Single Phase transformer | E.M.F equation of a transformer, No load Condition & On load Condition

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Single phase transformer

The basic theory of a transformer is not difficult to understand. To simplify matters as much as possible, let us first consider an ideal transformer, that is, one in which the resistance of the winding is negligible and the core has no losses.

Fig. Single-phase transformer

This is a single-phase transformer having two winds the primary winding and the secondary winding.

follow in the primary winding. Since the primary resistance is negligible and there are no losses in the core, the effective resistance is zero and the circuit is purely reactive. 

 Hence the current wave  Im lags the impressed voltage wave. The reactance of the circuit is very high and the magnetizing current is very small. This current in the N1 turns of the primary magnetizes the core and produces a flux ø that is at all times proportional to the current if the permeability of the circuit is assumed to be constant, and therefore in time phase with the current. 

The flux, by its rate of change, includes in the primary winding E1 which at every instant of times is equal in value and opposite in direction to V1. It is called the current e.m.f of the primary. 

The value that the primary current attains must be such that the flux which it produces in the core is of sufficient value to induce in the primary the required counter e.m.f. electro-motive force.

Since the flux also threads or links the secondary winding a voltage E2 is induced in the secondary, this voltage is likewise proportional to the rate of change of flux and so is in the time phase with E1, but it may have any value depending upon the number of turns N2 in the secondary.

E.M.F equation of a transformer

Let,

Fig. Phaser diagram of a transformer

  N1 = Number of turns in the primary winding 

  N2 = number of turns in the secondary winding

  øm= maximum flux in the core,

wb

= Bm. A,  – where Bm is the maximum flux density in the core and A is the core area,

  f = frequency of a.c. input Hz.

Transformer on no load

Fig. Transformer on no load

A transformer is said to be on no-load if its secondary side is open and the primary is connected to a sinusoidal alternating voltage V1. The alternating applied voltage will cause the flow of alternating current in the primary winding which will create alternating flux. This primary input current Io is under no-load condition supply. 

  1. Iron losses in the core  (for example. Hysteresis loss and eddy current loss.)
  2. A very small amount of copper loss in the primary (there being no copper loss in the secondary as it is open).

Transformer on load

Fig. Transformer on load

The transformer is said to be loaded when the secondary circuit of a transformer is complete through an impedance or load. The magnitude and phase of secondary current I2 with respect to secondary terminal voltage will depend upon the character of load, i.e, current I2 will be in phase, lag behind and lead the terminal voltage V2 respectively when the load is purely respective, inductive, and capacitive.

The secondary current I2 sets up its own ampere-turns and creates its own flux opposing the main flux. The opposing secondary flux weakens the primary flux momentarily and hence causes more current to flow in the primary.

  • Whatever the load condition, the net flux passing through the core is approximately the same as at no-load.
  • Since the core flux remains constant at all loads, the core loss almost remains constant under different loading conditions.

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