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APPENDIX

G


Fourier Series


A periodic waveformf(t)=f(t+T), which is said to be periodic with a periodT, fundamental
frequencyf= 1 /T, and fundamental radian frequencyω= 2 π/T, can be expressed in terms of
an infinite series (known as theFourier series) of sinusoidal signals. Expressed mathematically,
we have

f(t)=

a 0
2

+

∑∞

n= 1

(ancosnωt+bnsinnωt) (1)

where the coefficientsanandbnare given by

an=

2
T

∫T/^2

−T/ 2

f(t)cosnωt dt=

2
T

∫T

0

f(t)cosnωtdt, n= 0 , 1 , 2 , 3 , ... (2)

bn=

2
T

∫T/^2

−T/ 2

f(t)sinnωt dt=

2
T

∫T

0

f(t)sinnωtdt, n= 1 , 2 , 3 , ... (3)

The average value off(t), which is also known as the dc component, is given by

a 0
2

=

1
T

∫T

0

f(t) dt

COMPLEX (EXPONENTIAL) FOURIER SERIES


By making use of the trigonometric identities

cost=

1
2

(ejt+e−jt) (4)

sint=

1
2 j

(ejt−e−jt) (5)

wherej=


−1, one can express Equation (1) as follows in terms ofcomplex Fourier series:

f(t)=

∑∞

n=−∞

c ̄nejnωt (6)

where the complex coefficientsc ̄nare given by

c ̄n=

1
T

∫T/^2

−T/ 2

f(t)e−jnωtdt , n= 0 ,± 1 ,± 2 , ... (7)

The set of coefficients{ ̄cn}is often referred to as the Fourier spectrum. These coefficients are
related to the coefficientsanandbnof Equations (2) and (3) by

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