DC Motor, Basic Electrical Engineering, Btech first year

DC Motor | Btech Shots!

DC Motor


Working Principle

The principle on which DC Motor works is:

"When a current carrying conductor is placed in a magnetic field, it experiences a mechanical force"

The construction of both DC Generator and Motor is same, the only difference is here we provide energy to the machine. As we excite the armature, the conductors of the armature, placed in magnetic field, experience a mechanical force and the motor starts moving. The direction of rotation is given by Fleming Left Hand Rule.

"Outstretch three fingers of left hand namely first finger, middle finger and thumb such that they are mutually perpendicular to each other. If we point first finger in direction of magnetic field and middle finger in direction of current, then the thumb gives direction of force experienced by the conductor."


Back EMF

Once motor starts rotating its conductor will cut magnetic flux produced by field winding, so by Faraday's Law of Electromagnetic Induction there will be induced emf just like in case of emf induced in dc generator. This emf is called Back emf. \[ \boxed{E_b = \frac{\phi PNZ}{60A} } \] The role of back emf in starting and running of the motor is important. The presence of back emf makes the DC Motor a self-regulating machine i.e. it makes the dc motor to draw as much armature current as is sufficient to develop the required load torque.

dc motor, dc machines, basic electrical engineering, btech first year

\[ V_t = I_aR_a + E_b + V_{brush} \] Vt is the supply voltage and it has to take care of all the three factors.


Torque Equation of DC Motor

      Mechanical Power = Torque × Angular Velocity
\[ P = T \times \omega \] \[ E_bI_a = T \times \frac{2\pi N}{60} \] \[ \frac{\cancel{N}P\phi Z}{\cancel{60}A} \times I_a = T \times \frac{2\pi \cancel{N}}{\cancel{60}} \] \[ \boxed{T = \frac{1}{2\pi}\phi I_a \frac{PZ}{A} } \] \[ \boxed{T = 0.159 \phi I_a \frac{PZ}{A} } \] The unit is Newton-meter (Nm).


Types of DC Motor

There are three types of motors:

1) Series Motor
2) Shunt Motor
3) Compound Motor : Of 2 types
      a) Long Shunt Compound Motor
      b) Short Shunt Compound Motor

The construction of all these types are similar to dc generator.


DC Series Motor
dc motor, dc machines, basic electrical engineering, btech first year

\[ I_L = I_{se} = I_a \] \[ E_b + I_aR_a + I_{se}R_{se} - V_t = 0 \] \[ E_b + I_aR_a + I_aR_{se} - V_t = 0 \] \[ E_b + I_a(R_a + R_{Se}) - V_t = 0 \] \[ \boxed{V_t = E_b + T_a(R_a + R_{se}) + V_{brush} } \]


DC Shunt Motor
dc motor, dc machines, basic electrical engineering, btech first year

\[ I_L = I_{sh} + I_a \] \[ E_b + I_aR_a - V_t = 0 \] \[ \boxed{V_t = E_b + I_aR_a } \] \[ \boxed{I_{sh} = \frac{V_t}{R_{sh}} = \frac{E_b + I_aR_a}{R_{sh}} } \]


Compound DC Motor
Long Shunt
dc motor, dc machines, basic electrical engineering, btech first year

\[ I_L = I_{se} + I_{sh} \] Or \[ I_L = I_a + I_{sh} \] \[ E_b + I_aR_a + I_{se}R_{se} - V_t = 0 \] \[ \boxed{V_t = E_b + I_aR_a + I_{se}R_{se} } \] \[ \boxed{I_{sh} = \frac{V_t}{R_{sh}} = \frac{E_b + I_a(R_a + R_{se})}{R_{sh}} } \]


Short Shunt
dc motor, dc machines, basic electrical engineering, btech first year

\[ I_L = I_{se} \] \[ I_L = I_{se} = I_a + I_{sh} \] \[ E_b + I_aR_a + I_{se}R_{se} - V_t = 0 \] \[ \boxed{V_t = E_b + I_aR_a + I_{se}R_{se} } \] \[ \boxed{I_{sh} = \frac{V_t}{R_{sh}} = \frac{E_b + I_aR_a + I_{se}R_{se}}{R_{sh}} } \]





DC Generator, Basic Electrical Engineering, Btech first year

DC Generator | Btech Shots!

DC Generator


Principle of Operation

Basically, the principle of DC Generator is based on dynamically induced emf i.e. Faraday's Law of Electromagnetic Induction. This law states that :

"Whenever the magnetic flux linking with a conductor changes, an Electromagnetic Force (EMF) is set up in that conductor."

\[ \text{Dynamically induced emf }, e = \frac{d\phi}{dt} \] The direction of flux is given by Right Hand Thumb Rule which states that "if the thumb of the right hand represents direction of current then direction of the curled fingers represent direction of flux".

