Losses & Efficiency in a Transformer, Basic Electrical Engineering, Btech first year

Losses & Efficiency in a Transformer | Btech Shots!

Losses & Efficiency in a Transformer


Losses in Transformer

Loss in any machine is when your output is lesser than the input you gave. In transformer this is loss is in terms of power. As it is a static device, there are only electrical losses in a transformer, unlike a motor which also has mechanical losses. All types of losses are:

(a) Core Losses or Iron Losses

Losses occuring in the core of the transformer. These are:

Hysteresis loss in transformer : Hysteresis loss occurs when there is reversal in the process of magnetization in the transformer core. This loss depends upon the volume and grade of the iron, value of flux density and frequency of magnetic reversals.

Eddy Current Loss in transformer : In transformer, AC current is supplied to the primary winding which sets up alternating magnetizing flux. When this flux links with secondary winding, it produces induced emf in it. But some part of this flux also gets linked with other conducting parts like steel core or iron body, which results in induced emf in those parts, resulting in small circulating currents in them. This current is called as Eddy current. Due to these eddy currents, some energy is dissipated in the form of heat causing Eddy current loss in transformer.

(b) Copper Loss

Copper loss occurs due to the resistance of the windings of the transformer. For primary winding, it is \(I_1^2R_1 \) and for secondary winding, it is \(I_2^2R_2\) where \(I_1 \) is primary current, \(R_1\) is primary winding resistance, \(I_2\) is secondary current and \(R_2\) is secondary winding resistance. As you can see, Copper loss is directly proportional to square of current and current depends on load, it implies that copper loss varies with the load connected to the transformer.


Efficiency of Transformer

Efficiency is given by ratio of output power to the input power.
Transformers are the most highly efficient electrical machines. Most of the transformers have full load efficiency between 95% to 98.5% .
As due to high efficiency, output is nearly equal to input power, so it becomes an impractical to measure efficiency using ratio of output and input. So a better way is to calculate the losses, subtract them from input and then calculate the ratio, \[ \text{Efficieny } = \frac{\text{Input - Losses}}{\text{Input}} \]

Condition for Maximum Efficiency

Input Power \( = V_1I_1\cos{\phi_1} \)
Let,
Copper Loss \( = I_1^2R_1 \)
Iron Loss \( = W_i\) \[ \text{Efficiency } = 1 - \frac{\text{Losses}}{\text{Input}} \] \[ \eta = 1 - \frac{I_1^2R_1 + + W_i}{V_1I_1\cos{\phi_1}} \] \[ \eta = 1 - \frac{I_1^2R_1}{V_1I_1\cos{\phi_1}} - \frac{W_i}{V_1I_1\cos{\phi_1}} \] Differentiating w.r.t. \(I_1\) \[ \frac{d\eta}{dI_1} = 0 - \frac{R_1}{V_1\cos{\phi_1}} + \frac{W_i}{V_1I_1^2\cos{\phi_1}} \] \(\eta\) will be maximum at \(\large\frac{d\eta}{dI_1} = 0 \)
So, \[ \frac{R_1}{V_1\cos{\phi_1}} = \frac{W_i}{V_1I_1^2\cos{\phi_1}} \] \[ \frac{I_1^2R_1}{V_1I_1^2\cos{\phi_1}} = \frac{W_i}{V_1I_1^2\cos{\phi_1}} \] \[ \boxed{I_1^2R_1 = W_i} \] Hence the efficiency of the transformer will be maximum when copper loss is equal to the iron loss.




Ideal & Practical Transformer, Basic Electrical Engineering, Btech first year

Ideal & Practical Transformer | Btech Shots!

Ideal & Practical Transformer


Ideal Transformer

A ideal transformer is an imaginary transformer which has:

  • -> no copper losses
  • -> no iron loss in the core
  • -> no leakage flux

More on losses Here
In ideal transformer, input power = output power. Concept of such transformer exists to make problems easier.


Characteristics of Ideal Transformer

Zero Winding Resistance : Resistance of both primary and secondary winding is 0 i.e. both the coils are purely inductive in nature.

100% Efficiency : There are no losses in ideal transformer so the input power = output power \(\Rightarrow E_1I_1 = E_2I_2 \)

No leakage flux : The whole amount of flux is linked from primary to secondary winding, so there is no leakage flux.

No Iron loss : As the iron core is subjected to alternating flux there occurs eddy current and hysteresis loss in it. These two losses together are called Iron loss. It is 0 in ideal transformer.

