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Gandhinagar Institute of Technology
Subject Name And Code : DC machines and transformers (2130904)
Active Learning Assignment
Topic :Speed Control Methods For DC Motor
Guided By : Prof. Hitesh Manani
Branch : Electrical
Division : F2 Sem : 3rd
Academic year : 2015-16(odd)
Prepared by:
• Name
• Bhushan Borse
• Harshid Panchal
• Ajay Patel
• Enrollment no.
• 140120109002
• 140120109023
• 140120109025
Speed Control Methods Of
DC Motor
Speed Of A DC Motor
• We know, back emf of a DC motor Eb is the induced emf due to rotation of the armature in magnetic
field. Thus value of the Eb can be given by the EMF equation of a DC generator.
Eb = PØNZ/60A
Eb can also be given as,
Eb = V- IaRa
• thus from above equations
N = Eb
60A/PØZ
but, for a DC motor A, P and Z are constant
N α K Eb/Ø (where, K=constant)
thus, it shows speed is directly proportional to back emf and inversely proportional to the flux per pole.
(where,
P= no. of poles,
Ø=flux/pole,
N=speed in rpm,
Z=no. of armature
conductors,
A=parallel paths)
Speed Control Methods Of DC Motor
Speed Control Of Shunt Motor
1. Flux Control Method
It is seen that speed of the motor is inversely proportional to
flux. Thus by decreasing flux speed can be increased and vice
versa.
To control the flux, a rheostat is added in series with the field
winding, as shown in the circuit diagram. Adding more
resistance in series with field winding will increase the speed, as
it will decrease the flux.
Field current is relatively small and hence I2R loss is small, hence this method is quiet efficient. Though
speed can be increased by reducing flux with this method, it puts a limit to maximum speed as
weakening of flux beyond the limit will adversely affect the commutation.
2. Armature Control Method
Speed of the motor is directly proportional to the
back emf Eb and Eb = V- IaRa. That is when supply
voltage V and armature resistance Ra are kept
constant, speed is directly proportional to
armature current Ia. Thus if we add resistance in
series with armature, Ia decreases and hence speed
decreases.
Greater the resistance in series with armature,
greater the decrease in speed.
A) Multiple voltage control: In this method the, shunt filed is connected to a fixed
exciting voltage, and armature is supplied with different voltages. Voltage across
armature is changed with the help of a suitable switchgear. The speed is
approximately proportional to the voltage across the armature.
3. Voltage Control Method
B) Ward-Leonard System:
This system is used where very sensitive speed
control of motor is required (e.g. electric excavators,
elevators etc.) The arrangement of this system is as
required in the figure beside.
M2 is the motor whose speed control is required.
M1 may be any AC motor or DC motor with constant
speed.
G is the generator directly coupled to M1.
In this method the output from the generator G is fed to the armature of the motor M2 whose speed
is to be controlled. The output voltage of the generator G can be varied from zero to its maximum
value, and hence the armature voltage of the motor M2 is varied very smoothly. Hence very
smooth speed control of motor can be obtained by this method.
Speed Control Of Series Motor
1. Flux Control Method
A veriable resistance is connected parallel to the series
field as shown in fig (a).
This variable resistor is called as diverter, as desired
amount of current can be diverted through this resistor
and hence current through field coil can be decreased.
Hence flux can be decreased to desired amount and speed
can be increased.
A) Field divertor :
B) Armature divertor:
Divertor is connected across the armature as in fig (b).
For a given constant load torque, if armature current is
reduced then flux must increase. As, Ta α Ø Ia
This will result in increase in current taken from the supply and
hence flux Ø will increase and subsequently speed of the
motor will decrease.
C) Tapped field control:
As shown in fig (c) field coil is tapped dividing number
of turns. Thus we can select different value of Ø by
selecting different number of turns.
D) Paralleling field coils:
In this method, several speeds can be obtained by
regrouping coils as shown in fig (d).
2. Variable Resistance In Series With Armature
• By introducing resistance in series with armature, voltage across the armature can be reduced. And
hence, speed reduces in proportion with it.
3. Series-Parallel Control
• This system is widely used in electric traction, where two or more mechanically coupled series motors are
employed. For low speeds, motors are joined in series, and for higher speeds motors are joined in
parallel.
• When in series, the motors have the same current passing through them, although voltage across each
motor is divided. When in parallel, voltage across each motor is same although current gets divided.
