Schrage Motor Operation Principle and Characteristics of Schrage Motoron 24/2/2012 & Updated on 25/8/2018
Operation Principle of Schrage MotorAt standstill conditions due to three phase currents flowing in the primary winding a rotating field is produced. This rotating field cuts the secondary with a synchronous speed ns. Therefore according to Lenz’s law the rotor will rotate in a direction so as to oppose the cause i.e. to induce slip frequency emfs into secondary. Therefore the rotor rotates opposite to the direction of rotation of synchronously rotating field. Now air gap field is rotating at slip speed ns - nr with respect to secondary. Therefore the emf collected by the stationary brushes is at slip frequency and hence suitable for injection into secondary.
Speed Control of Schrage MotorSpeed control of schrage motor is possible by varying the injected emf into the motor which can be controlled by changing the angular displacement between the two brushes. To understand the speed control of schrage motor let us understand the speed control in WRIMs using injected emf method.
Consider the following rotor circuits (values are only for illustration purpose).
Let initially electrical torque (Te) = load torque (Tl) = 2Nm
Rotor current Ir = 2A.
Let sE2 = slip emf induced in the rotor ckt.
And Ej = emf injected in the rotor ckt.
Case 1: When Ej is in phase opposition to sE2 Now the rotor current becomes Ir = 1A. Therefore Te < Tl due to which motor decelerates. Therefore ωr decreases. That implies slip increases. Therefore ωr decreases till sE2 becomes 15V and Ir = 2A i.e till Te = Tl again.
Case 2: When Ej is in phase with sE2 Now the rotor current becomes 3A. Therefore Te > Tl due to which motor accelerates. Therefore ωr increases. That implies slip decreases. Therefore ωr increases till sE2 becomes 5V and Ir = 2A i.e till Te = Tl again. From the above analysis it can be seen that to increase speed the injected emf should be in phase with slip emf in the rotor. To decrease speed the injected emf should be out of phase with the slip emf in the rotor. Now based on the above principles we shall take a look at the speed control of schrage motor. In the above figure E20 = standstill emf induced in the secondary. sE20 = induced emf at any slip s. a, b = brush terminals. In fig (a) both the brushes are connected to the same commutator segment and hence are short circuited. The injected emf in this case is zero. Therefore rotor rotates with speed close to synchronous speed. In fig(b) the brushes a and b are separated by an angular displacement θ such that the tertiary winding axis between brushes a and b is coincident with secondary winding axis. Now on tracing the path BAabB we find that injected emf Ej is in phase opposition to E20. Therefore from above discussed principles speed of the motor shall decrease from what it was in case a. Hence the motor operates at sub synchronous speeds i.e. nr < ns. In fig(c) the brush positions are interchanged. Now on tracing the path BAabB we find that the injected emf is in phase with the standstill emf E20. Therefore speed of motor should increase from what it was in case a. Hence the motor operates at super synchronous speed i.e. nr > ns. For any brush separation θ the injected emf is given by From the equation it can be seen that minimum value of injected emf Ej = 0 at θ = 0 (i.e. when the brushes are short circuited). And maximum value of injected emf is Ej = Ejmax at θ = 90 degrees (i.e. when the brushes are one pole pitch apart).
Power Factor ControlTo improve power factor an angular displacement of ρ is introduced between tertiary winding axis and secondary winding axis. Now flux φ cuts the tertiary winding axis some time later after it has covered an angular displacement of ρ degrees. Therefore emf phasor – Ej in this case lags the emf phasor – Ej in case b by an angle ρ. The phasor diagram for the two cases is as shown below The phasor diagram has been constructed based on the following equations: I2 lags I2Z2 by some angle θ. I2’ is draw opposite to I2. The resultant of I2’ and magnetizing current I0 gives the primary current I1. From the phasor diagram it is clear that if the tertiary winding axis and secondary winding axis are displaced by an angle ρ then power factor improves.
Characteristics of Schrage MotorIf we apply KVL to secondary circuit then we get Under no load conditions I2 value is very small and hence the can be neglected. Therefore we have, Where, s0 is the no load slip Where, Ejmax is the transformer emf induced in the Tertiary winding. φm = max flux linkage fs = supply frequency Z = number of conductors in tertiary A = number of parallel paths Also Where, E20 = the transformer emf induced in the secondary. N2’ = effective number of turns in the secondary Now on substituting these values in the expression of no load slip we get This implies values of slip depend completely on machine constants and the brush separation. This shows that two different speeds are possible at no load depending on the phase of injected emf. The magnitude of these speeds can be controlled by adjusting the brush separation. Under load conditions Applications Used in drives requiring variable speed such as cranes, fan, centrifugal pumps, conveyors etc.
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