Rotating magnetic field

How rotating magnetic field is produced in Induction Motor ?

Consider 3-phase currents, displaced in time by 1200 as shown.

3 phase currents displaced by 120 degree in time from each other

When 3-phase windings displaced in space by 1200 are fed by these 3-phase currents, individual phases produce magnetic fluxes and the assumed positive directions of these fluxes are shown below.

stator winding displaced in space by 120 degree


Lets analyse each of these fluxes and their resultant Φ, at every instant of time 600 apart.


(1) when  Ï´=00
Rotating magnetic field
As fluxes will be proportional to these currents, Let their values be
    Rotating magnetic field
    Where,  Φm = maximum value of magnetic flux due to any phase.

Vectorically the fluxes are shown along with their resultant flux (in red )  Φ. The negative sign have been taken into account in vector diagram.  

Rotating magnetic field

The resultant flux  Φ  is given by 
 Î¦ = ΦB cos 300 + ΦY cos 300      

        

         = 1.5 Φ

So, resultant flux has magnitude equal to  1.5 Φm  and is vertically directed.

 (2) when Ï´=600
The individual fluxes will be
   Rotating magnetic field
    Represented in phasors as shown.
   
Rotating magnetic field


The resultant flux is given by
Φ = ΦR cos 300 + ΦY cos 300    
        Rotating magnetic field

So, resultant flux has magnitude 1.5 times maximum flux due to any phase and has rotated 600 clockwise.

(3) when Ï´=1200
      
     Rotating magnetic field
The individual fluxes along with the resultant are represented in  phasors as shown.

Rotating magnetic field


 The resultant flux is given by
 Î¦ = ΦR cos 300 + ΦB cos 300 
        Rotating magnetic field
So, resultant flux has magnitude 1.5Φm and has rotated 600 clockwise from last position.

(4) when Ï´=1800
     
      Rotating magnetic field
      
    The individual fluxes along with the resultant are represented in                 phasors as shown.
    
Rotating magnetic field



The resultant flux is given by
Φ = ΦY cos 300 + ΦB cos 300    
        Rotating magnetic field

Again, resultant flux has magnitude 1.5Φm and has rotated 600 clockwise from last position.
Similar analysis can be continued for next  Ï´s  upto full cycle i.e  Ï´=3600 .


From above, we observed that

(1) The resultant flux is of constant value = 1.5 Φm    i.e  1.5 times the    maximum value of flux due to any phase.

(2) The resultant flux rotates around the stator at a speed called synchronous speed.

Thus, it is true to assume that a rotating magnetic field is produced in space as if actual magnetic poles of permanent magnet were being rotated mechanically.