When an alternating voltage V1 is supplied to the primary winding of an ideal transformer, counter emf E1 is induced in the primary winding. Since there is no resistance, this induced emf E1 will be exactly equal to the applied voltage but in 180 degree opposite in phase.
The current drawn from the source produces required magnetic flux. As the primary winding resistance is 0, the current lags emf E1 by 90 degree. This is current is called Magnetizing current Iμ. This magnetizing current produces alternating magnetic flux φ. This flux gets linked with the secondary winding and emf E2 is induced by mutual induction. This E2 is in phase with E1. If the circuit is closed at secondary winding, then secondary current I2 is produced. \[ E_1I_1 = E_2I_2 \]

transformer, basic electrical engineering, btech first year

Practical Transformer

In practical transformer, we have all sorts of losses that were 0 in ideal transformer like winding reistance, leakage flux, and iron losses, all are there.
Here we are gonna study two cases:
(a) No load
(b) On load

Practical Transformer on No Load

In no load transformer, the circuit on the secondary side is open.

no load transformer, basic electrical engineering, btech first year

V1 is the primary voltage and I1 is the primary current. Now I1 has two components:
a) One component is responsible for generation of magnetic flux. This is called Magnetizing component of I1 and is denoted by Iμ
b) Second component which is responsible for magnetic losses (Hysterisis and Eddy current losses) and primary winding losses. This is called Core loss component of Ic .
So its equivalent circuit diagram is:

no load transformer, basic electrical engineering, btech first year


where on primary side,

  • V1 is Primary Voltage
  • R1 is Primary Winding Resistance
  • X1 is Primary Leakage Reactance
  • I0 is No Load Primary Current
  • Ic is Core Loss component of I1
  • Iμ is Magnetizing Component of I1
  • Rc is Core loss resistance
  • Xm is Magnetizing Reactance
  • N1 is Number of turns in Primary Winding
  • E1 is Primary induced Emf

  • On secondary side:
  • R2 is Secondary winding resistance
  • X2 is Secondary leakage reactance
  • N2 is Secondary winding turns
  • E2 is Secondary induced emf
  • V2 is Secondary terminal voltage


Phasor Diagram
no load transformer, basic electrical engineering, btech first year
Explanation

First we will start with reference line which is common to both primary and secondary curcuit, here it is flux φ. Now using KVL in primary circuit
\( V_1 = -E_1 + I_0R_1 + jI_0X_1 \)
There is no direct relation between φ and V1 so that we could directly draw phasor. But we have relation with E1 and φ, as φ is responsible for both E1 and E2. E1 and E2 both lag φ by 90 degrees. Here we will consider E1 < E2.
φ is produced due to magnetizing current Iμ therefore Iμ is in phase with φ. As we have -E1 in our equation (because it is in opposite direction of magnetizing current) so we will draw a phasor opposite to E1.
Ic is 90 degrees leading from Iμ so it is in phase with -E1 As I0 = Ic + Iμ , hence the phasor I0.
Now I0R1 is voltage drop in R1 and it is in phase with I0 , and as it is added to -E1 so the phasor of I0R1 will be drawn at the head of -E1. I0X1 is voltage drop across X1 and is 90 degrees leading I0R1, so it is drawn perpendicular to I0R1.
Now following the equation, V1 phasor is drawn adding all the quantities given in the equation.


Practical Transformer on Load

The secondary side is closed-circuited with a load.

practical transformer, transformer on load, basic electrical engineering, btech first year

Its equivalent circuit diagram:

practical transformer, transformer on load, basic electrical engineering, btech first year

where on primary side,

  • V1 is Primary Voltage
  • I1 is Primary Current
  • I'2 is Primary Current to neutralize the demagnitizing effects of I2, I'2 = K I2
  • I0 is No Load Primary Current
  • R1 is Primary Winding Resistance
  • X1 is Primary Leakage Reactance
  • Ic is Core Loss component of I1
  • Iμ is Magnetizing Component of I1
  • I'1 component of I1 (doubtful)
  • Rc is Core loss resistance
  • Xm is Magnetizing Reactance
  • N1 is Number of turns in Primary Winding
  • E1 is Primary induced Emf

  • On secondary side,
  • R2 is Secondary winding resistance
  • X2 is Secondary leakage reactance
  • N2 is Secondary winding turns
  • E2 is Secondary induced emf
  • V2 is Secondary voltage
  • I2 is Secondary current

Phasor Diagram
transformer on load, practical transformer, basic electrical engineering, btech first year
Explanation

Again we will start with refrence line, here it is φ.
Using KVL in secondary circuit,
\( V_2 = E_2 - I_2R_2 - jI_2X_2 \)
As there is no direct relation between V1 and φ so we will use the equation to draw all three quantities and then add them to get V1.
E2 and E1 lag φ by 90 degrees. Here we will consider E2 < E1. I2 lags E2 by phase difference of φ2
Now voltage drop I2R2 across R2 will be in phase with I2 but we need -I2R2 so we will it in opposite direction of I2. As it is to be added to E2 so it will be drawn at the head of E2.
I2X2 is voltage drop across X2 and is leading by 90 degrees from I2R2. Again it is -ve in magnitude.
Adding all the quantities we have V2.
Now in primary circuit,
V1 = - E1 + I1R1 + jI1X1
I1 = I'2 + I0 where I'2 = -KI2
I0 = Iμ + Ic
Again we will draw Iμ first as it is directly connected to φ, then Ic and then I0 .
I'2 is opposite to I2 and is added to I0. The resultant phasor is I1.
I1R1 is in phase with I1 and is added to -E1. I1X1 is 90 degrees leading I1R1.
Phase difference between V1 and I1 is φ1
Power Factor = cosφ1
Input Power = V1I1cosφ1

