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Circuit Analysis Using Fourier and Laplace Transforms
...... EE2015: Electrical Circuits and Networks
Nagendra Krishnapura
https://www.ee.iitm.ac.in/∼nagendra/
Department of Electrical Engineering
Indian Institute of Technology, Madras
Chennai, 600036, India
July-November 2017
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Nagendra Krishnapura https://www.ee.iitm.ac.in/∼nagendra/ Circuit Analysis Using Fourier and Laplace Transforms
.. Circuit Analysis Using Fourier and Laplace Transforms
Basedon
exp(st) being an eigenvector of linear systems
Steady-state response to exp(st) is H(s)exp(st) where H(s) is some scaling factor
Signals being representable as a sum(integral) of exponentials exp(st)
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Nagendra Krishnapura https://www.ee.iitm.ac.in/∼nagendra/ Circuit Analysis Using Fourier and Laplace Transforms
.. Fourier series
Periodic x(t) can be represented as sums of complex exponentials
x(t) periodic with period T0
Fundamental (radian) frequency ω = 2π/T
0 0
∞
x(t) = ∑ a exp(jkω t)
k 0
k=−∞
x(t) as a weighted sum of orthogonal basis vectors exp(jkω0t)
Fundamental frequency ω0 and its harmonics
ak: Strength of kth harmonic
Coefficients ak can be derived using the relationship
∫ T
a = 1 0 x(t)exp(−jkω t)dt
k T 0
0 0
“Inner product” of x(t) with exp(jkω0t)
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Nagendra Krishnapura https://www.ee.iitm.ac.in/∼nagendra/ Circuit Analysis Using Fourier and Laplace Transforms
.. Fourier series
Alternative form
∞
x(t) = a +∑b cos(kω t)+c sin(kω t)
0 k 0 k 0
k=1
Coefficients b and c can be derived using the relationship
k k
b = 2 ∫ T0 x(t)cos(kω t)dt
k T 0
0 0
c = 2 ∫ T0 x(t)sin(kω t)dt
k T 0
0 0
Another alternative form
∞
x(t) = a +∑d cos(kω t +ϕ )
0 k 0 k
k=1
Coefficients b and c can be derived using the relationship
k k
d = √b2+c2
k k k
(c )
−1 k
ϕ = −tan
k b
k . . . . . . . . . . . . . . . . . . . .
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Nagendra Krishnapura https://www.ee.iitm.ac.in/∼nagendra/ Circuit Analysis Using Fourier and Laplace Transforms
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