Basic Electrical Machines (8hrs) · Basics of Electrical & Electronics Engineering

their working principles

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their working principles

1. What "Their Working Principles" Means

This topic elaborates how single-phase and three-phase induction motors actually produce torque from the rotating magnetic field (RMF).

2. Three-Phase Induction Motor — Working

Sequence:

  1. 3-phase AC applied to stator windings 120° apart ⇒ creates RMF rotating at synchronous speed
Ns=120f/PN_s=120f/P

(e.g., 4-pole 50Hz ⇒1500 rpm) with constant magnitude.
2. RMF sweeps past rotor conductors (squirrel cage bars) ⇒ relative speed Ns−NN_s - N (where NN = rotor speed) ⇒ Faraday:

e=Blvrele=Blv_{rel}

induced in rotor bars.
3. Rotor bars short-circuited (end rings) ⇒ rotor currents I2I_2 flow (frequency f2=s⋅ff_2 = s·f, where slip

s=(Ns−N)/Nss=(N_s-N)/N_s

).
4. Lorentz force: rotor current I2I_2 in RMF BB experiences force

F=B⋅I2⋅lF = B·I_2·l

⇒ torque

T=F⋅rT = F·r

in direction of RMF ⇒ rotor follows RMF, accelerating.
5. Slip: rotor can never reach NsN_s (if N=NsN=N_s, relative speed zero ⇒ e=0e=0, I2=0I_2=0, T=0T=0 ⇒ friction slows). So 0<s≤10< s ≤1 (motoring: ss small 0.010.01–0.050.05 at rated load, s=1s=1 at standstill/start).

Why self-starting: RMF exists at start (s=1s=1), so torque at s=1s=1 >0 ⇒ starts.

3. Single-Phase Induction Motor — Working and Why Needs Help

  • With single winding, field is pulsating (not rotating):
B=Bmcosωt⋅cosθ=(Bm/2)[cos(ωt−θ)+cos(ωt+θ)]B = B_m cosωt·cosθ = (B_m/2)[cos(ωt-θ)+cos(ωt+θ)]

= two counter-rotating RMFs of half amplitude. At standstill, torques from both RMFs cancel ⇒ no starting torque (double-revolving field theory).

  • Starting aid: auxiliary winding + capacitor creates 90° phase shift ⇒ elliptical RMF ⇒ net torque >0 to start. Once started, auxiliary may be cut off (centrifugal switch), motor runs with pulsating field but now rotor sees unbalanced torque, continues.
  • Alternative: shaded-pole (copper ring on pole tip delays phase).

4. Worked Checks

(a) 3-phase 4-pole 50Hz Ns=1500, rotor N=1440 ⇒ s=0.04, rotor frequency f2= s·f=2Hz ⇒ rotor currents 2Hz.

(b) Need to reverse direction? Swap any two phases ⇒ RMF reverses ⇒ torque reverses.

(c) Single-phase at standstill: no torque, push rotor slightly ⇒ it picks direction of push (bistable) ⇒ needs starter.

5. Exam Points

  • Explain 3-phase RMF at Ns=120f/PN_s=120f/P and s=(Ns−N)/Nss=(N_s-N)/N_s with e=Blve=Blv → I2I_2 → F=BIlF=BIl → torque — 7-10 marks, very frequent (the most common working principle question).
  • Explain single-phase double-revolving field and why no starting torque, need capacitor/shaded pole — 5-7 marks, very frequent (almost certain to ask why single-phase not self-starting).
  • Mention f2=s⋅ff_2=s·f — 3 marks, frequent.
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