2. 2
Sinusoids and Phasor
Sinusoids and Phasor
C
Chapter 9
hapter 9
9.1 Motivation
9.2 Sinusoids’ features
9.3 Phasors
9.4 Phasor relationships for circuit elements
9.5 Impedance and admittance
9.6 Kirchhoff’s laws in the frequency domain
9.7 Impedance combinations
3. 3
How to determine
How to determine v(t)
v(t) and
and i(t)?
i(t)?
vs(t) = 10V
How can we apply what we have learned before to
determine i(t) and v(t)?
9.1 Motivation (1)
9.1 Motivation (1)
4. 4
• A sinusoid is a signal that has the form of the
sine or cosine function.
• A general expression for the sinusoid,
where
Vm = the amplitude of the sinusoid
ω = the angular frequency in radians/s
Ф = the phase
9.2 Sinusoids (1)
9.2 Sinusoids (1)
)
sin(
)
(
t
V
t
v m
5. 5
9.2 Sinusoids (2)
9.2 Sinusoids (2)
A periodic function is one that satisfies v(t) = v(t + nT), for
all t and for all integers n.
2
T
Hz
T
f
1
f
2
• Only two sinusoidal values with the same frequency can be
compared by their amplitude and phase difference.
• If phase difference is zero, they are in phase; if phase
difference is not zero, they are out of phase.
6. 6
9.2 Sinusoids (3)
9.2 Sinusoids (3)
Example 1
Given a sinusoid, , calculate its
amplitude, phase, angular frequency, period, and
frequency.
Solution:
Amplitude = 5, phase = –60o
, angular frequency
= 4rad/s, Period = 0.5 s, frequency = 2 Hz.
)
60
4
sin(
5 o
t
7. 7
9.2 Sinusoids (4)
9.2 Sinusoids (4)
Example 2
Find the phase angle between
and , does i1 lead or lag i2?
)
25
377
sin(
4
1
o
t
i
)
40
377
cos(
5
2
o
t
i
Solution:
Since sin(ωt+90o
) = cos ωt
therefore, i1 leads i2 155o
.
)
50
377
sin(
5
)
90
40
377
sin(
5
2
o
o
o
t
t
i
)
205
377
sin(
4
)
25
180
377
sin(
4
)
25
377
sin(
4
1
o
o
o
o
t
t
t
i
8. 8
• A phasor is a complex
number that represents the
amplitude and phase of a
sinusoid.
• It can be represented in one
of the following three forms:
9.3 Phasor (1)
9.3 Phasor (1)
r
z
j
re
z
)
sin
(cos
j
r
jy
x
z
a.Rectangul
ar
b.Polar
c.Exponenti
al
2
2
y
x
r
x
y
1
tan
where
9. 9
Example 3
• Evaluate the following complex numbers:
a.
b.
9.3 Phasor (2)
9.3 Phasor (2)
Solution:
a. –15.5 + j13.67
b. 8.293 + j2.2
]
60
5
j4)
1
j2)(
[(5 o
o
o
30
10
j4
3
40
3
j5
10
10. 10
Mathematic operation of complex number:
1. Addition
2. Subtraction
3. Multiplication
4. Division
5. Reciprocal
6. Square root
7. Complex conjugate
8. Euler’s identity
9.3 Phasor (3)
9.3 Phasor (3)
)
(
)
( 2
1
2
1
2
1 y
y
j
x
x
z
z
)
(
)
( 2
1
2
1
2
1 y
y
j
x
x
z
z
2
1
2
1
2
1
r
r
z
z
2
1
2
1
2
1
r
r
z
z
r
z
1
1
2
r
z
j
re
r
jy
x
z
sin
cos j
e j
11. 11
• Transform a sinusoid to and from the time
domain to the phasor domain:
(time domain) (phasor domain)
9.3 Phasor (4)
9.3 Phasor (4)
)
cos(
)
(
t
V
t
v m
m
V
V
• Amplitude and phase difference are two principal
concerns in the study of voltage and current sinusoids.
• Phasor will be defined from the cosine function in all our
proceeding study. If a voltage or current expression is in
the form of a sine, it will be changed to a cosine by
subtracting from the phase.
12. 12
Example 4
Transform the following sinusoids to phasors:
i = 6cos(50t – 40o
) A
v = –4sin(30t + 50o
) V
9.3 Phasor (5)
9.3 Phasor (5)
Solution:
a. I A
b. Since –sin(A) = cos(A+90o
);
v(t) = 4cos (30t+50o
+90o
) = 4cos(30t+140o
) V
Transform to phasor => V V
40
6
140
4
13. 13
Example 5:
Transform the sinusoids corresponding to
phasors:
a.
b.
9.3 Phasor (6)
9.3 Phasor (6)
V
30
10
V
A
j12)
j(5
I
Solution:
a) v(t) = 10cos(t + 210o
) V
b) Since
i(t) = 13cos(t + 22.62o
) A
22.62
13
)
12
5
(
tan
5
12
j5
12 1
2
2
I
14. 14
The differences between v(t) and V:
• v(t) is instantaneous or time-domain
representation
V is the frequency or phasor-domain
representation.
• v(t) is time dependent, V is not.
