M344 Lab 1The Vibrating Drum

Our goal is to develop equations that govern the vibrations of a circular drum. The wave equation in two spatial dimensions is
MATH
For a circular drum we need to write the right-hand side in polar coordinates. It can be shown (extra credit if you can show this) that in polar coordinates the wave equation is
MATH

Here, $u(r,\theta ,t)$ represents the vertical displacement of the drum head at a distance $r$ from the center of the drum, and at angle $\theta $ from the $x-axis$, and at time $t.$ This is where the Wikipedia article at http://en.wikipedia.org/wiki/Vibrations_of_a_circular_drum begins.


The eigenfunction solutions to this equation, both for the radially symmetric case and the full case, are given in the article. In order to satisfy a general initial condition, an infinite sum of the eigenfunction solutions would have to be taken.


Assume that $c=1$ and that the drum has radius $1$. We will start with the radially symmetric case. This means that $u(r,\theta ,t)$ does not depend on $\theta $, and so we can write just $u(r,t)$. The boundary conditions are $u(0,t)<\infty $ and $u(1,t)=1$. After separation of variables into $u(r,t)=R(r)T(t)$ the boundary conditions on $R(r)$ become $R(0)<\infty $ and $R(1)=0$.


In our text, the authors derive a series formula for Bessel functions by using a series solution to the Bessel differential equation. In the next part of the lab, we want to investigate how useful the series representation of Bessel functions is. In particular, how many terms in the series do we need in order to get useful results? We will try to replicate the results from the first bullet without the built-in Maple Bessel function.


Write a paper incorporating the two bullets above. Is the infinite series representation of a Bessel function practical for finding the higher modes of vibration of a drum? Explain why it is hard, but important, to calculate values of a Bessel function $J_{\nu }(r)$ for large $r$.

This document created by Scientific Notebook 4.1.