Linear Momentum — Question 4

Section 9-3 · Physics pages 1198–1199

Question 4 One velocity shift changes both momentum components A 3.0 kg particle has laboratory velocity (4, −2) m/s. Another inertial frame moves at (1, 3) m/s relative to the lab with parallel axes. x y⃗ v⃗ U⃗ v′ The velocity triangle expresses the Galilean relation between two inertial frames. (a) Find the momentum in both frames. (b) If the particle feels (6, 0) N, compare d⃗p/dt in the two frames.
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Question 4 - Solution One velocity shift changes both momentum components x y⃗ v⃗ U⃗ v′ (a) Derivation and calculation Compute momentum in each inertial frame:⃗ p = 3(4, −2) = (12, −6) kg m/s .⃗ v′ =⃗v −⃗U = (3, −5),⃗ p′ = 3(3, −5) = (9, −15) kg m/s . (b) Result and interpretation Because both m and the frame velocity are constant, d⃗p′ dt = d dt(⃗p −m⃗U) = d⃗p dt = (6, 0) N . Momenta differ, but their time derivatives agree in these Newtonian inertial frames. Physical check The difference⃗p −⃗p′ = m⃗U = (3, 9) kg m/s is constant.

Question 4

One velocity shift changes both momentum components

A 3.0kg3.0\,\mathrm{kg} particle has laboratory velocity (4,−2)m/s(4,-2)\,\mathrm{m/s}. Another inertial frame moves at (1,3)m/s(1,3)\,\mathrm{m/s} relative to the lab with parallel axes.

Diagram shown in the original SVG worksheet.

  1. Find the momentum in both frames.

  2. If the particle feels (6,0)N(6,0)\,\mathrm N, compare dp→/dtd\vec p/dt in the two frames.

Question 4 - Solution

One velocity shift changes both momentum components

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Compute momentum in each inertial frame: p→=3(4,−2)=(12,−6)kgm/s.\boxed{\vec p=3(4,-2)=(12,-6)\ \mathrm{kg\,m/s}}. v→′=v→−U→=(3,−5),p→′=3(3,−5)=(9,−15)kgm/s.\vec v^{\prime}=\vec v-\vec U=(3,-5),\qquad \boxed{\vec p^{\prime}=3(3,-5)=(9,-15)\ \mathrm{kg\,m/s}}.

(b) Result and interpretation

Because both mm and the frame velocity are constant, dp→′dt=ddt(p→−mU→)=dp→dt=(6,0)N.\frac{d\vec p^{\prime}}{dt}=\frac{d}{dt}(\vec p-m\vec U) =\frac{d\vec p}{dt}=\boxed{(6,0)\ \mathrm N}. Momenta differ, but their time derivatives agree in these Newtonian inertial frames.

Physical check

The difference p→−p→′=mU→=(3,9)\vec p-\vec p^{\prime}=m\vec U=(3,9) kg m/s is constant.