Higher Engineering Mathematics, Sixth Edition

(Nancy Kaufman) #1

Fourier series for a non-periodic function over range 2π 619


x

f(x) f(x) 5 x

22  2  0



2  3 

Figure 67.3


It is more convenient in this case to take the limits from 0
to2πinstead of from−πto+π.ThevalueoftheFourier
coefficientsareunalteredbythischangeoflimits.Hence


a 0 =

1
2 π

∫ 2 π

0

f(x)dx=

1
2 π

[∫π

0

xdx+

∫ 2 π

π

0dx

]

=

1
2 π

[
x^2
2


0

=

1
2 π

(
π^2
2

)
=

π
4

an=

1
π

∫ 2 π

0

f(x)cosnxdx

=

1
π

[∫π

0

xcosnxdx+

∫ 2 π

π

0dx

]

=

1
π

[
xsinnx
n

+

cosnx
n^2


0
(from Problem 1,by parts)

=

1
π

{[
πsinnπ
n

+

cosnπ
n^2

]

[
0 +

cos0
n^2

]}

=

1
πn^2

(cosnπ− 1 )

Whennis even,an=0.


Whennis odd,an=


− 2
πn^2

Hencea 1 =


− 2
π
,a 3 =

− 2
32 π
,a 5 =

− 2
52 π
, and so on

bn=

1
π

∫ 2 π

0

f(x)sinnxdx

=

1
π

[∫π

0

xsinnxdx−

∫ 2 π

π

0dx

]

=

1
π

[
−xcosnx
n

+

sinnx
n^2


0
(from Problem 1,by parts)

=

1
π

{[
−πcosnπ
n

+

sinnπ
n^2

]

[
0 +

sin0
n^2

]}

=

1
π

[
−πcosnπ
n

]
=

−cosnπ
n

Henceb 1 =−cosπ=1,b 2 =−

1
2

,b 3 =

1
3

, and so on.

Thus the Fourier series is:

f(x)=a 0 +

∑∞

n= 1

(ancosnx+bnsinnx)

i.e. f(x)=

π
4


2
π

cosx−

2
32 π

cos3x


2
52 π

cos5x−···+sinx


1
2

sin2x+

1
3

sin3x−···

i.e. f(x)

=

π
4


2
π

(
cosx+

cos3x
32

+

cos5x
52

+···

)

+

(
sinx−

1
2

sin2x+

1
3

sin3x−···

)

Problem 4. For the Fourier series of Problem 3:
(a) what is the sum of the series at the point of
discontinuity (i.e. atx=π)? (b) what is the
amplitude and phase angle of the third harmonic?
and (c) letx=0, and deduce a series forπ^2 /8.

(a) The sum of the Fourier series at the point of dis-
continuity is given by the arithmetic mean of the
two limiting values off(x)asxapproaches the
point of discontinuity from the two sides.
Hence sum of the series atx=πis
π− 0
2

=

π
2
(b) The third harmonic term of the Fourier series is
(

2
32 π

cos3x+

1
3

sin3x

)

This may also bewrittenin theformcsin( 3 x+α),

where amplitude,c=

√√


[(
− 2
32 π

) 2
+

(
1
3

) 2 ]

= 0. 341
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