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Shunt motor speed with series armature resistance

Short answer

With flux constant and a1 Ω series armature resistance: (i) at half-load torque, armature current remains 25 A, back emf drops to 205 V, giving 534.8 rpm; (ii) at full-load torque, armature current doubles to 50 A, back emf falls to 170 V, giving 443.5 rpm.

A 240 V dc shunt motor has armature winding resistance of 0.4 Ω0.4\ \Omega and field winding resistance of 120 Ω120\ \Omega. It draws a current of 27 A at half load and the corresponding speed is 600 rpm. i) If a resistance of 1 Ω1\ \Omega connected in series with the armature winding keeping the load torque constant to half load torque, calculate the new speed. ii) If a resistance of 1 Ω1\ \Omega connected in series with the armature winding and the load torque is increased to full load torque, calculate the new speed.

The flux is constant (shunt field across the supply), so torque ∝Ia\propto I_a and speed ∝Eb\propto E_b.

Field current: If=240/120=2I_f = 240/120 = 2 A.

Half-load condition:

Ia1=27−2=25 A,Eb1=240−25(0.4)=230 V,N1=600 rpmI_{a1} = 27 - 2 = 25\ \text{A}, \qquad E_{b1} = 240 - 25(0.4) = 230\ \text{V}, \qquad N_1 = 600\ \text{rpm}

With the extra 1 Ω, the armature circuit resistance is 0.4+1=1.4 Ω0.4 + 1 = 1.4\ \Omega.

(i) Load torque constant at half-load value

The torque is unchanged, so Ia2=Ia1=25I_{a2} = I_{a1} = 25 A.

Eb2=240−25(1.4)=205 VE_{b2} = 240 - 25(1.4) = 205\ \text{V} N2=600×205230=534.8 rpmN_2 = 600\times\frac{205}{230} = 534.8\ \text{rpm}

(ii) Load torque increased to full-load torque

Full-load torque is twice the half-load torque, so

Ia2=2×25=50 AI_{a2} = 2\times 25 = 50\ \text{A} Eb2=240−50(1.4)=170 VE_{b2} = 240 - 50(1.4) = 170\ \text{V} N2=600×170230=443.5 rpmN_2 = 600\times\frac{170}{230} = 443.5\ \text{rpm}

Answer: (i) 534.8 rpm534.8\ \text{rpm}; (ii) 443.5 rpm443.5\ \text{rpm}.

✓ Answer checked by Claude Opus 5.5 (high effort)

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