Kamis, 02 Maret 2017

DC GENERATOR

DC GENERATOR




     1. principle of DC generator
There are two types of generators, one is ac generator and other is DC generator. Whatever may be the types of generators, it always converts mechanical power to electrical power.
we will come to the topic of principle of DC generator. Now the loop is opened and connected it with a split ring as shown in the figure below. Split ring are made out of a conducting cylinder which cuts into two halves or segments insulated from each other. The external load terminals are connected with two carbon brushes which are rest on these split slip ring segments.

  • Working Principle of DC Generator

It is seen that in the first half of the revolution current flows always along ABLMCD i.e. brush no 1 in contact with segment a. In the next half revolution, in the figure the direction of the induced current in the coil is reversed. But at the same time the position of the segments a and b are also reversed which results that brush no 1 comes in touch with the segment b. Hence, the current in the load resistance again flows from L to M. The wave from of the current through the load circuit is as shown in the figure. This current is unidirectional.

This is basic working principle of DC generator, explained by single loop generator model. The position of the brushes of DC generator is so arranged that the change over of the segments a and b from one brush to other takes place when the plane of rotating coil is at right angle to the plane of the lines of force. It is so become in that position, the induced emf in the coil is zero.


   2. construction of DC Generator

  • Yoke of DC Generator
Yoke or the outer frame of DC generator serves two purposes,
·         It holds the magnetic pole cores of the generator and acts as cover of the generator.
·         It carries the magnetic field flux.

  • Pole Cores and Pole Shoes of DC Generator

There are mainly two types of construction available.
 One: Solid pole core, where it is made of a solid single piece of cast iron or cast steel.
Two: Laminated pole core, where it made of numbers of thin, limitations of annealed steel which are riveted together.

  • Armature Core of DC Generator

The purpose of armature core is to hold the armature winding and provide low reluctance path for the flux through the armature from N pole to S pole. Although a DC generator provides direct current but induced current in the armature is alternating in nature.

  • Armature Winding of DC Generator

Armature winding are generally formed wound. These are first wound in the form of flat rectangular coils and are then pulled into their proper shape in a coil puller. Various conductors of the coils are insulated from each other. The conductors are placed in the armature slots, which are lined with tough insulating material.


  • Commutator of DC Generator

The commutator plays a vital role in DC generator. It collects current from armature and sends it to the load as direct current. It actually takes alternating current from armature and converts it to direct current and then send it to external load.

  • Brushes of DC Generator

The brushes are made of carbon. These are rectangular block shaped. The only function of these carbon brushes of DC generator is to collect current from commutator segments. The brushes are housed in the rectangular box shaped brush holder or brush box. As shown in figure, the brush face is placed on the commutator segment which is attached to the brush holder.

  • Bearing of DC Generator

For small machine, ball bearing is used and for heavy duty DC generator, roller bearing is used. The bearing must always be lubricated properly for smooth operation and long life of generator.


3.  Characteristic of Separately Excited DC Generator

  • Magnetic or Open Circuit Characteristic of Separately Excited DC Generator

The curve which gives the relation between field current (If) and the
generated voltage (E0) in the armature on no load is called magnetic or open circuit characteristic of a DC generator. The plot of this curve is practically same for all types of generators, whether they are separately excited or self-excited. This curve is also known as no load saturation characteristic curve of DC generator.
  Here in this figure below we can see the variation of generated emf on no load with field current for different fixed speeds of the armature. For higher value of constant speed, the steepness of the curve is more. When the field current is zero, for the effect residual magnetism in the poles, there will be a small initial emf (OA) as show in figure.


Let us consider a separately excited DC generator giving its no load voltage E0 for a constant field current. If there is no armature reaction and armature voltage drop in the machine then the voltage will remain constant. Therefore, if we plot the rated voltage on the Y axis and load current on the X axis then the curve will be a straight line and parallel to X-axis as shown in figure below. Here, AB line indicating the no load voltage (E0).
When the generator is loaded then the voltage drops due to two main reasons-
1.      Due to armature reaction,
2.      Due to ohmic drop ( IaRa ).

