Acceleration — Question 8

Section 2-5 · Physics pages 226–227

Question 8 An accelerating reference contributes its own acceleration A cart moves along a platform parallel to a ground-fixed east-positive line. The platform origin has ground position XO(t) = t2, while the cart has platform-relative coordinate x′(t) = 8t −2t2. Both axes point east. In these expressions t is numerical seconds and positions are numerical metres, over 0 ≤t ≤3. At every event the cart’s ground position satisfies X(t) = XO(t) + x′(t). Use v = dx/dt and a = dv/dt in the appropriate reference. This is a coordinate comparison; no force law is required. east ground origin platform origin cart XO(t) x′(t) X(t) = XO(t) + x′(t) Schematic same-event coordinate decomposition; both coordinate axes point east. (a) Find the cart’s ground position function, its ground velocity and acceleration, and its platform-relative velocity and acceleration. (b) Derive the acceleration relation connecting the two references and the platform origin. Check it numerically. (c) At 1 s and 3 s, compare the cart’s motion direction and whether it is speeding up or slowing down in each reference. Use the smooth polynomial extensions at the endpoint if needed. (d) A student claims that acceleration is unchanged by any moving origin because a change of origin cancels in differences. Identify the missing distinction. Would a fixed origin offset or an origin moving with constant velocity contribute acceleration?
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Question 8 - Solution An accelerating reference contributes its own acceleration east ground origin platform origin cart XO(t) x′(t) X(t) = XO(t) + x′(t) (a) Combine positions before describing the ground motion. X(t) = 8t −t2 m , vX(t) = 8 −2t m/s , aX = −2 m/s2 . The numerical-time convention applies to these formulas. Relative to the platform, v′(t) = 8 −4t m/s , a′ = −4 m/s2 . (b) Differentiate the same-event coordinate relation twice. The first derivative gives vX = vO + v′. The second gives aX = aO + a′ . Here XO = t2 implies aO = +2 m/s2, so −2 = +2 + (−4) in m/s2. The nonzero acceleration of the origin supplies the difference between the cart’s two reported accelerations. (c) Compare velocity with acceleration in each reference. t = 1 : vXaX = 6(−2) < 0, v′a′ = 4(−4) < 0, t = 3 : vXaX = 2(−2) < 0, v′a′ = (−4)(−4) > 0. At 1 s, the ground velocity is +6 m/s and the local velocity is +4 m/s. Both descriptions are eastward with negative acceleration, hence decreasing speed. At 3 s, the ground velocity is +2 m/s, so the cart still moves east and slows relative to the ground. The local velocity is −4 m/s; together with local acceleration −4 m/s2, this means westward motion with increasing speed relative to the platform. These statements describe different reference histories and are compatible. (d) A time-dependent origin is not a fixed offset. A fixed spatial offset has zero first and second derivatives. An origin moving with constant velocity has a nonzero first derivative but zero second derivative, so it contributes no acceleration. An accelerating origin has a nonzero second derivative and cannot be removed as a constant. The student’s cancellation argument applies only to the appropriate time-independent or constant-velocity transformations, not to every moving reference.

Question 8

An accelerating reference contributes its own acceleration

A cart moves along a platform parallel to a ground-fixed east-positive line. The platform origin has ground position XO(t)=t2X_O(t)=t^2, while the cart has platform-relative coordinate x′(t)=8t−2t2x'(t)=8t-2t^2. Both axes point east. In these expressions tt is numerical seconds and positions are numerical metres, over 0≤t≤30\leq t\leq3.

At every event the cart’s ground position satisfies X(t)=XO(t)+x′(t).X(t)=X_O(t)+x'(t). Use v=dx/dtv=dx/dt and a=dv/dta=dv/dt in the appropriate reference. This is a coordinate comparison; no force law is required.

Diagram shown in the original SVG worksheet.

  1. Find the cart’s ground position function, its ground velocity and acceleration, and its platform-relative velocity and acceleration.

  2. Derive the acceleration relation connecting the two references and the platform origin. Check it numerically.

  3. At 1 s and 3 s, compare the cart’s motion direction and whether it is speeding up or slowing down in each reference. Use the smooth polynomial extensions at the endpoint if needed.

  4. A student claims that acceleration is unchanged by any moving origin because a change of origin cancels in differences. Identify the missing distinction. Would a fixed origin offset or an origin moving with constant velocity contribute acceleration?

Question 8 - Solution

An accelerating reference contributes its own acceleration

Diagram shown in the original SVG worksheet.

(a) Combine positions before describing the ground motion.

X(t)=8t−t2m,vX(t)=8−2tm/s,aX=−2m/s2.\boxed{X(t)=8t-t^2\ \mathrm{m}},\qquad \boxed{v_X(t)=8-2t\ \mathrm{m/s}},\qquad \boxed{a_X=-2\ \mathrm{m/s^2}}. The numerical-time convention applies to these formulas. Relative to the platform, v′(t)=8−4tm/s,a′=−4m/s2.\boxed{v'(t)=8-4t\ \mathrm{m/s}},\qquad \boxed{a'=-4\ \mathrm{m/s^2}}.

(b) Differentiate the same-event coordinate relation twice.

The first derivative gives vX=vO+v′v_X=v_O+v'. The second gives aX=aO+a′.\boxed{a_X=a_O+a'}. Here XO=t2X_O=t^2 implies aO=+2m/s2a_O=+2\ \mathrm{m/s^2}, so −2=+2+(−4)-2=+2+(-4) in m/s2\mathrm{m/s^2}. The nonzero acceleration of the origin supplies the difference between the cart’s two reported accelerations.

(c) Compare velocity with acceleration in each reference.

t=1:vXaX=6(−2)<0,v′a′=4(−4)<0,t=3:vXaX=2(−2)<0,v′a′=(−4)(−4)>0.\begin{aligned}t=1:&\quad v_Xa_X=6(-2)<0,\quad v\!\,^{\prime}a'=4(-4)<0,\\t=3:&\quad v_Xa_X=2(-2)<0,\quad v\!\,^{\prime}a'=(-4)(-4)>0.\end{aligned}

At 1 s, the ground velocity is +6m/s+6\ \mathrm{m/s} and the local velocity is +4m/s+4\ \mathrm{m/s}. Both descriptions are eastward with negative acceleration, hence decreasing speed.

At 3 s, the ground velocity is +2m/s+2\ \mathrm{m/s}, so the cart still moves east and slows relative to the ground. The local velocity is −4m/s-4\ \mathrm{m/s}; together with local acceleration −4m/s2-4\ \mathrm{m/s^2}, this means westward motion with increasing speed relative to the platform. These statements describe different reference histories and are compatible.

(d) A time-dependent origin is not a fixed offset.

A fixed spatial offset has zero first and second derivatives. An origin moving with constant velocity has a nonzero first derivative but zero second derivative, so it contributes no acceleration. An accelerating origin has a nonzero second derivative and cannot be removed as a constant. The student’s cancellation argument applies only to the appropriate time-independent or constant-velocity transformations, not to every moving reference.