ee22 part3 dc motor
TRANSCRIPT
-
8/9/2019 Ee22 Part3 Dc Motor
1/28
DC Motors
-
8/9/2019 Ee22 Part3 Dc Motor
2/28
Types of DC Motors
Separately excited DC motor
Shunt DC Motor
Permanent-magnet DC motor
Series DC motor
Compound DC motor
-
8/9/2019 Ee22 Part3 Dc Motor
3/28
Separately Excited DC Motor
-
8/9/2019 Ee22 Part3 Dc Motor
4/28
Shunt DC Motor
-
8/9/2019 Ee22 Part3 Dc Motor
5/28
Torque-Speed Characteristic of a Shunt
DC Motor
-
8/9/2019 Ee22 Part3 Dc Motor
6/28
-
8/9/2019 Ee22 Part3 Dc Motor
7/28
@ NO LOAD: EA1= VT= 250 V, n1= 1200 rpm
-
8/9/2019 Ee22 Part3 Dc Motor
8/28
-
8/9/2019 Ee22 Part3 Dc Motor
9/28
-
8/9/2019 Ee22 Part3 Dc Motor
10/28
-
8/9/2019 Ee22 Part3 Dc Motor
11/28
-
8/9/2019 Ee22 Part3 Dc Motor
12/28
-
8/9/2019 Ee22 Part3 Dc Motor
13/28
Nonlinear Analysis of a Shunt DC Motor
-
8/9/2019 Ee22 Part3 Dc Motor
14/28
Speed Control of Shunt DC Motors
-
8/9/2019 Ee22 Part3 Dc Motor
15/28
Adjusting the Field Resistance RF
What will happen if the field resistance goes to infinity,
i.e., an open filed circuit?
-
8/9/2019 Ee22 Part3 Dc Motor
16/28
Adjusting the Terminal Voltage
-
8/9/2019 Ee22 Part3 Dc Motor
17/28
Speed Regulation of DC Motors
-
8/9/2019 Ee22 Part3 Dc Motor
18/28
The Permanent-Magnet DC Motor
- Poles are made of permanent magnets- Common in smaller fractional and subfractional
horsepower size
Advantages: No need for field excitation
No field circuit copper losses
Can be made smaller than corresponding shunt dc motors
Disadvantages:
Has a lower induced torque per ampere of armature currentthan a shunt motor of the same size and construction.
Has the risk of demagnetization.
-
8/9/2019 Ee22 Part3 Dc Motor
19/28
The Series DC Motor
Equivalent Circuit:
VT= EA+ IA(RA+ RS)
= cIA ind = K IA= KcIA
2
-
8/9/2019 Ee22 Part3 Dc Motor
20/28
The torque-speed characteristic of a
series dc motor:
Kc
RR
Kc
VSA
ind
T 1
-
8/9/2019 Ee22 Part3 Dc Motor
21/28
Speed Control of Series DC Motors.
there is only one efficient way to change the
speed of a series dc motor.
That method is to change the terminal voltage
of the motor.
If terminal voltage is increased, the speed will
increase for any given torque.
-
8/9/2019 Ee22 Part3 Dc Motor
22/28
-
8/9/2019 Ee22 Part3 Dc Motor
23/28
Short-shunt connection:
-
8/9/2019 Ee22 Part3 Dc Motor
24/28
The EMF Equations
Long-shunt:
VT= EA+ IA(RA+ RS)
Short-shunt:
VT= EA+ IARA+ ILRS
Currents
IA= IL- IF
IF= VT/RF
The net mmf and the effective shunt field current Fnet= FF FSE- FAR
IF*= IF (NSE/NF) IAFAR/NF
-
8/9/2019 Ee22 Part3 Dc Motor
25/28
The Torque-Speed Characteristic of a Cumulatively Compounded DCMotor (CC)
There is a component of flux which is constant and anothercomponent which is proportional to its armature current (and thusto its load). Thus, CC motor has a higher starting torque than ashunt motor (whose flux is constant) but a lower starting torquethan a series motor (whose entire flux is proportional to armaturecurrent).
The CC motor combines the best features of both the shunt andseries motors. Like a series motor, it has extra torque for starting;like a shunt, it does not overspeed at no-load.
At light loads, the series field has a very small effect, so the motorbehaves approximately as a shunt dc motor. As the load gets verylarge, the series flux becomes quite important and the torque-speed curve begins to look like a series motors characteristic.
-
8/9/2019 Ee22 Part3 Dc Motor
26/28
Comparison of the torque-speed characteristic.:
The torque-speedcharacteristic of a cumulatively
compounded dc motor
compared to series and shunt
motors with the same full-load
rating.
The torque-speed
characteristic of acumulatively compounded
dc motor compared to a
shunt motor with the same
no-load speed.
-
8/9/2019 Ee22 Part3 Dc Motor
27/28
-
8/9/2019 Ee22 Part3 Dc Motor
28/28
End of Part 3