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MT-144
NETWORK ANALYSIS
Mechatronics Engineering
(13)
Sinusoids and Phasors
Contents
IntroductionSinusoidsPhasorsPhasor Relationships for Circuit ElementsImpedance and AdmittanceKirchhoffs Laws in the Frequency DomainImpedance CombinationsApplications
Introduction
AC is more efficient and economical to transmit power over long distance.A sinusoid is a signal that has the form of the sine or cosine function.Circuits driven by sinusoidal current (ac) or voltage sources are called ac circuits.Why sinusoid is important in circuit analysis?Nature itself is characteristically sinusoidal.A sinusoidal signal is easy to generate and transmit.Easy to handle mathematically
Sinusoids
Sinusoids (Contd)
A period function is one that satisfies
f(t) = f(t+nT), for all t and for all integers n.
The period T is the number of seconds per cycleThe cyclic frequency f = 1/T is the number of cycles per second
Sinusoids (Contd)
Sinusoids (Contd)
To compare sinusoidsUse the trigonometric identitiesUse the graphical approach
The Graphical Approach
Phasors
Sinusoids are easily expressed by using phasorsA phasor is a complex number that represents the amplitude and the phase of a sinusoid.Phasors provide a simple means of analyzing linear circuits excited by sinusoidal sources.
Phasors (Contd)
Important Mathematical Properties
Phasor Representation
Phasor Representation (Contd)
Phasor Diagram
Sinusoid-Phasor Transformation
Phasor Relationships for Resistor
Time domain
Phasor domain
Phasor diagram
Phasor Relationships for Inductor
Time domain
Phasor domain
Phasor diagram
Phasor Relationships for Capacitor
Phasor diagram
Time domain
Phasor domain
Impedance and Admittance
Impedance and Admittance (Contd)
Impedance and Admittance (Contd)
Impedance and Admittance (Contd)
KVL and KCL in the Phasor Domain
Series-Connected Impedance
Parallel-Connected Impedance
Y- Transformations
Example 1
Example 2
Example 3
-Y transformation
Applications: Phase Shifters
Leading
output
Phase Shifters (Contd)
Lagging
output
Example
Applications: AC Bridges
AC Bridges (Contd)
Bridge for measuring L
Bridge for measuring C
Summary
Transformation between sinusoid and phasor is given as
Impedance Z for R, L, and C are given as
Basic circuit laws apply to ac circuits in the same manner as they do for dc circuits.
)
(
2
2
seconds.
every
itself
repeats
sinusoid
The
sinusoid
the
of
argument
the
)
(radians/s
frequency
angular
the
sinusoid
the
of
amplitude
the
where
sin
)
(
voltage
sinusoidal
he
Consider t
T:period
T
T
T
t
V
t
V
t
v
m
m
p
p
w
w
=
=
=
=
=
=
)
(
)
2
sin(
)
2
(
sin
)
(
sin
)
(
:
Proof
)
(
)
(
t
v
n
t
V
n
t
V
nT
t
V
nT
t
v
t
v
nT
t
v
m
m
m
=
+
=
+
=
+
=
+
=
+
p
w
p
w
w
=
=
(Hz)
hertz
:
(rad/s)
second
per
radians
:
where
2
1
f
f
T
f
w
p
w
+
+
=
Phase
:
Argument
:
)
(
where
)
sin(
)
(
as
given
is
expression
general
more
A
f
f
w
f
w
t
t
V
t
v
m
f
f
by
by
say that
We
2
1
1
2
v
lags
v
v
leads
v
=
0
if
,
are
and
0
if
,
are
and
say that
We
2
1
2
1
f
f
se
out of pha
v
v
in phase
v
v
B
A
B
A
B
A
B
A
B
A
B
A
sin
sin
cos
cos
)
cos(
sin
cos
cos
sin
)
sin(
:
identities
ric
Trigonomet
m
=
=
=
=
-
=
-
=
sin
)
90
cos(
cos
)
90
sin(
cos
)
180
cos(
sin
)
180
sin(
t
t
t
t
t
t
t
t
w
w
w
w
w
w
w
w
m
=
+
=
-
=
+
-
tan
where
)
cos(
sin
cos
1
2
2
A
B
B
A
C
t
C
t
B
t
A
q
q
w
w
w
)
1
.
53
cos(
5
sin
4
cos
3
+
=
-
t
t
t
w
w
w
of
the
:
of
the
:
where
,
form
l
Exponentia
:
form
Polar
:
form
r
Rectangula
:
it.
