Upload
ramesh-babu
View
592
Download
0
Embed Size (px)
DESCRIPTION
Hi, this is my third material
Citation preview
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 – 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
𝒗𝒂 = 𝒊𝒂𝒓𝒂 + 𝑳𝑨𝑨 𝒅𝒊𝒂𝒅𝒕
+ 𝑳𝑨𝑭𝝎𝒓𝒊𝒇 − − −− 𝟏
𝒗𝒇 = 𝒊𝒇𝑹𝒇 + 𝑳𝑭𝑭 𝒅𝒊𝒇
𝒅𝒕 − − −− 𝟐
𝑻𝒆 = 𝑻𝑳 + 𝑱 𝒅𝝎𝒓
𝒅𝒕 + 𝑩𝒎𝝎𝒓 − −− − 𝟑
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
𝒗𝒂 = 𝒓𝒂 𝟏 + 𝑳𝑨𝑨
𝒓𝒂
𝒅
𝒅𝒕 𝒊𝒂 + 𝑳𝑨𝑭𝝎𝒓𝒊𝒇
𝒗𝒂 = 𝒓𝒂 𝟏 + 𝝉𝒂 𝝆 𝒊𝒂 + 𝑳𝑨𝑭𝝎𝒓𝒊𝒇−−−−−− 𝟒
𝑯𝒆𝒓𝒆, 𝝆 ⟶𝒅
𝒅𝒕
𝒗𝒇 = 𝑹𝒇 𝟏 + 𝑳𝑭𝑭
𝑹𝒇
𝝆 𝒊𝒇
𝒗𝒇 = 𝑹𝒇 𝟏 + 𝝉𝒇 𝝆 𝒊𝒇−−−−−−−(5)
𝑻𝒆 − 𝑻𝑳 = ( 𝑩𝒎 + 𝑱 𝝆) 𝝎𝒓 −− − − 𝟔
9/1
/20
13 1
1:4
8 A
MP
RB
/SC
E /D
ep
t. ofE
EE
23
𝝉𝒂 ⟶ Armature time constant
𝝉𝒇 ⟶ Field time constant
𝑺𝒐𝒍𝒗𝒊𝒏𝒈 𝒕𝒉𝒆 𝒆𝒒𝒖𝒂𝒕𝒊𝒐𝒏𝒔 𝟒 , 𝟓 𝒂𝒏𝒅 𝟔 𝒇𝒐𝒓 𝒊𝒂 ,
𝒊𝒇, 𝒂𝒏𝒅 𝝎𝒓 𝒚𝒊𝒆𝒍𝒅𝒔
𝒊𝒂 =
𝟏𝒓𝒂
𝝉𝒂𝝆 + 𝟏 𝒗𝒂 − 𝑳𝑨𝑭𝝎𝒓𝒊𝒇 − − −− 𝟕
𝒊𝒇 =
𝟏𝑹𝒇
𝝉𝒇𝝆 + 𝟏 𝒗𝒇 − −− − 𝟖
𝝎𝒓 =𝟏
𝑱𝝆 + 𝑩𝒎 𝑻𝒆 − 𝑻𝑳 −− − − 𝟗
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
𝑺𝒐𝒍𝒗𝒊𝒏𝒈 𝒕𝒉𝒆 𝒆𝒒𝒖𝒂𝒕𝒊𝒐𝒏𝒔 𝟏 , 𝟐 𝒂𝒏𝒅 𝟑 𝒇𝒐𝒓 𝒅𝒊𝒂
𝒅𝒕, 𝒅𝒊𝒇
𝒅𝒕
𝒂𝒏𝒅 𝒅𝝎𝒓
𝒅𝒕 𝒚𝒊𝒆𝒍𝒅𝒔
From (1)
𝒅𝒊𝒂𝒅𝒕
= −𝒓𝒂
𝑳𝑨𝑨
𝒊𝒂 − 𝑳𝑨𝑭
𝑳𝑨𝑨
𝒊𝒇𝝎𝒓 + 𝟏
𝑳𝑨𝑨
𝒗𝒂— 𝟏𝟎
From (2)
𝒅𝒊𝒇
𝒅𝒕= −
𝑹𝒇
𝑳𝑭𝑭
𝒊𝒂 + 𝟏
𝑳𝑭𝑭
𝒗𝒇— 𝟏𝟏
From (3)
𝒅𝝎𝒓
𝒅𝒕= −
𝑩𝒎
𝑱𝝎𝒓 +
𝑳𝑨𝑭
𝑱𝒊𝒇𝒊𝒂 −
𝟏
𝑱𝑻𝑳 − −(𝟏𝟐)
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
𝜌
𝒊𝒇𝒊𝒂𝝎𝒓
=
−𝑹𝒇
𝑳𝑭𝑭𝟎 𝟎
𝟎−𝒓𝒂
𝑳𝑨𝑨𝟎
𝟎 𝟎−𝑩𝒎
𝑱
𝒊𝒇𝒊𝒂𝝎𝒓
+
𝟎−𝑳𝑨𝑭𝝎𝒓
𝑳𝑨𝑨
𝑳𝑨𝑭𝒊𝒇𝒊𝒂
𝑱
+
𝟏
𝑳𝑭𝑭𝟎 𝟎
𝟎𝟏
𝑳𝑨𝑨𝟎
𝟎 𝟎−𝟏
𝑱
𝒗𝒇
𝒗𝒂
𝑻𝑳
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
𝒗𝒇 𝒊𝒔 𝒆𝒍𝒊𝒎𝒊𝒏𝒂𝒕𝒆𝒅
𝑳𝑨𝑭𝒊𝒇 𝒊𝒔 𝒓𝒆𝒑𝒍𝒂𝒄𝒆𝒅 𝒃𝒚 𝒌𝒗
𝒌𝒗 𝒊𝒔 𝒅𝒆𝒕𝒆𝒓𝒎𝒊𝒏𝒆𝒅 𝒃𝒚
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