Question 17.1: Induction-Motor Performance A certain 30-hp four-pole 440-V-...

Induction-Motor Performance
A certain 30-hp four-pole 440-V-rms 60-Hz three-phase delta-connected induction motor has

Rs = 1.2 Ω               R’r = 0.6 Ω

Xs = 2.0 Ω               X’r = 0.8 Ω

Xm = 50 Ω

Under load, the machine operates at 1746 rpm and has rotational losses of 900W. Find the power factor, the line current, the output power, copper losses, output torque, and efficiency.

The blue check mark means that this solution has been answered and checked by an expert. This guarantees that the final answer is accurate.
Learn more on how we answer questions.

From Table 17.1, we find that synchronous speed for a four-pole motor is ns = 1800 rpm. Then, we utilize Equation 17.16 to compute the slip:

s=\frac{\omega_s-\omega_m }{\omega_s}=\frac{n_s-n_m}{n_s}                (17.16)

s= \frac{n_s-n_m}{n_s} =\frac{1800-1746}{1800}=0.03

We can use the data given to draw the equivalent circuit shown in Figure 17.14 for one phase of the motor. The impedance seen by the source is

Z_s=1.2+j2+\frac{j50(0.6+19.4+j0.8)}{j50+0.6+19.4+j0.8}=1.2+j2+16.77+j7.392 =17.97+j9.392=20.28\angle 27.59^\circ \Omega

The power factor is the cosine of the impedance angle. Because the impedance is inductive, we know that the power factor is lagging:

power factor = cos(27.59°) = 88.63% lagging

For a delta-connected machine, the phase voltage is equal to the line voltage, which is specified to be 440V rms. The phase current is

\mathrm{I}_s =\frac{\mathrm{V}_s}{Z_s}=\frac{440\angle 0^\circ}{20.28\angle 27.59^\circ}=21.70\angle -27.59^\circ \mathrm{~A~rms}

Thus, the magnitude of the line current is

I_{\mathrm{line}}=I_s\sqrt{3}=21.70\sqrt{3}=37.59\mathrm{~A~rms}

The input power is

P_{\mathrm{in}}=3I_sV_s\cos{\theta}=3(21.70)440 \cos{(27.59^\circ)}=25.38\mathrm{~kW}

Next, we compute Vx and Ir:

\mathrm{V}_x=\mathrm{I}_s\frac{j50(0.6+19.4+j0.8)}{j50+0.6+19.4+j0.8}=21.70\angle -27.59^\circ \times 18.33\angle 23.78^\circ =397.8\angle -3.807^\circ \mathrm{~V~rms}

\mathrm{I}'_r=\frac{\mathrm{V}_x}{j0.8+0.6+19.4}=\frac{397.8\angle -3.807^\circ}{20.01\angle 1.718^\circ}=19.88\angle -5.52^\circ\mathrm{~A~rms}

The copper losses in the stator and rotor are

P_s=3R_sI_s^2=3(1.2)(21.70)^2=1695\mathrm{~W}

and

P_r=3R'_r(I'_r)^2=711.4\mathrm{~W}

Finally, the developed power is

P_{\mathrm{dev}}=3 \times \frac{1-s}{s}R'_r(I'_r)^2=3(19.4)(19.88)^2=23.00\mathrm{~kW}

As a check, we note that

P_{\mathrm{in}}=P_{\mathrm{dev}}+P_s+P_r

to within rounding error.
The output power is the developed power minus the rotational loss, given by

P_{\mathrm{out}}=P_{\mathrm{dev}}-P_{\mathrm{rot}}=23.00-0.900=22.1 \mathrm{~kW}

This corresponds to 29.62 hp, so the motor is operating at nearly its rated load. The output torque is

T_{\mathrm{out}}=\frac{P_{\mathrm{out}}}{\omega_{m}}=\frac{22,100}{1746(2\pi/60)}=120.9\mathrm{Nm}

The efficiency is

\eta =\frac{P_\mathrm{out}}{P_{\mathrm{in}}}\times 100%=\frac{22,100}{25,380}\times 100%=87.0%

Table 17.1. Synchronous Speed versus Number of Poles for f = 60 Hz

P

n_s

2

3600

4

1800

6

1200

8

900

10

720

12

600

17.14

Related Answered Questions