Coefficients for an exponential Fourier Series

Click For Summary
The discussion focuses on finding the Fourier series for the function f(θ) = e^(-α|θ|) over the interval -π < θ < π, with the series expressed in the form f(θ) = Σ c_n e^(inθ). The user attempts to derive the coefficients using cosine terms to simplify the calculations, but ends up with a complicated final expression. Feedback from other participants suggests simplifying terms involving cosine and sine functions, which leads to a cleaner result for the coefficients. Ultimately, the user successfully refines their expression for k_n, confirming the correctness of their method.
ElPimiento
Messages
16
Reaction score
0
I'm kinda just hoping someone can look over my work and tell me if I'm solving the problem correctly. Since my final answer is very messy, I don't trust it.

1. Homework Statement

We're asked to find the Fourier series for the following function:
$$
f(\theta)=e^{−\alpha \lvert \theta \rvert}}, \ \ \ \text{for} −\pi<\theta<\pi,
$$
where ##f(\theta + \pi) = f(\theta)##. Except our Fourier series has the form:
$$
f(\theta) = \sum_{-\infty}^{\infty} c_n e^{in\theta}
$$

Homework Equations


Variation on Euler:
$$
\cos{\theta} = \frac{1}{2}(e^{i\theta} + e^{-i\theta})
$$
Vector projection:
$$
proj_\vec{v}(\vec{u}) = \frac{\langle\vec{v}, \vec{u}\rangle}{\langle\vec{v}, \vec{v}\rangle}
$$

The Attempt at a Solution


So, supposing ##n## is an Integer, I First realized that every positive ##n## has a negative partner, hence our special Fourier series formula can be rewritten as
$$
\begin{align*}
\sum_{-\infty}^{\infty} c_n e^{in\theta}
& = c_0 + \sum_{-\infty}^{-1} (c_{n^{(-)}} e^{in\theta}) + \sum_{1}^{\infty} (c_{n^{(+)}} e^{in\theta}) \\
& = c_0 + \sum_{-\infty}^{\infty }k_n (e^{in\theta} + e^{-in\theta}) \\
& = \sum_{-\infty}^{\infty} k_n \cos(n\theta) \\
\end{align*}
$$
Where I have used the variation on Euler's Equation (above) and set ##k_n = (c_{n^{(-)}} + c_{n^{(+)}})/2##.
Then using the inner product:
$$
\langle f(x), g(x) \rangle = \int_{-\pi}^{\pi} dx f(x) g(x)
$$
I found that the coefficients should be:
##
\begin{align*}
k_n & = \frac{\langle e^{-\alpha \lvert \theta \rvert}, \cos(n \theta) \rangle}{\langle \cos(n \theta), cos(n \theta)\rangle} \\
& = \frac{\int_{-\pi}^{\pi} e^{-\alpha \lvert \theta \rvert} cos(n \theta)} {\int_{-\pi}^{\pi} cos^2(n \theta)} \\
& = \frac{\int_{0}^{\pi} e^{-\alpha \theta} cos(n \theta)} {\int_{0}^{\pi} cos^2(n \theta)} \ \ \ \ \ (\because \text{all the functions are even}) \\
& = - \frac{4 n (\frac{\alpha \cos(\pi n) - n \sin(\pi n)}{(\alpha^2 + n^2)e^{(\pi \alpha)}} - \frac{\alpha}{\alpha^2 + n^2} )} {2 \pi n + \sin(2 \pi n)} \\
\end{align*}
##
Which is a mess.

I used cosines hoping it would simplify the problem (since they're even and the resulting series starts at 0 instead of ##-\infty##), but it doesn't look like it did much good. So is the method at least right?
 
Last edited:
Physics news on Phys.org
ElPimiento said:
I'm kinda just hoping someone can look over my work and tell me if I'm solving the problem correctly. Since my final answer is very messy, I don't trust it.

