Diode Current Equation
Single Phase Transformer
Types of DC Motor Separately Excited Shunt Series Compound DC Motor
Shunt Wound DC Motor | DC Shunt Motor
Series Wound DC Motor or DC Series Motor
Compound Wound DC Motor or DC Compound Motor
Permanent Magnet DC Motor or PMDC Motor | Working Principle Construction
Brushless DC Motors
Electrical Motor | Types Classification and History of Motor
Working of Electric Motor
DC Motor or Direct Current Motor
Speed Regulation of DC Motor
Speed Control of DC Motor
Working or Operating Principle of DC Motor
Torque Equation of DC Motor
Construction of DC Motor | Yoke Poles Armature Field Winding Commutator Brushes of DC Motor
Lap Winding Simplex and Duplex Lap Winding
Testing of DC Machine
Swinburne Test of DC Machine
Losses in DC Machine
Ward Leonard Method of Speed Control
Armature Reaction in DC Machine
Commutation in DC Machine or Commutation in DC Generator or Motor
Methods of Improving Commutation
Starting Methods to limit Starting Current and Torque of DC Motor
3 Point Starter | Working Principle and Construction of Three Point Starter
4 Point Starter | Working Principle and Construction of Four Point Starter
Shunt Wound DC Motor | DC Shunt Motor
Voltage and Current Equation of a Shunt Wound DC MotorLet us now consider the voltage and current being supplied from the electrical terminal to the motor be given by E and Itotal respectively.
This supply current in case of the shunt wound DC motor is split up into 2 parts. Ia, flowing through the armature winding of resistance Ra and Ish flowing through the field winding of resistance Rsh. The voltage across both windings remains the same. From there we can write Itotal = Ia + Ish Thus we put this value of armature current Ia to get general voltage equation of a DC shunt motor. Now in general practice, when the motor is in its running condition, and supply voltage is constant the shunt field current given by, But we know Ish ∝ Φ i.e. field flux Φ is proportional to filed current Ish Thus the field flux remains more or less constant and for this reason a shunt wound DC motor is called a constant flux motor.
Construction of a Shunt Wound DC MotorThe construction of a dc shunt motor is pretty similar to other types of DC motor, as shown in the figure below. Just that there is one distinguishable feature in its designing which can be explained by taking into consideration, the torque generated by the motor. To produce a high torque,
- The armature winding must be exposed to an amount of current that’s much higher than the field windings current, as the torque is proportional to the armature current.
- The field winding must be wound with many turns to increase the flux linkage, as flux linkage between the field and armature winding is also proportional to the torque. Keeping these two above mentioned criterion in mind a dc shunt motor has been designed in a way, that the field winding possess much higher number of turns to increase net flux linkage and are lesser in diameter of conductor to increase resistance(reduce current flow) compared to the armature winding of the DC motor. And this is how a shunt wound DC motor is visibly distinguishable in static condition from the DC series motor (having thicker field coils) of the self excited type motor’s category.
Self-Speed Regulation of a Shunt Wound DC MotorA very important and interesting fact about the dc shunt motor, is in its ability to self regulate its speed on application of load to the shaft of the rotor terminals. This essentially means that on switching the motor running condition from no load to loaded, surprisingly there is no considerable change in speed of running, as would be expected in the absence of any speed regulating modifications from outside. Let us see how? Let us do a step-wise analysis to understand it better.
- Initially considering the motor to be running under no load or lightly loaded condition at a speed of N rpm.
- On adding a load to the shaft, the motor does slow down initially, but this is where the concept of self regulation comes into the picture.
- At the very onset of load introduction to a shunt wound DC motor, the speed definitely reduces, and along with speed also reduces the back emf, Eb. Since Eb ∝ N, given by, This can be graphically explained below.
- This reduction in the counter emf or the back emf Eb results in the increase of the net voltage. As net voltage Enet = E − Eb. Since supply voltage E remains constant.
- As a result of this increased amount of net voltage, the armature current increases and consequently the torque increases. Since, Ia ∝ Τ given by The change in armature current and torque on supplying load is graphically shown below.
- This increase in the amount of torque increases the speed and thus compensating for the speed loss on loading. Thus the final speed characteristic of a dc shunt motor, looks like.