Extra Solution 1.
See text and/or instructor's solution manual.
Answer.
.
Alternative
Answer.
,
where
for all
,
and
for all
.
Another
Answer.
.
Solution. Find
the Fourier Series
,
by computing the coefficients with Euler's
formulae:
(12.2)
,
and
(12.3)
.
First, calculate
.
Then
Second, calculate
.
Alternately,
is
an odd function so that
is
an odd function, and
for
all
.
Then Theorem
12.4 shows that
,
where the coefficients can be computed with the special
formula
.
Now calculate
Get The Answer.
Therefore,
.
We are done.
It is easy to rewrite
and
using
the well known facts
and
.
Therefore,
.
We are really done.
We have shown that
for
all
.
The even coefficients
can
be written
for
all
.
The even coefficients
can
be written
for
all
.
The odd coefficients
can
be written
for
all
.
Therefore,
,
where
for
all
, and
for
all
.
We are really really done.
Aside. We can
calculate a few terms in the sequences to confirm that they are the
same ( up to
).
Aside. We can
calculate a few terms in these series to verify that they are the
same ( up to
).
We are really done.
Aside. We can let Mathematica double check our work.
Aside. The Maple
commands are similar
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The partial lists of coefficients
and
are:
For illustration, we can sum the first few terms in these
series ( up to
).
Aside. The
function
can
be expressed in the form
.
We can compute a few terms of the Fourier series
of
using
Mathematica's built in procedure FourierTrigSeries.
.
Remark. Since
is
a point of discontinuity of
, we
know that
is
not defined at
, and
,
where
and
denote
the left-hand and right-hand limits,
respectively.
Convergence is not uniform on the closed
interval
, and
the overshooting of
is referred to as "Gibbs
phenomenon."
We are really really done.
Aside. There are at
least four solutions to this problem.
We can use Mathematica to sum the infinite
series.
However, these sum might not be as familiar as those studied in
calculus.
Aside. The Maple
commands are similar
We are really really really done.
Aside. We can graph these functions to verify they are correct.
We are really really really really done.
Aside. Let us
announce that in Section
12.2 we interpret the Fourier Series
as boundary values on the circle
,
and construct the harmonic function
inside the unit disk
with
.
The
harmonic function
, with
.

A
contour graph of the harmonic function
.
This solution is complements of the authors.
(c) 2010 John H. Mathews, Russell W. Howell