Phase difference between V2 and I2 is φ2
Power Factor = cosφ2
Input Power = V2I2cosφ2




Equivalent Circuit of Transformer, Basic Electrical Engineering, Btech first year

Equivalent Circuit of Transformer | Btech Shots!

Equivalent Circuit of Transformer


The concept of Equivalent Circuits exists to help us analyze transformer as by using this concept, we can transform all the parameters to either side. When referred to primary side, it is called Equivalent Circuit referred to primary side and when referred to secondary side, it is called Equivalent Circuit referred to secondary side.

transformer, basic electrical engineering, btech first year

Here \( I_1 = I_0 + I'_2 \)
The no load primary current \(I_0\) is very small in comparison to full load current around 2% to 5% of full load current. So, \[ I_1 \approx I'_2 \] So we will interchange the core loss and leakage flux loss part with the winding losses part as shown in the diagram. This is called Approximate Equivalent Circuit.

transformer, basic electrical engineering, btech first year

The core losses and flux losses are negligible, so we will remove them to further simply the circuit,

transformer, basic electrical engineering, btech first year

Now we can perform calculations:

Equivalent Circuit referred to Primary Side

This means shifting all the elements to the primary side.

transformer, basic electrical engineering, btech first year

\(R_{1e} \) is Equivalent resistance referred to primary
\(X_{1e} \) is Equivalent reactance referred to primary
Before we get into equations for equivalent resistance and reactance, get this formula for relation between resistance and turn ratio: \[ V_1 = I_1R_1 , V_2 = I_2R_2\] \[ \frac{V_1}{V_2} = \frac{I_1R_1}{I_2R_2} \] \[ \frac{R_1}{R_2} = \frac{V_1I_2}{V_2I_1} = \frac{N_1}{N_2}\frac{N_1}{N_2} \] \[ \frac{R_1}{R_2} = \left(\frac{N_1}{N_2} \right)^2 \] So if \(R_2\) is to be referred from secondary to primary side, then it will be written as \[ R_2\left(\frac{N_1}{N_2}\right)^2 \] And if \(R_1\) is to be referred from primary to secondary side, then it will be written as \[ R_1\left(\frac{N_2}{N_1}\right)^2 \] So writing equations for equivalent resistance and reactance, \[ R_{1e} = R_1 + R_2\left(\frac{N_1}{N_2} \right)^2 \] \[ X_{1e} = X_1 + X_2\left(\frac{N_1}{N_2} \right)^2 \]

Equivalent Circuit referred to Secondary Side

This means shifting all the elements to the secondary side.

transformer, basic electrical engineering, btech first year

\(R_{2e} \) is Equivalent resistance referred to secondary
\(X_{2e} \) is Equivalent reactance referred to secondary
\[ R_{2e} = R_2 + R_1\left(\frac{N_2}{N_1} \right)^2 \] \[ X_{2e} = X_2 + X_1\left(\frac{N_2}{N_1} \right)^2 \]




Auto Transformer, Basic Electrical Engineering, Btech first year

Auto Transformer | Btech Shots!

Auto Transformer


Auto Transformer is a transformer in which both primary and secondary side share same single winding i.e. one single winding is used as primary winding as well as secondary winding.

auto transformer, basic electrical engineering, btech first year

Here bc is called the common winding as it is shared by both primary and secondary sides. ab is called the series winding as it is in series with common winding.

Step Down Auto Transformer
auto transformer, basic electrical engineering, btech first year

