Newton's Second Law — Question 7

Section 5-5 · Physics pages 704–705

Question 7 An accelerating coordinate system changes the equation’s form A 2 kg particle has physical horizontal net force +6 N in inertial frame G. Observer B accelerates at +1 m/s2 relative to G with nonrotating parallel axes. 2 kg Fphysical = 6 N B aB/G = 1 m/s2 The dashed observer frame accelerates right relative to inertial G. (a) Find the particle’s acceleration in G and relative to B. (b) Compare maP/B with the physical force. (c) What extra effective term would make the equation work in B?
Show solutionHide solution
Question 7 - Solution An accelerating coordinate system changes the equation’s form 2 kg Fphysical = 6 N B aB/G = 1 m/s2 (a) Apply the law in the inertial frame first. aP/G = 6/2 = 3, aP/B = aP/G −aB/G = 3 −1 = 2 m/s2 aP/G = 6/2 = 3 m/s2. Relative acceleration is aP/B = 3 −1 = 2 m/s2. (b) Identify the mismatch. maP/B = 2(2) = 4 N̸ = Fphysical = 6 N maP/B = 4 N, whereas the physical net force is 6 N. Substituting an accelerating observer’s coordinate acceleration directly into the inertial equation is invalid. (c) Subtract the frame acceleration term. maP/B = Fphysical −maB/G = 6 −2(1) = 4 N maP/B = Fphysical −maB/G = 6 −2 = 4 N. The effective −2 N term arises from the chosen coordinates, not a newly identified physical agent acting on the particle.

Question 7

An accelerating coordinate system changes the equation’s form

A 2 kg particle has physical horizontal net force +6 N in inertial frame G. Observer B accelerates at +1 m/s2^2 relative to G with nonrotating parallel axes.

Diagram shown in the original SVG worksheet.

  1. Find the particle’s acceleration in G and relative to B.

  2. Compare maP/Bm a_{P/B} with the physical force.

  3. What extra effective term would make the equation work in B?

Question 7 - Solution

An accelerating coordinate system changes the equation’s form

Diagram shown in the original SVG worksheet.

(a) Apply the law in the inertial frame first.

aP/G=6/2=3,aP/B=aP/G−aB/G=3−1=2m/s2a_{P/G}=6/2=3,\quad\boxed{a_{P/B}=a_{P/G}-a_{B/G}=3-1=2\,\mathrm{m/s^2}} aP/G=6/2=3a_{P/G}=6/2=3 m/s2^2. Relative acceleration is aP/B=3−1=2a_{P/B}=3-1=2 m/s2^2.

(b) Identify the mismatch.

maP/B=2(2)=4N≠Fphysical=6Nma_{P/B}=2(2)=4\,\mathrm N\ne F_{\mathrm{physical}}=6\,\mathrm N maP/B=4ma_{P/B}=4 N, whereas the physical net force is 6 N. Substituting an accelerating observer’s coordinate acceleration directly into the inertial equation is invalid.

(c) Subtract the frame acceleration term.

maP/B=Fphysical−maB/G=6−2(1)=4Nma_{P/B}=F_{\mathrm{physical}}-ma_{B/G}=6-2(1)=4\,\mathrm N maP/B=Fphysical−maB/G=6−2=4m a_{P/B}=F_{\mathrm{physical}}-m a_{B/G}=6-2=4 N. The effective −2-2 N term arises from the chosen coordinates, not a newly identified physical agent acting on the particle.