Fourier Series to Fourier Integral

In summary, the Fourier series representation of a periodic function of period 2L can be converted to a Fourier integral form by taking the limit as n approaches infinity. This results in an expression involving a constant term and two integrals with functions A(w) and B(w). These functions are defined as the Fourier coefficients of the original function f(x).
  • #1
AlfredVioleta
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1. Question

[tex] Consider\ any\ periodic\ function\ f(x)\ of\ period\ 2L\ that\ can\ be\ represented\ by\ a\ Fourier\ series:\

{f(x)= a_0 + \sum_{n=1}^\infty\ a_ncos\ w_nx + b_nsin\ w_nx}\ ,\ w_n= {n\pi x\over \ L } [/tex]



[tex] How\ do\ I\ get\ this\ form\ :\ f(x)= \int_{0}^{\infty}\ [A(w)cos\ wx + B(w)sin\ wx ]\ dw\ ,\ A(w)= {1\over \pi}\int_{-\infty}^{\infty}\ f(v)cos\ wv\ dv\ , B(w) = {1\over \pi}\int_{-\infty}^{\infty}\ f(v)sin\ wv\ dv? [/tex]



2. The attempt at a solution

[tex] Denoting\ the\ variable\ of\ integration\ by\ v(why\ so?)\ i.e.\ f(x)= {1\over 2L}\int_{-L}^{L}\ {f(v)}\ dv + {1\over L}\sum_{n=1}^\infty\ [(cos\ w_nx) \int_{-L}^{L}\ {f(v)cos\ w_nv}\ dv + (sin\ w_nx) \int_{-L}^{L}\ {f(v)sin\ w_nv}\ dv][/tex]


[tex] To\ convert\ to\ a\ Fourier\ integral,\ set\ \Delta w= w_{n+1} - w_n = {\pi\over \ L}\ ,it\ follows\ that\ f(x)= {1\over 2L}\int_{-L}^{L}\ {f(v)}\ dv + {1\over \pi}\sum_{n=1}^\infty\ [(cos\ w_nx) \Delta w\int_{-L}^{L}\ {f(v)cos\ w_nv}\ dv + (sin\ w_nx) \Delta w\int_{-L}^{L}\ {f(v)sin\ w_nv}\ dv] [/tex]
 
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  • #2
Taking\ the\ limit\ as\ n\rightarrow \infty \ ,\ f(x)= {1\over 2L}\int_{-L}^{L}\ {f(v)}\ dv + {1\over \pi}\int_{-\infty}^{\infty}\ [cos\ wx\int_{-L}^{L}\ {f(v)cos\ wv}\ dv + sin\ wx\int_{-L}^{L}\ {f(v)sin\ wv}\ dv]\ dw Defining\ A(w)= {1\over \pi}\int_{-L}^{L}\ {f(v)cos\ wv}\ dv\ and\ B(w)= {1\over \pi}\int_{-L}^{L}\ {f(v)sin\ wv}\ dv\ ,\ the\ expression\ for\ the\ Fourier\ integral\ form\ of\ the\ function\ is\ given\ as\ :\ f(x)= {1\over 2L}\int_{-L}^{L}\ {f(v)}\ dv + {1\over \pi}\int_{-\infty}^{\infty}\ [A(w)cos\ wx + B(w)sin\ wx ]\ dw
 

Related to Fourier Series to Fourier Integral

1. What is a Fourier Series?

A Fourier Series is a mathematical representation of a periodic function, which can be decomposed into a sum of sinusoidal functions with different frequencies, amplitudes, and phases.

2. What is the purpose of a Fourier Series?

The purpose of a Fourier Series is to represent a complex periodic function in terms of simpler sinusoidal functions, making it easier to analyze and understand the behavior of the original function.

3. What is the difference between Fourier Series and Fourier Transform?

A Fourier Series is used to represent a periodic function, while a Fourier Transform is used to represent a non-periodic function. Fourier Transform is also a continuous function, while Fourier Series is a discrete function.

4. What is the relationship between Fourier Series and Fourier Integral?

A Fourier Series is a special case of a Fourier Integral, where the original function is periodic. Fourier Integral is a more general representation of a function, and it can be applied to both periodic and non-periodic functions.

5. How is a Fourier Series calculated?

A Fourier Series can be calculated using the Fourier coefficients, which are obtained by integrating the original function with the appropriate trigonometric functions. These coefficients are then used to construct the Fourier Series equation.

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