Average Acceleration and Instantaneous Acceleration — Question 6

Section 4-3 · Physics pages 502–503

Question 6 A constant acceleration need not point along displacement A particle begins at the origin with⃗v0 = (4, 1) m/s and constant⃗a = (−2, 3) m/s2. x y O⃗ v0 = (4, 1) m/s⃗ a = (−2, 3) m/s2 Schematic; labels specify the data. Arrow lengths are not a common scale. (a) Find v and r at 2 s. (b) Find the time when the horizontal velocity vanishes and decide whether the particle stops. (c) Find the average acceleration and average velocity over the first 2 s. Explain why these vectors need not be parallel.
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Question 6 - Solution A constant acceleration need not point along displacement x y O⃗ v0 = (4, 1) m/s⃗ a = (−2, 3) m/s2 (a) Apply the component equations.⃗ v(2) = (4, 1) + 2(−2, 3) = (0, 7) m/s ,⃗ r(2) = 2(4, 1) + 2(−2, 3) = (4, 8) m⃗ v =⃗v0 +⃗at and⃗r =⃗v0t + 1 2⃗at2. At 2 s these give⃗v = (0, 7) m/s and⃗r = (4, 8) m. The two vector equations carry different powers of time. (b) Check the other component at the same time. 4 −2t = 0 ⇒t = 2 s, vy = 1 + 3(2) = 7 m/s̸ = 0 vx = (4 −2t/s) m/s vanishes at 2 s, but vy = 7 m/s then. The motion has a turning x coordinate without coming to rest. The x acceleration remains negative after this instant, making x motion reverse. (c) Average different physical changes.⃗ aav = (0, 7) −(4, 1) 2 = (−2, 3) m/s2,⃗ vav = (2, 4) m/s Average acceleration is (−2, 3) m/s2, equal to the constant a. Average velocity is (4, 8) m/(2 s) = (2, 4) m/s. Acceleration tracks change of velocity; average velocity tracks change of position, so their directions are not constrained to agree.

Question 6

A constant acceleration need not point along displacement

A particle begins at the origin with v→0=(4,1)\vec v_0=(4,1) m/s and constant a→=(−2,3)\vec a=(-2,3) m/s2^2.

Diagram shown in the original SVG worksheet.

  1. Find v and r at 2 s.

  2. Find the time when the horizontal velocity vanishes and decide whether the particle stops.

  3. Find the average acceleration and average velocity over the first 2 s. Explain why these vectors need not be parallel.

Question 6 - Solution

A constant acceleration need not point along displacement

Diagram shown in the original SVG worksheet.

(a) Apply the component equations.

v→(2)=(4,1)+2(−2,3)=(0,7)m/s,r→(2)=2(4,1)+2(−2,3)=(4,8)m\vec v(2)=(4,1)+2(-2,3)=\boxed{(0,7)\,\mathrm{m/s}},\quad\vec r(2)=2(4,1)+2(-2,3)=(4,8)\,\mathrm m v→=v→0+a→t\vec v=\vec v_0+\vec a t and r→=v→0t+12a→t2\vec r=\vec v_0t+\tfrac12\vec a t^2. At 2 s these give v→=(0,7)\vec v=(0,7) m/s and r→=(4,8)\vec r=(4,8) m. The two vector equations carry different powers of time.

(b) Check the other component at the same time.

4−2t=0⇒t=2s,vy=1+3(2)=7m/s≠04-2t=0\ \Rightarrow\ t=2\,\mathrm s,\quad v_y=1+3(2)=7\,\mathrm{m/s}\ne0 vx=(4−2t/s)m/sv_x=(4-2t/\mathrm s)\ \mathrm{m/s} vanishes at 2 s, but vy=7v_y=7 m/s then. The motion has a turning x coordinate without coming to rest. The x acceleration remains negative after this instant, making x motion reverse.

(c) Average different physical changes.

a→av=(0,7)−(4,1)2=(−2,3)m/s2,v→av=(2,4)m/s\vec a_{\mathrm{av}}=\frac{(0,7)-(4,1)}2=(-2,3)\,\mathrm{m/s^2},\quad\vec v_{\mathrm{av}}=(2,4)\,\mathrm{m/s} Average acceleration is (−2,3)(-2,3) m/s2^2, equal to the constant a. Average velocity is (4,8)m/(2s)=(2,4)(4,8)\ \mathrm m/(2\ \mathrm s)=(2,4) m/s. Acceleration tracks change of velocity; average velocity tracks change of position, so their directions are not constrained to agree.