represent
to
ways
three
are
their
,
number
complex
a
g
Considerin
+
=
z
phase
z
magnitude
r
re
r
jy
x
z
z
j
f
f
f
)
sin
(cos
sin
,
cos
as
and
obtain
can
we
,
and
know
we
If
tan
,
as
and
get
can
we
,
and
Given
form
l
Exponentia
:
form
Polar
:
form
r
Rectangula
:
1
2
2
f
f
f
f
f
f
f
f
f
f
j
r
r
jy
x
z
r
y
r
x
y
x
r
x
y
y
x
r
r
y
x
re
r
jy
x
z
j
+
=
=
+
=
=
=
=
+
=
+
=
-
f
f
f
f
f
f
f
-
=
-
=
=
-
=
-
=
+
=
-
+
-
=
-
+
+
+
=
+
*
r
jy
x
z
r
z
r
z
r
r
z
z
r
r
z
z
y
y
j
x
x
z
z
y
y
j
x
x
z
z
2
1
1
)
(
)
(
)
(
)
(
)
(
)
(
2
1
2
1
2
1
2
1
2
1
2
1
2
1
2
1
2
1
2
1
2
1
2
1
:
Conjugate
Complex
:
Root
Square
:
Reciprocal
:
Division
:
tion
Multiplica
:
on
Substracti
:
Addition
2
2
2
2
2
1
1
1
1
1
f
f
f
=
+
=
=
+
=
=
+
=
r
jy
x
z
r
jy
x
z
r
jy
x
z
.
)
(
sinusoid
the
of
tion
representa
phasor
the
is
)
Re(
)
(
)
Re(
)
Re(
)
cos(
)
(
)
Im(
sin
)
Re(
cos
sin
cos
)
(
t
v
V
e
V
e
t
v
e
e
V
e
V
t
V
t
v
e
e
j
e
m
j
m
t
j
t
j
j
m
t
j
m
m
j
j
j
V
V
V
f
f
w
f
f
f
f
f
w
w
f
f
w
f
f
f
=
=
=
=
=
+
=
=
=
+
=
+
Q
f
=
m
V
V
q
-
=
m
I
I
[
]
w
w
w
w
w
f
w
w
f
w
w
f
f
w
w
w
f
f
w
j
vdt
j
dt
dv
e
j
e
e
V
e
e
e
e
V
t
V
t
V
dt
t
dv
V
t
V
t
v
t
j
t
j
j
m
j
j
j
t
j
m
m
m
m
m
V
V
V
V
Similarly,
)
Re(
)
(
Re
)
Re(
)
90
cos(
)
sin(
)
(
)
cos(
)
(
90
90
=
=
=
+
+
=
+
-
=
=
+
=
I
V
I
R
RI
t
RI
iR
v
I
t
I
i
m
m
m
m
=
=
+
=
=
=
+
=
f
f
w
f
f
w
)
cos(
law,
s
Ohm'
By
)
cos(
is
resistor
rough the
current th
the
If
I
V
I
L
j
t
LI
dt
di
L
v
I
t
I
i
m
m
m
w
f
w
w
f
f
w
=
+
+
=
=
=
+
=
)
90
cos(
is
inductor
the
across
voltage
The
)
cos(
is
inductor
rough the
current th
the
If
V
I
V
C
j
t
CV
dt
dv
C
i
V
t
V
v
m
m
m
w
f
w
w
f
f
w
=
+
+
=
=
=
+
=
)
90
cos(
is
capacitor
rough the
current th
The
)
cos(
is
capacitor
the
across
voltage
the
If
1
1
1
Admittance
Impedance
Element
current
phasor
the
is
tage
phasor vol
the
is
re
whe
(S)
1
:
Admittance
,
)
(
:
Impedance
L
j
C
j
C
C
j
L
j
L
R
R
R
w
w
w
w
=
=
=
=
=
=
=
W
=
Y
Z
Y
Z
Y
Z
I
V
Z
Y
I
V
Z
C
j
w
1
=
Z
L
j
w
=
Z
=
w
w
0
-
=
+
=
+
=
voltage
leads
current
since
leading
or
capacitive
:
voltage
lags
current
since
lagging
or
inductive
:
then
positive,
is
If
negative
is
when
capacitive
positive
is
when
inductive
be
to
said
is
impedance
The
reactance
:
resistance
:
where
jX
R
jX
R
X
X
X
X
R
jX
R
Z
Z
Z
=
=
=
+
=
=
+
=
-
sin
cos
and
tan
where
1
2
2
q
q
q
q
Z
Z
Z
Z
Z
X
R
R
X
X
R
jX
R
+
-
=
+
=
+
-
=
-
-
+
=
+
=
+
+
=
=
2
2
2
2
2
2
1
1
e
susceptanc
:
e
conductanc
:
where
1
X
R
X
B
X
R
R
G
X
R
jX
R
jX
R
jX
R
jX
R
jX
R
jB
G
B
G
jB
G
Z
Y
0
)
Re(
)
Re(
)
Re(
as
written
be
can
This
0
)
cos(
)
cos(
)
cos(
form.
cosine
in
written
be
may
ge
each volta
state,
steady
sinusoidal
In the
0
loop.
closed
a
around
voltages
the
be
,
,...,
,
let
KVL,
For
2
1
2
1
2
2
1
1
2
1
2
1
=
+
+
+
=
+
+
+
+
+
+
=
+
+
+
t
j
j
mn
t
j
j
m
t
j
j
m
n
mn
m
m
n
n
e
e
V
e
e
V
e
e
V
t
V
t
V
t
V
v
v
v
v
v
v
n
w
q
w
q
w
q
q
w
q
w
q
w
(
)
[
]
0
phasor.
for
holds
KCL
manner,
similar
a
In
!