  • Internal or Total Characteristic of Separately Excited DC Generator

The internal characteristic of the separately excited DC generator is obtained by subtracting the drops due to
armature reaction from no load voltage. This curve of actually generated voltage ( Eg ) will be slightly dropping. Here, AC line in the diagram indicating the actually generated voltage (Eg ) with respect to load current. This curve is also called total characteristic of separately excited DC generator.

  • External Characteristic of Separately Excited DC Generator

The external characteristic of the separately excited DC generator is obtained by subtracting the drops due to ohmic

loss ( Ia Ra ) in the armature from generated voltage ( Eg ).
Terminal voltage(V) = Eg - Ia Ra. This curve gives the relation between the terminal voltage (V) and load current. The external characteristic curve lies below the internal characteristic curve. Here, AD line in the diagram below is indicating the change in terminal voltage(V) with increasing load current. It can be seen from figure that when load current increases then the terminal voltage decreases slightly. This decrease in terminal voltage can be maintained easily by increasing the field current and thus increasing the generated voltage. Therefore, we can get constant terminal voltage.

Separately excited DC generators have many advantages over self-excited DC generators. It can operate in stable condition with any field excitation and gives wide range of output voltage. The main disadvantage of these kinds of generators is that it is very expensive of providing a separate excitation source.



    4.  EMF Equation of DC Generator

The derivation of EMF equation for DC generator has two parts:
  • Induced EMF of one conductor
  • Induced EMF of the generator

One Armature Conductor

For one revolution of the conductor, Let, Φ = Flux produced by each pole in weber (Wb) and P = number of poles in the DC generator. therefore, Total flux produced by aptionall the poles



And, Time taken to complete one revolution
Where, N = speed of the armature conductor in rpm.
Induced emf of one conductor is



Derivation for Induced EMF for DC Generator

Let us suppose there are Z total numbers of conductor in a generator, and arranged in such a manner that all parallel paths are always in series. Here, Z = total numbers of conductor A = number of parallel paths Then, Z/A = number of conductors connected in series We know that induced emf in each path is same across the line Therefore, Induced emf of DC generator E = emf of one conductor × number of conductor connected in series.
Induced emf of DC generator is



Simple wave wound generator Numbers of parallel paths are only 2 = A Therefore, Induced emf for wave type of winding generator is Simple lap-wound generator Here, number of parallel paths is equal to number of conductors in one path i.e. P = A Therefore,

 Induced emf for lap-wound generator is 




5.  Self Excited DC Generators

What are Self Excited DC Generators

The small amount of magnetism is present in the rotor iron. This residual magnetic field of the main poles, induced electromotive force in the stator coils, which produces initial current in the field windings. Due to flow of small current in the coil, an increase in magnetic field occurs. As a result, voltage output increases, in turn, increases the field current. This process continues as long as the electromotive force in the armature is more than the voltage drop in the field winding. But, after at certain level, field poles get saturated, and at that point electric equilibrium is reached, and no further increase in armature emf and increase in current. The resistance of the field winding has certain fixed value, at which self-excitation can be achieved. This resistance value may vary according to electric parameters of the generator.

Types of DC Generators

DC Generators are classified on the basis of the position of the field coils and armature in the circuit and on the way of excitation.

  •  Series Wound Generators

In series wound generators, field winding and the armature winding are connected in series so that current that passes through external circuit and through field windings, passes from armature as shown in the figure below. The field coil of series wound generator has low resistance, consist of a few turns of thick wire. If the load resistance decreases, then current flow increases. As a result magnetic field and output voltage increases in the circuit. In such type generator, output voltage varies directly with respect to load current which is not required in most of the application. Due to this reason, such types of generators are rarely used.

 

  •  Shunt Wound DC Generators

In this type of generator, the field winding is wired parallel to the armature winding so that voltage is same across the circuit. Here, field winding has many numbers of turns for the desired high resistance so that fewer armatures current can pass through field winding and the reaming passes through load. So, IA = IW + IL In shunt wound generator, as they are connected parallel, current in the parallel branches are independent of each other. Hence, the output voltage almost constant and if it varies then it varies inversely with respect to load current. This is because of the voltage drop as armature
resistance increases.

