Work and Rotational Kinetic Energy — Question 6

Section 10-9 · Physics pages 1542–1543

Question 6 Shaft power and electrical input are different quantities A motor delivers 120 W of mechanical shaft power at steady angular speed 20 rad/s. Its electrical-to-mechanical efficiency is 0.80. The only mechanical load is a resisting torque. motor Pelec 120 W shaft motor loss Electrical input splits into mechanical shaft output and internal motor losses. (a) Find shaft torque, electrical input power and motor loss rate. (b) If the same mechanical power is delivered at 10 rad/s, what torque is required? Does the original steady load automatically permit that operating point?
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Question 6 - Solution Shaft power and electrical input are different quantities motor Pelec 120 W shaft motor loss (a) Derivation and calculation At steady speed, shaft power is torque times angular velocity: τ = Pshaft ω = 120 20 = 6.0 N m . Pelec = Pshaft η = 120 0.80 = 150 W , Ploss = 150 −120 = 30 W . (b) Result and interpretation At the lower rate with the same mechanical power, τ10 = 120 10 = 12 N m . Steady operation requires τload = −12 N m. Retaining only a −6 N m load leaves τnet = +6 N m and causes acceleration. Physical check Power and speed determine the delivered torque, but a matching load is also needed for equilibrium.

Question 6

Shaft power and electrical input are different quantities

A motor delivers 120W120\,\mathrm W of mechanical shaft power at steady angular speed 20rad/s20\,\mathrm{rad/s}. Its electrical-to-mechanical efficiency is 0.800.80. The only mechanical load is a resisting torque.

Diagram shown in the original SVG worksheet.

  1. Find shaft torque, electrical input power and motor loss rate.

  2. If the same mechanical power is delivered at 10rad/s10\,\mathrm{rad/s}, what torque is required? Does the original steady load automatically permit that operating point?

Question 6 - Solution

Shaft power and electrical input are different quantities

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

At steady speed, shaft power is torque times angular velocity: τ=Pshaftω=12020=6.0Nm.\boxed{\tau=\frac{P_{\mathrm{shaft}}}\omega=\frac{120}{20}=6.0\ \mathrm{N\,m}}. Pelec=Pshaftη=1200.80=150W,Ploss=150−120=30W.\boxed{P_{\mathrm{elec}}=\frac{P_{\mathrm{shaft}}}\eta=\frac{120}{0.80}=150\ \mathrm W},\qquad \boxed{P_{\mathrm{loss}}=150-120=30\ \mathrm W}.

(b) Result and interpretation

At the lower rate with the same mechanical power, τ10=12010=12Nm.\boxed{\tau_{10}=\frac{120}{10}=12\ \mathrm{N\,m}}. Steady operation requires τload=−12\tau_{\mathrm{load}}=-12 N m. Retaining only a −6-6 N m load leaves τnet=+6\tau_{\mathrm{net}}=+6 N m and causes acceleration.

Physical check

Power and speed determine the delivered torque, but a matching load is also needed for equilibrium.