The Center of Mass — Question 5

Section 9-1 · Physics pages 1160–1161

Question 5 Reassembling grouped masses A 6.0 kg assembly has center (1, 2) m and a 4.0 kg assembly has center (6, −3) m. Their internal shapes are unspecified. x y 6 kg 4 kg (1, 2) (6, −3) Each extended assembly is represented by its mass at its own center; coordinates are in meters. (a) Find the center of mass of both assemblies together. (b) The first assembly is reshaped without moving its own center. Can the overall center change? Prove your answer.
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Question 5 - Solution Reassembling grouped masses x y 6 kg 4 kg (1, 2) (6, −3) (a) Derivation and calculation The group centers contain all required first-moment information: M = 6 + 4 = 10 kg, M⃗R = 6(1, 2) + 4(6, −3) = (30, 0) kg m.⃗ R = (3, 0) m . (b) Result and interpretation For any grouping of particles, ∑ i mi⃗ri = ∑ g ∑ i∈g mi⃗ri = ∑ g Mg⃗Rg. Reshaping a group with fixed mass and fixed group center leaves this sum unchanged. Therefore ∆⃗R =⃗0 . Physical check The combined center divides the line between the two group centers in the inverse ratio of their masses.

Question 5

Reassembling grouped masses

A 6.0kg6.0\,\mathrm{kg} assembly has center (1,2)m(1,2)\,\mathrm m and a 4.0kg4.0\,\mathrm{kg} assembly has center (6,−3)m(6,-3)\,\mathrm m. Their internal shapes are unspecified.

Diagram shown in the original SVG worksheet.

  1. Find the center of mass of both assemblies together.

  2. The first assembly is reshaped without moving its own center. Can the overall center change? Prove your answer.

Question 5 - Solution

Reassembling grouped masses

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The group centers contain all required first-moment information: M=6+4=10kg,MR→=6(1,2)+4(6,−3)=(30,0)kgm.M=6+4=10\ \mathrm{kg},\qquad M\vec R=6(1,2)+4(6,-3)=(30,0)\ \mathrm{kg\,m}. R→=(3,0)m.\boxed{\vec R=(3,0)\ \mathrm m}.

(b) Result and interpretation

For any grouping of particles, ∑imir→i=∑g∑i∈gmir→i=∑gMgR→g.\sum_i m_i\vec r_i=\sum_g\sum_{i\in g}m_i\vec r_i =\sum_g M_g\vec R_g. Reshaping a group with fixed mass and fixed group center leaves this sum unchanged. Therefore ΔR→=0→\Delta\vec R=\boxed{\vec0}.

Physical check

The combined center divides the line between the two group centers in the inverse ratio of their masses.