Emf Equation of a DC Generator

As the armature rotates, a voltage is generated in its coils. In the case of a generator, the emf of rotation is called the Generated emf or Armature emf and is denoted as Er = Eg. In the case of a motor, the emf of rotation is known as Back emf or Counter emf and represented as Er = Eb.The expression for emf is same for both the operations. I.e., for Generator as well as for Motor.

Derivation of EMF Equation of a DC Machine – Generator and Motor

Let,

  • P – Number of poles of the machine
  • ϕ – Flux per pole in Weber.
  • Z – Total number of armature conductors.
  • N – Speed of armature in revolution per minute (r.p.m).
  • A – Number of parallel paths in the armature winding.

In one revolution of the armature, the flux cut by one conductor is given as

EMF-EQUATION-OF-DC-GENERATOR-EQ1

Time taken to complete one revolution is given as

EMF-EQUATION-OF-DC-GENERATOR-EQ2

Therefore, the average induced e.m.f in one conductor will be

EMF-EQUATION-OF-DC-GENERATOR-EQ3

Putting the value of (t) from Equation (2) in the equation (3) we will get

EMF-EQUATION-OF-DC-GENERATOR-EQ4

The number of conductors connected in series in each parallel path = Z/A.

Therefore, the average induced e.m.f across each parallel path or the armature terminals is given by the equation shown below.

EMF-EQUATION-OF-DC-GENERATOR-EQ5

Where n is the speed in revolution per second (r.p.s) and given as

EMF-EQUATION-OF-DC-GENERATOR-EQ6

For a given machine, the number of poles and the number of conductors per parallel path (Z/A) are constant. Hence, the equation (5) can be written as

EMF-EQUATION-OF-DC-GENERATOR-EQ7

Where, K is a constant and given as

EMF-EQUATION-OF-DC-GENERATOR-EQ8

Therefore, the average induced emf equation can also be written as

EMF-EQUATION-OF-DC-GENERATOR-EQ9

Where K1 is another constant and hence induced emf equation can be written as

EMF-EQUATION-OF-DC-GENERATOR-EQ10

Where ω is the angular velocity in radians/second is represented as

EMF-EQUATION-OF-DC-GENERATOR-EQ11

Thus, it is clear that the induced emf is directly proportional to the speed and flux per pole. The polarity of induced emf depends upon the direction of the magnetic field and the direction of rotation. If either of the two is reverse the polarity changes, but if two are reversed the polarity remains unchanged.

This induced emf is a fundamental phenomenon for all the DC Machines whether they are working as a generator or motor.

If the machine DC Machine is working as a Generator, the induced emf is given by the equation shown below.

EMF-EQUATION-OF-DC-GENERATOR-EQ12

Where Eg is the Generated Emf

If the machine DC Machine is working as a Motor, the induced emf is given by the equation shown below.

EMF-EQUATION-OF-DC-GENERATOR-EQ13

In a motor, the induced emf is called Back Emf (Eb) because it acts opposite to the supply voltage.

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