Prove only using Fourier Series

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Homework Help Overview

The discussion revolves around proving the equality \(\sum_{n=1}^{\infty} \frac{1}{n^4} = \frac{\pi^4}{90}\) using Fourier Series, specifically by considering the Fourier Series of the function \(f(x) = x^2\) and exploring related functions like \(f(x) = x^4\).

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the Fourier Series of \(f(x) = x^2\) and its implications for \(\sum_{n=1}^{\infty} \frac{1}{n^2}\). Some attempt to extend this to \(f(x) = x^4\) to derive \(\sum_{n=1}^{\infty} \frac{1}{n^4}\). Questions arise regarding the correctness of their approaches and the relationships between the series derived from different functions.

Discussion Status

There is an ongoing exploration of the Fourier Series for both \(f(x) = x^2\) and \(f(x) = x^4\). Some participants express uncertainty about their calculations and seek clarification on the connections between the results. While several approaches have been suggested, there is no explicit consensus on the final steps needed to complete the proof.

Contextual Notes

Participants note constraints regarding the use of results strictly from Fourier Analysis and express concerns about the correctness of their interpretations and calculations. There is also mention of the need to connect the results from different functions to achieve the desired proof.

Oxymoron
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Prove only using Fourier Series!

By considering the Fourier Series of f(x)=x^2 prove that

\sum_{n=1}^{\infty} \frac{1}{n^4} = \frac{\pi^4}{90}
 
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Ok, so I considered the Fourier Series of f(x)=x^2 and found that

\sum_{n=1}^{\infty}\frac{1}{n^2} = \frac{\pi^2}{6}

Here is how I did it

a_0 = \frac{1}{2\pi}\int_{-\pi}^{\pi}x^2dx = \frac{2\pi^2}{3} = \frac{2\pi^{2m}}{2m+1} when m = 1

a_0 = \frac{1}{\pi}\int_{-\pi}^{\pi}x^2\cos(nx)dx = \frac{4}{n^2}(-1)^n

Since the function is even, b_n = 0.

Hence the Fourier Series can be written explicitly as

x^2 = \frac{\pi^2n}{2n+1} + \sum_{n=1}^{\infty}a_n \cos(nx)

And since n=1 we have

x^2 = \frac{\pi^2}{3} + 4\sum_{n=1}^{\infty}\frac{(-1)^n\cos(nx)}{n^2}

Since x \equiv \pi we know \cos(nx)=(-1)^n, so

\pi^2 = \frac{\pi^2}{3} + 4\sum_{n=1}^{\infty}\frac{1}{n^2}

and rearranging

\sum_{n=1}^{\infty}\frac{1}{n^2} = \frac{\pi^2}{6} = \zeta(2)
 
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Then I tried to do the same for f(x)=x^4, for the reason that now n=2 and I will have an expression for \sum\frac{1}{n^4}. I came close, but not close enough.

I know that

\sum_{n=1}^{\infty} = \frac{\pi^4}{90} = \zeta(4)

but I am only allowed to use results from Fourier Analysis. Is there anyone who can help? Or perhaps has an idea?
 
I am not sure I am 100% correct but what I got is slightly different from what we need.
We have
\sum_{n=1}^{\infty}\frac{1}{n^2} = \frac{\pi^2}{6}

If we consider the Fourier series of f(x)=x^4

x^4 = \frac{\pi}{5} + \sum_{n=1}^{\infty}(-1)^n \left( \frac{8 \pi^2}{n^2} - \frac{48}{n^4 \pi} \right) \cos(nx)

when x = \pi,

\pi^4 = \frac{\pi^4}{5} + \sum_{n=1}^{\infty} \left( \frac{8 \pi^2}{n^2} - \frac{48}{n^4 \pi} \right)

rearraging,

\sum_{n=1}^{\infty}\frac{1}{n^4} = \frac{8\pi^4}{15} \times \frac{\pi}{48}=\frac{\pi^5}{90}
 
a_0 = \frac{1}{2\pi}\int_{-\pi}^{\pi}x^2dx = \frac{2\pi^2}{3} = \frac{2\pi^{2m}}{2m+1}

If this is a0 WHAT is "m"?

