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Induction motor plugging: braking current and torque

Short answer

Initial braking current is 5.0 times full-load current (54.0 A) and braking torque is 0.641 T_fl. To limit maximum braking current to 1.5 times full-load current, insert 53.4 Ω per phase in the rotor circuit (23.7 Ω referred to stator); initial braking torque becomes 1.43 T_fl.

A 400 V, star connected, 3-phase, 6 pole, 50 Hz induction motor with parameters referred to the stator are given below: r1 = r2' = 1 Ω and x1 = x2' = 2 Ω. This motor is to be braked by plugging from initial full load speed of 950 rpm. Stator to rotor turn ratio is 2:3. Find: i) Calculate the initial braking current and torque as the ratio of their full load values. ii) What resistance must be inserted in the rotor circuit to reduce the maximum braking current to 1.5 times full load current? What will be the initial braking torque now?

Data: Vph=400/3=230.94V_{ph} = 400/\sqrt3 = 230.94 V, r1=r2′=1 Ωr_1 = r_2' = 1\ \Omega, x1=x2′=2 Ωx_1 = x_2' = 2\ \Omega, 6 poles, 50 Hz. Magnetising branch neglected (approximate circuit).

Ns=120fP=120×506=1000 rpmsfl=1000−9501000=0.05sb=Ns+NNs=1000+9501000=1.95  (plugging)\begin{aligned} N_s &= \frac{120 f}{P} = \frac{120\times50}{6} = 1000\ \text{rpm} \\ s_{fl} &= \frac{1000-950}{1000} = 0.05 \\ s_b &= \frac{N_s + N}{N_s} = \frac{1000+950}{1000} = 1.95 \ \ (\text{plugging}) \end{aligned}

i) Initial braking current and torque

I=Vph(r1+r2′/s)2+(x1+x2′)2I = \frac{V_{ph}}{\sqrt{(r_1 + r_2'/s)^2 + (x_1+x_2')^2}} Ifl=230.94(1+20)2+42=230.9421.378=10.80 AIb=230.94(1+0.5128)2+42=230.944.276=54.00 AIbIfl=5.00\begin{aligned} I_{fl} &= \frac{230.94}{\sqrt{(1+20)^2 + 4^2}} = \frac{230.94}{21.378} = 10.80\ \text{A} \\ I_b &= \frac{230.94}{\sqrt{(1+0.5128)^2 + 4^2}} = \frac{230.94}{4.276} = 54.00\ \text{A} \\ \frac{I_b}{I_{fl}} &= 5.00 \end{aligned}

Torque T=3I2r2′ωssT = \dfrac{3 I^2 r_2'}{\omega_s s}, so

TbTfl=(IbIfl)2sflsb=5.002×0.051.95=0.641\begin{aligned} \frac{T_b}{T_{fl}} &= \left(\frac{I_b}{I_{fl}}\right)^2 \frac{s_{fl}}{s_b} = 5.00^2 \times \frac{0.05}{1.95} = 0.641 \end{aligned}

Answer (i): Ib=5.0 IflI_b = 5.0\, I_{fl} (54.0 A), Tb=0.641 TflT_b = 0.641\, T_{fl}.

ii) Rotor resistance for Ib=1.5 IflI_b = 1.5\, I_{fl}

The braking current is largest at the start (s=1.95s = 1.95). Required impedance:

Z=230.941.5×10.80=14.25 Ω1+R2′1.95=14.252−42=13.68R2′=24.72 Ω  (total, referred to stator)\begin{aligned} Z &= \frac{230.94}{1.5\times10.80} = 14.25\ \Omega \\ 1 + \frac{R_2'}{1.95} &= \sqrt{14.25^2 - 4^2} = 13.68 \\ R_2' &= 24.72\ \Omega \ \ (\text{total, referred to stator}) \end{aligned}

External resistance referred to stator =24.72−1=23.72 Ω= 24.72 - 1 = 23.72\ \Omega.

Referring to the rotor (stator : rotor turns = 2 : 3, so Rrotor=R′×(3/2)2R_{rotor} = R' \times (3/2)^2):

Rext=23.72×2.25=53.38 Ω per phaseR_{ext} = 23.72 \times 2.25 = 53.38\ \Omega \ \text{per phase}

New initial braking torque:

Tb′Tfl=(1.5Ifl)2(24.72/1.95)Ifl2(1/0.05)=2.25×12.6820=1.43\begin{aligned} \frac{T_b'}{T_{fl}} &= \frac{(1.5 I_{fl})^2 (24.72/1.95)}{I_{fl}^2 (1/0.05)} = \frac{2.25 \times 12.68}{20} = 1.43 \end{aligned}

Answer (ii): insert 53.4 Ω per phase in the rotor (23.7 Ω referred to stator); initial braking torque = 1.43 × full-load torque.

Adding rotor resistance reduces the current but raises the torque, because the rotor power factor improves at high slip.

✓ Answer checked by Claude Opus 5.5 (high effort)

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