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Magnetization Current in a Real transformer

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Magnetization Current in a Real transformer. Although the output of the transformer is open circuit, there will still be current flow in the primary windings Magnetization current, i M Core-loss current, i h+e. The relation between current and flux is proportional since. - PowerPoint PPT Presentation

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Magnetization Current in a Real transformer

Although the output of the transformer is open circuit, there will still be current flow in the primary windings

• Magnetization current, iM • Core-loss current, ih+e

The relation between current and flux is proportional since F Ni R

Ri

N

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Magnetization Current in a Real transformer

Therefore, in theory, if the flux produce in core is sinusoidal, therefore the current should also be a perfect sinusoidal. Unfortunately, this is not true

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Magnetization Current in a Real transformer

current in a transformer has the following characteristics:

• It is not sinusoidal but a combination of high frequency oscillation

• The current lags the voltage at 90o• At saturation, the high frequency components will be extreme

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Magnetization Current in a Real transformer

Core-loss current:

• Eddy current loss> Eddy current is dependent upon the rate of change of flux• Hysteresis loss > a non linear loss

At no-load, the primary windings is known as the excitation current

ex m h ei i i

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Magnetization Current in a Real transformer

The equivalent circuit of a transformer

Taking into account real transformer, there are several losses that has to be taken into account in order to accurately model the transformer, namely:

1- Copper (I2R) Losses 2- Eddy current Losses 3- Hysteresis Losses 4- Leakage flux

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Equivalent Circuit a) referred to primary side b) referred to secondary side

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Approximate equivalent circuit

Approximate equivalent circuit c) Referred to primary side (no exicitation) d) Referred to secondary side (no excitation).

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Example 3

A not-quite-ideal transformer having 90 turns on the primary and 2250 turns on the secondary is connected to a 120 V, 60 hz source. The coupling between the primary and the secondary is perfect but the magnetizing current is 4 A. calculate:

a. The effective voltage across the secondary terminalsb. The peak voltage across the secondary terminals.c. The instantaneous voltage across the secondary when the

instantaneous voltage across the primary is 37 V.

Ans: 3000V, 4242 V, 925 V.

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Example 4

An ideal transformer having 90 turns on the primary and 2250 turns on the secondary is connected to a 200 V, 50 Hz source. The load across the secondary draws a current of 2 A at a power factor of 80 per cent lagging. Calculate :

a. The effective value of the primary currentb. The instantaneous current in the primary when the

instantaneous current in the secondary is 100 mA.c. The peak flux linked by the secondary winding.

Ans: 50 A, 2.5 A, 10 mWb.

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Example 5

Calculate voltage E and current I in the circuit of Fig. shown below, knowing that the ideal transformer T has a primary to secondary turns ratio of 1;100.

Ans: 800 V, 2 A.

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Determination of transformer parameters: Open Circuit Test

Total excitation admittance, YE = GC - jBMMC X

jR

11

The magnitude of the excitation admittance (referred to primary),

OC

OCE V

IY

The angle of the admittance ,from the circuit power factor.

OCOC

OC

IV

P1cos

The power factor is always lagging for a real transformer. Hence,

OC

OCE V

IY MC

EE jXR

YZ

1Hence

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Determination of transformer parameters: Short Circuit Test

• Magnitude of series impedance:

• Power factor:

SC

SCSE I

VZ

SCSC

SC

IV

PPF cos

000

00

SC

SC

SC

SCSE

I

V

I

VZ

)()( 22

SPSPSE

eqeqSE

XaXjRaRZ

jXRZ

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Three Phase Transformer

• Three phase transformer consists of 3 transformers.• It is connected independently or in combination of 3

transformers. • Primary and secondary windings can be connected as wye

(Y) or delta (∆)• Thus, there are 4 types of connections:

– Wye – wye (Y-Y) – Wye – delta (Y-∆) – Delta – wye (∆-Y)– Delta – delta (∆-∆)

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The autotransformer• On some occasions it is desirable to change voltage levels

by only a small amount. A special-purpose transformer, called an autotransformer, is used in these cases.

The voltages in the coils are related to the voltages at the terminals by the Equations

And the currents in the coils are related to the currents at the terminals by the equations the relationship between the two

sides of an autotransformer

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3 phase Transformer

3 phase transformer connected independently

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Three Phase Transformer

Three phase transformer connected to a common core with three legs

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Connection Y-Y

Three Phase transformer Y-Y connection

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Transformer Connection Y-Y

aV

V

V

V

S

P

LS

LP

3

3

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Transformer Y-∆ Connection

aV

V

V

V

V

V

LS

LP

S

P

LS

LP

3

3

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Transformer ∆-Y Connection

aV

V

V

V

V

V

LS

LP

S

P

LS

LP

3

3

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Transformer ∆-∆ Connection

aV

V

V

V

S

P

LS

LP

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Three-phase transformation using two transformers

In addition to the standard three-phase transformer connections, there are ways to perform three-phase transformation with only two transformers

Some of the more important two-transformer connections are1. The open- Δ (or V-V) connection2. The open-Y-open- Δ connection3. The Scott-T connection

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Instrument transformers

Instrument transformers are small transformers intended to supply low values of current and voltage to measuring instruments and protective relays.

Current transformer (CT)> used in measurement of high current 1. It’s a step up transformer2. Secondary side is usually rated up to 5 A3. Primary circuit have few turns

Potencial transformer (CT) > used in measurement of high voltage 1. It’s a step down transformer2. Secondary side is usually rated 110 V

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