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Introductory lecture notes on Partial Differential Equations - ⃝ Anthony Peirce.
Not to be copied, used, or revised without explicit written permission from the copyright owner.
Lecture 14: Half Range Fourier Series: even and odd
functions
(Compiled 4 August 2017)
In this lecture we consider the Fourier Expansions for Even and Odd functions, which give rise to cosine and sine half
range Fourier Expansions. If we are only given values of a function f(x) over half of the range [0,L], we can define two
different extensions of f to the full range [−L,L], which yield distinct Fourier Expansions. The even extension gives rise
to a half range cosine series, while the odd extension gives rise to a half range sine series.
Key Concepts: Even and Odd Functions; Half Range Fourier Expansions; Even and Odd Extensions
14.1 Even and Odd Functions
Even: f(−x) = f(x)
Odd: f(−x) = −f(x)
14.1.1 Integrals of Even and Odd Functions
L 0 L
∫ f(x)dx= ∫ f(x)dx+∫ f(x)dx (14.1)
−L −L 0
L
∫ [ ]
= f(−x)+f(x) dx (14.2)
0
L
= 2∫ f(x)dx f even (14.3)
0
0 f odd.
Notes: Let E(x) represent an even function and O(x) an odd function.
(1) If f(x) = E(x)·O(x) then f(−x) = E(−x)O(−x) = −E(x)O(x) = −f(x) ⇒ f is odd.
(2) E (x)·E (x) → even.
1 2
(3) O (x)·O (x) → even.
1 2
(4) Any function can be expressed as a sum of an even part and an odd part:
1 [ ] 1 [ ]
f(x) = 2 f(x)+f(−x) +2 f(x)−f(−x) . (14.4)
| {z } | {z }
even part odd part
2
1[ ] 1[ ]
Check: Let E(x) = 2 f(x)+f(−x) . Then E(−x) = 2 f(−x)+f(x) = E(x) even. Similarly let
1[ ]
O(x) = 2 f(x)−f(−x) (14.5)
1[ ]
O(−x)= 2 f(−x)−f(x) =−O(x) odd. (14.6)
14.2 Consequences of the Even/Odd Property for Fourier Series
(I) Let f(x) be Even-Cosine Series:
L L
a = 1 ∫ f(x)cos(nπx) dx= 2 ∫ f(x)cos(nπx) dx (14.7)
n L | {z } L L L
−L even 0
L
b = 1 ∫ f(x)sin(nπx) dx=0. (14.8)
n L L
−L | {z }
odd
Therefore
L
∞ ( ) ∫ ( )
f(x) = a0 + ∑ancos nπx ; an = 2 f(x)cos nπx dx. (14.9)
2 n=1 L L L
0
(II) Let f(x) be Odd-Sine Series:
L
a = 1 ∫ f(x)cos(nπx) dx=0 (14.10)
n L L
−L | {z }
odd
L L
b = 1 ∫ f(x)sin(nπx) dx= 2 ∫ f(x)sin(nπx) dx
n L L L L
−L | {z } 0
even
Therefore
L
∞ ( ) ∫ ( )
f(x) = ∑b sin nπx ; b = 2 f(x)sin nπx dx.
n L n L L
n=1 −0
(III) Since any function can be written as the sum of an even and odd part, we can interpret the cos and sin series
as even/odd:
even odd
f(x) = 1[ ] 1[ ] (14.11)
2 f(x)+f(−x) +2 f(x)−f(−x)
{ ∞ } {∞ }
= a0 +∑ancos(nπx) + ∑bnsin(nπx)
2 n=1 L n=1 L
Fourier Series 3
where
L L
a = 2 ∫ 1[f(x)+f(−x)]cos(nπx) dx= 1 ∫ f(x)cos(nπx) dx
n L 2 L L L
0 −L
L L
b = 2 ∫ 1[f(x)−f(−x)]sin(nπx) dx= 1 ∫ f(x)sin(nπx) dx.
n L 2 L L L
0 −L
14.3 Half-Range Expansions
If we are given a function f(x) on an interval [0,L] and we want to represent f by a Fourier Series we have two
choices - a Cosine Series or a Sine Series.
Cosine Series:
∞ ( )
a ∑ nπx
f(x) = 0 + a cos (14.12)
2 n L
n=1
L
a = 2 ∫ f(x)cos(nπx) dx. (14.13)
n L L
0
Sine Series:
∞ ( )
f(x) = ∑b sin nπx (14.14)
n L
n=1
L
bn = 2 ∫ f(x)sin(nπx) dx. (14.15)
L L
0
Example 14.1 Expand f(x) = x, 0 < x < 2 in a half-range (a) Sine Series, (b) Cosine Series.
(a) Sine Series: (L=2)
L
bn = 2 ∫ f(t)sin nπtdt (14.16)
L ℓ
0
2
=∫ tsin nπtdt (14.17)
2
0
2
2 ∫
tcos nπt 2 nπ
2
=− (nπ) + cos tdt (14.18)
2 nπ 2
0 0
( )2
4 2 (nπ ) 2
=− cos(nπ)+ sin t (14.19)
nπ nπ 2
0
4 n
=−nπ(−1) (14.20)
Therefore
∞ n+1 ( )
f(t) = 4 ∑ (−1) sin nπt . (14.21)
π n=1 n 2
4
∞ n+1 ( )
f(1) = 1 = 4 ∑ (−1) sin nπ (14.22)
π n=1 n 2
therefore π = 1− 1 + 1 − 1 +··· (14.23)
4 3 5 7
(b) Cosine Series: (L=2)
2
∫ 2 2
2 t
a = tdt = =2 (14.24)
0 2 2
0 0
2 ( ) ( ) 2
∫ ∫
nπ 2 nπ 2 2 nπ
a = tcos tdt = tsin↗ t − sin tdt
n 2 nπ 2 nπ 2
0
0 0
( )2 2
2 nπ 4
=+ cos t = {cosnπ−1} (14.25)
2 2
nπ 2 n π
0
Therefore
∞ [ n ]
f(t) = 1+ 4 ∑ (−1) −1 cosnπt (14.26)
π2 n2 2
n=1
∞
=1− 8 ∑cos(2n+1)πt/(2n+1)2. (14.27)
π2 2
n=0
The cosine series converges faster than Sine Series.
∞ 2
f(2) = 2 = 1+ 8 ∑ 1 , π =1+ 1 + 1 +···
2 2 2 2
π n=0 (2n+1) 8 3 5
Example 14.2 Periodic Extension: Assume that f(x) = x, 0 < x < 2 represents one full period of the function so
that f(x+2) = f(x). 2L = 2 ⇒ L = 1.
L 1 2
∫ ∫ ∫ 2 2
1 x
a0 = f(x)dx = f(x)dx = xdx= =2 (14.28)
L 2
−L −1 0 0
since f(x+2) = f(2). (14.29)
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