Module 6. D.C. machines

Lesson 23

TYPES AND CHARACTERISTICS OF D.C. GENERATORS

23.1  Types of D.C. Generators

D.C. generators can be classified as:

1.   Permanent magnet type

2.   Electromagnet type

23.2  Permanent Magnet Type

In this type of generator the poles are made of permanent magnet. The poles do not require any windings. Such type of D.C. generators are of small size. These are employed mainly in dynamo in cycles and bikes. It is not used for industrial purpose because:

a.       It would require large magnet which is economically not feasible.

b.      Magnetic strength decreases with time so magnetic flux will not remain constant.

23.3  Electromagnet Type

The poles of D.C. generator is magnetized using windings. Electromagnetic type generators can further classifies as:

(i)     Externally exited D.C. generator,

(ii)   Self-exited D.C. generator.

23.3.1  External or separately excited D.C. generators

A D.C. generator whose field magnet winding is supplied from an independent external D.C. source (e.g., a battery etc.) is called a separately excited generator. Fig. (23.1) shows the connections of a separately excited generator. The voltage output depends upon the speed of rotation of armature and the field current (Eg =PΦ ZN/60 A). The greater the speed and field current, greater is the generated e.m.f. It may be noted that separately excited D.C. generators are rarely used in practice. The D.C. generators are normally of self-excited type

 

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Fig. 23.1 External or separately excited D.C. generators

 

 

Armature current, Ia = IL

Terminal Voltage, V = EgIaRa

Electric power developed = EgIa

Power delivered to load = 

23.3.2  Self-excited D.C. generators

A D.C. generator whose field magnet winding is supplied with current from the output of the generator itself is called a self-excited generator. There are three types of self-excited generators depending upon the manner in which the field winding is connected to the armature, namely;

(i) Series generator

(ii) Shunt generator

(iii) Compound generator

23.3.2.1  Series generator

In a series wound generator, the field winding is connected in series with armature winding so that whole armature current flows through the field winding as well as the load. (Fig. 23.2) shows the connections of a series wound generator. Since the field winding carries the whole of load current, it has a few turns of thick wire having low resistance. Series generators are rarely used except for special purposes e.g., boosters.

 

Armature current, Ia = Ise = IL = I(say)

Terminal voltage, V = Eg – I (Ra + Rse)

Power developed in armature = EgIa

Power delivered to load

            =

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Fig. 23.2 Series generator

23.3.2.2  Shunt generator

In a shunt generator, the field winding is connected in parallel with the armature winding so that terminal voltage of the generator is applied across it. The shunt field winding has many turns of fine wire having high resistance. Therefore, only a part of armature current flows through shunt field winding and the rest flows through the load. (Fig. 23.3) shows the connections of a shunt-wound generator.

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Fig. 23.3 Shunt generator

 

Shunt field current, Ish =  V/Rsh

Armature current, Ia = IL + Ish

Terminal voltage, V = EgIaRa

Power developed in armature = EgIa

Power delivered to load = VIL

23.3.2.3  Compound generator

In a compound-wound generator, there are two sets of field windings on each pole—one is in series and the other in parallel with the armature. A compound wound generator may be:

(a) Short Shunt in which only shunt field winding is in parallel with the armature winding (Fig. 23.4).

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Fig. 23.4 Short shunt generator

 

(b) Long Shunt in which shunt field winding is in parallel with both series field and armature winding (Fig. 23.5).

 

http://electricalandelectronics.org/wp-content/uploads/2009/05/compound-generator.pnghttp://electricalandelectronics.org/wp-content/uploads/2009/05/compound-generator.png

Fig. 23.5 Long shunt generator

 

 

 

Short shunt

            Series field current, Ise = IL

            Shunt field current,

            Terminal Voltage, V = EgIaRaIseRse

            Power developed in armature = EgIa

            Power delivered to load = VIL

Long shunt

            Series field current, Ise = Ia = IL + Ish

            Shunt field current, Ish = V/Rsh

            Terminal voltage, V = EgIa (Ra + Rse)

            Power developed in armature = EgIa

            Power delivered to load = VIL

 

23.4  Efficiency of d.c. generators

Various power stages in the case of a d.c generator are shown in Fig. 23.6.

Fig. 23.6 Various losses

Mechanical Efficiency

Mechanical losses = Iron + Friction losses

Electrical Efficiency

Overall Efficiency

In general generator efficiency = Output / (Output + losses)
The condtion for maximum efficiency of generator is given by


i.e Variable loss = Constant loss.