Background.
Consider the second order linear differential equation
(1) .
Rewrite this equation in the form , then
use the substitutions and and
rewrite the differential equation (1) in the form
(2) .
Definition (Analytic). The
functions
and
are analytic at
if they have
Taylor series expansions with radius of
convergence
and ,
respectively. That is
which
converges for
and
which
converges for
Definition (Ordinary
Point). If the functions
and
are analytic at
,
then the point
is called an
ordinary point of the differential equation
.
Otherwise, the point
is called a
singular point.
Definition (Regular
Singular Point). Assume that
is a singular point of (1) and that
and
are analytic at
.
They will have Maclaurin series expansions with radius of convergence
and ,
respectively. That is
which
converges for
and
which
converges for
Then the point
is called a regular singular point of the
differential equation (1).
Method of Frobenius.
This method is attributed to the german mathemematican
Ferdinand Georg Frobenius (1849-1917 ). Assume
that
is
regular singular point of the differential equation
.
A
Frobenius series (generalized Laurent series)
of the form
can be used to solve the differential equation. The parameter
must be chosen so that when the series is substituted into the D.E. the
coefficient of the smallest power of
is zero. This is called the indicial equation. Next, a recursive equation for
the coefficients is obtained by setting the coefficient of equal
to zero. Caveat: There are some instances when only one Frobenius solution can
be constructed.
Definition (Indicial
Equation). The parameter
in the Frobenius series is a root of the indicial equation
.
Assuming that the singular point is ,
we can calculate
as follows:
and
The Recursive Formulas.
For each root
of the indicial equation, recursive formulas are used to calculate the unknown
coefficients
. This
is custom work because a numerical value for
is easier use.
Application of the Vibrating Drum
The two dimensional wave equation is ,
in rectangular coordinates it is ,
and in polar coordinates it is .
Consider a drum head that a flexible circular membrane of radius
. Assume
that it is struck in the center and this produces radial vibrations only where
the displacement depends only on time
and distance
from the center. Then
satisfies the D.E.
.
Surface equation for the vibrating drum.
The solution we are seeking in Example 7 is
where the boundary condition
requires that , hence .
Therefore the fundamental solutions to the wave equation for the drum head is
, for n
= 1,2,3.
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