Torque Revisited — Question 8

Section 11-5 · Physics pages 1646–1647

Question 8 Some force systems have torque that no origin shift removes A force system has resultant⃗F = 5ˆz N and moment⃗τO = (2, 3, 4) N m. For an origin shifted by⃗a, use⃗τA =⃗τO −⃗a ×⃗F.⃗ F = 5ˆz τ∥ˆz⃗ τ⊥⃗ τO resultant An origin shift can remove transverse moment but cannot change the component parallel to the force. (a) Can any origin make the total torque zero? (b) Find an origin shift that removes the transverse torque components.
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Question 8 - Solution Some force systems have torque that no origin shift removes⃗ F = 5ˆz τ∥ˆz⃗ τ⊥⃗ τO resultant (a) Derivation and calculation For any origin shift,⃗ τA =⃗τO −⃗a ×⃗F. The subtracted term is perpendicular to⃗F = 5ˆz, so τA,z = τO,z = 4 N m . No origin makes the full torque zero. Equivalently, the invariant⃗τA ·⃗F = 20 N2 m̸ = 0 proves impossibility. (b) Result and interpretation Write⃗a = (ax, ay, az). Then⃗ a ×⃗F = (5ay, −5ax, 0). Choose 5ay = 2 and −5ax = 3: ax = −.600 m, ay = .400 m, az arbitrary . The residual torque is⃗τA = 4ˆz N m . Physical check Shifts along the resultant force leave the torque unchanged, explaining the arbitrary az.

Question 8

Some force systems have torque that no origin shift removes

A force system has resultant F→=5ẑN\vec F=5\hat z\,\mathrm N and moment τ→O=(2,3,4)Nm\vec\tau_O=(2,3,4)\,\mathrm{N\,m}. For an origin shifted by a→\vec a, use τ→A=τ→O−a→×F→\vec\tau_A=\vec\tau_O-\vec a\times\vec F.

Diagram shown in the original SVG worksheet.

  1. Can any origin make the total torque zero?

  2. Find an origin shift that removes the transverse torque components.

Question 8 - Solution

Some force systems have torque that no origin shift removes

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For any origin shift, τ→A=τ→O−a→×F→.\vec\tau_A=\vec\tau_O-\vec a\times\vec F. The subtracted term is perpendicular to F→=5ẑ\vec F=5\hat z, so τA,z=τO,z=4Nm.\boxed{\tau_{A,z}=\tau_{O,z}=4\ \mathrm{N\,m}}. No origin makes the full torque zero. Equivalently, the invariant τ→A⋅F→=20N2m≠0\vec\tau_A\cdot\vec F=20\ \mathrm{N^2\,m}\ne0 proves impossibility.

(b) Result and interpretation

Write a→=(ax,ay,az)\vec a=(a_x,a_y,a_z). Then a→×F→=(5ay,−5ax,0).\vec a\times\vec F=(5a_y,-5a_x,0). Choose 5ay=25a_y=2 and −5ax=3-5a_x=3: ax=−.600m,ay=.400m,azarbitrary.\boxed{a_x=-.600\ \mathrm m,\qquad a_y=.400\ \mathrm m,\qquad a_z\ \text{arbitrary}}. The residual torque is τ→A=4ẑNm\boxed{\vec\tau_A=4\hat z\ \mathrm{N\,m}}.

Physical check

Shifts along the resultant force leave the torque unchanged, explaining the arbitrary aza_z.