Now the question arise, how do we change the flux? The answer is relative motion between the conductor and the flux. So there are two ways to do that:

1) Keep the conductor stationary and move the flux
2) Keep the flux stationary and move the conductor

In DC generator, we keep the flux stationary and move the conductor. The device that moves this conductor is called Prime Mover. Some examples of Prime Mover are: diesel engine, diesel turbine, steam turbine etc.

Now the next question arises, what is the direction of this induced emf? For that we have Fleming's Right Hand Rule:

"If the three fingers of right hand, namely thumb, index finger and middle finger are outstretched so that each one of them is at right angles with the remaining two and if in this position the index finger is made to point in the direction of flux, thumb in the direction of the relative motion of conductor w.r.t. flux then the outstretched middle finger gives the direction of induced emf in the conductor"

While in DC Motors, the rule used is Fleming's Left Hand Rule (not right hand rule).

The emf induced is alternating in nature. So the question arises: if the induced emf is alternating, how is it a DC Generator? The answer is a rectifier called as Commutator. This device is not electronic, instead its entirely mechanical.

"Commutator is a device used in DC Generator to convert alternating induced emf to unidirectional DC emf"

Construction

The construction remains same for both generator and motor.

dc generator, dc machines, basic electrical engineering, btech first year

Yoke : It is the outermost protective cover of the machine. It protects all the components from dust, moisture etc. It serves as a mechanical support to the parts. It also provides low reluctance path for the flux, so its made up of Cast Iron as it is a magnetic material.

Pole : The pole has two parts:

dc generator, dc machines, basic electrical engineering, btech first year

     Pole Core : It carries field windings which are responsible for production of magnetic flux.
     Pole Shoe : It covers the maximum armature conductor to cut flux so that we have maximum induced emf.
As flux passes through it, it should provide a low reluctance path so it is made up of Cast Iron.

Field Winding : It is the coil or wire that carries the current which is responsible for the production of flux. It is made up of Copper.

Armature : That part where the emf is induced. It is made up of Cast Iron.
  Armature Conductor : That part which takes the voltage or current out of armature to the commutator

Commutator : That part which rectifies AC emf to DC.

Brushes : It takes out the voltage or current from the Commutator to the terminals. It is made up of Carbon.


Emf Equation of DC Generator

Before we derive the emf equation, let's define some terms:
Let P = number of poles in the generator
φ = flux produced by each pole
N = speed of armature of generator (in rpm)
Z = total number of conductors in armature
A = number of parallel paths in which armature conductors are distributed
So by Faraday's Law of Electromagnetic Induction:
      e = Rate of cutting of the flux
\[ e = \frac{d\phi}{dt} \]     Total flux = Flux produced by each pole × number of poles
    So, total flux = φ × P
    Time required to complete one revolution = 60/N
\[ e = \frac{\phi P}{\large\frac{60}{N}} \] \[ e = \frac{\phi PN}{60} \] This emf is for one conductor
As Z conductors are distributed in A parallel paths, effective number of conductors will be Z/A, so \[ E = \frac{\phi PN}{60}\times\frac{Z}{A} \] \[ \boxed{E = \frac{\phi PNZ}{60A} } \]


Types of Generators

On the basis of Excitation of field winding, there are two types of generators:
1) Seperately Excited Generator
2) Self Excited DC Generator


Seperately Excited Generator

A DC Generator whose field winding or coil is energised by a seperate or external DC source is called a seperately excited DC Generator.

dc generator, dc machines, basic electrical engineering, btech first year
Self Excited Generator

Self-excited generators are the generators which get excited with the initial current in the field coils.

What actually happens is: there is a small amount of magnetism present in the rotor iron. This residual magnetic field of the main poles, induces an emf 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,which in turn, increases the field current. This process continues as long as the emf 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 takes place.

Based on the connection of field winding to the armature, there are 3 types of generator

1) Series Generator
2) Shunt (Parallel) Generator
3) Compound Generator : Of 2 types
      a) Long Shunt Compound Motor
      b) Short Shunt Compound Motor


Series Wound Generator

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.

The field coil of series-wound generator has low resistance, and consists of a few turns of thick wire. If the load resistance decreases, then the current flow increases. As a result magnetic field and output voltage increases in the circuit. In such generators, output voltage varies directly with respect to load current which is not required in most of the applications. Due to this, it is not used a lot.

dc generator, dc machines, basic electrical engineering, btech first year

\[ I_{se} = I_a = I_L \]
Applying KVL we get, \[ E_g - I_aR_A - I_{se}R_{se} - V_t = 0 \] \[ E_g = V_t + I_aR_A + I_{se}R_{se} + V_{brush} \] \[ \boxed{E_g = V_t + I_a(R_a + R_{se}) + V_{brush}} \] where IaRa is Armature resistance drop, Eb is back emf and Vbrush is brush resistance drop


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 armature current can pass through the field winding and the remaining passes through load.

