# Equivalent Circuit of Transformer referred to Primary and Secondary

## Equivalent Circuit of Transformer

Equivalent**impedance of transformer**is essential to be calculated because the electrical power transformer is an electrical power system equipment for estimating different parameters of electrical power system which may be required to calculate total internal impedance of an electrical power transformer, viewing from primary side or secondary side as per requirement. This calculation requires

**equivalent circuit of transformer referred to primary**or

**equivalent circuit of transformer referred to secondary**sides respectively. Percentage impedance is also very essential parameter of transformer. Special attention is to be given to this parameter during installing a transformer in an existing electrical power system. Percentage impedance of different power transformers should be properly matched during parallel operation of power transformers. The percentage impedance can be derived from equivalent

**impedance of transformer**so, it can be said that

**equivalent circuit of transformer**is also required during calculation of % impedance.

## Equivalent Circuit of Transformer Referred to Primary

For drawing**equivalent circuit of transformer referred to primary**, first we have to establish general

**equivalent circuit of transformer**then, we will modify it for referring from primary side. For doing this, first we need to recall the complete vector diagram of a transformer which is shown in the figure below. Let us consider the transformation ratio be, In the figure above, the applied voltage to the primary is V

_{1}and voltage across the primary winding is E

_{1}. Total current supplied to primary is I

_{1}. So the voltage V

_{1}applied to the primary is partly dropped by I

_{1}Z

_{1}or I

_{1}R

_{1}+ j.I

_{1}X

_{1}before it appears across primary winding.

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The voltage appeared across winding is countered by primary induced emf E_{1}. So voltage equation of this portion of the transformer can be written as,
The equivalent circuit for that equation can be drawn as below,
From the vector diagram above, it is found that the total primary current I_{1} has two components, one is no - load component I_{o} and the other is load component I_{2}′. As this primary current has two components or branches, so there must be a parallel path with primary winding of transformer.

This parallel path of current is known as excitation branch of equivalent circuit of transformer. The resistive and reactive branches of the excitation circuit can be represented as

_{2}′ flows through the primary winding of transformer and induced voltage across the winding is E

_{1}as shown in the figure right. This induced voltage E

_{1}transforms to secondary and it is E

_{2}and load component of primary current I

_{2}′ is transformed to secondary as secondary current I

_{2}. Current of secondary is I

_{2}. So the voltage E

_{2}across secondary winding is partly dropped by I

_{2}Z

_{2}or I

_{2}R

_{2}+ j.I

_{2}X

_{2}before it appears across load. The load voltage is V

_{2}. The complete equivalent circuit of transformer is shown below.

Now if we see the voltage drop in secondary from primary side, then it would be ′K′ times greater and would be written as K.Z_{2}.I_{2}.
Again I_{2}′.N_{1} = I_{2}.N_{2}
Therefore,
From above equation, secondary impedance of transformer referred to primary is,
So, the complete equivalent circuit of transformer referred to primary is shown in the figure below,

### Approximate Equivalent Circuit of Transformer

Since I_{o}is very small compared to I

_{1}, it is less than 5% of full load primary current, I

_{o}changes the voltage drop insignificantly. Hence, it is good approximation to ignore the excitation circuit in approximate equivalent circuit of transformer. The winding resistance and reactance being in series can now be combined into equivalent resistance and reactance of transformer, referred to any particular side. In this case it is side 1 or primary side.