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In split-phase motor, the auxiliary winding is made up of
Thick wire with fewer turns
Thin wire with fewer turns
Thin wire with many turns
Thick wire with many turns
Thin wire with fewer turns
In a split-phase single-phase induction motor, the auxiliary (starting) winding is made up of thin wire with fewer turns compared to the main winding. This design gives the auxiliary winding high resistance and low inductive reactance, resulting in a high RA/XA ratio. Consequently, the current in the auxiliary winding leads the current in the main winding, creating the phase difference necessary to generate a rotating magnetic field for starting.
In a split-phase single-phase induction motor, the auxiliary (starting) winding is made up of thin wire with fewer turns compared to the main winding. This design gives the auxiliary winding high resistance and low inductive reactance, resulting in a high RA/XA ratio. Consequently, the current in the auxiliary winding leads the current in the main winding, creating the phase difference necessary to generate a rotating magnetic field for starting.
tanθa=RaXa — Phase angle of Auxiliary Winding current
tanθm=RmXm — Phase angle of Main Winding current
α=θm−θa — Phase difference between Main and Auxiliary currents
Ts∝IaImsinα — Starting torque equation
Single-phase induction motors are not self-starting because a single-phase AC current produces a pulsating magnetic field rather than a rotating one. By splitting the single phase into two parallel circuits (main and auxiliary windings) with different R/X ratios, a phase shift α (typically 30° to 40°) is produced between their respective currents, Im and Ia. This phase difference creates a revolving magnetic field that generates the torque needed to start the motor.
The auxiliary winding has high resistance (Ra) and low inductance (Xa) due to its thin wire and fewer turns.
The main winding consists of thick wire with many turns, giving it low resistance (Rm) and high inductance (Xm).
The centrifugal switch disconnects the auxiliary winding once the motor reaches approximately 75% to 80% of synchronous speed.
The phase difference α achieved in a resistance split-phase motor is typically around 30° to 40°.
Low cost and simple construction.
No capacitors required for starting.
Reliable operational performance for low-torque applications.
Low starting torque (typically 1.5 to 2 times full-load torque).
High starting current.
Poor power factor during starting.
Small blowers and fans
Washing machines
Centrifugal pumps
Small machine tools and grinders
| Feature | Auxiliary Winding | Main Winding |
|---|---|---|
Wire Gauge/Thickness | Thin wire (high gauge) | Thick wire (low gauge) |
Number of Turns | Fewer turns | Many turns |
Resistance (R) | High (Ra) | Low (Rm) |
Inductive Reactance (X) | Low (Xa) | High (Xm) |
Current Phase Relationship | Current Ia is nearly in phase with voltage | Current Im lags voltage by a large angle |
Option A (Thick wire with fewer turns) is incorrect because thick wire reduces resistance, which would lower the R/X ratio needed for the auxiliary winding.
Option C (Thin wire with many turns) is incorrect because adding many turns increases inductance (Xa∝N2), preventing Ia from leading Im.
Option D (Thick wire with many turns) describes the Main Winding, which requires low resistance and high reactance to produce a lagging current.
B is correct — Thin wire provides high resistance while fewer turns keep the reactance low, creating the high R/X ratio required for phase splitting.
Remember that starting torque is proportional to sinα. Resistance split-phase motors give α≈30°−40°, whereas capacitor-start motors achieve α≈90°, yielding much higher starting torque.