Newton's Third Law — Question 9

Section 5-7 · Physics pages 748–749

Question 9 A third-law pair cancels even when neither body is in equilibrium In common axes A exerts (3, −4, 2) N on B. A also has external force (1, 2, 0) N; B also has external force (−2, 1, 5) N. A B⃗ FA→B = (3, −4, 2) N⃗ FB→A = −⃗FA→B⃗ Fext,A = (1, 2, 0) N⃗ Fext,B = (−2, 1, 5) N Interaction map; connection arrows identify agent and recipient, not spatial vector directions. (a) Find B’s force on A. (b) Find the individual net forces. (c) Find the combined-system external resultant and verify the cancellation.
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Question 9 - Solution A third-law pair cancels even when neither body is in equilibrium A B⃗ FA→B = (3, −4, 2) N⃗ FB→A = −⃗FA→B⃗ Fext,A = (1, 2, 0) N⃗ Fext,B = (−2, 1, 5) N (a) Reverse every component.⃗ FB→A = −⃗FA→B = (−3, 4, −2) N⃗ FB→A = (−3, 4, −2) N. (b) Add forces for each recipient.⃗ RA = (1, 2, 0) + (−3, 4, −2) = (−2, 6, −2),⃗ RB = (1, −3, 7) N A’s resultant is (1, 2, 0) + (−3, 4, −2) = (−2, 6, −2) N. B’s is (−2, 1, 5) + (3, −4, 2) = (1, −3, 7) N. (c) Sum the body equations.⃗ RA +⃗RB = (−1, 3, 5) = (1, 2, 0) + (−2, 1, 5) N The resultants sum to (−1, 3, 5) N, equal to the sum of the two external forces. The mutual pair cancels regardless of either body’s acceleration or mass.

Question 9

A third-law pair cancels even when neither body is in equilibrium

In common axes A exerts (3,−4,2)(3,-4,2) N on B. A also has external force (1,2,0)(1,2,0) N; B also has external force (−2,1,5)(-2,1,5) N.

Diagram shown in the original SVG worksheet.

  1. Find B’s force on A.

  2. Find the individual net forces.

  3. Find the combined-system external resultant and verify the cancellation.

Question 9 - Solution

A third-law pair cancels even when neither body is in equilibrium

Diagram shown in the original SVG worksheet.

(a) Reverse every component.

F→B→A=−F→A→B=(−3,4,−2)N\boxed{\vec F_{B\to A}=-\vec F_{A\to B}=(-3,4,-2)\,\mathrm N} F→B→A=(−3,4,−2)\vec F_{B\to A}=(-3,4,-2) N.

(b) Add forces for each recipient.

R→A=(1,2,0)+(−3,4,−2)=(−2,6,−2),R→B=(1,−3,7)N\vec R_A=(1,2,0)+(-3,4,-2)=(-2,6,-2),\quad\vec R_B=(1,-3,7)\quad\mathrm N A’s resultant is (1,2,0)+(−3,4,−2)=(−2,6,−2)(1,2,0)+(-3,4,-2)=(-2,6,-2) N. B’s is (−2,1,5)+(3,−4,2)=(1,−3,7)(-2,1,5)+(3,-4,2)=(1,-3,7) N.

(c) Sum the body equations.

R→A+R→B=(−1,3,5)=(1,2,0)+(−2,1,5)N\vec R_A+\vec R_B=(-1,3,5)=(1,2,0)+(-2,1,5)\quad\mathrm N The resultants sum to (−1,3,5)(-1,3,5) N, equal to the sum of the two external forces. The mutual pair cancels regardless of either body’s acceleration or mass.