PHYSICAL STRUCTURE9
/1/2
013 1
1:4
8 A
M
1
PR
B /S
CE
/De
pt. o
fEE
E
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
2
PE 9211 Analysis of Electrical Machines
Dynamic Characteristics of Permanent Magnet DC Motor
Modes of Dynamic operation
1. Starting from stall
2. Changes in load torque
Condition: The machine supplied from a
constant β voltage source
9/1
/20
13 1
1:4
8 A
M
3
PR
B /S
CE
/De
pt. o
fEE
E
Mathematical Model of a PMDC Motor: 9
/1/2
013 1
1:4
8 A
M
4
PR
B /S
CE
/De
pt. o
fEE
E
This motor consists of two first order differential equation and two
algebraic equation
Armature current equation,
9/1
/20
13 1
1:4
8 A
M
5
PR
B /S
CE
/De
pt. o
fEE
E
Speed equation,
9/1
/20
13 1
1:4
8 A
M
6
PR
B /S
CE
/De
pt. o
fEE
E
9/1
/20
13 1
1:4
8 A
M
7
PR
B /S
CE
/De
pt. o
fEE
E
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
8
Simulink Model of PMDC Motor
Motor Parameters
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
9
Solving armature current equation
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
10
Solving Speed equation
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
11
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
12
Dynamic performance during starting
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
13
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
14
Dynamic Characteristics of DC Shunt Motor
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
15
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
16
Simulink Model of DC Shunt Motor:
Fig shows the Simulink model of DC Shunt Motor. It is constructed using
subsystems for solving each differential equations (i.e.) armature
current, field current and torque equation.
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
17
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
18
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
19
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
20
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
21
Time domain block diagrams and state equations
Shunt connected dc machine
W.K.T
ππ = ππππ + π³π¨π¨ π πππ π
+ π³π¨πππππ β β ββ π
ππ = πππΉπ + π³ππ π ππ
π π β β ββ π
π»π = π»π³ + π± π ππ
π π + π©πππ β ββ β π
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
22
Equations (1),(2) and (3) can be written in terms of its time constants
ππ = ππ π + π³π¨π¨
ππ
π
π π ππ + π³π¨πππππ
ππ = ππ π + ππ π ππ + π³π¨πππππββββββ π
π―πππ, π βΆπ
π π
ππ = πΉπ π + π³ππ
πΉπ
π ππ
ππ = πΉπ π + ππ π ππβββββββ(5)
π»π β π»π³ = ( π©π + π± π) ππ ββ β β π
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
23
ππ βΆ Armature time constant
ππ βΆ Field time constant
πΊππππππ πππ πππππππππ π , π πππ π πππ ππ ,
ππ, πππ ππ πππππ π
ππ =
πππ
πππ + π ππ β π³π¨πππππ β β ββ π
ππ =
ππΉπ
πππ + π ππ β ββ β π
ππ =π
π±π + π©π π»π β π»π³ ββ β β π
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
24
Time domain block diagram of a shunt connected dc machine
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
25
πΊππππππ πππ πππππππππ π , π πππ π πππ π ππ
π π, π ππ
π π
πππ π ππ
π π πππππ π
From (1)
π πππ π
= βππ
π³π¨π¨
ππ β π³π¨π
π³π¨π¨
ππππ + π
π³π¨π¨
ππβ ππ
From (2)
π ππ
π π= β
πΉπ
π³ππ
ππ + π
π³ππ
ππβ ππ
From (3)
π ππ
π π= β
π©π
π±ππ +
π³π¨π
π±ππππ β
π
π±π»π³ β β(ππ)
State equation of shunt dc machine
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
26
π
ππππππ
=
βπΉπ
π³πππ π
πβππ
π³π¨π¨π
π πβπ©π
π±
ππππππ
+
πβπ³π¨πππ
π³π¨π¨
π³π¨πππππ
π±
+
π
π³πππ π
ππ
π³π¨π¨π
π πβπ
π±
ππ
ππ
π»π³
State equations in matrix form or vector matrix form
Note: The second term on the right side contains the product of state
variables causing the system to be nonlinear.
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
27
Permanent Magnet dc Machine
ππ ππ ππππππππππ
π³π¨πππ ππ ππππππππ ππ ππ
ππ ππ π πππππππππ ππ
Strength of the magnetReluctance of the ironNo. of turns in the armature winding
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
28
W.K.T
Above eqns. (1) and (2) can be written in terms of its time constants
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
29Time domain block diagram of a permanent magnet DC machine
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
30
State Equation of a permanent magnet DC machine
From (1)
From (2)
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
31
The form in which the state equations are expressed in above eqn.
is called the fundamental form.
OR
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
32
Advantages to using the state space representation compared with other methods.
1.The ability to easily handle systems with multiple inputs and outputs;
2.The system model includes the internal state variables as well as the output variable;
3.The model directly provides a time-domain solution, the matrix/vector modeling is very efficient from a computational standpoint for computer implementation
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
33
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
34
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
35
404349
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
36
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
37
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
38
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
39
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
40
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
41
34
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
42
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
43
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
44
34
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
45
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
46
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
47
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
48
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
49
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
50
34
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
51
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
52