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8/10/2019 Circuits_VI.pdf
1/13
Fundamentals ofElectrical Engineering
Circuits with Capacitors and Inductors
Solving circuits for sinusoidal sources
8/10/2019 Circuits_VI.pdf
2/13
Using Impedances The circuit consists of sources and any number of
resistors, capacitors and inductors
Pretend the sources are complex exponentials havinga frequencyf
Consider each element an impedance
Use voltage divider, current divider, series/parallelrules to relate output variables complex amplitude to
the complex amplitude of the source
element impedance
R R
C 1
j2
f CL j2f L
8/10/2019 Circuits_VI.pdf
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Sinusoidal Sources
vin+
R
C vout
+
Vin+
Vout
+
ZC
ZR
Voutej2ft = 1
j2fRC+ 1Vine
j2ft
vin(t) =A cos2f0t =1
2
Ae
j2f0t +Aej2f0t
vin(t) =Aej2f0t = vout(t) =
1
j2f0RC+ 1Aej2f0t
vin(t) =Aej2f0t = vout(t) =
1j2f0RC+ 1
Aej2f0t
8/10/2019 Circuits_VI.pdf
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Sinusoidal Sources
vin+
R
C vout
+
Vin+
Vout
+
ZC
ZR
vin = Vinej2ft
Since the circuit elements and KVL/KCL are linear,superposition applies
vin(t) =A cos2f0t =1
2
Aej2
f0t +Aej2f0t
vout(t) = 12
1
j2f0RC+ 1Aej2f0t + 1
j2f0RC+ 1Aej2f0t
8/10/2019 Circuits_VI.pdf
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Sinusoidal Sources Note that
vin(t) =12
Aej
2f0t +Aej2f0t
vin(t) = Re[Aej2f0t]
vout(t) =1
2
1
j2f0RC+ 1Aej2f0t +
1
j2f0RC+ 1Aej2f0t
vout(t) = Re
1j2f0RC+ 1
Aej2f0t
vout(t) = Re
1
42f20R2C2 + 1ejtan
1 2f0RCAej2f0t
= Re
A
42f20R2C2 + 1
ej(2f0ttan1 2f0RC)
=
A42f20R2C2 + 1 cos(2
f0t
tan
1
2
f0RC)
8/10/2019 Circuits_VI.pdf
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Output for a Sinusoidal Source
vin+
R
C vout
+
vout(t) = A
42f2
0R2C2 + 1
cos(2f0t tan1 2f0RC)
vout(t) = Re 1j2f0RC+ 1Ae
j2f0t
Vout =1
j2f0RC+ 1Vin
vin(t) =A cos(2
f0t) = Re[Aej2f0t
]
8/10/2019 Circuits_VI.pdf
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Sinusoidal SourcesIn general, vin(t) =A cos(2f0t+ ) = Re[Ae
jej2f0t]
Vin
Using impedances, find that Vout=H(f0) Vin
The transfer function captures the amplitude
change and phase shift that the circuit imposes
H(f0) =Vout
Vin
vout(t) = ReH(f0)Vine
j2f0t
=|H(f0)| |Vin| cos
2f0t+ + H(f0)
H(f0) = 1
j2f0RC+ 1 =
1
42f20R2C2 + 1
ej tan1
2f0RC
8/10/2019 Circuits_VI.pdf
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Sinusoidal SourcesNote that if vin(t) =A sin(2f0t+ ) = Im[Ae
jej2f0t]
vout(t) = ImH(f0)Vine
j2f0t
=|H(f0)| |Vin|sin
2f0t+ + H(f0)
cos 2ft = sin
2ft+
2
= Im
ej
2 ej2ft
You can use eitherthe real or imaginary part in yourcalculations
sin 2ft = cos
2ft
2
= Re
e
j
2 ej2
ft
8/10/2019 Circuits_VI.pdf
9/13
Using Impedances The circuit consists of sources and any number of
resistors, capacitors and inductors
Pretend the sources are complex exponentials havinga frequencyf
Consider each element an impedance
Use voltage divider, current divider, series/parallelrules to relate output variables complex amplitude tothe complex amplitude of the source (the transferfunction)
Express the source as the real (or imaginary) part of acomplex exponential
Output is the real (or imaginary) part of the transferfunction times the complex exponential representingthe source
8/10/2019 Circuits_VI.pdf
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An Example+
+
vout
1
2 4vin vin(t) = 10 sin(t/2)
Whats the transfer function?
Whats the output for the given input voltage?
8/10/2019 Circuits_VI.pdf
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An Example
Vin
+
+
Vout4s
1/s
2
s =j2f
+
+
vout
1
2 4vin
8/10/2019 Circuits_VI.pdf
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An Example
Vin
+
+
Vout4s
1/s
2
s =j2f
+
+
vout
1
2 4vin
vin
(t) = 10 sin(t/2)
H(s) = 4s2
4s2 + 2s+ 1 orH(f) =
162f2
162f2 +j4f+ 1
2f=
1
2=
f=
1
4 H 1
4
=
1
1 +j + 1 =j
vout(t) = Im[10jejt/2] = Im
10ej(t/2+
2)
= 10 sint/2 +
2
= 10 cos(t/2)
= Im 10ejt/2
8/10/2019 Circuits_VI.pdf
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WhatNotto Do
+
+
vout
1
2 4vin
H(f) = 162f2
162f2 +j4f+ 1
vin(t) = 10 sin(t/2)
vout(t) = Im
H
1
4
10 sin(t/2)
vout(t) = ImH 1
4
10ejt/2
vout(t) =H
1
4
10 sin(t/2)
!
= Im 10ejt/2