As per double field revolving theory, a sinusoidally alternating flux can be looked upon as the combination of two revolving fluxes:

1
equal in magnitude to that of the alternating flux, rotating at synchronous speed in the same direction
2
of half the magnitude to that of the alternating flux, rotating at synchronous speed in the same direction
3
equal in magnitude to that of the alternating flux, rotating at synchronous speed in the opposite direction
4
of half the magnitude to that of the alternating flux, rotating at synchronous speed in the opposite direction

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