Same question: if
x^2 = \frac{\pi^2n}{2n+1} + \sum_{n=1}^{\infty}a_n \cos(nx)

What does the "n" in the term before the sum mean?
 
I think I really made a mistake. The Fourier series of x^4 should be:

x^4 = \frac{\pi^4}{5} + \sum_{n=1}^{\infty} \left( (-1)^n \frac{8(n^2\pi^2-6)}{n^4} \cos(nx) \right)

then put x = \pi, the result follows
 
Sorry HallsovIvy, the n in the term before the sum should be "m". The m's are not summed, but the n's are - as you probably can guess.
 
Kelvin, that's is the same Fourier Series as I got. However I can't see the connection between the two. I've played around with substituting \pi for x, but I cannot get the required result.

Is there any chance you (or someone else) could post the last remaining steps in this proof for me.
 
Kelvin said:
I think I really made a mistake. The Fourier series of x^4 should be:

x^4 = \frac{\pi^4}{5} + \sum_{n=1}^{\infty} \left( (-1)^n \frac{8(n^2\pi^2-6)}{n^4} \cos(nx) \right)

then put x = \pi, the result follows

so putting x=\pi,

\pi^4 = \frac{\pi^4}{5} + \sum_{n=1}^{\infty} \left( (-1)^n \frac{8(n^2\pi^2-6)}{n^4} (-1)^n \right)

\frac{4\pi^4}{5} = \sum_{n=1}^{\infty} \left( \frac{8(n^2\pi^2-6)}{n^4} \right)

\frac{4\pi^4}{5} = 8\pi^2 \sum_{n=1}^{\infty} \frac{1}{n^2} - 48 \sum_{n=1}^{\infty}\frac{1}{n^4}

using the result that

\sum_{n=1}^{\infty}\frac{1}{n^2} = \frac{\pi^2}{6}

\sum_{n=1}^{\infty}\frac{1}{n^4} = \frac{8\pi^4}{15} \times \frac{1}{48}=\frac{\pi^4}{90}
 
  • #10
OMG! I forgot that I could use the result from the first part ! Thanks Kelvin.

I wonder if anyone here knows how to do it the "easy" way? You know, using the general hypergeometric function. I'd be impressed! :0
 
  • #11
Oxymoron said:
OMG! I forgot that I could use the result from the first part ! Thanks Kelvin.

I wonder if anyone here knows how to do it the "easy" way? You know, using the general hypergeometric function. I'd be impressed! :0

Maybe I am missing something, but I am wondering how showing the result based on the Fourier series of f(x)=x^4 is satisfying the problem you originally posed

Oxymoron said:
By considering the Fourier Series of f(x)=x^2 prove that

\sum_{n=1}^{\infty} \frac{1}{n^4} = \frac{\pi^4}{90}

Did you state the problem incorrectly? Is there some simple connection between the series for f(x)=x^4 and f(x)=x^2 that I am missing? OR does the original problems still need to be solved?
 
  • #12
OlderDan,

From what I can gather, the question asked to to find a Fourier series for a particular function, then notice that it looked almost like what we wanted. Then it required a little but of imagination to guess that the actual answer we want will require us to find the Fourier series of a slightly different function. Lo and behold, f(x) = x^4 does the trick because you get the \sum\frac{1}{n^4} instead of the \sum\frac{1}{n^2} you get from the Fourier series of f(x) = x^2.

I thought was that this was going to be hard to solve, since I haven't been formally introduced to the Riemann Zeta Function (which is \zeta(4) = \frac{\pi^4}{90}). But in hindsight, the Fourier analysis involved is not far above second year uni.
 

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