DC Generators MCQ Quiz - Objective Question with Answer for DC Generators - Download Free PDF

Function of the commutator in the DC machine:

• A commutator consists of a set of copper segments, fixed around the part of the circumference of the rotating machine, or the rotor, and a set of spring-loaded brushes fixed to the stationary frame of the machine.
• The main function of the commutator in the DC machine is to collect the current from the armature conductor as well as supply the current to the load using brushes. And also provides uni-directional torque for the DC motor. 
• The commutator can be built with a huge number of segments in the edge form of hard-drawn copper.
• The segments in the commutator are protected by the thin mica layer.

Concept

The generated EMF in a DC generator is given by:

\(E={NPϕ Z\over 60A} \)

where, E = EMF generated

N = Speed in RPM

P = Number of poles

ϕ = Flux per pole

Z = No. of conductors

A = No. of parallel paths

Explanation

From the above expression, we observed that the induced EMF is inversely proportional to the no. of parallel paths.

So, if the number of parallel paths (A) in a DC generator is increased, the generated EMF will decrease.

Explanation:

The application of DC Motors are as follows:

DC shunt motor

• Shunt DC motors are utilized in Centrifugal Pumps, Lifts, Weaving Machines, Lathe Machines, Blowers, Fans, Conveyors, Spinning Machines, and other applications where a consistent speed is required.
   

DC series motor 

• DC series motors are used where high starting torque is required. Major applications for DC motors are elevators, steel mills, rolling mills, locomotives, and excavators.
   

Cumulative compound DC motor

• It has high starting torque and has varying speeds within limits i.e. it has self-adjustable speed with changing load. These are used where we require sudden heavy loads for a short duration.​
• Hence, it is used for driving constant speed line shafts, lathes, constant speed head centrifugal pumps, fans woodworking machines, reciprocating pumps, etc.
   

Differentially compound DC motor

• The differential compound generators are used for arc welding purposes where a large voltage drop and constant current are required.

Applications of DC generators

Compound generator:

A compound generator is commonly used in DC welding machines because it combines the characteristics of both series and shunt generators:

• It provides a relatively stable voltage (like a shunt generator).
• It can handle sudden load changes well (like a series generator).
• This ensures a consistent arc, which is crucial for welding quality.

Shunt generator:

• Shunt generators are known for providing a relatively constant output voltage, making them suitable for several practical applications such as battery charging, electroplating and electrolysis.

Series generator:

• Used in early electric traction, arc lighting, and boosting voltage in long DC lines.

Permanent magnet generator:

• Used in wind turbines, small hydro generators, bicycles (dynamo), portable generators, engine ignition systems, and renewable energy systems for efficient, maintenance-free power generation.

Lap winding

Lap winding is a type of armature winding in which the coil terminals are connected in such a way that the number of parallel paths is equal to the number of poles.

A = P 

where, A = Number of parallel paths

P = Number of poles

Calculation

Given, P = 4 

The number of parallel paths is given by:

A = 4 

Total armature current (I_a) = 100 A

The current per parallel path is:

\(I_p={I_a\over 4}={100\over 4}\)

I_p = 25 A

• When two generators are operating in parallel, the load may be shifted from one shunt generator to another merely by adjusting the field excitation
• If generator 1 is to be shut down, the whole load can be shifted onto generator 2 provided it has the capacity to supply that load
• In that case, the field current of generator 1 gradually reduces to zero

Important Points:

For stable parallel operation, the most suitable type of DC generator is a shunt generator as it has slightly drooping characteristics. If there is any tendency for a generator to supply more or less than its proper share of load it changes system voltage which certainly opposes this tendency. This restores the original division of load. Thus the shunt generators automatically remain in parallel, once they are paralleled.

The characteristics of dc shunt generator are shown below

Fleming right-hand thumb rule:

When a conductor such as a wire attached to a circuit moves through a magnetic field, an electric current is induced in the wire due to Faraday's law of induction. 

Fleming's right-hand rule (for generators) shows the direction of induced current when a conductor attached to a circuit moves in a magnetic field.

• The thumb is pointed in the direction of the motion of the conductor relative to the magnetic field.
• The first finger is pointed in the direction of the magnetic field. (north to south)
• Then the second finger represents the direction of the induced or generated current within the conductor (from the terminal with lower electric potential to the terminal with higher electric potential, as in a voltage source)

Conclusion:

The direction of induced emf is known by Flemings right-hand thumb rule

Based on the connection of armature and field windings DC generators can be classified as:

Therefore, the machine shown in the question represents a DC long shunt compound generator.

The correct answer is option "3'.

Concept :- For differential compound generator it is positive (Poorest positive regulation among all)

• The voltage regulation of a generator is defined as the change in the voltage drop from no load to full load to full load voltage.
• Voltage regulation = (no-load voltage - full load voltage)/full load voltage
• In the case of a series generator, the field is connected in series with the armature. Any increase in load current causes an increase in the field and hence the terminal voltage rises.
• Hence it has negative voltage regulation and it has the poorest voltage regulation.

During on-load conditions, the differentially compounded DC generator has the poorest voltage regulation as shown.

During the no-load condition, the DC series generator has the poorest voltage regulation.

