tinuous, periodic function f(x) with period 2π can be written as a series: (0.1) where f(x) = fo + Σ(an cos(nx) + bn sin(nx) n>1 ㅠ 1 ƒo = = = ["*_* f(x) dx; ㅠ -T an (f(x), cos(nx)) bn = (f(x), sin(nx)). The constant term fo “centralizes” the function f so that = [" (f(x) – fo) dx = 0 π The numbers an and bn are called the Fourier coefficients of the func- tion f(x). For small values of n, the functions cos(nx) and sin(nx) capture to the low frequencies; when n is large, cos(nx) and sin(nx) capture high frequencies. Thus we can use the Fourier expansion to approximate periodic functions. Suppose now th we have a periodic function f(x) with period 2 such that f(x) = { ㅠ + 1 if -π ≤ x < 0 1- if 0 ≤ x < T on the interval [-T, π). Plot the graph of f(x) over the R and then compute an approximation of f(x) by using its Fourier expansion as in Equation (0.1) up to and including n 4. =
tinuous, periodic function f(x) with period 2π can be written as a series: (0.1) where f(x) = fo + Σ(an cos(nx) + bn sin(nx) n>1 ㅠ 1 ƒo = = = ["*_* f(x) dx; ㅠ -T an (f(x), cos(nx)) bn = (f(x), sin(nx)). The constant term fo “centralizes” the function f so that = [" (f(x) – fo) dx = 0 π The numbers an and bn are called the Fourier coefficients of the func- tion f(x). For small values of n, the functions cos(nx) and sin(nx) capture to the low frequencies; when n is large, cos(nx) and sin(nx) capture high frequencies. Thus we can use the Fourier expansion to approximate periodic functions. Suppose now th we have a periodic function f(x) with period 2 such that f(x) = { ㅠ + 1 if -π ≤ x < 0 1- if 0 ≤ x < T on the interval [-T, π). Plot the graph of f(x) over the R and then compute an approximation of f(x) by using its Fourier expansion as in Equation (0.1) up to and including n 4. =
Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
Problem 1RQ
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