Time — Question 3

Section 1-5 · Physics pages 96–97

Question 3 Two reaction delays can cancel, or reinforce a timing error An observer starts a perfect stopwatch after event A and stops it after event B. The start reaction delay is rs and the stop reaction delay is re, both measured positively after the corresponding event. The stopwatch displays M = 12.480 s. time Event A tA Start click tA + rs Event B tB Stop click tB + re stopwatch interval M Schematic timing sequence, not to scale. The stopwatch runs between clicks, while the desired duration is between events A and B. (a) Derive a relation between M and the true event interval ∆t = tB −tA. Evaluate ∆t using nominal delays rs = 0.180 s and re = 0.260 s. (b) Now replace the nominal delays by hard bounds rs ∈[0.140, 0.220] s and re ∈[0.200, 0.320] s. Every pair of allowed delays is possible. Find the full allowed interval for ∆t. (c) A student subtracts the sum rs + re from the displayed time. Explain why the two delays enter with opposite signs instead. (d) Under what condition do reaction delays cancel exactly? Does using the same observer guar- antee that condition, or justify eliminating the bounds by repeated trials? Treat stopwatch resolution and timebase error as negligible here; the only errors modeled are the two reaction delays.
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Question 3 - Solution Two reaction delays can cancel, or reinforce a timing error time Event A tA Start click tA + rs Event B tB Stop click tB + re stopwatch interval M (a) Write the two click times before subtracting. M = (tB + re) −(tA + rs) = ∆t + re −rs, ∆t = M −re + rs. With the nominal delays, ∆t = (12.480 −0.260 + 0.180) s = 12.400 s . (b) Use the extreme allowed combinations. The smallest true interval uses the largest stop delay and smallest start delay; the largest uses the opposite pair: ∆tmin = (12.480 −0.320 + 0.140) s = 12.300 s, ∆tmax = (12.480 −0.200 + 0.220) s = 12.500 s. Thus ∆t ∈[12.300, 12.500] s . These are hard bounds, not a probabilistic confidence interval. (c) Starting late omits time; stopping late adds time. A delayed start shortens the measured interval, whereas a delayed stop lengthens it. Their net contribution to M is re −rs, not their sum. Subtracting both would incorrectly treat the delayed start as added running time. (d) State the cancellation condition. M −∆t = re −rs = 0 ⇐⇒re = rs. Exact cancellation requires re = rs for the trial. One observer may react differently to different events or cues, so identity of the observer is insufficient. Repetition alone does not remove an unknown systematic difference. Any claim that averaging narrows these bounds would require additional, justified information about the delays or their statistical behavior.

Question 3

Two reaction delays can cancel, or reinforce a timing error

An observer starts a perfect stopwatch after event A and stops it after event B. The start reaction delay is rsr_s and the stop reaction delay is rer_e, both measured positively after the corresponding event. The stopwatch displays M=12.480sM=12.480\ \mathrm{s}.

Diagram shown in the original SVG worksheet.

  1. Derive a relation between MM and the true event interval Δt=tB−tA\Delta t=t_B-t_A. Evaluate Δt\Delta t using nominal delays rs=0.180sr_s=0.180\ \mathrm{s} and re=0.260sr_e=0.260\ \mathrm{s}.

  2. Now replace the nominal delays by hard bounds rs∈[0.140,0.220]sr_s\in[0.140,0.220]\ \mathrm{s} and re∈[0.200,0.320]sr_e\in[0.200,0.320]\ \mathrm{s}. Every pair of allowed delays is possible. Find the full allowed interval for Δt\Delta t.

  3. A student subtracts the sum rs+rer_s+r_e from the displayed time. Explain why the two delays enter with opposite signs instead.

  4. Under what condition do reaction delays cancel exactly? Does using the same observer guarantee that condition, or justify eliminating the bounds by repeated trials?

Treat stopwatch resolution and timebase error as negligible here; the only errors modeled are the two reaction delays.

Question 3 - Solution

Two reaction delays can cancel, or reinforce a timing error

Diagram shown in the original SVG worksheet.

(a) Write the two click times before subtracting.

M=(tB+re)−(tA+rs)=Δt+re−rs,Δt=M−re+rs.M=(t_B+r_e)-(t_A+r_s)=\Delta t+r_e-r_s, \qquad \Delta t=M-r_e+r_s. With the nominal delays, Δt=(12.480−0.260+0.180)s=12.400s.\Delta t=(12.480-0.260+0.180)\ \mathrm{s} =\boxed{12.400\ \mathrm{s}}.

(b) Use the extreme allowed combinations.

The smallest true interval uses the largest stop delay and smallest start delay; the largest uses the opposite pair: Δtmin=(12.480−0.320+0.140)s=12.300s,\Delta t_{\min}=(12.480-0.320+0.140)\ \mathrm{s}=12.300\ \mathrm{s}, Δtmax=(12.480−0.200+0.220)s=12.500s.\Delta t_{\max}=(12.480-0.200+0.220)\ \mathrm{s}=12.500\ \mathrm{s}. Thus Δt∈[12.300,12.500]s\boxed{\Delta t\in[12.300,12.500]\ \mathrm{s}}. These are hard bounds, not a probabilistic confidence interval.

(c) Starting late omits time; stopping late adds time.

A delayed start shortens the measured interval, whereas a delayed stop lengthens it. Their net contribution to MM is re−rsr_e-r_s, not their sum. Subtracting both would incorrectly treat the delayed start as added running time.

(d) State the cancellation condition.

M−Δt=re−rs=0⇔re=rs.M-\Delta t=r_e-r_s=0\ \Longleftrightarrow\ r_e=r_s.

Exact cancellation requires re=rsr_e=r_s for the trial. One observer may react differently to different events or cues, so identity of the observer is insufficient. Repetition alone does not remove an unknown systematic difference. Any claim that averaging narrows these bounds would require additional, justified information about the delays or their statistical behavior.