The electromotive force (EMF) equation of a synchronous reluctance motor can be expressed as ( E = 4.44 \times f \times \Phi \times T ), where ( E ) is the induced EMF, ( f ) is the frequency of the supply voltage, ( \Phi ) is the magnetic flux per pole, and ( T ) is the number of turns per phase winding. In synchronous reluctance motors, the EMF is generated due to the rotor's reluctance variation in the magnetic field, rather than traditional winding-induced EMF, which is typical in other motor types. The motor operates at synchronous speed determined by the supply frequency and number of poles, contributing to its efficiency and performance characteristics.
induction motor never runs at synchronous speed, if it does so there would not be any relative speed between stator flux and rotor and no emf will induce in rotor and we can not apply motor principle as we need current carrying conductor in magnetic field.
The emf equation of signal phase transform
During the operation of a DC motor, EMF is created across its terminals using an external source. Whereas, in a DC generator EMF is created across its terminal based on principle of dynamically induced EMF. So talking in terms of EMF, in DC motor EMF is consumed by the motor coil and utilized to rotate the axle. On the other hand, in DC generator EMF developed across coil is transfered to a load or a battery and consumed by them.
because at start the motor draws larger quantity of current and this may affected the rotor windings in order to limit current always resistance is connected.
The usual way is with a synchronous generator connected to the distribution system.
ediot
f=4.44fqm
induction motor never runs at synchronous speed, if it does so there would not be any relative speed between stator flux and rotor and no emf will induce in rotor and we can not apply motor principle as we need current carrying conductor in magnetic field.
The emf equation of signal phase transform
Synchronous impedance is also known as the EMF method. It is a ratio of open circuits to short circuits, when they both are referred to the same field excitation.
In dc motor, the armature conductors are revolving in the magnetic field and emf is induced in the armature conductors. The direction of the induced emf is in opposite direction to the applied voltage as per Flemings left hand rule. So, the induced emf in motor is called as back emf or counter emf. Vydehi
equation of ac machine
During the operation of a DC motor, EMF is created across its terminals using an external source. Whereas, in a DC generator EMF is created across its terminal based on principle of dynamically induced EMF. So talking in terms of EMF, in DC motor EMF is consumed by the motor coil and utilized to rotate the axle. On the other hand, in DC generator EMF developed across coil is transfered to a load or a battery and consumed by them.
because at start the motor draws larger quantity of current and this may affected the rotor windings in order to limit current always resistance is connected.
BACK emf induced in a motor's coil that tends to reduce the current in the coil of the motor. The answer should be 'back'.
synchronous generator is similar to the principle of laws of electro magnetic induction that is "whenever the magnetic flux linking in a conductor that time emf is induced at the ends of the conductor "
at the time of starting when syncchronous torque is zero , i.e. when the motor starts with the help of starting torque , the armature current required to produce sync. torque is zero. If V = E(b) i.e. When back emf E(b) equals supply voltage.