Newton's Second Law for a System of Particles — Question 2

Section 9-2 · Physics pages 1174–1175

Question 2 Unequal accelerations can share one center Two particles of 2.0 and 4.0 kg have instantaneous accelerations (3, −1) and (−1, 2) m/s2 in an inertial frame. x y 2 kg⃗ a1 4 kg⃗ a2 The acceleration vectors enter the center equation with their respective mass weights. (a) Find the center acceleration and total external force. (b) Can the net force on each particle be inferred? Can the separate external force on each be inferred without interaction information?
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Question 2 - Solution Unequal accelerations can share one center x y 2 kg⃗ a1 4 kg⃗ a2 (a) Derivation and calculation Form the mass-weighted acceleration: M⃗aC = 2(3, −1) + 4(−1, 2) = (2, 6) N.⃗ aC = (1/3, 1) m/s2 ,⃗ Fext = (2, 6) N . (b) Result and interpretation Each measured acceleration fixes the corresponding total force:⃗ F1,total = (6, −2) N ,⃗ F2,total = (−4, 8) N . But⃗Fi,total =⃗Fi,ext +⃗Fi,int. Without the interaction force, the separate external contributions are not identifiable. Physical check The total particle forces add to the net external force because internal action-reaction pairs cancel.

Question 2

Unequal accelerations can share one center

Two particles of 2.02.0 and 4.0kg4.0\,\mathrm{kg} have instantaneous accelerations (3,−1)(3,-1) and (−1,2)m/s2(-1,2)\,\mathrm{m/s^2} in an inertial frame.

Diagram shown in the original SVG worksheet.

  1. Find the center acceleration and total external force.

  2. Can the net force on each particle be inferred? Can the separate external force on each be inferred without interaction information?

Question 2 - Solution

Unequal accelerations can share one center

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Form the mass-weighted acceleration: Ma→C=2(3,−1)+4(−1,2)=(2,6)N.M\vec a_C=2(3,-1)+4(-1,2)=(2,6)\ \mathrm N. a→C=(1/3,1)m/s2,F→ext=(2,6)N.\boxed{\vec a_C=(1/3,1)\ \mathrm{m/s^2}},\qquad \boxed{\vec F_{\mathrm{ext}}=(2,6)\ \mathrm N}.

(b) Result and interpretation

Each measured acceleration fixes the corresponding total force: F→1,total=(6,−2)N,F→2,total=(−4,8)N.\boxed{\vec F_{1,\mathrm{total}}=(6,-2)\ \mathrm N},\qquad \boxed{\vec F_{2,\mathrm{total}}=(-4,8)\ \mathrm N}. But F→i,total=F→i,ext+F→i,int\vec F_{i,\mathrm{total}}=\vec F_{i,\mathrm{ext}}+\vec F_{i,\mathrm{int}}. Without the interaction force, the separate external contributions are not identifiable.

Physical check

The total particle forces add to the net external force because internal action-reaction pairs cancel.