Combination Wound Generator

Compound wound generator is advanced version of series wound generator and shunt wound generator. the working principle of the generator is the combination of two types so that it prevail over the disadvantages of both. It has both types of winding; series field and shunt field winding. On the basis of their connection, compound wound generators are of two types- short shunt compound generator and long shunt compound generator.

Long Shunt Compound Generator

Here the shunt field winding is connected parallel to armature only as shown in figure. Series winding is then connected in series.

  • Short Shunt Compound Generator

Here the shunt field winding is connected parallel to armature only as shown in figure. Series winding is then connected in series


6.  DC Generators Performance Curves

Performance Curve of Compound Wound DC Generator

At no load, the performance curve of this type of DC generator is same as that of shunt field generators because at no load, there is no current in the series field winding. When the load increases, then the terminal voltage drops due to the shunt DC generator,but the voltage rise in the series DC generator compensates the voltage drop. For these reason the terminal >voltage remains constant. The terminal voltage can also make higher or lower by controlling the amp-turns of the series field winding. In the diagram below, the curve FG is showing this characteristic.


7.  Applications of DC Generators

There are various types of DC generators available for several types of services. The applications of these DC generators based on their characteristic are discussed below:

  • Applications of Separately Excited DC Generators
This type of DC generators are generally more expensive than self-excited DC generators because of their requirement of separate excitation source. Because of that their applications are restricted. They are generally used where the use of self-excited generators are unsatisfactory.
1.      Because of their ability of giving wide range of voltage output, they are generally used for testing purpose in the laboratories.
2.      Separately excited generators operate in a stable condition with any variation in field excitation. Because of this property they are used as supply source of DC motors, whose speeds are to be controlled for various applications. Example- Ward Leonard Systems of speed control.

  • Applications of Shunt Wound DC Generators
The application of shunt generators is very much restricted for its dropping voltage characteristic. They are used to supply power to the apparatus situated very close to its position. These type of DC generators generally give constant terminal voltage for small distance operation with the help of field regulators from no load to full load.
1.      They are used for general lighting.
2.      They are used to charge battery because they can be made to give constant output voltage.
3.      They are used for giving the excitation to the alternators.
4.      They are also used for small power supply.
Applications of Series Wound DC Generators
These types of generators are restricted for the use of power supply because of their increasing terminal oltage characteristic with the increase in load current from no load to full load. We can clearly see this characteristic from the characteristic curve of series wound generator. They give constant current in the dropping portion of the characteristic curve. For this property they can be used as constant current source and employed for various applications.
1.      They are used for supplying field excitation current in DC locomotives for regenerative breaking.
2.      This types of generators are used as boosters to compensate the voltage drop in the feeder in various types of distribution systems such as railway service.
3.      In series arc lightening this type of generators are mainly used.

  • Applications of Compound Wound DC Generators
Among various types of DC generators, the compound wound DC generators are most widely used because of its compensating property. Depending upon number of series field turns, the cumulatively compounded generators may be over compounded, flat compounded and under compounded. We can get desired terminal voltage by compensating the drop due to armature reaction and ohmic drop in the in the line. Such generators have various applications.
1.      Cumulative compound wound generators are generally used for lighting, power supply purpose and for heavy power services because of their constant voltage property. They are mainly made over compounded.
2.      Cumulative compound wound generators are also used for driving a motor.
3.      For small distance operation, such as power supply for hotels, offices, homes and lodges, the flat compounded generators are generally used.
4.      The differential compound wound generators, because of their large demagnetization armature reaction, are used for arc welding where huge voltage drop and constant current is required.
At present time the applications of DC generators become very limited because of technical and economic reasons. Now a days the electric power is mainly generated in the form of alternating current with the help of various power electronics devices.

 Sources:
  • https://www.electrical4u.com/principle-of-dc-generator/
  • https://www.electrical4u.com/self-excited-generators/
  • https://www.electrical4u.com/emf-equation-of-dc-generator/
  • https://www.electrical4u.com/construction-of-dc-generator-yoke-pole-armature-brushes-of-dc-generator/