Free-Fall Acceleration — Question 2

Section 2-8 · Physics pages 274–275

Question 2 Equal impact speeds do not imply equal flight times Two small balls of different masses are released simultaneously from the same height H = 30 m above the ground in separate vertical lanes. Ball U is thrown upward at u = 10 m/s; ball D is thrown downward at the same speed. Treat each as a point in free fall with constant g = 10 m/s2 and no air resistance. Use ground-based upward-positive coordinates. ground release level U: +u D: −u H both: ay = −g Separate vertical lanes; identical release height and initial speed magnitudes. (a) Derive each positive ground-contact time in terms of H, u, g, then evaluate them. Find their difference without subtracting rounded numbers. (b) Determine both velocities immediately before impact. Why can their speeds agree even though their flight times differ? (c) Explain the time difference by considering U’s return to its release height. Does mass enter any of these results? (d) A student asserts that U spends equal times rising and falling because free fall is symmetric. State the correct symmetry and identify the unequal heights that invalidate this claim for the whole flight.
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Question 2 - Solution Equal impact speeds do not imply equal flight times ground release level U: +u D: −u H both: ay = −g (a) Keep the sign of each initial velocity. The trajectories are yU = H + ut −gt2/2 and yD = H −ut −gt2/2. Their positive roots are TU = u + √ u2 + 2gH g , TD = −u + √ u2 + 2gH g . Here √ u2 + 2gH = 10 √ 7 m/s, so TU = 1 + √ 7 ≈3.646 s, TD = −1 + √ 7 ≈1.646 s. Thus TU −TD = 2u/g = 2.00 s exactly in the stated model. (b) Select the downward branch at ground contact. For either ball, v2 = u2 + 2gH. Both are descending on contact, hence vU = vD = −10 √ 7 ≈−26.46 m/s . The squared relation depends on initial speed and net height change, while the time equations also retain initial direction and the extra upward excursion. (c) Match states at the same height. U returns to its release height after 2u/g = 2 s with velocity −u. Its remaining flight starts from exactly the height and velocity that D had at release, so its remaining duration is TD. Mass does not enter the ideal free-fall equations; differing air resistance would be a change of model. (d) Symmetry applies between equal heights. tup = u g = 1 s, tdown = √ u2 + 2gH g = √ 7 s > tup. U rises for u/g = 1 s through u2/(2g) = 5 m. It falls from its top height of 35 m to the ground, taking TU −1 = √ 7 s. Equal times apply to ascent and descent between the release level and the top, not between the top and a lower landing level.

Question 2

Equal impact speeds do not imply equal flight times

Two small balls of different masses are released simultaneously from the same height H=30mH=30\ \mathrm{m} above the ground in separate vertical lanes. Ball U is thrown upward at u=10m/su=10\ \mathrm{m/s}; ball D is thrown downward at the same speed. Treat each as a point in free fall with constant g=10m/s2g=10\ \mathrm{m/s^2} and no air resistance. Use ground-based upward-positive coordinates.

Diagram shown in the original SVG worksheet.

  1. Derive each positive ground-contact time in terms of H,u,gH,u,g, then evaluate them. Find their difference without subtracting rounded numbers.

  2. Determine both velocities immediately before impact. Why can their speeds agree even though their flight times differ?

  3. Explain the time difference by considering U’s return to its release height. Does mass enter any of these results?

  4. A student asserts that U spends equal times rising and falling because free fall is symmetric. State the correct symmetry and identify the unequal heights that invalidate this claim for the whole flight.

Question 2 - Solution

Equal impact speeds do not imply equal flight times

Diagram shown in the original SVG worksheet.

(a) Keep the sign of each initial velocity.

The trajectories are yU=H+ut−gt2/2y_U=H+ut-gt^2/2 and yD=H−ut−gt2/2y_D=H-ut-gt^2/2. Their positive roots are TU=u+u2+2gHg,TD=−u+u2+2gHg.\boxed{T_U=\frac{u+\sqrt{u^2+2gH}}{g}},\qquad \boxed{T_D=\frac{-u+\sqrt{u^2+2gH}}{g}}. Here u2+2gH=107m/s\sqrt{u^2+2gH}=10\sqrt7\ \mathrm{m/s}, so TU=1+7≈3.646s,TD=−1+7≈1.646s.T_U=1+\sqrt7\approx3.646\ \mathrm{s},\quad T_D=-1+\sqrt7\approx1.646\ \mathrm{s}. Thus TU−TD=2u/g=2.00s\boxed{T_U-T_D=2u/g=2.00\ \mathrm{s}} exactly in the stated model.

(b) Select the downward branch at ground contact.

For either ball, v2=u2+2gHv^2=u^2+2gH. Both are descending on contact, hence vU=vD=−107≈−26.46m/s.\boxed{v_U=v_D=-10\sqrt7\approx-26.46\ \mathrm{m/s}}. The squared relation depends on initial speed and net height change, while the time equations also retain initial direction and the extra upward excursion.

(c) Match states at the same height.

U returns to its release height after 2u/g=2s2u/g=2\ \mathrm{s} with velocity −u-u. Its remaining flight starts from exactly the height and velocity that D had at release, so its remaining duration is TDT_D. Mass does not enter the ideal free-fall equations; differing air resistance would be a change of model.

(d) Symmetry applies between equal heights.

tup=ug=1s,tdown=u2+2gHg=7s>tup.t_{\mathrm{up}}=\frac ug=1\ \mathrm{s},\qquad t_{\mathrm{down}}=\frac{\sqrt{u^2+2gH}}g=\sqrt7\ \mathrm{s}>t_{\mathrm{up}}.

U rises for u/g=1su/g=1\ \mathrm{s} through u2/(2g)=5mu^2/(2g)=5\ \mathrm{m}. It falls from its top height of 35 m to the ground, taking TU−1=7sT_U-1=\sqrt7\ \mathrm{s}. Equal times apply to ascent and descent between the release level and the top, not between the top and a lower landing level.