Fall 2009/JonathanS: Difference between revisions
Jump to navigation
Jump to search
Line 5: | Line 5: | ||
== 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>\ |
:<math>{\mathrm{d}^2\theta\over \mathrm{d}t^2}+{9.81\over 0.5}\theta=0.</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 |
|||
⚫ | |||
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>\Rightarrow</math> <math>\s^2\theta-s\theta(0)-\theta^{ '}(0)+19.62\theta=0</math> |
Revision as of 12:54, 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
- Failed to parse (unknown function "\s"): {\displaystyle \s^2\theta-s\theta(0)-\theta^{ '}(0)+19.62\theta=0}