Average Velocity and Instantaneous Velocity — Question 4

Section 4-2 · Physics pages 478–479

Question 4 A turning coordinate is not necessarily a stopped particle With u = t/(1 s), a particle follows⃗r = [(u −2)2ˆı + 3uˆȷ] m. Consider times near t = 2 s. 2 s Schematic sideways parabola; the arrow at the leftmost point is vertical. (a) Find the instantaneous velocity at 2 s and decide whether the particle is at rest. (b) Describe the signs of the horizontal velocity just before and after 2 s. (c) Find the average velocity from 1 s to 3 s and compare its direction with the tangent at 2 s.
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Question 4 - Solution A turning coordinate is not necessarily a stopped particle 2 s (a) Both velocity components must vanish for rest.⃗ v = (2(u −2), 3) m/s ⇒⃗ v(2 s) = (0, 3) m/s Differentiation gives⃗v = [2(u −2)ˆı + 3ˆȷ] m/s. At 2 s it is 3ˆȷ m/s. The particle moves upward at 3 m/s even though its x coordinate has a minimum. (b) Track reversal in one coordinate. sgn(vx) = sgn(u −2), vy = 3 m/s > 0 vx < 0 before 2 s and vx > 0 after it, so horizontal motion changes from leftward to rightward. Meanwhile vy = 3 m/s never changes sign. The full trajectory has a vertical tangent at the turning x coordinate. (c) Evaluate the symmetric interval.⃗ vav = (1, 9) −(1, 3) 2 = (0, 3) m/s =⃗v(2 s) The two positions are (1, 3) and (1, 9) m, giving average velocity (0, 3) m/s. Here it equals the midpoint instantaneous velocity. Equal endpoint x coordinates mean zero average horizontal velocity, not zero horizontal velocity throughout the interval.

Question 4

A turning coordinate is not necessarily a stopped particle

With u=t/(1s)u=t/(1\ \mathrm s), a particle follows r→=[(u−2)2ı̂+3uȷ̂]\vec r=[(u-2)^2\hat\imath+3u\hat\jmath] m. Consider times near t=2t=2 s.

Diagram shown in the original SVG worksheet.

  1. Find the instantaneous velocity at 2 s and decide whether the particle is at rest.

  2. Describe the signs of the horizontal velocity just before and after 2 s.

  3. Find the average velocity from 1 s to 3 s and compare its direction with the tangent at 2 s.

Question 4 - Solution

A turning coordinate is not necessarily a stopped particle

Diagram shown in the original SVG worksheet.

(a) Both velocity components must vanish for rest.

v→=(2(u−2),3)m/s⇒v→(2s)=(0,3)m/s\vec v=(2(u-2),3)\,\mathrm{m/s}\ \Rightarrow\ \boxed{\vec v(2\,\mathrm s)=(0,3)\,\mathrm{m/s}} Differentiation gives v→=[2(u−2)ı̂+3ȷ̂]\vec v=[2(u-2)\hat\imath+3\hat\jmath] m/s. At 2 s it is 3ȷ̂3\hat\jmath m/s. The particle moves upward at 3 m/s even though its x coordinate has a minimum.

(b) Track reversal in one coordinate.

sgn⁡(vx)=sgn⁡(u−2),vy=3m/s>0\operatorname{sgn}(v_x)=\operatorname{sgn}(u-2),\quad v_y=3\,\mathrm{m/s}>0 vx<0v_x<0 before 2 s and vx>0v_x>0 after it, so horizontal motion changes from leftward to rightward. Meanwhile vy=3v_y=3 m/s never changes sign. The full trajectory has a vertical tangent at the turning x coordinate.

(c) Evaluate the symmetric interval.

v→av=(1,9)−(1,3)2=(0,3)m/s=v→(2s)\vec v_{\mathrm{av}}=\frac{(1,9)-(1,3)}{2}=(0,3)\,\mathrm{m/s}=\vec v(2\,\mathrm s) The two positions are (1,3)(1,3) and (1,9)(1,9) m, giving average velocity (0,3)(0,3) m/s. Here it equals the midpoint instantaneous velocity. Equal endpoint x coordinates mean zero average horizontal velocity, not zero horizontal velocity throughout the interval.