Torque on a Current Loop — Question 9

Section 28-8 · Physics pages 4628–4629

Question 9 Current commutation produces a nonzero mean torque over a full revolution A motor coil has peak torque tau0=NIAB. With fixed current direction its signed torque about the shaft is τ0 sin θ. An ideal commutator reverses the current whenever needed so that the driving torque is τ0| sin θ|. θ τ π 2π τ0 Schematic; labels, not drawing lengths, specify the data. (a) Find the angle-averaged torque with and without commutation. (b) Find the mechanical work per revolution with commutation and explain where that energy is supplied.
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Question 9 - Solution Current commutation produces a nonzero mean torque over a full revolution θ τ π 2π τ0 (a) Method and calculation ⟨τ⟩fixed = 1 2π ∫2π 0 τ0 sin θ dθ = 0. ⟨τ⟩comm = τ0 2π ∫2π 0 | sin θ| dθ = 2τ0 π . (b) Interpretation and further calculation Wturn = ∫2π 0 τ0| sin θ| dθ = 4τ0. Welectrical ≥Wturn with equality only when losses are absent. The maintained-current source supplies this energy through the motor circuit. Physical check The average is over angle; it equals a time average only for uniform rotational speed.

Question 9

Current commutation produces a nonzero mean torque over a full revolution

A motor coil has peak torque tau0=NIAB. With fixed current direction its signed torque about the shaft is τ0sin⁡θ\tau_0\sin\theta. An ideal commutator reverses the current whenever needed so that the driving torque is τ0|sin⁡θ|\tau_0|\sin\theta|.

Diagram shown in the original SVG worksheet.

  1. Find the angle-averaged torque with and without commutation.

  2. Find the mechanical work per revolution with commutation and explain where that energy is supplied.

Question 9 - Solution

Current commutation produces a nonzero mean torque over a full revolution

Diagram shown in the original SVG worksheet.

(a) Method and calculation

⟨τ⟩fixed=12π∫02πτ0sin⁡θdθ=0.\langle\tau\rangle_{\mathrm{fixed}}=\frac1{2\pi}\int_0^{2\pi}\tau_0\sin\theta\,d\theta=0.⟨τ⟩comm=τ02π∫02π|sin⁡θ|dθ=2τ0π.\langle\tau\rangle_{\mathrm{comm}}=\frac{\tau_0}{2\pi}\int_0^{2\pi}|\sin\theta|\,d\theta=\frac{2\tau_0}{\pi}.

(b) Interpretation and further calculation

Wturn=∫02πτ0|sin⁡θ|dθ=4τ0.W_{\mathrm{turn}}=\int_0^{2\pi}\tau_0|\sin\theta|\,d\theta=4\tau_0.Welectrical≥Wturnwith equality only when losses are absent.W_{\mathrm{electrical}}\ge W_{\mathrm{turn}}\quad\text{with equality only when losses are absent}.The maintained-current source supplies this energy through the motor circuit.

Physical check

The average is over angle; it equals a time average only for uniform rotational speed.