How do we find the Fourier coefficient for a cosine term in a Fourier series?

Click For Summary
SUMMARY

The discussion focuses on finding the Fourier coefficient \( A_n \) in a Fourier series defined as \( f(x) = \sum_{n=0}^{\infty} A_n \cos\frac{n\pi x}{L} + B_n \sin\frac{n\pi x}{L} \). The method involves multiplying both sides by \( \cos\frac{m\pi x}{L} \) and integrating over the interval \([-L, L]\), leveraging the orthogonality of sine and cosine functions. The key conclusion is that the sum simplifies to a single term when \( m = n \), leading to the formula \( A_m = \frac{1}{L} \int_{-L}^{L} f(x) \cos\frac{m\pi x}{L} dx \).

PREREQUISITES
  • Understanding of Fourier series and their components
  • Knowledge of orthogonality in trigonometric functions
  • Familiarity with integration techniques over defined intervals
  • Basic concepts of partial differential equations (PDEs)
NEXT STEPS
  • Study the derivation of Fourier series coefficients in detail
  • Learn about the properties of orthogonal functions in functional analysis
  • Explore applications of Fourier series in solving PDEs
  • Investigate numerical methods for approximating Fourier coefficients
USEFUL FOR

Mathematicians, physicists, and engineers who are working with Fourier series and need to compute Fourier coefficients for various applications, particularly in the context of solving partial differential equations.

member 428835
hey pf!

okay, so if you've studied PDEs you know the value of a Fourier series, and the difficulty of determining a Fourier coefficient. my question relates to finding this coefficient. briefly, i'll define a Fourier series as f(x)=\sum_{n=0}^{\infty} A_n\cos\frac{n\pi x}{L}+B_n\sin\frac{n\pi x}{L} when solving for A_n one way (the only way i know) is to multiply both sides by \cos\frac{m\pi x}{L}. now, when we integrate over [-L,L] the sine term vanishes by its orthogonality with cosine and we are left with \int_{-L}^{L}f(x)\cos\frac{m\pi x}{L}dx=\sum_{n=0}^{\infty} A_n \int_{-L}^{L} \cos\frac{m\pi x}{L}\cos\frac{n\pi x}{L}dx, where the r.h.s=0 if m \neq n thus we know m = n (for now let's assume m=n \neq 0). m = n \implies \int_{-L}^{L} \cos\frac{m\pi x}{L}\cos\frac{n\pi x}{L}dx=L thus \sum_{n=1}^{\infty}A_n=\frac{1}{L}\int_{-L}^{L}f(x)\cos\frac{n\pi x}{L}dx but every book i see states simply A_n=\frac{1}{L}\int_{-L}^{L}f(x)\cos\frac{n\pi x}{L}dx where did the sum go?
 
Physics news on Phys.org
joshmccraney said:
...
now, when we integrate over [-L,L] the sine term vanishes by its orthogonality with cosine and we are left with \int_{-L}^{L}f(x)\cos\frac{m\pi x}{L}dx=\sum_{n=0}^{\infty} A_n \int_{-L}^{L} \cos\frac{m\pi x}{L}\cos\frac{n\pi x}{L}dx, where the r.h.s=0 if m \neq n

Exactly. Which means only one term of the sum is left, the n=m term, so this equation is identical to

\int_{-L}^{L}f(x)\cos\frac{m\pi x}{L}dx= A_m \int_{-L}^{L} \cos\frac{m\pi x}{L}\cos\frac{m\pi x}{L}dx

Does that make sense?

jason
 
  • Like
Likes   Reactions: 1 person
jasonRF said:
Exactly. Which means only one term of the sum is left, the n=m term, so this equation is identical to

\int_{-L}^{L}f(x)\cos\frac{m\pi x}{L}dx= A_m \int_{-L}^{L} \cos\frac{m\pi x}{L}\cos\frac{m\pi x}{L}dx

wait, does this mean \sum\int_{-L}^{L}f(x)\cos\frac{m\pi x}{L}dx= A_m \int_{-L}^{L} \cos\frac{m\pi x}{L}\cos\frac{m\pi x}{L}dx is equivalent to \int_{-L}^{L}f(x)\cos\frac{m\pi x}{L}dx= \sum A_m \int_{-L}^{L} \cos\frac{m\pi x}{L}\cos\frac{m\pi x}{L}dx
could you explain?
 
never mind, i see what you mean now! thanks!
 
"Where did the sum go?" is the wrong question.

The right question is "where do the parentheses go?"

Answer:
$$\int_{-L}^{L}f (x) \cos\frac{m\pi x}{L} dx = \sum_{n=0}^{\infty} \left( A_n \int_{-L}^{L} \cos \frac{m\pi x}{L} \cos \frac{n\pi x}{L} dx \right)$$

and all the integrals on the right hand side are zero, except when ##m = n##.
 

Similar threads

  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 7 ·
Replies
7
Views
3K
Replies
28
Views
6K
  • · Replies 4 ·
Replies
4
Views
3K
Replies
1
Views
2K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K