Methods of Improving Commutation-E.M.F. Commutation

Author: arjun
Category: Armature Reaction and Commutation, Direct Current Machines, Electrical Machines

In this method, an arrangement is made to neutralize the reactance voltage by producing a reversing voltage in the coil undergoing commutation. The reversing voltage acts in opposition to the reactance voltage and neutralizes it to some extent. If the reversing voltage is equal to the reactance voltage, the effect of the latter is completely wiped out and we get sparkless commutation. The reversing voltage may be produced in the following two ways:
(i) By brush shifting
(ii) By using interpoles or compoles
(i) By brush shifting
In this method, the brushes are given sufficient forward lead (for a generator) to bring the short-circuited coil (i.e., coil undergoing commutation) under the influence of the next pole of opposite polarity. Since the short-circuited coil is now in the reversing field, the reversing voltage produced cancels the reactance voltage. This method suffers from the following drawbacks:

(a) The reactance voltage depends upon armature current. Therefore, the brush shift will depend on the magnitude of armature current which keeps on changing. This necessitates frequent shifting of brushes.
(b) The greater the armature current, the greater must be the forward lead for a generator. This increases the demagnetizing effect of armature reaction and further weakens the main field.
(ii) By using interpoles or compoles
The best method of neutralizing reactance voltage is by, using interpoles or compoles.

Interpoles or Compoles
The best way to produce reversing voltage to neutralize the reactance voltage is by using interpoles or compoles. These are small poles fixed to the yoke and spaced mid-way between the main poles (See Fig. 2.13). They are wound with comparatively few turns and connected in series with the armature so that they
carry armature current. Their polarity is the same as the next main pole ahead in the direction of rotation for a generator (See Fig. 2.13). Connections for a d.c. generator with interpoles is shown in Fig. (2.14).

Functions of Interpoles
The machines fitted with interpoles have their brushes set on geometrical neutral axis (no lead). The interpoles perform the following two functions:
(i) As their polarity is the same as the main pole ahead (for a generator), they induce an e.m.f. in the coil (undergoing commutation) which opposes reactance voltage. This leads to sparkless commutation. The e.m.f. induced
by compoles is known as commutating or reversing e.m.f. Since the interpoles carry the armature current and the reactance voltage is also proportional to armature current, the neutralization of reactance voltage is
automatic.
(ii) The m.m.f. of the compoles neutralizes the cross-magnetizing effect of armature reaction in small region in the space between the main poles. It is because the two m.m.f.s oppose each other in this region.

Fig. (2.15) shows the circuit diagram of a shunt generator with commutating winding and compensating winding. Both these windings are connected in series with the armature and so they carry the armature current. However, the functions they perform must be understood clearly. The main function of commutating winding is to produce reversing (or commutating) e.m.f. in order to cancel the reactance voltage. In addition to this, the m.m.f. of the commutating winding neutralizes the crossmagnetizing ampere-turns in the space between the main poles. The compensating winding neutralizes the cross-magnetizing effect of armature reaction under the pole faces.

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3 Responses to “Methods of Improving Commutation-E.M.F. Commutation”

  1. Indranil Says:

    1.How to select a suitable converter for a DC motor.
    2.How to calculate the PIV of thyrister

  2. Harish Shukla Says:

    We have a long shunt DC motor rated 55KW, 220VDC, 284A, 1500rpm. Our system voltage is 240 VDC ( 235V near motor terminal). During noload trial we found motor current to be around 17A only. During load trial we found that current is varying from 265A to 320A and stablises at that point. There is also variation in speed 1505 to 1570. When we shifted the brush position 3mm towards direction of rotation we found current varying from 220A to 275A. What could be the possible reason?

  3. edith Says:

    This v. brilliant! Thanks alot

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