\{f^{ ''}(t)\}=s^2F(s)-sf(0)-f^{ '}(0)</math>
:<math>\mathcal{L}\{f^{ ''}(t)\}=s^2F(s)-sf(0)-f^{ '}(0)</math>

We have

:<math>\mathcal{L}\{{\mathrm{d}^2\theta\over \mathrm{d}t^2}+{g\over \ell}\theta\}=s^2F(s)-sf(0)-f^{ '}(0)+{g\over \ell}\theta</math>
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>\Rightarrow</math> <math>\s^2\theta-s\theta(0)-\theta^{ '}(0)+19.62\theta=0</math>

Revision as of 13:54, 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

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