Torque — Question 10

Section 10-7 · Physics pages 1510–1511

Question 10 Changing the moment origin exposes a nonzero resultant A planar force system has resultant⃗Fnet = (4, 6) N and torque τO,z = 10 N m about the origin. A new origin is at⃗a = (1, 2) m. x y zero-moment line A = (1, 2)⃗ Fnet The zero-moment origins lie on a line parallel to the resultant; drawing coordinates are schematic. (a) Find torque about the new origin. (b) Find the locus of origins about which the torque is zero.
Show solutionHide solution
Question 10 - Solution Changing the moment origin exposes a nonzero resultant x y zero-moment line A = (1, 2)⃗ Fnet (a) Derivation and calculation Translate all position vectors by −⃗a:⃗ τA = ∑ (⃗ri −⃗a) ×⃗Fi =⃗τO −⃗a ×⃗Fnet. τA,z = 10 −[1(6) −2(4)] = 12 N m . (b) Result and interpretation For a general origin (ax, ay), set the new moment to zero: 10 −(6ax −4ay) = 0 ⇒6ax −4ay = 10 . Its normal (6, −4) is perpendicular to the resultant (4, 6) because 6(4) −4(6) = 0. The moment depends on origin when the resultant is nonzero. Physical check Shifting any origin along the resultant direction leaves its moment unchanged.

Question 10

Changing the moment origin exposes a nonzero resultant

A planar force system has resultant F→net=(4,6)N\vec F_{\mathrm{net}}=(4,6)\,\mathrm N and torque τO,z=10Nm\tau_{O,z}=10\,\mathrm{N\,m} about the origin. A new origin is at a→=(1,2)m\vec a=(1,2)\,\mathrm m.

Diagram shown in the original SVG worksheet.

  1. Find torque about the new origin.

  2. Find the locus of origins about which the torque is zero.

Question 10 - Solution

Changing the moment origin exposes a nonzero resultant

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Translate all position vectors by −a→-\vec a: τ→A=∑(r→i−a→)×F→i=τ→O−a→×F→net.\vec\tau_A=\sum(\vec r_i-\vec a)\times\vec F_i =\vec\tau_O-\vec a\times\vec F_{\mathrm{net}}. τA,z=10−[1(6)−2(4)]=12Nm.\boxed{\tau_{A,z}=10-[1(6)-2(4)]=12\ \mathrm{N\,m}}.

(b) Result and interpretation

For a general origin (ax,ay)(a_x,a_y), set the new moment to zero: 10−(6ax−4ay)=0⇒6ax−4ay=10.10-(6a_x-4a_y)=0\Rightarrow\boxed{6a_x-4a_y=10}. Its normal (6,−4)(6,-4) is perpendicular to the resultant (4,6)(4,6) because 6(4)−4(6)=06(4)-4(6)=0. The moment depends on origin when the resultant is nonzero.

Physical check

Shifting any origin along the resultant direction leaves its moment unchanged.