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for
Dirichlet Problem for the Disk
Chapter 12 Fourier Series and the Laplace Transform
12.2 The Dirichlet Problem for the Unit Disk
We have emphasized
practical applications of harmonic functions to steady state
temperatures, electrostatics, and fluid flow in Chapter
11.
In Section
11.2 we introduced the N-Value Dirichlet problem, and
showed how to solve Laplace's equation
,
in the upper-half plane, for a harmonic
function
that has certain specified boundary values on the real
axis.
Now we will develop the solution to the Dirichlet problem in the
closed unit disk
.
Dirichlet Problem for the Unit
Disk
Given a real valued
function
that
is both piecewise continuous and a bounded function.
Let
be
considered as boundary values on the unit circle
, in
the sense that
(12.10)
, at
points
on
the unit circle.
The Dirichlet
problem for the closed unit disk
is
to extend
to
be
for
,
where
is
harmonic in the unit disk and take on the boundary values
(12.10) at points
where
is
continuous.
Our first method
of solution uses the Fourier Series representation
for
that
was developed in Section
12.1.
Theorem 12.7 (Extended Fourier Series in
the unit disk). Let
be
the boundary values on the unit circle
,
(12.10.1)
.
If
has
the Fourier series representation
,
then
(12.11.1)
,
solves the Dirichlet problem and is a harmonic function in the unit
disk
.
We can motivate
Theorem 12.7 if we are allowed to make the following
claim:
The series in (12.11.1) takes on the
boundary values in Equation (12.10.1) at
points on
where
the radial limits exist, that is
Furthermore, Exercise 12 in Section
3.3 shows that each of the terms,
and
are
harmonic,
and so it is reasonable to conclude that the infinite series
representing
in
Equation (12.11.1) will be
harmonic.
Remark. The radial limits
will exist except at the finite number of points
where
is
discontinuous.
There are details regarding the convergence of the series and the
existence of radial limits that are left for advanced study.
Example 12.3. Find
the function
that
is harmonic in the unit disk
and takes on the boundary values
.
Solution.
Using the result
of Example 12.1 in Section
12.1, we write the Fourier series
for
,
.
Using Equation (12.11.1) for the
extended Fourier series solution of the Dirichlet problem, we
obtain
.
The series representations
of
take
on the prescribed boundary values at points
where
is
continuous.
The boundary function
is
discontinuous at
, which
corresponds to
; which
are points where
was
not prescribed.
The approximations and ![]()
,
and the true solutions and ![]()
are
shown in the figures below.
Figure
12.13.A. The functions
and
.
Figure
12.13.B. The functions
and
.
Our next result, Theorem 12.8, is the
analog to Theorem 11.3, Poisson's integral formula for the upper
half-plane, that was introduced in Section
11.3.
It shows that the value of the harmonic
function
inside
the unit disk is a special "average of the
values
on
the boundary."
In the integrand the function
is multiplied by the Poisson
kernel
which
includes the variables
.
Theorem 12.8 (Poisson Integral Formula in
the unit disk). Let
be
the boundary values on the unit circle
,
(12.10.2)
.
If
is
both piecewise continuous and bounded, then
(12.11.2)
,
,
solves the Dirichlet problem and is a harmonic function in the unit
disk
.
Observation. The integrand is
taken over the unit circle where the parameter of integration
is
, and
the numerator includes the function
.
Corollary 12.1 (N-Value
Dirichlet solution for the unit
disk). Assume that
.
If
is
the boundary value function on the unit circle
,
(12.10.3)
then
(12.11.3)
,
solves the Dirichlet problem and is a harmonic function in the unit
disk
.
Proof. Use the
indefinite integral
.
Then
![[Graphics:Images/DirichletProblemDiskMod_gr_111.gif]](dirichletproblemdisk/DirichletProblemDiskMod/Images/DirichletProblemDiskMod_gr_111.gif)
Remark. When applying formula (12.11.3) it is necessary to pay attention and to use appropriate branches and to beware of branch cuts.
Extra Example
1. Find the function
that
is harmonic in the unit disk
,
and takes on the boundary values
Figure
1. The graphs
of
and
.
Solution using Fourier series.
In Exercise 9 in Section
12.1, we showed that the Fourier series
for
can be written as
.
Use Equation (12.11.3) to construct
the extended Fourier series solution of the Dirichlet problem.
Therefore, the Fourier series solution is
.
Solution using Poisson's
integral.
Use the known anti-derivative
and
get
Therefore, the Poisson integral solution is
.
Solution using N-Value Dirichlet
formula.
Set
and
and
then use the
formula (12.11.3) and
get
![[Graphics:Images/DirichletProblemDiskMod_gr_127.gif]](dirichletproblemdisk/DirichletProblemDiskMod/Images/DirichletProblemDiskMod_gr_127.gif)
Therefore, the N-Value Dirichlet solution is
.
Remark. This is just a
straightforward way of calculating the Poisson integral solution, and
is recommended for working some of the exercises.
Extra Example
2. Find the function
that
is harmonic in the unit disk
,
and takes on the boundary values
.
Figure
2. The graphs
of
and
.
Remarks. Some
integrals of the form
are
readily available.
For
the
computer algebra systems Mathematica and Maple can be used to
obtain the following formulae.
![]()
The software Maple will also compute the above integrals, but the
Maple syntax will use the notation
and
.
The first integral
can
easily be verified using techniques from calculus.
Caveat. It is beyond
the scope of this book to use the other two integrals
involving
.
Exercises for Section 12.2. The Dirichlet Problem for the Unit Disk
Vibrations in Mechanical Systems
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