In shunt wound generator, the output voltage is almost constant and if it varies then it varies inversely with respect to load current.

dc generator, dc machines, basic electrical engineering, btech first year

\[ I_a = I_{sh} + I_L \] \[ E_g - T_aR_a - V_t = 0 \] \[ \boxed{E_g = V_t + I_aR_a + V_{brush} } \] \[ \boxed{I_{sh} = \frac{V_t}{R_{sh}} = \frac{E_g - I_aR_a}{R_{sh}} } \]


Compound Generator

Compound Wound Generator is the best of both worlds i.e. series and shunt wound generators. On the basis of their connection they are of two types:

1) Long Shunt Compound Generator
2) Short Shunt Compound Generator


Long Shunt Compound Generator

The connection is made as shown in the diagram:

dc generator, dc machines, basic electrical engineering, btech first year

\[ I_{se} = I_a = I_{sh} = I_L \] \[ E_g = V_t + I_aR_a + I_{se}R_{se} + V_{brush} \] \[ = V_t + I_aR_a + I_{a}R_{se} + V_{brush} \] \[ \boxed{E_g = V_t + I_a(R_a + R_{se}) + V_{brush} } \] \[ \boxed{I_{sh} = \frac{V_t}{R_{sh}} = \frac{E_g - I_a(R_a + R_{se})}{R_{sh}} } \]


Short Shunt Compound Generator

The connection is made as shown in the diagram:

dc generator, dc machines, basic electrical engineering, btech first year

\[ I_{se} = I_L \] \[ I_a = I_{sh} + I_{se} \] \[ E_g - I_aR_a - I_{se}R_{se} - V_t = 0 \] \[ \boxed{E_g = V_t + I_aR_a + I_{se}R_{se} + V_{brush} } \] \[ \boxed{I_{sh} = \frac{V_t}{R_{sh}} = \frac{E_g - I_aR_a - I_{se}R_{se}}{R_{sh}} } \]





3 Phase Induction Motor, Basic Electrical Engineering, Btech first year

3 Phase Induction Motor | Btech Shots!

3 Phase Induction Motor


Construction

To understand its principle we need to know its construction. It has mainly two parts:

1) Stator
2) Rotor

3 phase induction motor, basic electrical engineering, btech first year
Stator

It is the stationary part of the machine. It ha windings called Stator winding. 3-phase supply is provided to these windings. It also provides mechanical strength to the machine.

Rotor

It is a rotatory part of Induction motor. It has windings called Rotor winding. The conductors are placed on the periphery of the rotor.


On the basis of applications of Induction Motor they are of two types:

1) Slip Ring or Wound Rotor
2) Squirrel Cage Rotor


Squirrel Cage Rotor
3 phase induction motor, basic electrical engineering, btech first year

Squirrel Cage Rotors are used where constant speed is required. In this type, both the end rings are permanently short-circuited. The conductors made up of Aluminium and Copper are placed between the end rings hence these are also short-circuited.
Hence the overall resistance of the rotor is constant and is used for the constant speed application. Example: Elevators.


Slip Ring or Wound Rotor
3 phase induction motor, basic electrical engineering, btech first year

This type of rotor construction is used where high starting torque is required.
In this type of rotor, Aluminium and Copper conductors are connected with the external Rheostat so that by varying resistance, the overall resistance of the rotor can be varied.


Working Principle

When 3 phase supply is given to the stator winding, a rotating magnetic field with speed called as Synchronous Speed (Ns) is generated. It rotates in clockwise direction.

As the magnetic field is rotating and the conductors are stationary, due to relative motion between magnetic flux and conductor, magnetic field gets cut and an emf is induced. Hence current starts flowing in rotor winidng.

Now as the conductors are current carrying and is placed in magnetic field, a torque is exerted on the rotor and the rotor starts to rotate in clockwise direction with a speed called as rotor speed.


Let's define some basic terms that we use with induction motor.


Slip Speed

It is the difference between Synchronous speed and rotor speed. \[ \text{Slip Speed } = N_S - N_R \]

Slip

It is defined as the ratio of Slip Speed to the Synchronous speed. \[ S = \frac{N_S - N_R}{N_S} \]
1) When the motor is standing still \[ N_R = 0 \Rightarrow \boxed{S = 1} \] 2) at NR = NS \[ \boxed{S = 0} \]


Applications

Induction motor is used in fans, vaccum cleaners, washing machines, centrifugal pumps etc.





Electrical Machines, Basic Electrical Engineering, Btech first year

Electrical Machines | Btech Shots!

Electrical Machines


Topics that we are going to study in this unit:

Principle of Transformer & its emf equation, Basic Electrical Engineering, Btech first year

Principle & Emf Equation of Transformer | Btech Shots!

