Title: Circular Membrane Problem
1Circular Membrane Problem
2The circular membrane has a radius of
a
3Lets return to the study of the wave equation
with a circular boundary condition
Has separable solutions
where
.
4Lets return to the study of the wave equation
with a circular boundary condition
Has separable solutions
where
.
5Lets return to the study of the wave equation
with a circular boundary condition
Has separable solutions
where
.
6Lets return to the study of the wave equation
with a circular boundary condition
Has separable solutions
where
.
7Lets return to the study of the wave equation
with a circular boundary condition
Has separable solutions
where
.
8Lets return to the study of the wave equation
with a circular boundary condition
Has separable solutions
where
.
Bessels Equation
9Boundary conditions make this a Sturm-Liouville
problem on 0,a.
The BC at the (regular singular) point
is
finite.
10The radial factor of the solution is a Bessel
function of the first kind
11The radial factor of the solution is a Bessel
function of the first kind
Bessel functions are to cylindrical waves what
cosines/sines are to waves on a straight line.
12The radial factor of the solution is a Bessel
function of the first kind
However, Bessel functions are NOT periodic and
the distance between zeros is NOT constant.
13The only remaining BOUNDARY CONDITION of the
circular membrane problem is that
at
This implies that
.
Therefore
nth positive zero of
(And let .)
14Therefore
Which is a solution of a SL problem with
eigenvalue
and weight function
.
(See lecture 11.)
15Therefore we have the SS
And the GS
(See (13.1.1) of the notes.)
16So we now have the GS of the circular membrane
problem.
What about ICs?
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20As an aside, here is a plot of
21Plot of
REMEMBER
Unlike the sine and cosine functions
The roots of are not equally spaced.
22Plot of
REMEMBER
Unlike the sine and cosine functions
The roots of are not equally spaced.
However, the procedure is still analogous to the
sine case of the 1D wave equation.
23So, recall that we have
24As shown in section 12, the Sturm-Liouville
theory gives us
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26Therefore
where