#### Rothert's MMF Method or Ampere-Turn Method of finding voltage regulation of alternator is the converse of the EMF method. In a synchronous generator or alternator, the MMF is due to field ampere-turns ( i.e., the product of field current and number of turns in field winding ). The terminal voltage produced by field MMF of the alternator is the vector sum of the following,- The MMF necessary to induce rated terminal voltage by the field ampere-turns on no-load. This can be obtained by performing the open-circuit test on the alternator.
- The MMF produced by field ampere-turns has to overcome the demagnetizing effect of armature reaction and impedance drop to produce full-load current when the alternator is loaded. This value is obtained by a short-circuit test.

Here, we can see that similar to EMF or synchronous impedance method, the MMF method also utilizes data obtained from O.C. and S.C. tests. In this method, when the alternator is loaded change in terminal voltage due to armature leakage reactance is replaced by the additional armature reaction MMF, and combined with the existing armature reaction MMF. So that the entire drop in the alternator is due to armature reaction MMF.

In an alternator under short-circuit condition the impedance drop i.e., due to armature resistance and armature leakage reactance is usually very small and can be neglected. Hence in a short-circuit test, to circulate full-load current, the MMf by field ampere-turns has to overcome the drop due to the armature reaction effect only. Therefore under short-circuit condition the power factor of such a purely reactive circuit with an armature reaction effect is almost zero lagging.

We know that the at lagging p.f. the armature reaction effect is wholly demagnetizing. Thus the field MMF required to produce a full-load current has to overcome the armature reaction effect which is entirely demagnetizing in nature.

#### The above figure shows the field MMF required to induce rated terminal voltage under open-circuit condition F_{O}, and field MMF required to circulate full-load current under short-circuit condition F_{AR}.

## Phasor Diagram of MMF Method :

#### Let us consider when the load power factor has any value, either lagging or leading. Then the resultant MMF is determined by vector addition of F_{O} and F_{AR}.

### For Lagging Power Factor :

#### The below shows the phasor diagram at lagging power factor i.e., the phase current I_{aph} lags the phase voltage V_{ph} by an angle cos Ï†. Here the rated terminal voltage of open-circuit test F_{o} lies at a right angle to V_{ph}. Since the armature reaction is due to the armature current I_{aph}, the component F_{AR} lies in phase with the current I_{aph}.

#### Since the field MMF has to overcome the armature reaction effect to produce rated terminal voltage. The resultant field MMF F_{R} is obtained by taking -F_{AR} vectorially to F_{O} as shown above.

From the triangle OCB,- AC = F
_{AR} sin Ï† - BC = F
_{AR} cos Ï†

Therefore,

_{AR}sin Ï†_{AR}cos Ï†### For Leading Power Factor :

#### Similarly, the phasor diagram if the load power factor is leading, where phase current I_{aph} leads the phase voltage V_{ph} is shown below. The resultant F_{R} is obtained by adding -F_{AR} to F_{O}.

#### From the triangle OCB,- AC = F
_{AR} sin Ï† - BC = F
_{AR} cos Ï†

Therefore,

_{AR}sin Ï†_{AR}cos Ï†