Torque Revisited — Question 5

Section 11-5 · Physics pages 1640–1641

Question 5 Uniform gravity acts at the center of mass for torque calculations Three particles lie at (0, 0), (2, 0) and (0, 3) m, with masses 1, 2 and 3 kg respectively. Gravity is uniform,⃗g = −10ˆy m/s2. x y 1 kg 2 kg 3 kg Schematic; labels, not drawing lengths, specify the data. (a) Find the gravity torque about the origin by summing particles. (b) Locate the center of mass and verify an equivalent single resultant.
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Question 5 - Solution Uniform gravity acts at the center of mass for torque calculations x y 1 kg 2 kg 3 kg (a) Derivation and calculation Each downward force is⃗Fi = −10miˆy. Thus τz,i = xiFiy = −10mixi, τz = −10[1(0) + 2(2) + 3(0)] = −40 N m . (b) Result and interpretation The total mass and mass-center coordinates are M = 6 kg, xC = 1(0) + 2(2) + 3(0) 6 = 2 3 m, yC = 1(0) + 2(0) + 3(3) 6 = 3 2 m. The resultant⃗Fg = −60ˆy N at C gives⃗ rC ×⃗Fg = −40ˆz N m , consistent with ∑⃗ri × mi⃗g =⃗rC × M⃗g for uniform gravity. Physical check Only horizontal lever arms matter for the moment of vertical gravitational forces.

Question 5

Uniform gravity acts at the center of mass for torque calculations

Three particles lie at (0,0)(0,0), (2,0)(2,0) and (0,3)m(0,3)\,\mathrm m, with masses 11, 22 and 3kg3\,\mathrm{kg} respectively. Gravity is uniform, g→=−10ŷm/s2\vec g=-10\hat y\,\mathrm{m/s^2}.

Diagram shown in the original SVG worksheet.

  1. Find the gravity torque about the origin by summing particles.

  2. Locate the center of mass and verify an equivalent single resultant.

Question 5 - Solution

Uniform gravity acts at the center of mass for torque calculations

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Each downward force is F→i=−10miŷ\vec F_i=-10m_i\hat y. Thus τz,i=xiFiy=−10mixi,\tau_{z,i}=x_iF_{iy}=-10m_ix_i, τz=−10[1(0)+2(2)+3(0)]=−40Nm.\boxed{\tau_z=-10[1(0)+2(2)+3(0)]=-40\ \mathrm{N\,m}}.

(b) Result and interpretation

The total mass and mass-center coordinates are M=6kg,xC=1(0)+2(2)+3(0)6=23m,M=6\ \mathrm{kg},\quad x_C=\frac{1(0)+2(2)+3(0)}6=\frac23\ \mathrm m, yC=1(0)+2(0)+3(3)6=32m.y_C=\frac{1(0)+2(0)+3(3)}6=\frac32\ \mathrm m. The resultant F→g=−60ŷ\vec F_g=-60\hat y N at CC gives r→C×F→g=−40ẑNm,\boxed{\vec r_C\times\vec F_g=-40\hat z\ \mathrm{N\,m}}, consistent with ∑r→i×mig→=r→C×Mg→\sum\vec r_i\times m_i\vec g=\vec r_C\times M\vec g for uniform gravity.

Physical check

Only horizontal lever arms matter for the moment of vertical gravitational forces.