Math 309B/C Winter 2012, Homework 5
Due February 15
- Sketch the following functions and determine whether the
following functions are odd or even whenever they are defined
(in the given intervals if there are any)
- $\tan x$ Answer: This function is odd since
$\tan(-x)=\frac{\sin(-x)}{\cos(-x)}=\frac{-\sin x}{\cos
x}=-\tan x$.
- $x(x^{2}-1)$ for $x\in [-1,1]$ Answer: This
function (call it $f(x)$) is odd since
\[f(-x)=(-x)((-x)^{2}-1)=-x(x^2-1)=-f(x).\]
- $x^{3}$
- Find the Fourier series of the following functions and
determine their values at the given points.
- Let $f$ be the $2$-periodic function defined by
$f(x)=\frac{x}{|x|}$ for $x\in [-1,1]$. Find the values of
its Fourier series in $[-1,1]$. What is the value at $x=3$?
Answer: Note that $|x|=\left\{\begin{array}{cc} x
& x\geq 0 \\ -x & x\leq 0\end{array}\right.$. Hence,
$\frac{x}{|x|}=\left\{\begin{array}{cc} 1 & 0
- Let $f=\left\{\begin{array}{cc} x+\pi &
2x-2\pi\end{array}\right.$ and $f(x+4)=f(x)$. Find the
Fourier series and the values in $[-2,2]$.
- Let $f$ be the
$1$-periodic function $f(x)=(1+\frac{x}{|x|})x^{2}$ for
$x\in [-1/2,1/2]$. Find its Fourier series and its values
in $[-1/2,1/2]$.
- Let $f(x)=\left\{\begin{array}{cc} 0 & 1<|x|<2
\\ x & |x|<1.\end{array}\right.$, and $f(x+4)=f(x)$
(so $f$ is $4$-periodic). Find the values of the Fourier
series in $[-2,2]$. Answer: Note that this function
is odd. So $a_0=a_n=0$. And, since $f$ is zero outside the
interval $-1,1$, \begin{align*} b_{n} &
=\frac{1}{2}\int_{-2}^{2}f(x)\sin\frac{n\pi x}{2}
=\frac{1}{2}\int_{-1}^{1}f(x)\sin \frac{n\pi x}{2}
=\int_{0}^{1}f(x)\sin \frac{n\pi x}{2} =\int_{0}^{1}x\sin
\frac{n\pi x}{2} =-\frac{x\cos \frac{n\pi
x}{2}}{\frac{n\pi}{2}}|_{0}^{1}
+\frac{2}{n\pi}\int_{0}^{1}\cos \frac{n\pi x}{2}\\ &
=\frac{-2\cos \frac{n\pi }{2}}{n\pi}+\frac{4}{n^2 \pi^2}\sin
\frac{n\pi x}{2}|_{0}^{1} =-\frac{2\cos
\frac{n\pi}{2}}{n\pi}+\frac{4}{n^2 \pi^2}\sin
\frac{n\pi }{2}.\end{align*} So the Fourier series is \[F(x)
=\sum_{n=1}^{\infty}(-\frac{2\cos
\frac{n\pi}{2}}{n\pi}+\frac{4}{n^2 \pi^2}\sin
\frac{n\pi }{2})\sin \frac{n\pi x}{2}).\] The values of $F$
on $[-2,2]$ are equal to $f(x)$ wherever $f$ is continuous,
so that's everywhere except for $-1$ and $1$. At $1$, it is
equal to the average of the left and right limits of $f$ at
$1$, so
\[F(1)=\frac{f(1+)+f(1-)}{2}=\frac{1+0}{2}=\frac{1}{2}.\]
Similarly, $F(-1)=\frac{1}{2}$.
- Let $f(x)=x^{3}$ for
- Show that the derivative of an even function is odd and the
derivative of an odd function is even. Answer: If $f$
is even, then $f(x)=f(-x)$. Differentiating both sides of this
equation (and using chain rule) gives $f'(x)=-f'(-x)$, hence
$-f'(x)=f'(-x)$, so $f'$ is odd. A similar proof works if $f$ is
odd.
- Show that if $f$ and $g$ are odd, then $f(g(x))$ is odd, and
if $f$ is odd and $g$ is even, then $f(g(x))$ and $g(f(x))$ are
even.
The next exercise shows how the Fourier coefficients can tell you
how nice or smooth your function is. Basically, if your have a
nice enough first derivative, then your Fourier coefficients will
be converging to zero at a certain rate (like $\frac{1}{m}$-fast).
Hence, if you have a Fourier series whose Fourier coefficients
are, say, $\frac{1}{m^{2/3}}$, this means that your function's
derivative must either be unbounded, or is not piecewise
continuous.
- Show that if $f$ is continuous $2L$-periodic function and its
derivative is bounded (i.e. for all $x$, $|f'|\leq M$ for some
$M>0$), and $a_{m}=\frac{1}{L}\int_{-L}^{L}f(x)\cos
\frac{m\pi x}{L}$ are its cosine Fourier coefficients, then
$|a_{m}|\leq \frac{2ML}{m\pi}$. Hint: Recall that if
$|g|\leq M$, then $\left|\int_{a}^{b}g\right|\leq M(b-a)$. Find
a similar bound for $b_{m}$.
Answer: \begin{align*} |La_{m}| &
=\left|\int_{-L}^{L}f(x)\cos \frac{n\pi x}{L}\right|
=\left|\frac{Lf(x)\sin \frac{n\pi
x}{L}}{n\pi}|_{-L}^{L}-\frac{L}{n\pi}\int_{-L}^{L}f'(x)\sin
\frac{n\pi x}{L}\right| \\ &
=\left|\frac{L}{n\pi}\int_{-L}^{L}f'(x)\sin \frac{n\pi
x}{L}\right| \\ & \leq
\frac{L}{n\pi}\int_{-L}^{L}|f'(x)|\cdot|\sin \frac{n\pi x}{L}|\\
& \leq \frac{L}{n\pi}\int_{-L}^{L}M\cdot
1=\frac{2L^{2}M}{n\pi} \end{align*} and hence $|a_{m}|\leq
\frac{2LM}{n\pi}$.