Transcript DC Motors

DC MOTORS
SEE 3433
ELECTRICAL MACHINES
DC MOTOR
- Shunt motors
- Separately excited
- Series (we’ll look briefly)
DC MOTORS
DC MOTOR
+ -
+ -
DC motor
DC MOTOR
+
Va
-
Load torque opposing
the motor torque
+
Vf
+ -
+ Tm
Tload
DC motor
Mechanical Load: fans,
blowers, Compressors,
DC MOTOR
+
V
-
+
V
+ -
+ Tm
Tload
DC motor
F = mg
DC MOTOR
Hoist
DC MOTOR
- Some applications require the control the speed
- Some applications require the control the torque
- In order to control the torque or speed we need to know the T-
characteristics of the motor and the mechanical load
Intersections between the two characteristics will
determine the operating point
DC MOTOR
Shunt motor
If
Vt = IaRa + Ea
It
It = Ia + If
Rcf
+
Ia
Ra
Vt
Ea = k
Te = kIa
Rcw
Te

Tload
Mechanical
load

k = Vt - IaRa

Vt  IaR a
k

Vt
Ra

T
2 e
k (k)
Three possible methods of speed control:
Field flux
Armature voltage Vt
Armature resistance Ra

Vt
Ra

T
2 e
k (k)

Vt
kT
Vt
R T
 a e2
k T  k T  
Varying Vt

TL
Vt ↓
Te
Requires variable DC supply

Vt
kT
Vt
R T
 a e2
k T  k T  
Varying Vt

TL
Vt ↓
Te
Requires variable DC supply
Vt  (k T ) 
R a Te
k T 
Varying Vt

TL
Constant TL
Te
Requires variable DC supply
Vt  (k T ) 
Vt
R a Te
k T 
Vt  (k T)  IaRa
Vt,rated
Varying Vt
Constant TL
Ia R a
base

Introduction

Vt
R T
 a e2
k T  k T  
Varying Ra

Vt
kT
TL
Ra ↑
Te
Simple control
Losses in external resistor


Vt
kT
Vt
R T
 a e2
k T  k T  
Varying 
TL
↓
Te
Not possible for PM motor
Maximum torque capability reduces
Method of speed control in DC motor drives
Armature voltage control : retain maximum torque capability
Field flux control (i.e. flux reduced) : reduce maximum torque capability
For wide range of speed control
0 to base  armature voltage, above base  field flux reduction
Armature voltage control
Field flux control
Te
Maximum
Torque capability
base

Te
Maximum
Torque capability
base

P Te
Constant torque
Constant power
Pmax

base
0 to base  armature voltage,
P = EaIa,max = kaIa,max
above base  field flux reduction
Pmax = EaIa,max = kabaseIa,max
   1/
0 to base  armature voltage,
above base  field flux reduction
0 to base  armature voltage,
If
Rcf
above base  field flux reduction
It
+
Ia
Ra
Rcw
Vt

BUT there are problems !
0 to base  armature voltage,
If
Rcf
above base  field flux reduction
It
+
Ia
Ra
Rcw
Vt

Controlling Vt will also affect If
Controlling If via Rcf caused losses  I2R
0 to base  armature voltage,
above base  field flux reduction
Separately Excited DC motor
DC supply
for armature
What if we have an AC supply ?
DC supply
for field
3-phase AC
source
Separately Excited DC motor
AC to DC
converter
+
Vdc
+
Vdc
-
-
Armature voltage control
AC to DC
converter
Field voltage control