Theory of Wave Transmission a Treatise On Transmission of Power By Vibrations

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At starting a^ = a = a, and we have Mq = 0. It follows that the motor is not self-starting, and will require an impulse to set it rotating. Put ttj = rt — rtj = sa then a^ = a{i — s) -}- a -^ 2a and if s is small, we have flA2i The torque is practically a maximum when S = Cas and we see that for this value the second term in the bracket becomes 2 s- 1+4:^ 2 which is negligible.
The maximum torque is, therefore, about ^ _ asA^ _ A2 ■""• ~ 2S ~ 2C which is similar to the value found for three-pha
...se motors, having the factor 2 instead of 3 as multiplier of the torque due to a single phase in the rotor.
Collector Motors. — The motors described above develop a comixiratively small starting torque, which can only be increased by devices involving a loss of energy. Such motors are not adapted to cases in which a variable speed is required without loss of power. In order, therefore, to obtain high starting torques -it is necessary to employ a different construction.
"5 ii6 WAVE TRAXSMISSIOX OF POWER The characteristic feature of this type of motor is that the currents produced by tlic pistons of the rotor are collected and suitably distributed by a fixed member, which we shall call a collector, or distributer.


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