Here \( V_H =\) High Voltage
\( V_L =\) Low Voltage
\( I_H =\) High Voltage Current
\( I_L =\) Low Voltage Current
\( T_{ac} =\) number of turns across ac
\( T_H =\) number of turns across high voltage side \(= T_{ac} \)
\( T_{bc} =\) number of turns across bc
\( T_L =\) number of turns across low voltage side \(= T_{bc} \)
\(T_{ab} =\) number of turns across ab
\( T_{ab} = T_H - T_L \) Also, \( I_H = I_{ab} \)
And when load is connected, \(I = I_{cb} \) Now in auto transformer, we study two types of ratios: Circuit Voltage Ratio (CVR) and Winding Voltage Ratio (WVR).
CVR is the ratio of voltages in primary and secondary circuits \[ CVR = \frac{V_H}{V_L} = \frac{T_H}{T_L} = a_A \Rightarrow \text{ Transformation Ratio } \longrightarrow (1) \] WVR is the ratio voltages in the windings of the primary and secondary sides \[ WVR = \frac{V_{ab}}{V_{bc}} = a \] I flows only when load is connected and flows in opposite direction of IH. So the flux produced by I tries to reduce the flux produced by IH but the value of flux by IH is such that it nullifies the effect of flux by I. So the mmf by IH becomes equal to the mmf by I. \[ I_{ab}T_{ab} = I_{bc}T_{bc} \] \[ I_H(T_H - T_L) = IT_L \] \[ \boxed{\frac{I}{I_H} = \frac{T_H - T_L}{T_L} = \frac{T_H}{T_L} - 1 = a_A - 1 } \longrightarrow (2) \] WVR: \[ a = \frac{V_{ab}}{V_{bc}} = \frac{T_{ab}}{T_{bc}} = \frac{T_H - T_L}{T_L} = \frac{T_H}{T_L} - 1 \] \[ \boxed{a = a_A - 1 } \longrightarrow (3) \] Applying KCL at point b \[ I_H + I = I_L \] \[ I = I_L - I_H \] \[ \frac{I}{I_H} = \frac{I_L - I_H}{I_H} \longrightarrow (4) \] From equation (2) \[ a_A - 1 = \frac{I_L - I_H}{I_H} \] \[ \boxed{a_A = \frac{I_L}{I_H} } \] \[ \Rightarrow \boxed{a_A = \frac{V_H}{V_L} = \frac{T_H}{T_L} = \frac{I_L}{I_H}} \] \[ \text{And } \boxed{a = a_A - 1} \]

Step Up Auto Transformer
auto transformer, basic electrical engineering, btech first year

All the calculations are same as in step down transformer, just the directions of currents change.


Saving in Conductor Material

As auto transformer uses single winding, it uses less matrial i.e. Copper in comparison to two winding transformers. To determine saving of Copper, we calculate weight of copper used.

Now the weight of copper used depends upon :

Current : because the flow of current depends upon the area of cross section of the turns of the winding. So larger the current means larger the area which in turn means more amount of Copper used

Number of Turns : larger the number of turns means more amount of Copper used.

auto transformer, basic electrical engineering, btech first year

For two winding transformer,
Weight of primary winding \( \propto N_1I_1 \)
Weight of secondary winding \( \propto N_2I_2 \)
Total Weight of Copper used \( \propto N_1I_1 + N_2I_2 \)
Weight of Copper in auto transformer \(\propto (N_1 - N_2)I_1 + N_2(I_2 - I_1) \) \[ \frac{\text{Weight of Copper in auto transformer}}{\text{Weight of Copper in ordinary transformer}} \] \[ = \frac{(N_1 - N_2)I_1 + N_2(I_2 - I_1)}{N_1I_1 + N_2I_2} \] \[ = \frac{N_1I_1 - N_2I_1 + N_2I_2 - N_2I_1}{N_1I_1 + N_2I_2} \] \[ = \frac{N_1I_1 - 2N_2I_1 + N_2I_2}{N_1I_1 + N_2I_2} \] As \(N_1I_1 = N_2I_2 \) \[ = \frac{2N_2I_2 - 2N_2I_1}{2N_2I_2} \] \[ = 1 - \frac{I_1}{I_2} \] \[ = \boxed{1 - K} \] \[\Rightarrow \text{Weight of copper in ordinary transformer} = (1 - K)\times\text{Weight of copper in auto transformer} \] So, Saving of Copper = Weight of copper in ordinary transformer - Weight of copper in auto transformer \[ = W_0 - (1 - K)W_0 \] \[ = W_0 - W_0 + KW_0 \] \[ \boxed{\text{Saving of Copper } = KW_0} \] When \(K \approx 1 \) saving is maximum


Advantages and Disdvantages

Due to single winding, it has lot of advantages when compared with 2 winding transformer and some disadvantages as well.

Advantages

a) In 2 winding transformer, transfer of energy occurs with the help of mutual induction only, but in auto transformer, due to single winding, energy transfer occurs through mutual induction as well as conduction of current.

b) Due to single winding, less material is used.

c) Due to single winding, leakage flux is very low.

d) Due to single winding, secondary winding resistance is very low.

e) It is of small size when compared to 2 winding transformer.


Disdvantages

a) If by mistake, the secondary side is open i.e. not connected to the winding, then all the high voltage will be transferred to the load, thus damaging the load.

b) Due to low impedance, an increase in short circuit current will damage the load.


Applications

a) In large power systems

b) In laborateries as variable transformer

c) Synchronous motor and induction motor are not self-starting, so it is used as a starter.





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