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22-Elec-A6 Power Systems and Machines · December 2014

Question 2 of 6: Induction Motor

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Exam format. Professional Engineers Ontario / Engineers Canada national examination 07-Elec-A6 Power Systems and Machines, Fall (December) 2014. Closed book; approved Casio/Sharp calculator; formula sheet supplied. Part A is compulsory (20 multiple-choice questions, 1 mark each, −½ per wrong answer). Part B asks the candidate to solve any 4 of 5 problems; a complete paper is FIVE questions. All AC quantities are RMS; three-phase voltages are line-to-line and powers are totals unless noted. Every Part B problem is worked below as a study resource.

Reference texts.

Question 2 — Induction Motor

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. A 460 V (line-to-line), 60 Hz, four-pole, Y-connected induction motor running at slip $s=0.03$, with the per-phase equivalent-circuit parameters below and 455 W of core loss.

Given data (per phase, referred to the stator)
Line voltage $V_{LL}$460 VStator resistance $R_1$$0.641\ \Omega$
Rotor resistance $R_2$$0.300\ \Omega$Stator reactance $X_1$$0.750\ \Omega$
Rotor reactance $X_2$$0.500\ \Omega$Magnetizing reactance $X_m$$26.3\ \Omega$
Core loss $P_{core}$455 WSlip $s$ / poles $p$0.03 / 4

Find. Stator current, shaft (mechanical) speed, shaft output power, output torque, and efficiency at 3% slip.

Approach. Reduce the per-phase circuit to an input impedance (rotor branch $R_2/s+jX_2$ in parallel with $jX_m$, in series with $R_1+jX_1$), find $I_1$, then follow the Chapman power flow $P_{in}\to P_{SCL}\to P_{AG}\to P_{conv}\to P_{out}$, subtracting the core loss at the shaft.

V₁ = 265.6 V+−R₁ = 0.641X₁ = 0.750AjXₘ = 26.3R₂/s = 10.0X₂ = 0.500I₁R₂/s = 0.300/0.03 = 10.0 Ω (rotor branch)
Per-phase equivalent circuit (referred to the stator). The rotor branch resistance is $R_2/s=0.300/0.03=10.0\ \Omega$; the lossless $jX_m$ carries the magnetizing current, and the 455 W core loss is accounted as a rotational loss at the shaft.
  1. Per-phase voltage. $V_1=V_{LL}/\sqrt3=460/\sqrt3=265.6\ \text{V}$.
  2. Rotor branch and its parallel with the magnetizing reactance. $Z_2=\dfrac{R_2}{s}+jX_2=10.0+j0.5\ \Omega$, and $Z_f=\dfrac{jX_m\,Z_2}{jX_m+Z_2}=9.21\angle23.3^\circ=8.45+j3.65\ \Omega$.
  3. Input impedance and stator current. $Z_{in}=R_1+jX_1+Z_f=9.09+j4.40=10.10\angle25.8^\circ\ \Omega$, so $$I_1=\frac{V_1}{Z_{in}}=\frac{265.6\angle0^\circ}{10.10\angle25.8^\circ}=\boxed{26.3\ \text{A}\ \angle{-25.8^\circ}}$$ a lagging power factor of $\cos 25.8^\circ=0.900$.
  4. Synchronous and shaft speed. $n_s=\dfrac{120f}{p}=\dfrac{120\cdot60}{4}=1800\ \text{rpm}$; the shaft runs at $n_m=(1-s)n_s=0.97\times1800=\boxed{1746\ \text{rpm}}$ ($\omega_m=182.8\ \text{rad/s}$).
  5. Input power and stator copper loss. $P_{in}=\sqrt3\,V_{LL}I_L\cos\theta=\sqrt3(460)(26.3)(0.900)=18.86\ \text{kW}$; $P_{SCL}=3I_1^2R_1=3(26.3)^2(0.641)=1.33\ \text{kW}$.
  6. Air-gap and converted power. Because $jX_m$ absorbs no real power, $P_{AG}=P_{in}-P_{SCL}=17.53\ \text{kW}$, the rotor copper loss is $P_{RCL}=sP_{AG}=0.526\ \text{kW}$, and the developed (converted) power is $P_{conv}=(1-s)P_{AG}=17.01\ \text{kW}$.
  7. Shaft output, torque and efficiency. Subtract the 455 W core (rotational) loss: $$P_{out}=P_{conv}-P_{core}=17.01-0.455=\boxed{16.55\ \text{kW}}$$ $T_{out}=P_{out}/\omega_m=16550/182.8=\boxed{90.5\ \text{N}\cdot\text{m}}$, and $\eta=P_{out}/P_{in}=16.55/18.86=\boxed{87.7\%}$.
Question 2 — results at $s=3\%$
QuantityValue
(a) Stator current $I_1$$26.3\ \text{A}\ \angle{-25.8^\circ}$ (pf 0.900 lag)
(b) Shaft speed $n_m$1746 rpm
(c) Output power $P_{out}$16.55 kW (22.2 hp)
(d) Output torque $T_{out}$$90.5\ \text{N}\cdot\text{m}$
(e) Efficiency $\eta$87.7%