!
phasor!
for
holds
KVL
0
,
any
for
0
Since
0
Re
then
,
Let
0
Re
2
1
2
1
2
1
2
1
2
1
=
+
+
+
=
+
+
+
=
+
+
+
=
=
+
+
+
n
n
t
j
t
j
n
j
mk
K
t
j
j
mn
j
m
j
m
t
e
e
e
V
e
e
V
e
V
e
V
k
n
I
I
I
V
V
V
V
V
V
V
w
w
q
w
q
q
q
)
(
gives
KVL
Applying
2
1
2
1
n
n
Z
Z
Z
I
V
V
V
V
+
+
+
=
+
+
+
=
V
Z
Z
V
Z
V
I
Z
Z
Z
I
V
Z
eq
k
k
eq
n
eq
=
=
+
+
+
=
=
,
2
1
)
1
1
1
(
gives
KCL
Applying
2
1
2
1
n
n
Z
Z
Z
V
I
I
I
I
+
+
+
=
+
+
+
=
I
Y
Y
I
Y
I
V
Y
Y
Y
V
I
Y
eq
k
k
eq
n
eq
=
=
+
+
+
=
=
,
2
1
3
1
3
3
2
2
1
2
1
3
3
2
2
1
1
1
3
3
2
2
1
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
+
+
=
+
+
=
+
+
=
-
c
b
a
ion:
Convers
Y
c
b
a
b
a
c
b
a
a
c
c
b
a
c
b
ion:
Y Convers
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
+
+
=
+
+
=
+
+
=
-
3
2
1
(
)
(
)
(
)
(
)
(
)
(
)
07
.
11
22
.
3
8
11
10
8
2
3
10
10
8
||
2
3
10
2
.
0
8
||
10
1
3
2
1
||
H
2
.
0
8
F
10
3
F
2
in
j
j
j
j
j
j
j
j
j
m
j
m
j
m
m
-
=
+
+
-
+
-
=
+
-
+
-
=
+
+
+
=
+
=
+
W
+
W
w
w
w
Z
Z
Z
Z
rad/s.
50
for
Find
in
=
w
Z
(t).
Find
o
v
[
]
(
)
(
)
(
)
)
96
.
15
4
cos(
15
.
17
)
(
96
.
15
15
.
17
15
20
96
.
30
8575
.
0
15
20
100
60
100
25
||
20
60
25
||
20
4
,
15
20
)
15
4
cos(
20
+
=
=
-
=
-
+
=
-
+
-
=
=
-
=
-
=
t
t
v
j
j
j
j
j
j
t
v
Sol:
o
s
o
s
s
V
V
V
w
.
Find
I
(
)
(
)
-
=
=
=
=
+
=
+
+
-
+
+
=
-
=
-
=
=
=
+
=
+
-
+
-
=
204
.
4
666
.
3
204
.
4
64
.
13
0
50
204
.
4
64
.
13
1
6
.
13
8
6
||
3
12
2
.
3
6
.
1
10
)
4
2
(
8
2
.
3
10
)
8
(
4
8
.
0
6
.
1
8
4
2
4
)
4
2
(
4
Z
V
I
Z
Z
Z
Z
Z
Z
Z
j
j
j
j
j
j
j
j
j
j
j
j
Sol:
cn
bn
an
cn
bn
an
i
i
i
o
RC
C
R
RC
RC
j
RC
j
C
j
R
R
V
V
V
V
+
=
+
=
+
=
-
w
w
w
w
w
w
1
tan
1
1
1
1
2
2
2
(
)
i
i
i
o
RC
C
R
RC
j
C
j
R
C
j
V
V
V
V
-
+
=
+
=
+
=
-
w
w
w
w
w
1
2
2
2
tan
1
1
1
1
1
1
=
=
=
-
=
=
-
-
=
-
=
-
=
-
-
=
-
=
90
3
1
45
3
2
45
2
2
45
2
2
20
20
20
45
3
2
24
12
4
12
20
4
12
20
40
)
20
20
(
20
)
20
20
(
||
20
1
1
1
i
o
i
i
i
j
j
j
j
j
j
j
j
Sol:
V
V
V
V
V
V
V
Z
Z
V
Z
leading..
90
of
phase
a
provide
to
circuit
an
Design
RC
2
1
3
1
3
2
3
2
1
2
3
2
2
1
2
1
2
1
:
condition
Balanced
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
Z
V
Z
Z
Z
V
V
Z
Z
Z
V
V
V
=
=
+
=
+
+
=
=
+
=
=
x
x
x
x
s
x
x
s
s
x
L
R
R
L
2
1
=
s
x
C
R
R
C
2
1
=
C
j
L
j
R
C
L
R
w
w
1
,
,
=
=
=
Z
Z
Z
f
f
w
=
+
=
m
m
V
t
V
t
v
V
)
cos(
)
(