Principle & Emf Equation of Transformer


Transformer is a device that is used to transfer electrical energy from one circuit to another using the phenomena of Mututal Induction. Keeping the energy conserved (it does not generate energy), it is used to increase or decrease voltage.

Working Principle

A basic transformer consists of two coils (or windings), one coil is connected to power supply. This power supply is alternating in nature (transformers don't work on dc). The alternating current passed through the coil generates flux which is also alternating in nature. Some part of this flux links with the second coil. As it is continuously changing, there must be a changing flux linkage in the second coil due to Mututal Induction. This changing flux in the second coil generates emf in the coil.

Primary Winding

The winding to which energy is supplied and generates flux to be transferred to second coil is called Primary Winding.

Secondary Winding

The winding in which emf is induced due to the flux transferred from the primary winding is called Secondary Winding. This gives us the desired output voltage.

transformer, basic electrical engineering, btech first year

However, this isn't how the transformers are built because a lot of flux does not get linked with the secondary winding and it gets wasted. In real transformer, this wastage of flux should be as minimum as possible, for that purpose core is used.

Core

The core provides a low reluctance path, through which maximum amount of flux generated by primary winding is passed and linked with the secondary winding.


So basically the transformer consists of 3 main parts: Primary Winding, Core and Secondary Winding.

transformer, basic electrical engineering, btech first year

Emf Equation

Let the primary winding of the transformer is connected to power supply. As a result of which flux \(\phi \) is generated in the primary winding. This flux is alternating in nature therefore, \[ \phi = \phi _m\sin{\omega t} \]

transformer, basic electrical engineering, btech first year

By Faraday's Law of Electromagnetic Induction and Lenz's Law: \[ e = -N \frac{d\phi}{dt} \] Emf induced at primary side: \[ e_1 = N_1 \frac{d\phi}{dt} \] where \(N_1\) is number of turns in primary winding \[ \Rightarrow e_1 = -N_1\frac{d(\phi_m \sin{\omega t})}{dt} \] \[ e_1 = -N_1\omega \phi_m \cos{\omega t} \] \[ e_1 = N_1\omega \phi_m (-\cos{\omega t}) \] \[ -\cos{\omega t} = \sin{(\theta - 90^o)} ,\hspace{20pt} \omega = 2\pi f \] \[ e_1 = \phi_m 2\pi fN_1 \sin{(\omega t -90^o)} \] Comparing with standard equation of emf \[ e_1 = E_{m1}\sin{(\omega t + \psi)} \] \[ E_{m1} = 2\pi f \phi_m N_1, \hspace{15pt} \psi = -90^o \] RMS value of emf = \(\frac{E_{m1}}{\sqrt{2}} \) \[ = \frac{2\pi f \phi_m N_1}{\sqrt{2}} \] \[ \boxed{E_1 = 4.44 \phi_m f N_1 } \] Similarly secondary side emf: \[ \boxed{E_2 = 4.44 \phi_m f N_2 } \] As \(\psi = -90^o \Rightarrow E_1 \text{ and } E_2 \) lag flux \(\phi \) by 90o

Phasor Diagram
transformer, basic electrical engineering, btech first year
Ratios in a Transformer

\[ E_1 = 4.44 \phi_m f N_1 \] \[ E_2 = 4.44 \phi_m f N_2 \] \[ \frac{E_1}{E_2} = \frac{4.44 \phi_m f N_1}{4.44 \phi_m f N_2} \] \[ \boxed{\frac{E_1}{E_2} = \frac{N_1}{N_2} } \] If we neglect resistance and leakage reactance \[ E_1 \approx V_1 \text{ & } E_2 \approx V_2 \] \[ \boxed{\frac{E_2}{E_1} = \frac{V_2}{V_1} = \frac{N_2}{N_1} = K \text{ (Turns ratio)} } \] It is also called as Voltage Ratio

Primary side power = Secondary side power \[ \Rightarrow V_1I_1 = V_2I_2 \] \[ \frac{V_2}{V_1} = \frac{I_1}{I_2} \] \[ \boxed{\frac{V_2}{V_1} = \frac{I_1}{I_2} = \frac{N_2}{N_1} = K } \] It is called as current ratio


Step Up & Step Down Transformer

In Step Up Transformer, voltage on the secondary side is greater than voltage on the primary side \[ V_2 > V_1 \] \[ \Rightarrow K > 1 \] \[ \Rightarrow I_1 > I_2 \] In Step Down Transformer, voltage on the primary side is greater than voltage on the secondary side \[ V_1 > V_2 \] \[ \Rightarrow K \lt 1 \] \[ \Rightarrow I_2 > I_1 \]




DC Motor, Basic Electrical Engineering, Btech first year

DC Motor | Btech Shots! DC Motor ...