Working Principle of Alternator
Construction of Alternator
Rating of Alternator
Armature Winding of Alternator
Armature Reaction of Alternator
Phasor Diagram for Synchronous Generator
Working Principle of DC Generator
Construction of DC Generator
Commutation in DC Machine
Methods of Improving Commutation
Frog Leg, Drum and Gramme Ring Winding
Types of DC Generators
Magnetization Curve of DC Generator
Characteristic of Separately Excited DC Gen
Characteristic of DC Shunt Generator
Characteristics of DC Series Generator
Characteristic of DC Compound Generators
Armature Reaction in DC Machine
DC Generators Performance Curves
Applications of DC Generators
Testing of DC Machine
Swinburne’s Test of DC Machine
Differential Protection of Generator
When the DC generator is driven by a prime mover then an emf is induced in the armature. The generated emf in the armature is given by an expression
is constant for a given machine.it is replaced by K in this equation.
φ is the flux per pole,
P is the no. of poles,
N is the no. of revolution made by armature per minute,
Z is the no. of armature conductors,
A is no. of parallel paths.
Now, from the equation we can clearly see that the generated emf is directly proportional to the product of flux per pole and the speed of the armature.
If the speed is constant, then the generated emf is directly proportional to the flux per pole.
It is obvious that, as the excitation current or field current (If) increases from its initial value, the flux and hence generated emf is increased with the field current.
Magnetization curve of a DC generator has a great importance because it represents the saturation of the magnetic circuit. For this reason this curve is also called saturation curve.
According to the molecular theory of magnetism the molecules of a magnetic material, which is not magnetized, are not arranged in definite order. When current passed through the magnetic material then its molecules are arranged in definite order. Up to a certain value of field current the maximum molecules are arranged. In this stage the flux established in the pole increased directly with the field currant and the generated voltage is also increased. Here, in this curve, point B to point C is showing this phenomena and this portion of the magnetization curve is almost a straight line. Above a certain point (point C in this curve) the nu-magnetized molecules become very fewer and it became very difficult to further increase in pole flux.This point is called saturation point. Point C is also known as the knee of the magnetization curve. A small increase in magnetism require very large field current above the saturation point. That is why upper portion of the curve (point C to point D) is bend as shown in figure.
In ferromagnetic materials, the magnetic power and the generated voltage increase with the increase of the current flow through the coils. When current is reduced to zero, there is still magnetic power left in those coils core. This phenomena is called residual magnetism. The core of a DC machine is made of ferromagnetic material.