What is an Electric generator? (back to basics)

[Steven Mill]

Hi, the following article has been written by a member of the Electrical Engineering community who want to contribute to the blog with this first article about electric generators.

Electric Generator is a machine that converts mechanical energy to electric energy. The mechanical energy can be supplied by the prime mover which combustion engine, steam engine, can water falling through turbine or even an electric motor or any such mechanism that can be a source of mechanical energy. Usually this energy is obtained from a rotating shaft that is also called the armature of the generator. The electric energy then produced can be used for power transmission to commercial, industrial or even domestic level. Generators supply current which usually has a frequency of 50 Hz, which is used here.

An electric generator has two parts:

• Stator
• Rotor

The stator comprises of the stationary magnetic poles, whereas the rotating armature is included in the rotor.

Working of an Electric Generator

Generators usually work on Faraday’s law of Electro Magnetic induction. This law explains that by rotating an electric conductor in a magnetic field, an emf is induced, which creates a flow of charges. When the conductor rotates in the magnetic field, a voltage difference is created between its two ends and the flux in it changes and an emf is induced which is proportional to the rate of change of flux (e=-N dΦ/dt) and hence the current flows. The electric conductor rotating is called the armature of the generator.
This phenomenon is shown in the figure below:

When the side of the conductor is perpendicular to the magnetic fields, the rate of change of flux is minimum in it.

Types of Electric generator

There are five major types of electric generators, classified according to the manner in which their field flux is produced:

1) Separately Excited Generator: In a separately excited generator, the field flux is derived from a separate power source independent of the generator itself.

2) Shunt Generator: In a shunt Generator, the field flux is derived by connecting the field circuit directly across the terminals of the generator.

3) Series generator: In series Generator, the field flux is produced by connecting the field circuit in series with the armature of the generator.

4) Commutatively Compound Generator: In commutatively compounded generator, both a shunt and a series field are present and their efforts are additive.

5) Differentially compound Generator: In a differentially compounded generator, both a shunt and a series field are present, but their efforts are subtracted.

• 1. Separately Excited Generator

The equivalent circuit of a separately excited generator is shown below:

Here the total voltage is represented by V_T.

I_a is the armature current and V_a is the armature voltage. I_L is the load current and E_A is the induced emf. The relation between them is given as:

V_T = E_A – I_aR_a

Where I_L = I_a.

Its output characteristics are the graph of I_L versus E_A.

This graph is ideally a straight line but usually deviates due to the armature reaction.

• 2. Shunt Generator

A shunt generator is a generator that supplies its own field current by having its field connected directly across the terminals of the machine. The equivalent circuit of a shunt generator is shown below:

In the circuit, the armature current of the machine supplies both the field circuit and the load attached to the machine. The relation between the three currents is as follow:

I_a = I_F + I_L

Where;

I_a = armature current.

I_F = field circuit current

I_L = load current

The Kirchhoff’s voltage law equation for the armature circuit of this machine is:

V_T = E_A – I_AR_A

This type of generator has a distinct advantage over the separated excited generator that no external power supply is required for the field circuit.

The Graph of its output characteristics is as follows:

• 3. Series Generator

The series generator is the generator whose field is connected in series with its armature. Since its armature has a much higher current than the shunt field, the series field winding will only have a few turns but a thicker wire.

Its equivalent circuit is shown below:

Here: I_A = I_L = I_S.

And its Kirchhoff’s law equation is written as:

V_T = E_A – I_A (R_A + R_S)

The graph of its output characteristics is as shown:

• 4. Commutatively Compounded Generator

A commutatively compounded generator is one in which there are both series and shunt fields, connected so that the magneto motive forces from the two fields are such that they add up.

It can also be further divided into two categories:

• Long Shunt Compound
• Short Shunt Compound

The equivalent circuit for these types of generators is shown below:

The equations for a commutatively compound generator are:

I_A = I_F + I_L

VT = E_A – I_A (R_A + R_S)

The graph of the terminal characteristics of a commutatively compound Generator is as follow:

• 5. Differentially Compound Electric Generator

In this type of Generator, the shunt and series field windings, both are present but their magneto motive forces produced are such that they subtract from each other and the net magneto motive force is much less. The equivalent circuit of a differentially compound generator is more or less the same as the commutatively compound generator, just the directions of the magneto motive forces produced inside the circuit are different. Its current equations can be written as:

I_F* = I_F + I_eq

Its terminal voltage versus load current graph is as shown:

[Anonymous]

Nice of you to share. I found it interesting.
Bill

[Author]

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