Projectile Motion Analyzed — Question 1

Section 4-5 · Physics pages 532–533

Question 1 An elevated launch breaks the equal-height flight-time shortcut A projectile leaves (0, 20) m with velocity (8, 15) m/s and lands on y=0. Neglect air resistance and use uniform g = 10 m/s2 downward. Unless stated otherwise, x is horizontal and y upward. x release Schematic trajectory; use the given data for numerical values. (a) Find the landing time, explaining the rejected root. (b) Find the horizontal range and impact velocity. (c) Compare ascent time with the time from apex to landing. Why are they unequal?
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Question 1 - Solution An elevated launch breaks the equal-height flight-time shortcut x release (a) Set the final height, not the displacement, to zero. 0 = 20 + 15T −5T 2 = −5(T −4)(T + 1) ⇒ T = 4 s (T ≥0) 0 = 20 + 15t −5t2 for t in seconds. Factoring gives (t −4)(t + 1) = 0, so the physical landing is at 4 s. The root −1 s is a backward extrapolation before launch. (b) Evaluate both components at impact. R = 8(4) = 32 m,⃗ vf = (8, 15 −40) = (8, −25) m/s, vf = √ 689 m/s Range is 8(4) = 32 m. The impact velocity is (8, 15 −40) = (8, −25) m/s, speed √ 689 ≈26.249 m/s. The horizontal component remains unchanged throughout flight. (c) Use the apex as an intermediate event. t↑= v0y/g = 1.5 s, t↓= T −t↑= 2.5 s The apex occurs at 1.5 s, so ascent takes 1.5 s and descent to the floor takes 2.5 s. Landing is 20 m below release, so the descending part covers extra vertical distance. The equal-height formula T = 2v0y/g = 3 s would stop at the release height, not the floor.

Question 1

An elevated launch breaks the equal-height flight-time shortcut

A projectile leaves (0,20)(0,20) m with velocity (8,15)(8,15) m/s and lands on y=0. Neglect air resistance and use uniform g=10m/s2g=10\ \mathrm{m/s^2} downward. Unless stated otherwise, x is horizontal and y upward.

Diagram shown in the original SVG worksheet.

  1. Find the landing time, explaining the rejected root.

  2. Find the horizontal range and impact velocity.

  3. Compare ascent time with the time from apex to landing. Why are they unequal?

Question 1 - Solution

An elevated launch breaks the equal-height flight-time shortcut

Diagram shown in the original SVG worksheet.

(a) Set the final height, not the displacement, to zero.

0=20+15T−5T2=−5(T−4)(T+1)⇒T=4s(T≥0)0=20+15T-5T^2=-5(T-4)(T+1)\ \Rightarrow\ \boxed{T=4\,\mathrm s}\quad(T\ge0) 0=20+15t−5t20=20+15t-5t^2 for t in seconds. Factoring gives (t−4)(t+1)=0(t-4)(t+1)=0, so the physical landing is at 4 s. The root −1-1 s is a backward extrapolation before launch.

(b) Evaluate both components at impact.

R=8(4)=32m,v→f=(8,15−40)=(8,−25)m/s,vf=689m/sR=8(4)=32\,\mathrm m,\quad\vec v_f=(8,15-40)=(8,-25)\,\mathrm{m/s},\quad v_f=\sqrt{689}\,\mathrm{m/s} Range is 8(4)=328(4)=32 m. The impact velocity is (8,15−40)=(8,−25)(8,15-40)=(8,-25) m/s, speed 689≈26.249\sqrt{689}\approx26.249 m/s. The horizontal component remains unchanged throughout flight.

(c) Use the apex as an intermediate event.

t↑=v0y/g=1.5s,t↓=T−t↑=2.5st_\uparrow=v_{0y}/g=1.5\,\mathrm s,\quad t_\downarrow=T-t_\uparrow=2.5\,\mathrm s The apex occurs at 1.5 s, so ascent takes 1.5 s and descent to the floor takes 2.5 s. Landing is 20 m below release, so the descending part covers extra vertical distance. The equal-height formula T=2v0y/g=3T=2v_{0y}/g=3 s would stop at the release height, not the floor.