Free-Fall Acceleration — Question 8

Section 2-8 · Physics pages 286–287

Question 8 A last-second observation can create an inadmissible root A point is dropped from rest and falls to the ground under constant g = 10 m/s2 with negligible air resistance. During the last ∆= 1.00 s before impact, it travels exactly f = 5/9 of the total drop height. The whole flight lasts at least one second. t 0 T −∆ T distance (1 −f)H distance fH last interval ∆= 1 s Schematic time partition; the marked distances are traveled during the two intervals. (a) Express the last-second distance as the difference between two positions, using total fall duration T. Derive the quadratic equation for T. (b) Find both algebraic roots and select the admissible one. Determine the total height and the distances traveled before and during the last second. (c) Find speed at the beginning of the last second and immediately before impact. Verify the last-second distance using its average speed. (d) For general 0 < f < 1 and a last interval of length ∆, derive the physically admissible expression for T. Explain why the other branch corresponds to extending the trajectory to a time before release.
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Question 8 - Solution A last-second observation can create an inadmissible root t 0 T −∆ T distance (1 −f)H distance fH last interval ∆= 1 s (a) Subtract distances measured from the same release event. The total height is H = gT 2/2. Because T ≥∆, the final interval starts at a valid elapsed time T −∆. Its distance is Dlast = 1 2g[T 2 −(T −∆)2] = gT∆−1 2g∆2. Setting this equal to fH gives fT 2 −2∆T + ∆2 = 0. For the stated values, 5T 2 −18T + 9 = 0 with numerical seconds. (b) The time domain rejects an otherwise valid algebraic root. 5T 2 −18T + 9 = (5T −3)(T −3) = 0; T ≥1 s ⇒T = 3 s. The roots are T = 3.00 s and T = 0.600 s. The latter is shorter than the stipulated last second, so it is inadmissible. Thus T = 3.00 s , H = 45.0 m . By T −∆= 2 s, the point has fallen 20 m; during the last second it falls 25 m. Indeed 25/45 = 5/9. (c) Check against the interval’s actual endpoint speeds. The downward speeds are 20 m/s at 2 s and 30 m/s at 3 s. Their mean is 25 m/s, so the last-second distance is (25 m/s)(1 s) = 25 m. (d) Apply the domain before choosing a square-root branch. Since f = 1 −(1 −∆/T)2 and T ≥∆, the quantity 1 −∆/T is nonnegative. Therefore T = ∆ 1 −√1 −f = ∆(1 + √1 −f) f . The other root is ∆/(1 + √1 −f) < ∆. It would evaluate the position at T −∆< 0, before release. An algebraic continuation of the parabola does not make that earlier interval part of the specified fall.

Question 8

A last-second observation can create an inadmissible root

A point is dropped from rest and falls to the ground under constant g=10m/s2g=10\ \mathrm{m/s^2} with negligible air resistance. During the last Δ=1.00s\Delta=1.00\ \mathrm{s} before impact, it travels exactly f=5/9f=5/9 of the total drop height. The whole flight lasts at least one second.

Diagram shown in the original SVG worksheet.

  1. Express the last-second distance as the difference between two positions, using total fall duration TT. Derive the quadratic equation for TT.

  2. Find both algebraic roots and select the admissible one. Determine the total height and the distances traveled before and during the last second.

  3. Find speed at the beginning of the last second and immediately before impact. Verify the last-second distance using its average speed.

  4. For general 0<f<10<f<1 and a last interval of length Δ\Delta, derive the physically admissible expression for TT. Explain why the other branch corresponds to extending the trajectory to a time before release.

Question 8 - Solution

A last-second observation can create an inadmissible root

Diagram shown in the original SVG worksheet.

(a) Subtract distances measured from the same release event.

The total height is H=gT2/2H=gT^2/2. Because T≥ΔT\geq\Delta, the final interval starts at a valid elapsed time T−ΔT-\Delta. Its distance is Dlast=12g[T2−(T−Δ)2]=gTΔ−12gΔ2.D_{\mathrm{last}}=\tfrac12g[T^2-(T-\Delta)^2] =gT\Delta-\tfrac12g\Delta^2. Setting this equal to fHfH gives fT2−2ΔT+Δ2=0fT^2-2\Delta T+\Delta^2=0. For the stated values, 5T2−18T+9=0\boxed{5T^2-18T+9=0} with numerical seconds.

(b) The time domain rejects an otherwise valid algebraic root.

5T2−18T+9=(5T−3)(T−3)=0;T≥1s⇒T=3s.5T^2-18T+9=(5T-3)(T-3)=0;\qquad T\geq1\ \mathrm{s}\Rightarrow T=3\ \mathrm{s}.

The roots are T=3.00sT=3.00\ \mathrm{s} and T=0.600sT=0.600\ \mathrm{s}. The latter is shorter than the stipulated last second, so it is inadmissible. Thus T=3.00s,H=45.0m.\boxed{T=3.00\ \mathrm{s}},\qquad\boxed{H=45.0\ \mathrm{m}}. By T−Δ=2sT-\Delta=2\ \mathrm{s}, the point has fallen 20 m; during the last second it falls 25 m. Indeed 25/45=5/925/45=5/9.

(c) Check against the interval’s actual endpoint speeds.

The downward speeds are 20m/s\boxed{20\ \mathrm{m/s}} at 2 s and 30m/s\boxed{30\ \mathrm{m/s}} at 3 s. Their mean is 25 m/s, so the last-second distance is (25m/s)(1s)=25m(25\ \mathrm{m/s})(1\ \mathrm{s})=25\ \mathrm{m}.

(d) Apply the domain before choosing a square-root branch.

Since f=1−(1−Δ/T)2f=1-(1-\Delta/T)^2 and T≥ΔT\geq\Delta, the quantity 1−Δ/T1-\Delta/T is nonnegative. Therefore T=Δ1−1−f=Δ(1+1−f)f.\boxed{T=\frac{\Delta}{1-\sqrt{1-f}}} =\frac{\Delta(1+\sqrt{1-f})}{f}. The other root is Δ/(1+1−f)<Δ\Delta/(1+\sqrt{1-f})<\Delta. It would evaluate the position at T−Δ<0T-\Delta<0, before release. An algebraic continuation of the parabola does not make that earlier interval part of the specified fall.