Explanation: The magnetomotive force produced by a set of balanced polyphase currents in a symmetrical set of sinusoidally distributed winding is:
Eq. 5.15
Ft=(Ns x Is,max x ms / 2) x cos(ws x t + alfa,s - theta), in Amperes.
The vector addition of the stator magnetomotive force Fst and the rotor magnetomotive force Frt gives the net or magnetizing magnetomotive force:
Eq. 5.26
Fmt=Fmax x cos(ws x t + alfa,m - theta), in Amperes
From Eq. 5.15, this magnetizing force can be considered as the result of a magnetizing component of the stator current. In phase a, this current component would be:
Eq. 5.27
Ima=Ims,max x sin(ws x t + alfa,m)
where:
Eq. 5.28
Ims,max = 2 x Fmax / (Ns x ms), in Amperes.
With the rotor open circuited, all of the stator current Is (notice that this is rms value) can be considered as magnetizing current Ims (again, rms value). From Eq. 5.27, the magnetizing current in phase a is:
Eq. 5.69
Ima=Ims,max x sin(ws x t + alfa,m) in Amperes.
Tying this result to the original posting 2.9 A (assumed rms value)
Ima,rms=2.9A=Ims,max/sqrt2.
See Reference:
Gordon R. Slemon "Magnetoelectric Devices, Transducers, Transformers, and Machines," John Wiley and Sons, Inc., 1966, Chapter 5 Polyphase Machines (or a similar textbook).