Key Points

•  Voltage regulation of shunt generator is positive
• For series generator, it  is negative (Poorest negative voltage regulation among all)
• For over compound generator it is negative
• For under compound it is positive
• For, flat compound generator it is zero (lowest Voltage regulation among all)
• For differential compound generator it is positive (Poorest positive regulation among all)

Concept:

The current in each parallel path \(= \frac{I}{A}\)

A is the number of parallel paths

In a wave wound generator, number of parallel paths = 2

In a lap wound generator, number of parallel paths = number of poles

Calculation:

Power (P) = 20 kW

Voltage (V) = 200 V

Total current \(I = \frac{P}{V} = \frac{{20 \times {{10}^3}}}{{200}} = 100\;A\)

Number of parallel paths = 2

Armature reaction:

The effect of armature flux (ϕa) on main field flux (ϕm) is called armature reaction.

The armature reaction mmf produces two undesirable effects on the main field flux and these are

(1) Net reduction in the main field flux per pole

(2) Distortion of the main field flux wave along the air gap periphery.

The armature mmf in a dc machine is stationary with respect to field poles but rotating with respect to armature.

• Armature reaction of unsaturated DC machine results in cross – magnetizing effect.
• Armature reaction distorts the main flux, hence the position of M.N.A. gets shifted (M.N.A. is perpendicular to the flux lines of main field flux).
• Brushes should be placed on the M.N.A., otherwise, it will lead to sparking at the surface of brushes. So, due to the armature reaction, it is hard to determine the exact position of the MNA.
• For a loaded dc generator, MNA will be shifted in the direction of the rotation.
• While for a loaded dc motor, MNA will be shifted in the direction opposite to that of the rotation.

The above figure shows the constructional details of a simple 4-pole DC machine.

Yoke:

• The outer frame of a dc machine is called a yoke.
• It is made up of cast iron or steel. In small DC machines, it is made up of cast iron and in the case of large DC machines, it is made up of cast steel.
• It not only provides mechanical strength to the whole assembly but also carries the magnetic flux produced by the field winding.

Key Points

Type of material used for the construction of the DC machine:

Concept:

The EMF equation of a DC Machine is

\({E_b} = \frac{{NPϕ Z}}{{60A}}\)

From the above equation,

\(N \propto \frac{{{E_b}}}{ϕ }\)

In a dc generator, induced emf is

Eg = V + IaRa

In a dc motor, back emf is

Eb = V – IaRa

Where,

N is the speed in rpm

ϕ is the flux per pole

P is the number of poles

Z is the number of conductors

V is the terminal voltage

Ia is the armature current

Ra is the armature resistance

Calculation:

Given-

V = 200, R_a = 0.2 Ω, I_a = 20 A, ϕ₂ = 1.1 ϕ₁

Let ϕ₁ = Generator flux, ϕ₂ = Motor flux, N₁ = Generator speed, N₂ = Motor speed 

∴ \({E_g} = 200 + 20 \times 0.2 = 204\ V\)

\(\begin{array}{l} {E_b} = 200 - 20 \times 0.2 = 196\ V\\ \frac{{{N_2}}}{{{N_1}}} = \frac{{{E_b}}}{{{E_g}}} \times \frac{{{ϕ _1}}}{{{ϕ _2}}} = \frac{{196}}{{204}} \times \frac{{{ϕ _1}}}{{1.1{ϕ _1}}} = 0.87 \end{array}\)

Given that:

DC generator wit Pole (P) = 6

Conductor = 480 (Z)

For lap winding armature resistance Ra = 0.06 Ω

When the generator is connected as lap winding then

\({R_a} = {R_{Lap}} = \frac{{Z/P}}{{m.p}} \cdot \frac{{\rho \ell }}{A} = \frac{Z}{{{P^2}}}\frac{{\rho \ell }}{A}\)        (Parallel path = m.p and m = 1)

Now, when the generator is connected as wave winding.

\({R_{wave}} = \frac{Z}{{\left( {{A_p}} \right)}} \cdot \frac{{\rho \ell }}{A}\)

In wave winding, the no. of parallel paths = A = 2

No. of conductors in each parallel path (AP) = \(\frac{Z}{2}\)

\({\left( {{R_a}} \right)_{wave}} = \frac{Z}{4}\frac{{\rho \ell }}{A}\)

\(\frac{{{{\left( {{R_a}} \right)}_{lap}}}}{{{{\left( {{R_a}} \right)}_{wave}}}} = \frac{{\left( {\frac{Z}{{{P^2}}}\frac{{\rho \ell }}{A}} \right)}}{{\left( {\frac{Z}{4} \cdot \frac{{\rho \ell }}{A}} \right)}} = \frac{4}{{{P^2}}} = \frac{4}{{{6^2}}} = \frac{1}{9}\)

⇒ (Ra)wave = 9 × (Ra)lap

= 9 × 0.06 = 0.54 Ω 

Alternate Method

 A²_lap × R_lap = A²_wave × R_wave

In lap winding A = P = 6

R_lap = 0.06 Ω

In wave winding A = 2

6² × 0.06 = 2² × Rwave

Rwave = 9 × 0.06 = 0.54 Ω 

If back emf of a dc motor vanishes suddenly, motor circuit will try to retain back emf by drawing more current from supply.

The voltage equation of dc motor is, E_b = V – I_aR_a

As the back emf vanishes zero, the whole supply voltage appears across armature and heavy current flows.