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FIG.1 THERE IS THE MODEL OF TWO STATOR THREE PHASE ELECTRICAL MACHINE
         WITH CONDUCTIVE ROTOR. PHASES ON BOTH SIDES OF THE STATOR ARE
       CONNECTED IN SERIES AND GENERATE THE SAME MAGNETO MOTIVE FORCE.
             THE SAME MODEL I SUPPOSE, YOU HAVE IN YOUR ALTERNATOR.



                                       STATOR 1


      PHASE U                   PHASE V                       PHASE W




                                        ROTOR
                                    (CONDUCTIVE FOR
                                     MAGNETIC FIELD)




     PHASE U                    PHASE V                      PHASE W


                                        STATOR 2




                    POSITIVE
                    TERMINAL
                                          FIG.2. TO MAKE IT SIMPLE, I TOOK THE TIME
                                          MOMENT, WHEN CURRENT FLOWS THROUGH
                                                    TWO PHASES - U AND V

PHASE U
                     CURRENT
                      FLOW




                   CURRENT                    PHASE V
                    FLOW




                                              NEGATIVE
                                              TERMINAL
FIG.3 BROCKEN ARROWOS REPRESENT MAGNETIC FIELD FROM THE CURRENT,
                                      FLOWS ONLY THROUGH PHASE U




                                                    STATOR 1


                    PHASE U                  PHASE V                       PHASE W




                                                           ROTOR
                                                       (CONDUCTIVE FOR
                                                        MAGNETIC FIELD)




                   PHASE U                   PHASE V                      PHASE W


                                                    STATOR 2


 THIS CHART
REPRESENTS
  MAGNETO-
MOTIVE FORCE
DISTRIBUTION
 INSIDE THE
WORKING GAP
   OF THE
 ELECTRICAL
  MACHINE
    WHEN       0              120                                                    360
                                                         240
  CURRENT
   FLOWS
  THROUGH
  PHASE U.
FIG.4 BROCKEN ARROWOS REPRESENT MAGNETIC FIELD FROM THE CURRENT,
                                      FLOWS ONLY THROUGH PHASE V




                                                    STATOR 1


                    PHASE U                  PHASE V                       PHASE W




                                                           ROTOR
                                                       (CONDUCTIVE FOR
                                                        MAGNETIC FIELD)




                   PHASE U                   PHASE V                      PHASE W


                                                    STATOR 2


 THIS CHART
REPRESENTS
  MAGNETO-
MOTIVE FORCE
DISTRIBUTION
 INSIDE THE
WORKING GAP
   OF THE
 ELECTRICAL
  MACHINE
    WHEN       0              120                                                    360
                                                         240
  CURRENT
   FLOWS
  THROUGH
  PHASE V.
FIG.5. WE CAN SEE THAT COMBINED DISTRIBUTION OF MAGNETO-MOTIVE FORCE (OR
              MAGNETIC FIELD FROM THE CURRENT, FLOWING THOUGH PHASES U AND V) HAS
          ASYMMETRICAL SHAPE. IF WE USE FOURIER SERIES TO DESCRIBE THIS GRAPH, WE WILL
              SEE, THAT IT HAS NOT ONLY ODD HARMONICS, BUT ALSO EVEN HARMONICS. THIS
            HARMONICS DON'T PRODUCE ANY USEFUL TORQUE IN THREE PHASE SYSTEM, THEY
            INTERFERE WITH MAJOR HARMONICS AND CREATE PULSATION OF THE TORQUE AND
                                          POWER LOSSES.



PHASE U




          0               120                   240                      360




PHASE V




          0               120                   240                      360




 PHASE
  U+V

          0               120                   240                      360
FIG.6. LET US SHIFT STATOR 2 ON 180 ELECTRICAL DEGREES AGAINST
                                                         STATOR 1




                                                           STATOR 1


                         PHASE U                   PHASE V                      PHASE W




                                                           ROTOR
                                                       (CONDUCTIVE FOR
                                                        MAGNETIC FIELD)




SHIFT STATOR 2
    ON 180                           PHASE V                        PHASE U                     PHASE V
  ELECTRICAL
   DEGREES
                                                                          STATOR 2



     PHASE U
    STATOR 1
   MAGNETO-
     MOTIVE
      FORCE
  DISTRIBUTION   0                 120                        240                         360




   PHASE U
   STATOR 2
  MAGNETO-
    MOTIVE       0                 120                        240                         360
    FORCE
 DISTRIBUTION




  COMBINED
  MAGNETO-
    MOTIVE
    FORCE
     FROM
  PHASES U
   ON BOTH                          120                                                      360
                     0                                          240
   STATORS
FIG.7. ON THIS FIGURE THE MAGNETO-MOTIVE FORCE IS
                   COMBINED FROM PHASES U AND V. THE RESULTING FIGURE IS
                   SYMMETRICAL AND VERY CLOSE TO THE FIRST HARMONIC OF
                   FOURIER SERIES. THERE ARE ONLY ODD HARMONIC NUMBERS
                     PRESENT. THIS METHOD ALLOWS US TO ELIMINATE EVEN
                                HARMONIC NUMBERS COMPLETELY.




