Consider a dc motor as shown below. Voltage equation
of the motor will be
V=Eb+IaRa ......
by KVL
Or
Ia= (V-Eb)/Ra
At starting, when the motor is stationary i.e speed,
N=0, there will be no back emf.
Eb=(P
ΦZN)/60A
Eb=0
Therefore, Ia= V/Ra
Consequently, if the motor is directly switched on to the mains, the armature will
draw a heavy current because of small armature resistance, Ra.
For example, a 10 kw, 250-v shunt motor with armature
resistance Ra=0.2 Ω if switched on directly, will draw 1250 A
current, whereas the rated current is only 40A. Its more than 30 times.
Such high current may cause problems as :-
- Burning of armature due to excessive heating (Ia2Ra).
- Damaging commutator and brushes due to heavy sparking.
- High starting torque
Ta ∝ Ia ..... Φ is practically constant in a dc shunt motor
Thus quick acceleration may damage rotating parts of the motor.
4. Large
dips in supply line to which motor is connected, affecting working of other devices connected
on the same line.
In view of this, the
armature current must be limited to a value that can be commuted safely. This
is accomplished by inserting a variable resistance in series with the armature
circuit.
The resistance is gradually reduced as motor gains speed (and back
emf, Eb starts appearing) and eventually cut out completely as motor
gains speed.
This explains necessity of starter in dc motor and also highlights the importance of back emf.