The Linear Momentum of a System of Particles — Question 3

Section 9-4 · Physics pages 1216–1217

Question 3 The frame in which total momentum vanishes A system of mass 8.0 kg has total laboratory momentum (24, −16) kg m/s. x y⃗ Pi⃗ Jext The chosen frame removes the initial center motion; a later external impulse still changes system momentum. (a) Find the velocity of an inertial frame in which its total momentum is zero at that instant. (b) If the system later experiences a constant force (0, 8) N for 2 s, is its momentum still zero in that same frame?
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Question 3 - Solution The frame in which total momentum vanishes x y⃗ Pi⃗ Jext (a) Derivation and calculation Under a fixed inertial-frame shift,⃗ P ′ = ∑ i mi(⃗vi −⃗U) =⃗P −M⃗U.⃗ P ′ i =⃗0 ⇒⃗U = (24, −16) 8 = (3, −2) m/s . (b) Result and interpretation The frame velocity remains fixed after the force begins:⃗ P ′ f =⃗P ′ i + ∫2 0 (0, 8) dt = (0, 16) kg m/s . A frame that continuously follows the accelerating center would no longer be inertial. Physical check The same external impulse changes total momentum by the same amount in both inertial frames.

Question 3

The frame in which total momentum vanishes

A system of mass 8.0kg8.0\,\mathrm{kg} has total laboratory momentum (24,−16)kgm/s(24,-16)\,\mathrm{kg\,m/s}.

Diagram shown in the original SVG worksheet.

  1. Find the velocity of an inertial frame in which its total momentum is zero at that instant.

  2. If the system later experiences a constant force (0,8)N(0,8)\,\mathrm N for 2s2\,\mathrm s, is its momentum still zero in that same frame?

Question 3 - Solution

The frame in which total momentum vanishes

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Under a fixed inertial-frame shift, P→′=∑imi(v→i−U→)=P→−MU→.\vec P^{\prime}=\sum_i m_i(\vec v_i-\vec U)=\vec P-M\vec U. P→i′=0→⇒U→=(24,−16)8=(3,−2)m/s.\vec P_i^{\prime}=\vec0\Rightarrow\boxed{\vec U=\frac{(24,-16)}8=(3,-2)\ \mathrm{m/s}}.

(b) Result and interpretation

The frame velocity remains fixed after the force begins: P→f′=P→i′+∫02(0,8)dt=(0,16)kgm/s.\vec P_f^{\prime}=\vec P_i^{\prime}+\int_0^2(0,8)\,dt =\boxed{(0,16)\ \mathrm{kg\,m/s}}. A frame that continuously follows the accelerating center would no longer be inertial.

Physical check

The same external impulse changes total momentum by the same amount in both inertial frames.