 PHASE U




               0             120                   240                 360




   PHASE V
  (TO MAKE
  THIS GRAF
    WE USE
  THE SAME
 APPROACH
 , AS ABOVE
     FOR
   PHASE U,
  ONLY IT IS   0             120                   240                 360
   SHIFTED
    120 EL.
  DEGREES.




PHASE U
 AND V




               0             120                   240                 360

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Two Stator Motor Model Explanation

  • 1. FIG.1 THERE IS THE MODEL OF TWO STATOR THREE PHASE ELECTRICAL MACHINE WITH CONDUCTIVE ROTOR. PHASES ON BOTH SIDES OF THE STATOR ARE CONNECTED IN SERIES AND GENERATE THE SAME MAGNETO MOTIVE FORCE. THE SAME MODEL I SUPPOSE, YOU HAVE IN YOUR ALTERNATOR. STATOR 1 PHASE U PHASE V PHASE W ROTOR (CONDUCTIVE FOR MAGNETIC FIELD) PHASE U PHASE V PHASE W STATOR 2 POSITIVE TERMINAL FIG.2. TO MAKE IT SIMPLE, I TOOK THE TIME MOMENT, WHEN CURRENT FLOWS THROUGH TWO PHASES - U AND V PHASE U CURRENT FLOW CURRENT PHASE V FLOW NEGATIVE TERMINAL
  • 2. FIG.3 BROCKEN ARROWOS REPRESENT MAGNETIC FIELD FROM THE CURRENT, FLOWS ONLY THROUGH PHASE U STATOR 1 PHASE U PHASE V PHASE W ROTOR (CONDUCTIVE FOR MAGNETIC FIELD) PHASE U PHASE V PHASE W STATOR 2 THIS CHART REPRESENTS MAGNETO- MOTIVE FORCE DISTRIBUTION INSIDE THE WORKING GAP OF THE ELECTRICAL MACHINE WHEN 0 120 360 240 CURRENT FLOWS THROUGH PHASE U.
  • 3. FIG.4 BROCKEN ARROWOS REPRESENT MAGNETIC FIELD FROM THE CURRENT, FLOWS ONLY THROUGH PHASE V STATOR 1 PHASE U PHASE V PHASE W ROTOR (CONDUCTIVE FOR MAGNETIC FIELD) PHASE U PHASE V PHASE W STATOR 2 THIS CHART REPRESENTS MAGNETO- MOTIVE FORCE DISTRIBUTION INSIDE THE WORKING GAP OF THE ELECTRICAL MACHINE WHEN 0 120 360 240 CURRENT FLOWS THROUGH PHASE V.
  • 4. FIG.5. WE CAN SEE THAT COMBINED DISTRIBUTION OF MAGNETO-MOTIVE FORCE (OR MAGNETIC FIELD FROM THE CURRENT, FLOWING THOUGH PHASES U AND V) HAS ASYMMETRICAL SHAPE. IF WE USE FOURIER SERIES TO DESCRIBE THIS GRAPH, WE WILL SEE, THAT IT HAS NOT ONLY ODD HARMONICS, BUT ALSO EVEN HARMONICS. THIS HARMONICS DON'T PRODUCE ANY USEFUL TORQUE IN THREE PHASE SYSTEM, THEY INTERFERE WITH MAJOR HARMONICS AND CREATE PULSATION OF THE TORQUE AND POWER LOSSES. PHASE U 0 120 240 360 PHASE V 0 120 240 360 PHASE U+V 0 120 240 360
  • 5. FIG.6. LET US SHIFT STATOR 2 ON 180 ELECTRICAL DEGREES AGAINST STATOR 1 STATOR 1 PHASE U PHASE V PHASE W ROTOR (CONDUCTIVE FOR MAGNETIC FIELD) SHIFT STATOR 2 ON 180 PHASE V PHASE U PHASE V ELECTRICAL DEGREES STATOR 2 PHASE U STATOR 1 MAGNETO- MOTIVE FORCE DISTRIBUTION 0 120 240 360 PHASE U STATOR 2 MAGNETO- MOTIVE 0 120 240 360 FORCE DISTRIBUTION COMBINED MAGNETO- MOTIVE FORCE FROM PHASES U ON BOTH 120 360 0 240 STATORS
  • 6. FIG.7. ON THIS FIGURE THE MAGNETO-MOTIVE FORCE IS COMBINED FROM PHASES U AND V. THE RESULTING FIGURE IS SYMMETRICAL AND VERY CLOSE TO THE FIRST HARMONIC OF FOURIER SERIES. THERE ARE ONLY ODD HARMONIC NUMBERS PRESENT. THIS METHOD ALLOWS US TO ELIMINATE EVEN HARMONIC NUMBERS COMPLETELY. PHASE U 0 120 240 360 PHASE V (TO MAKE THIS GRAF WE USE THE SAME APPROACH , AS ABOVE FOR PHASE U, ONLY IT IS 0 120 240 360 SHIFTED 120 EL. DEGREES. PHASE U AND V 0 120 240 360