Mathematical Physics Vol 1
6.2 The fundamental convergence theorem for Fourier series
313
Properties of even/odd functions
a) If a function is even, then
ℓ Z
ℓ Z 0
f ( x ) d x = 2
f ( x ) d x .
− ℓ
b) If a function is odd, then
ℓ Z
f ( x ) d x = 0 .
− ℓ
c) A product of even functions p ( x )= f ( x ) · g ( x ) is an even function p ( − x )= f ( − x ) · g ( − x )= f ( x ) · g ( x )= p ( x ) . d) A product of odd functions is an even function p ( − x )= f ( − x ) · g ( − x )=( − 1 ) f ( x ) · ( − 1 ) g ( x )= f ( x ) · g ( x )= p ( x ) . e) A product of an even function f ( x ) and an odd function g ( x ) is an odd function p ( − x )= f ( − x ) · g ( − x )= f ( x ) · ( − 1 ) g ( x )= − f ( x ) · g ( x )= − p ( x ) . These properties are used in calculating the Fourier series coefficients a k and b k , when f ( x ) is an even or odd function. Namely, as the product of f ( x ) and sin x (sin x is an odd function), or cos x (cos x is an even function) appear under integral (6.12), then, depending on f ( x ) and the given the properties a)-d), some coefficients can be equal to zero. Fourier cosine series and Fourier sine series Let f ( x ) be an even function. Then p ( x ) = f ( x ) cos x is an even function, and q ( x ) = f ( x ) sin x is an odd function. Using the properties of these function, we obtain the follow ing Fourier coefficients
1 ℓ Z 1 ℓ Z 1 ℓ Z
2 ℓ Z
ℓ
ℓ
a 0 =
f ( x ) d x =
f ( x ) d x ,
0
− ℓ
2 ℓ Z
k π x ℓ
k π x ℓ
ℓ
ℓ
a k =
f ( x ) cos
d x =
f ( x ) cos
d x ,
(6.16)
0
− ℓ
k π x ℓ
ℓ
b k =
f ( x ) sin
d x = 0 .
− ℓ
In this special case, the Fourier series takes the form
∞ ∑ k = 1
k π ℓ
a 0 2
f ( x )=
a k cos
x .
(6.17)
+
In this case it is said that the function is expanded into a Fourier cosine series , where coefficients a k are determined by relations (6.16). Let f ( x ) be an odd function. Then p ( x )= f ( x ) cos x is an odd function, and q ( x )= f ( x ) sin x is an even function. Using the properties of these function, we obtain the following Fourier
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