Projectile Motion — Question 3

Section 4-4 · Physics pages 516–517

Question 3 The apex is not a zero-acceleration point A projectile leaves the origin with⃗v0 = (12, 16) m/s. Use fixed horizontal x and upward y, neglect air resistance, and take uniform g = 10 m/s2. After release,⃗a = −gˆȷ. x y⃗ a The highest point has horizontal velocity and downward acceleration. (a) Find the time, position and speed at the apex. (b) Find the acceleration there and explain what changes immediately before and after the apex. (c) Would a strictly vertical launch have zero acceleration at its apex? Distinguish the velocity condition.
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Question 3 - Solution The apex is not a zero-acceleration point x y⃗ a (a) Set the vertical velocity to zero. 0 = vy = 16 −10ta ⇒ta = 1.6 s, (xa, ya) = (19.2, 12.8) m, va = 12 m/s vy = (16 −10t/s) m/s vanishes at 1.6 s. Then x = 19.2 m and y = 16(1.6) −5(1.6)2 = 12.8 m. Velocity is (12, 0) m/s, so apex speed is 12 m/s. (b) Retain gravity at every point. ay = dvy dt = −10 m/s2, vy(ta −ϵ) = 10ϵ, vy(ta + ϵ) = −10ϵ Acceleration remains (0, −10) m/s2. Just before the apex vy > 0; just after it vy < 0. The y velocity changes continuously through zero because its derivative stays negative. No pause or switch in gravity is required. (c) Zero velocity does not eliminate its derivative. v0x = 0 :⃗ v(ta) =⃗0,⃗ a(ta) = −gˆj̸ =⃗0 For a vertical launch vx = 0, so the entire velocity is momentarily zero at the apex. Acceleration is still downward with magnitude g. A horizontal component distinguishes a moving apex from a momentarily stationary one; it does not change gravity.

Question 3

The apex is not a zero-acceleration point

A projectile leaves the origin with v→0=(12,16)\vec v_0=(12,16) m/s. Use fixed horizontal x and upward y, neglect air resistance, and take uniform g=10m/s2g=10\ \mathrm{m/s^2}. After release, a→=−gȷ̂\vec a=-g\hat\jmath.

Diagram shown in the original SVG worksheet.

  1. Find the time, position and speed at the apex.

  2. Find the acceleration there and explain what changes immediately before and after the apex.

  3. Would a strictly vertical launch have zero acceleration at its apex? Distinguish the velocity condition.

Question 3 - Solution

The apex is not a zero-acceleration point

Diagram shown in the original SVG worksheet.

(a) Set the vertical velocity to zero.

0=vy=16−10ta⇒ta=1.6s,(xa,ya)=(19.2,12.8)m,va=12m/s0=v_y=16-10t_a\ \Rightarrow\ t_a=1.6\,\mathrm s,\quad\boxed{(x_a,y_a)=(19.2,12.8)\,\mathrm m,\ v_a=12\,\mathrm{m/s}} vy=(16−10t/s)m/sv_y=(16-10t/\mathrm s)\ \mathrm{m/s} vanishes at 1.6 s. Then x=19.2x=19.2 m and y=16(1.6)−5(1.6)2=12.8y=16(1.6)-5(1.6)^2=12.8 m. Velocity is (12,0)(12,0) m/s, so apex speed is 12 m/s.

(b) Retain gravity at every point.

ay=dvydt=−10m/s2,vy(ta−ϵ)=10ϵ,vy(ta+ϵ)=−10ϵa_y=\frac{dv_y}{dt}=-10\,\mathrm{m/s^2},\quad v_y(t_a-\epsilon)=10\epsilon,\quad v_y(t_a+\epsilon)=-10\epsilon Acceleration remains (0,−10)(0,-10) m/s2^2. Just before the apex vy>0v_y>0; just after it vy<0v_y<0. The y velocity changes continuously through zero because its derivative stays negative. No pause or switch in gravity is required.

(c) Zero velocity does not eliminate its derivative.

v0x=0:v→(ta)=0→,a→(ta)=−gĵ≠0→v_{0x}=0:\quad\vec v(t_a)=\vec0,\quad\vec a(t_a)=-g\hat j\ne\vec0 For a vertical launch vx=0v_x=0, so the entire velocity is momentarily zero at the apex. Acceleration is still downward with magnitude g. A horizontal component distinguishes a moving apex from a momentarily stationary one; it does not change gravity.