Torque — Question 6

Section 10-7 · Physics pages 1502–1503

Question 6 Only the torque component along a fixed axis drives that axis A force⃗F = (0, 5, −1) N acts at⃗r = (1, 2, 3) m on a body mounted on a fixed z shaft. x y z⃗ r⃗ F τz Oblique schematic: a force creates a full torque vector, but the shaft selects its axial component. (a) Find the full torque vector and its z component. (b) Explain why using the torque magnitude in a scalar equation for rotation about z would be wrong.
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Question 6 - Solution Only the torque component along a fixed axis drives that axis x y z⃗ r⃗ F τz (a) Derivation and calculation Expand the cross product component by component:⃗ τ = (yFz −zFy, zFx −xFz, xFy −yFx ).⃗ τ = (2(−1) −3(5), 3(0) −1(−1), 1(5) −2(0)) = (−17, 1, 5) N m . (b) Result and interpretation The fixed-z rotational equation uses the projection: τz =⃗τ · ˆz = 5 N m , |⃗τ| = √ (−17)2 + 12 + 52 = √ 315 N m. Transverse components are not moments driving the permitted z rotation. Shaft supports constrain the other rotations and can supply reaction moments. Physical check Projection retains the sign and axis information that a nonnegative magnitude would discard.

Question 6

Only the torque component along a fixed axis drives that axis

A force F→=(0,5,−1)N\vec F=(0,5,-1)\,\mathrm N acts at r→=(1,2,3)m\vec r=(1,2,3)\,\mathrm m on a body mounted on a fixed zz shaft.

Diagram shown in the original SVG worksheet.

  1. Find the full torque vector and its zz component.

  2. Explain why using the torque magnitude in a scalar equation for rotation about zz would be wrong.

Question 6 - Solution

Only the torque component along a fixed axis drives that axis

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Expand the cross product component by component: τ→=(yFz−zFy,zFx−xFz,xFy−yFx).\vec\tau=\bigl(yF_z-zF_y,\ zF_x-xF_z,\ xF_y-yF_x\bigr). τ→=(2(−1)−3(5),3(0)−1(−1),1(5)−2(0))=(−17,1,5)Nm.\boxed{\vec\tau=(2(-1)-3(5),\ 3(0)-1(-1),\ 1(5)-2(0)) =(-17,1,5)\ \mathrm{N\,m}}.

(b) Result and interpretation

The fixed-zz rotational equation uses the projection: τz=τ→⋅ẑ=5Nm,|τ→|=(−17)2+12+52=315Nm.\boxed{\tau_z=\vec\tau\cdot\hat z=5\ \mathrm{N\,m}},\qquad |\vec\tau|=\sqrt{(-17)^2+1^2+5^2}=\sqrt{315}\ \mathrm{N\,m}. Transverse components are not moments driving the permitted zz rotation. Shaft supports constrain the other rotations and can supply reaction moments.

Physical check

Projection retains the sign and axis information that a nonnegative magnitude would discard.