A three-phase Y-connected 220-V (line-to-line) 7.5-kW 60-Hz six-pole induction motor has the following parameter values in Ω/phase referred to the stator:
R_1 = 0.294 \quad R_2 = 0.144 \\X_1 = 0.503 \quad X_2 = 0.209 \quad X_m = 13.25
The total friction, windage, and core losses may be assumed to be constant at 403 W, independent of load.
For a slip of 2 percent, compute the speed, output torque and power, stator current, power factor, and efficiency when the motor is operated at rated voltage and frequency.
Let the impedance Z_f (Fig. 6.11 a) represent the per phase impedance presented to the stator by the magnetizing reactance and the rotor. Thus, from Fig. 6.11 a
Z_f = R_f + jX_f = \left(\frac{R_2}{s} – jX_2\right) \text{in parallel with} j X_m
Substitution of numerical values gives, for s = 0.02,
R_f + jX_f = 5.41 + j3.11 Ω
The stator input impedance can now be calculated as
Z_{in}= R_1 + jX_1 + Z_f = 5.70 + j3.61 = 6.75 ∠32.3° Ω
The line-to-neutral terminal voltage is equal to
V_1= \frac{220}{\sqrt{3}} = 127 V
and hence the stator current can be calculated as
\hat{I}_1 =\frac{V_1}{Z_{in}}= \frac{127}{6.75 ∠32.3°}= 18.8 ∠-32.3° A
The stator current is thus 18.8 A and the power factor is equal to cos (-32.3°) = 0.845 lagging.
The synchronous speed can be found from Eq. 4.41
n_s=\left( \frac{120}{poles}\right)f_e=\left(\frac{120}{6}\right) 60 = 1200 r/min
or from Eq. 6.26
ω_s=\frac{4πf_e}{poles} = \left( \frac{2}{poles}\right)ω_e \quad \quad \quad (6.26)
ω_s=\frac{4πf_e}{poles} = 125.7 rad/sec
The rotor speed is
n = (1 – s)n_s = (0.98)1200 = 1176 r/min
or
ω_m = (1 – s)ω_s = (0.98)125.7 = 123.2 rad/sec
From Eq. 6.17,
P_{gap}=n_{ph}I_2^2 \left( \frac{R_2}{s}\right)
Note however that because the only resistance included in Z_f is R_2/s, the power dissipated in Z_f is equal to the power dissipated in R_2/s and hence we can write
P_{gap} = n_{ph}I_1^2R_f = 3(18.8)^2(5.41) = 5740 W
We can now calculate P_{mech} from Eq. 6.21 and the shaft output power from Eq. 6.27. Thus
P_{mech}= n_{ph} I_2^2 R_2 \left( \frac{1-s}{s}\right) \quad \quad (6.21)
P_{shaft}= P_{mech} – P_{rot} \quad \quad \quad (6.27)
\begin{aligned}P_{shaft}&= P_{mech} – P_{rot} = (1 -s)P_{gap} – P_{rot}\\ &= (0.98)5740 – 403 = 5220 W\end{aligned}
and the shaft output torque can be found from Eq. 6.28 as
T_{shaft}=\frac{P_{shaft}}{ω_m}= T_{mech} – T_{rot} (6.28)
T_{shaft}=\frac{P_{shaft}}{ω_m}=\frac{5220}{123.2} = 42.4 N. m
The efficiency is calculated as the ratio of shaft output power to stator input power. The input power is given by
\begin{aligned}P_{in} & = n_{ph}Re[\hat{V}_1 \hat{I}_1^*] = 3Re[127(18.8 ∠32.3°)] \\ & = 3 × 127 × 18.8 \cos (32.2°) = 6060 W \end{aligned}
Thus the efficiency η is equal to
η=\frac{P_{shaft}}{P_{in}}=\frac{5220}{6060} = 0.861 = 86.1\%
The complete performance characteristics of the motor can be determined by repeating these calculations for other assumed values of slip.