The machine is connected to a dc source and a current flows through the armature conductors. A torque is devolved and the machine rotates in the anticlockwise direction. This torque drives the devce (e.g. late, pump, etc.) which is mechanically coupled to the motor. As the conductors rotate in the magnetic field, an emf is induced in the conductors. The direction of this emf is the same. (a). This emf opposes the flow of current in the machine and is thus opposite in direction to the applied voltage. This induced emf because it opposes the applied voltage) is known as back emf or counter emf of the motor of applied voltage must be sufficient to overcome the back emf as well as to overcome the voltage drop in the armature. The back emf Eb is the voltage induced due to roation of the armature and its magnitude is Eb = Ke NФ
Tuesday, 24 June 2014
Driving and Retarding Torques, Back EMF
The machine is connected to a dc source and a current flows through the armature conductors. A torque is devolved and the machine rotates in the anticlockwise direction. This torque drives the devce (e.g. late, pump, etc.) which is mechanically coupled to the motor. As the conductors rotate in the magnetic field, an emf is induced in the conductors. The direction of this emf is the same. (a). This emf opposes the flow of current in the machine and is thus opposite in direction to the applied voltage. This induced emf because it opposes the applied voltage) is known as back emf or counter emf of the motor of applied voltage must be sufficient to overcome the back emf as well as to overcome the voltage drop in the armature. The back emf Eb is the voltage induced due to roation of the armature and its magnitude is Eb = Ke NФ
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