• v(t) is always real with no complex term, V is
generally complex.
Note: Phasor analysis applies only when frequency is
constant; when it is applied to two or more sinusoid
signals only if they have the same frequency.
9.3 Phasor (7)
9.3 Phasor (7)
15. 15
9.3 Phasor (8)
9.3 Phasor (8)
Relationship between differential, integral operation
in phasor listed as follow:
)
(t
v
V
V
dt
dv
V
j
vdt
j
V
16. 16
Example 6
Use phasor approach, determine the current i(t)
in a circuit described by the integro-differential
equation.
9.3 Phasor (9)
9.3 Phasor (9)
Answer: i(t) = 4.642cos(2t + 143.2o
) A
)
75
2
cos(
50
3
8
4 t
dt
di
idt
i
17. 17
• In-class exercise for Unit 6a, we can derive the differential
equations for the following circuit in order to solve for vo(t)
in phase domain Vo.
9.3 Phasor (10)
9.3 Phasor (10)
)
15
4
sin(
3
400
20
3
5
0
0
2
2
o
o
t
v
dt
dv
dt
v
d
•However, the derivation may sometimes be very tedious.
Is there any quicker and more systematic methods to do it?
18. 18
The answer is YES!
9.3 Phasor (11)
9.3 Phasor (11)
Instead of first deriving the differential equation
and then transforming it into phasor to solve
for Vo, we can transform all the RLC
components into phasor first, then apply the
KCL laws and other theorems to set up a
phasor equation involving Vo directly.
19. 19
9.4 Phasor Relationships
9.4 Phasor Relationships
for Circuit Elements (1)
for Circuit Elements (1)
Resistor: Inductor: Capacitor:
20. 20
9.4 Phasor Relationships
9.4 Phasor Relationships
for Circuit Elements (2)
for Circuit Elements (2)
Summary of voltage-current relationship
Element Time domain Frequency domain
R
L
C
Ri
v RI
V
dt
di
L
v LI
j
V
dt
dv
C
i
C
j
I
V
21. 21
9.4 Phasor Relationships
9.4 Phasor Relationships
for Circuit Elements (3)
for Circuit Elements (3)
Example 7
If voltage v(t) = 6cos(100t – 30o
) is applied to a 50 μF
capacitor, calculate the current, i(t), through the
capacitor.
Answer: i(t) = 30 cos(100t + 60o
) mA
22. 22
• The impedance Z of a circuit is the ratio of the phasor
voltage V to the phasor current I, measured in ohms Ω.
where R = Re, Z is the resistance and X = Im, Z is the
reactance. Positive X is for L and negative X is for C.
• The admittance Y is the reciprocal of impedance,
measured in siemens (S).
9.5 Impedance and Admittance (1)
9.5 Impedance and Admittance (1)
jX
R
I
V
Z
V
I
Z
Y
1
23. 23
9.5 Impedance and Admittance (2)
9.5 Impedance and Admittance (2)
R
Y
1
L
j
Y
1
C
j
Y
Impedances and admittances of passive elements
Element Impedance Admittance
R
L
C
R
Z
L
j
Z
C
j
Z
1
24. 24
9.5 Impedance and Admittance (3)
9.5 Impedance and Admittance (3)
L
j
Z
C
j
Z
1
Z
Z
;
0
;
0
0
;
;
0
Z
Z
25. 25
9.5 Impedance and Admittance (4)
9.5 Impedance and Admittance (4)
After we know how to convert RLC components
from time to phasor domain, we can transform
a time domain circuit into a phasor/frequency
domain circuit.
Hence, we can apply the KCL laws and other
theorems to directly set up phasor equations
involving our target variable(s) for solving.
26. 26
9.5 Impedance and Admittance (5)
9.5 Impedance and Admittance (5)
Example 8
Refer to Figure below, determine v(t) and i(t).
Answers: i(t) = 1.118cos(10t – 26.56o
) A; v(t) = 2.236cos(10t + 63.43o
) V
)
10
cos(
5 t
vs
27. 27
9.6 Kirchhoff’s Laws
9.6 Kirchhoff’s Laws
in the Frequency Domain (1)
in the Frequency Domain (1)
• Both KVL and KCL are hold in the phasor
domain or more commonly called frequency
domain.
• Moreover, the variables to be handled are
phasors, which are complex numbers.
• All the mathematical operations involved are
now in complex domain.
28. 28
9.7 Impedance Combinations (1)
9.7 Impedance Combinations (1)
• The following principles used for DC circuit
analysis all apply to AC circuit.
• For example:
a. voltage division
b. current division
c. circuit reduction
d. impedance equivalence
e. Y-Δ transformation
29. 29
9.7 Impedance Combinations (2)
9.7 Impedance Combinations (2)
Example 9
Determine the input impedance of the circuit in figure below
at ω =10 rad/s.
Answer: Zin = 32.38 – j73.76
![9
Example 3
• Evaluate the following complex numbers:
a.
b.
9.3 Phasor (2)
9.3 Phasor (2)
Solution:
a. –15.5 + j13.67
b. 8.293 + j2.2
]
60
5
j4)
1
j2)(
[(5 o
o
o
30
10
j4
3
40
3
j5
10
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