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

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To find the Fourier coefficient for a cosine term in a Fourier series, the integral of the function multiplied by the cosine term is evaluated over the interval [-L, L]. The orthogonality of sine and cosine ensures that only the term where the indices match contributes to the sum, simplifying the equation. This leads to the conclusion that the coefficient A_m can be directly calculated using the integral of the function with the cosine term. The confusion arises from the interpretation of the summation, which is resolved by recognizing that only the matching term remains. Understanding the placement of parentheses clarifies the relationship between the integrals and the coefficients.
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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?
 
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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
 
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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##.
 

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