• http://www.electricaleasy.com/
• https://www.surplusrecord.com/cgi-
bin/adpop.pl?846819
References :

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methods to control speed of dc motors

  • 1. Gandhinagar Institute of Technology Subject Name And Code : DC machines and transformers (2130904) Active Learning Assignment Topic :Speed Control Methods For DC Motor Guided By : Prof. Hitesh Manani Branch : Electrical Division : F2 Sem : 3rd Academic year : 2015-16(odd)
  • 2. Prepared by: • Name • Bhushan Borse • Harshid Panchal • Ajay Patel • Enrollment no. • 140120109002 • 140120109023 • 140120109025
  • 3. Speed Control Methods Of DC Motor
  • 4. Speed Of A DC Motor • We know, back emf of a DC motor Eb is the induced emf due to rotation of the armature in magnetic field. Thus value of the Eb can be given by the EMF equation of a DC generator. Eb = PØNZ/60A Eb can also be given as, Eb = V- IaRa • thus from above equations N = Eb 60A/PØZ but, for a DC motor A, P and Z are constant N α K Eb/Ø (where, K=constant) thus, it shows speed is directly proportional to back emf and inversely proportional to the flux per pole. (where, P= no. of poles, Ø=flux/pole, N=speed in rpm, Z=no. of armature conductors, A=parallel paths)
  • 5. Speed Control Methods Of DC Motor Speed Control Of Shunt Motor 1. Flux Control Method It is seen that speed of the motor is inversely proportional to flux. Thus by decreasing flux speed can be increased and vice versa. To control the flux, a rheostat is added in series with the field winding, as shown in the circuit diagram. Adding more resistance in series with field winding will increase the speed, as it will decrease the flux. Field current is relatively small and hence I2R loss is small, hence this method is quiet efficient. Though speed can be increased by reducing flux with this method, it puts a limit to maximum speed as weakening of flux beyond the limit will adversely affect the commutation.
  • 6. 2. Armature Control Method Speed of the motor is directly proportional to the back emf Eb and Eb = V- IaRa. That is when supply voltage V and armature resistance Ra are kept constant, speed is directly proportional to armature current Ia. Thus if we add resistance in series with armature, Ia decreases and hence speed decreases. Greater the resistance in series with armature, greater the decrease in speed.
  • 7. A) Multiple voltage control: In this method the, shunt filed is connected to a fixed exciting voltage, and armature is supplied with different voltages. Voltage across armature is changed with the help of a suitable switchgear. The speed is approximately proportional to the voltage across the armature. 3. Voltage Control Method
  • 8. B) Ward-Leonard System: This system is used where very sensitive speed control of motor is required (e.g. electric excavators, elevators etc.) The arrangement of this system is as required in the figure beside. M2 is the motor whose speed control is required. M1 may be any AC motor or DC motor with constant speed. G is the generator directly coupled to M1. In this method the output from the generator G is fed to the armature of the motor M2 whose speed is to be controlled. The output voltage of the generator G can be varied from zero to its maximum value, and hence the armature voltage of the motor M2 is varied very smoothly. Hence very smooth speed control of motor can be obtained by this method.
  • 9. Speed Control Of Series Motor 1. Flux Control Method A veriable resistance is connected parallel to the series field as shown in fig (a). This variable resistor is called as diverter, as desired amount of current can be diverted through this resistor and hence current through field coil can be decreased. Hence flux can be decreased to desired amount and speed can be increased. A) Field divertor :
  • 10. B) Armature divertor: Divertor is connected across the armature as in fig (b). For a given constant load torque, if armature current is reduced then flux must increase. As, Ta α Ø Ia This will result in increase in current taken from the supply and hence flux Ø will increase and subsequently speed of the motor will decrease.
  • 11. C) Tapped field control: As shown in fig (c) field coil is tapped dividing number of turns. Thus we can select different value of Ø by selecting different number of turns.
  • 12. D) Paralleling field coils: In this method, several speeds can be obtained by regrouping coils as shown in fig (d).
  • 13. 2. Variable Resistance In Series With Armature • By introducing resistance in series with armature, voltage across the armature can be reduced. And hence, speed reduces in proportion with it. 3. Series-Parallel Control • This system is widely used in electric traction, where two or more mechanically coupled series motors are employed. For low speeds, motors are joined in series, and for higher speeds motors are joined in parallel. • When in series, the motors have the same current passing through them, although voltage across each motor is divided. When in parallel, voltage across each motor is same although current gets divided.