1. Homework Statement

We're asked to find the Fourier series for the following function:
$$
f(\theta)=e^{−\alpha \lvert \theta \rvert}}, \ \ \ \text{for} −\pi<\theta<\pi,
$$
where ##f(\theta + \pi) = f(\theta)##. Except our Fourier series has the form:
$$
f(\theta) = \sum_{-\infty}^{\infty} c_n e^{in\theta}
$$

Homework Equations


Variation on Euler:
$$
\cos{\theta} = \frac{1}{2}(e^{i\theta} + e^{-i\theta})
$$
Vector projection:
$$
proj_\vec{v}(\vec{u}) = \frac{\langle\vec{v}, \vec{u}\rangle}{\langle\vec{v}, \vec{v}\rangle}
$$

The Attempt at a Solution


So, supposing ##n## is an Integer, I First realized that every positive ##n## has a negative partner, hence our special Fourier series formula can be rewritten as
$$
\begin{align*}
\sum_{-\infty}^{\infty} c_n e^{in\theta}
& = c_0 + \sum_{-\infty}^{-1} (c_{n^{(-)}} e^{in\theta}) + \sum_{1}^{\infty} (c_{n^{(+)}} e^{in\theta}) \\
& = c_0 + \sum_{-\infty}^{\infty }k_n (e^{in\theta} + e^{-in\theta}) \\
& = \sum_{-\infty}^{\infty} k_n \cos(n\theta) \\
\end{align*}
$$
Where I have used the variation on Euler's Equation (above) and set ##k_n = (c_{n^{(-)}} + c_{n^{(+)}})/2##.
Then using the inner product:
$$
\langle f(x), g(x) \rangle = \int_{-\pi}^{\pi} dx f(x) g(x)
$$
I found that the coefficients should be:
##
\begin{align*}
k_n & = \frac{\langle e^{-\alpha \lvert \theta \rvert}, \cos(n \theta) \rangle}{\langle \cos(n \theta), cos(n \theta)\rangle} \\
& = \frac{\int_{-\pi}^{\pi} e^{-\alpha \lvert \theta \rvert} cos(n \theta)} {\int_{-\pi}^{\pi} cos^2(n \theta)} \\
& = \frac{\int_{0}^{\pi} e^{-\alpha \theta} cos(n \theta)} {\int_{0}^{\pi} cos^2(n \theta)} \ \ \ \ \ (\because \text{all the functions are even}) \\
& = - \frac{4 n (\frac{\alpha \cos(\pi n) - n \sin(\pi n)}{(\alpha^2 + n^2)e^{(\pi \alpha)}} - \frac{\alpha}{\alpha^2 + n^2} )} {2 \pi n + \sin(2 \pi n)} \\
\end{align*}
##
Which is a mess.

I used cosines hoping it would simplify the problem (since they're even and the resulting series starts at 0 instead of ##-\infty##), but it doesn't look like it did much good. So is the method at least right?
Why don't you simplify ##\cos(\pi n), \sin(\pi n)## and ##\sin (2 \pi n)##? Remember that ##n## is an integer.

When you do that you get a result that agrees with that obtained using Maple.
 
  • Like
Likes ElPimiento
Oh duh, I should've realized that >~<.
Thanks though! That cleaned it up nicely:
$$
k_n = -\frac{2 \alpha (e^{\pi \alpha} - 1)}{\pi (\alpha^2 + n^2)}
$$
 
ElPimiento said:
Oh duh, I should've realized that >~<.
Thanks though! That cleaned it up nicely:
$$
k_n = -\frac{2 \alpha (e^{\pi \alpha} - 1)}{\pi (\alpha^2 + n^2)}
$$
Woops! got a little too excited with the cancelation:
$$
\begin{align*}
k_n
& = -\frac{2 \, {\left(\frac{\left(-1\right)^{n} \alpha}{\alpha^{2} e^{\left(\pi \alpha\right)} + n^{2} e^{\left(\pi \alpha\right)}} - \frac{\alpha}{\alpha^{2} + n^{2}}\right)}}{\pi} \\
& = - \frac{2 \alpha ((-1)^n e^{- \pi \alpha} - 1)}{\pi (\alpha^2 + n^2)} \\
\end{align*}
$$
 
Last edited:
Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

Similar threads

  • · Replies 14 ·
Replies
14
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
3
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 16 ·
Replies
16
Views
2K
Replies
1
Views
2K