Projectile Motion — Question 8

Section 4-4 · Physics pages 526–527

Question 8 Gravity makes equal downward departures from a tangent line A projectile is launched with⃗v0 = (8, 6) m/s from the origin. Define the reference point⃗ rstraight(t) =⃗v0t, which would occur if acceleration vanished. Use fixed horizontal x and upward y, neglect air resistance, and take uniform g = 10 m/s2. After release,⃗a = −gˆȷ. no-gravity reference drop Compare both constructions at one common elapsed time. (a) Find the vector difference between actual and reference positions at time t. (b) Evaluate the two positions and their separation at 1 s. (c) Does the downward separation depend on horizontal launch speed? Explain why the reference line is not a second real path under the stated gravity.
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Question 8 - Solution Gravity makes equal downward departures from a tangent line no-gravity reference drop (a) Subtract the two vector histories.⃗ r −⃗rstraight = (⃗ v0t −1 2gt2ˆj ) −⃗v0t = −1 2gt2ˆj Actual position is⃗r =⃗v0t −1 2gt2ˆȷ. Hence⃗r −⃗rstraight = −1 2gt2ˆȷ: a purely downward departure with no horizontal difference. (b) Compare at the same time.⃗ rstraight(1) = (8, 6) m,⃗ r(1) = (8, 1) m, ∆⃗r = (0, −5) m At 1 s the reference point is (8, 6) m and the actual projectile is (8, 1) m. Their separation is 5 m downward. This compares simultaneous positions, not the shortest distance from the parabola to the reference line. (c) Identify the counterfactual assumption. ∂ ∂v0x ( −1 2gt2) = 0,⃗ astraight =⃗0̸ = −gˆj The departure depends only on g and elapsed time for the same initial position and velocity. Horizontal launch speed changes x but not the vertical shortfall at a fixed time. The straight reference path omits gravity and therefore serves as a construction, not another possible trajectory under the full stated model.

Question 8

Gravity makes equal downward departures from a tangent line

A projectile is launched with v→0=(8,6)\vec v_0=(8,6) m/s from the origin. Define the reference point r→straight(t)=v→0t\vec r_{\mathrm{straight}}(t)=\vec v_0t, which would occur if acceleration vanished. 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 vector difference between actual and reference positions at time t.

  2. Evaluate the two positions and their separation at 1 s.

  3. Does the downward separation depend on horizontal launch speed? Explain why the reference line is not a second real path under the stated gravity.

Question 8 - Solution

Gravity makes equal downward departures from a tangent line

Diagram shown in the original SVG worksheet.

(a) Subtract the two vector histories.

r→−r→straight=(v→0t−12gt2ĵ)−v→0t=−12gt2ĵ\boxed{\vec r-\vec r_{\mathrm{straight}}=\left(\vec v_0t-\tfrac12gt^2\hat j\right)-\vec v_0t=-\tfrac12gt^2\hat j} Actual position is r→=v→0t−12gt2ȷ̂\vec r=\vec v_0t-\tfrac12gt^2\hat\jmath. Hence r→−r→straight=−12gt2ȷ̂\vec r-\vec r_{\mathrm{straight}}=-\tfrac12gt^2\hat\jmath: a purely downward departure with no horizontal difference.

(b) Compare at the same time.

r→straight(1)=(8,6)m,r→(1)=(8,1)m,Δr→=(0,−5)m\vec r_{\mathrm{straight}}(1)=(8,6)\,\mathrm m,\quad\vec r(1)=(8,1)\,\mathrm m,\quad\Delta\vec r=(0,-5)\,\mathrm m At 1 s the reference point is (8,6)(8,6) m and the actual projectile is (8,1)(8,1) m. Their separation is 5 m downward. This compares simultaneous positions, not the shortest distance from the parabola to the reference line.

(c) Identify the counterfactual assumption.

∂∂v0x(−12gt2)=0,a→straight=0→≠−gĵ\frac{\partial}{\partial v_{0x}}\left(-\tfrac12gt^2\right)=0,\quad\vec a_{\mathrm{straight}}=\vec0\ne-g\hat j The departure depends only on g and elapsed time for the same initial position and velocity. Horizontal launch speed changes x but not the vertical shortfall at a fixed time. The straight reference path omits gravity and therefore serves as a construction, not another possible trajectory under the full stated model.