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
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Chapter2: Second-order Linear Odes
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(d) Joseph Fourier (21 March 1768 16 May 1830) said that any con-
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
ƒo = ²/7 ["*_* ƒ(x) dx;
ㅠ
-π
an (f(x), cos(n.x))
=
bn (f(x), sin(nx)).
The constant term fo "centralizes" the function f so that
[(f(x) – fo) dx = 0
=
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 that we have a periodic function f(x) with period 2
such that
f(x) =
={
π
+ 1 if − π ≤ x < 0
x
1- if 0 ≤ x < π
on the interval [—π, 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.
:
Transcribed Image Text:(d) Joseph Fourier (21 March 1768 16 May 1830) said that any con- 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 ƒo = ²/7 ["*_* ƒ(x) dx; ㅠ -π an (f(x), cos(n.x)) = bn (f(x), sin(nx)). The constant term fo "centralizes" the function f so that [(f(x) – fo) dx = 0 = 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 that we have a periodic function f(x) with period 2 such that f(x) = ={ π + 1 if − π ≤ x < 0 x 1- if 0 ≤ x < π on the interval [—π, 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. :
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