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SPEED CONTROL OF DC
MOTOR
Prepared By
Mrs. D.Sharmitha AP/EEE
Kumaraguru College of Technology
Coimbatore
Governing Equations
1.Eb = PØNZ/60A
(where, P = no. of poles, Ø = flux/pole, N = speed in rpm, Z = no. of armature
conductors, A = parallel paths)
2. Eb = V- IaRa
thus,
3.N = E
b
60A/PØZ (A, P and Z are constants, Hence)
4. N ∝ K E
b/Ø (where, K=constant)
Speed Control Of Shunt Motor
1. Flux Control Method
 To control the flux, a rheostat is added in series with the field winding
 Adding more resistance in series with the field winding will increase the speed
as it decreases the flux.
 In shunt motors, as field current is relatively very small, Ish2R loss is small
and, hence, this method is quite efficient.
 Though speed can be increased above the rated value 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.
Armature Control Method
• Eb = V - IaRa. when the supply voltage V and the armature resistance
Ra are kept constant, speed is directly proportional to the armature
current Ia.
• Thus, if we add a resistance in series with the armature, Ia decreases
and, hence, the speed also decreases.
• Greater the resistance in series with the armature, greater the
decrease in speed.
3. Voltage Control Method
I.Multiple voltage control:
 In this method, the shunt field 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.
II.Ward-Leonard System:
 This system is used where very sensitive speed control of motor is required
(e.g electric excavators, elevators etc.).
 M2 is the motor whose speed control is required.
M1 may be any AC motor or DC motor with constant speed.
G is a 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 by means of its field regulator and, hence, the armature
voltage of the motor M2 is varied very smoothly.
 Hence, very smooth speed control of the dc motor can be obtained by this
method.
Speed Control Of Series Motor
1.FLUX CONTROL METHOD
Field divertor:
 A veritable resistance is connected parallel to the series field as shown in fig (a).
 This variable resistor is called as divertor, as the 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 the desired amount and speed can be increased.
Armature divertor:
 For a given constant load torque, if armature current is reduced then flux must
increase. As, Ta ∝ Øia
 This will result in an increase in current taken from the supply and hence flux Ø
will increase and subsequently speed of the motor will decrease.
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.
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 a resistance in series with the 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, the motors are connected in series, and for higher speeds the
motors are connected in parallel.
 When in series, the motors have the same current passing through them,
although voltage across each motor is divided.
 When in parallel, the voltage across each motor is same although the current
gets divided.
THANK YOU

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Speed control of DC motor

  • 1. SPEED CONTROL OF DC MOTOR Prepared By Mrs. D.Sharmitha AP/EEE Kumaraguru College of Technology Coimbatore
  • 2. Governing Equations 1.Eb = PØNZ/60A (where, P = no. of poles, Ø = flux/pole, N = speed in rpm, Z = no. of armature conductors, A = parallel paths) 2. Eb = V- IaRa thus, 3.N = E b 60A/PØZ (A, P and Z are constants, Hence) 4. N ∝ K E b/Ø (where, K=constant)
  • 3. Speed Control Of Shunt Motor 1. Flux Control Method  To control the flux, a rheostat is added in series with the field winding  Adding more resistance in series with the field winding will increase the speed as it decreases the flux.  In shunt motors, as field current is relatively very small, Ish2R loss is small and, hence, this method is quite efficient.  Though speed can be increased above the rated value 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.
  • 4. Armature Control Method • Eb = V - IaRa. when the supply voltage V and the armature resistance Ra are kept constant, speed is directly proportional to the armature current Ia. • Thus, if we add a resistance in series with the armature, Ia decreases and, hence, the speed also decreases. • Greater the resistance in series with the armature, greater the decrease in speed.
  • 5. 3. Voltage Control Method I.Multiple voltage control:  In this method, the shunt field 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. II.Ward-Leonard System:
  • 6.  This system is used where very sensitive speed control of motor is required (e.g electric excavators, elevators etc.).  M2 is the motor whose speed control is required. M1 may be any AC motor or DC motor with constant speed. G is a 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 by means of its field regulator and, hence, the armature voltage of the motor M2 is varied very smoothly.  Hence, very smooth speed control of the dc motor can be obtained by this method.
  • 7. Speed Control Of Series Motor 1.FLUX CONTROL METHOD
  • 8. Field divertor:  A veritable resistance is connected parallel to the series field as shown in fig (a).  This variable resistor is called as divertor, as the 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 the desired amount and speed can be increased. Armature divertor:  For a given constant load torque, if armature current is reduced then flux must increase. As, Ta ∝ Øia  This will result in an increase in current taken from the supply and hence flux Ø will increase and subsequently speed of the motor will decrease. 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. Paralleling field coils:  In this method, several speeds can be obtained by regrouping coils as shown in fig (d).
  • 9. 2. Variable Resistance In Series With Armature  By introducing a resistance in series with the 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, the motors are connected in series, and for higher speeds the motors are connected in parallel.  When in series, the motors have the same current passing through them, although voltage across each motor is divided.  When in parallel, the voltage across each motor is same although the current gets divided.