Math 414-501 Spring 2020
Current Assignment
Assignment 6 - Due Friday, 3/6/2020.
- Read sections 2.1 and 2.2.
- Problems.
- Chapter 2 exercises: 1, 2, 4.
- Find the Fourier transform of $f(t) = e^{-|t|}$. In
addition, use this transform and the properties listed in Theorem
2.6 to find the Fourier transforms of the following functions:
- $te^{-|t|}$ (Use #2.)
- $e^{-2|t-3|}$ (#6 and #7)
- ${\rm sign}(t)e^{-|t|}$ (Hint: differentiate $e^{-|t|}$;
use #4.)
- $(1+(t-2)^2)^{-1}$ (Hint: How is this function related to
$\hat f(\lambda)$, where $f(t)=e^{-|t|}$? Once you've gotten this, use
#6.)
- Find the Fouirer transforms of these functions.
- $g(t) = \left\{\begin{array}{cl} 1 & \text{if }-1 \le t \le 2 \\
0 & \text{otherwise}.
\end{array}
\right.$
- $h(t) = \left\{\begin{array}{cl} -1 & \text{if }-3 \le t \le 0 \\
1 & \text{if }\ 0 < t \le 3 \\
0 & \text{otherwise}.
\end{array}
\right.$
Points and solutions.
- (25 pts.) Chapter 2, #2.
\[ \hat f(\lambda)= (2\pi)^{-1/2} \int_{-\infty}^\infty
f(t)e^{-i\lambda t}dt = (2\pi)^{-1/2}\int_{-\pi}^\pi
\underbrace{\sin(3t)}_{odd}e^{-i\lambda t}dt=
(2\pi)^{-1/2}i\int_{-\pi}^\pi \sin(3t)\sin(\lambda
t)dt\]
Usiing the trig identity $\sin(a)\sin(b) =
\frac{1}{2}\big(\cos(a-b)-\cos(a+b)\big)$, we have, if $|\lambda| \not=
3$, then
\[
\begin{aligned} \int_{-\pi}^\pi \sin(3t)\sin(\lambda t)dt &=
\frac{1}{2}\int_{-\pi}^\pi \bigg(\cos((3-\lambda)t) - \cos(
(3+\lambda)t)\bigg)dt\\
&= \frac{2\sin((3-\lambda)\pi)}{2(3-\lambda)}-
\frac{2\sin((3+\lambda)\pi)}{2(3+\lambda)} \\ &=-\sin(\lambda
\pi)\big(\frac{1}{3+\lambda}+ \frac{1}{3-\lambda}\big)
=-\frac{6\sin(\lambda \pi)}{9-\lambda^2}.
\end{aligned}
\]
Putting everything together and doing some algebra, we see that
\[ \hat f(\lambda)= -3i\sqrt{\frac{2}{\pi}}\frac{\sin(\lambda
\pi)}{9-\lambda^2} \]
- (25 pts. for $\hat f$.) Since $f(t)$ is even,
\[ \hat f(\lambda) = 2(2\pi)^{-1/2}
\int_0^\infty e^{-t}\cos(\lambda t)dt.
\]
This is a standard integral
and is fairly easy to do. Actualy, there are other ways to do it:
\[\begin{aligned} f(\lambda) &= (2\pi)^{-1/2} \int_{-\infty}^\infty
e^{-|t| -i\lambda t}dt\\
&= (2\pi)^{-1/2} \int_{-\infty}^0 e^{t-i\lambda
t}dt+ (2\pi)^{-1/2} \int_0^\infty e^{-t +i\lambda t}dt \\ &=
(2\pi)^{-1/2}\big(\frac{1}{1-i\lambda}+ \frac{1}{1+i\lambda}\big) =
\sqrt{\frac{2}{\pi}}\frac{1}{1+\lambda^2}
\end{aligned}\]
(If they get the factors with $\pi$ wrong, just take a point off.)
- (15 pts.) By #2, $\mathcal F(te^{-|t|}) = i
\frac{d}{d\lambda}\big(\sqrt{\frac{2}{\pi}}\frac{1}{1+\lambda^2}\big)=
-i\sqrt{\frac{2}{\pi}}\frac{2\lambda}{(1+\lambda^2)^2}$
- Skip.
- Skip.
- (15 pts.) This one is slighty tricky. By the inversion theorem (or what I
called the quartet in class), $ e^{-|\lambda|}=\mathcal
F(\sqrt{\frac{2}{\pi}}(1+t^2)^{-1})$, so $
\sqrt{\frac{\pi}{2}}e^{-|\lambda|}=\mathcal F((1+t^2)^{-1})$. By #6,
$\mathcal F((1+(t-2)^2)^{-1}) =
e^{-2i\lambda}\sqrt{\frac{\pi}{2}}e^{-|\lambda|}$
- (20 pts.) Grade part (b).
\[\begin{aligned} \mathcal F(h)=&\frac{1}{\sqrt{2\pi}}\int_{-3}^0
(-1)e^{-i\lambda t}dt + \int_{0}^3 e^{-i\lambda t}dt\\
&=\frac{1}{-i\lambda\sqrt{2\pi}}\big(-(1-e^{3i\lambda})+(e^{-3i\lambda}-1)
\big)\\ &=\frac{2}{-i\lambda\sqrt{2\pi}}\big(\cos(3\lambda)-1\big)
=\frac{-2i}{\lambda\sqrt{2\pi}}\big(1-\cos(3\lambda)\big) \end{aligned}\]
Updated 2/28/2020.