Average Velocity and Instantaneous Velocity — Question 7

Section 4-2 · Physics pages 484–485

Question 7 Rest requires simultaneous component zeros For t ≥0, let u = t/(1 s) and⃗r(t) = (u2 −2u, u3/3 −u2) m. t (s) v (m/s) 0 1 2 vx vy Solid: horizontal velocity. Dashed: vertical velocity. A stop requires simultaneous zeros. (a) Find both velocity components and every time at which either component vanishes. (b) Is the particle ever completely at rest? Find the speed at 1 s. (c) Find the average velocity from 0 to 2 s and explain why its horizontal component can vanish without an interval of rest.
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Question 7 - Solution Rest requires simultaneous component zeros t (s) v (m/s) 0 1 2 vx vy (a) Differentiate and solve each component equation. vx = (2u −2) m/s, vy = u(u −2) m/s, Zx = {1}, Zy = {0, 2}⃗ v = (2u −2, u2 −2u) m/s. The horizontal root is u = 1; vertical roots are u = 0 and u = 2. They are different times. (b) Intersect, rather than combine, the root sets. Zx ∩Zy = ∅,⃗ v(1 s) = (0, −1) m/s, v = 1 m/s There is no common root, so the particle is never at rest for t ≥0. At 1 s its velocity is (0, −1) m/s and its speed is 1 m/s. A vanishing component alone indicates alignment of the velocity with the other axis. (c) Use the endpoint difference.⃗ vav = (0, −4/3) −(0, 0) 2 = (0, −2/3) m/s⃗ r(0) = (0, 0) m and⃗r(2 s) = (0, −4/3) m. Average velocity is (0, −2/3) m/s. The horizontal motion reverses and cancels in displacement; it is not absent throughout the interval.

Question 7

Rest requires simultaneous component zeros

For t≥0t\geq0, let u=t/(1s)u=t/(1\ \mathrm s) and r→(t)=(u2−2u,u3/3−u2)\vec r(t)=(u^2-2u,\ u^3/3-u^2) m.

Diagram shown in the original SVG worksheet.

  1. Find both velocity components and every time at which either component vanishes.

  2. Is the particle ever completely at rest? Find the speed at 1 s.

  3. Find the average velocity from 0 to 2 s and explain why its horizontal component can vanish without an interval of rest.

Question 7 - Solution

Rest requires simultaneous component zeros

Diagram shown in the original SVG worksheet.

(a) Differentiate and solve each component equation.

vx=(2u−2)m/s,vy=u(u−2)m/s,Zx={1},Zy={0,2}v_x=(2u-2)\,\mathrm{m/s},\quad v_y=u(u-2)\,\mathrm{m/s},\quad Z_x=\{1\},\quad Z_y=\{0,2\} v→=(2u−2,u2−2u)\vec v=(2u-2,u^2-2u) m/s. The horizontal root is u=1u=1; vertical roots are u=0u=0 and u=2u=2. They are different times.

(b) Intersect, rather than combine, the root sets.

Zx∩Zy=⌀,v→(1s)=(0,−1)m/s,v=1m/sZ_x\cap Z_y=\varnothing,\quad\boxed{\vec v(1\,\mathrm s)=(0,-1)\,\mathrm{m/s},\quad v=1\,\mathrm{m/s}} There is no common root, so the particle is never at rest for t≥0t\geq0. At 1 s its velocity is (0,−1)(0,-1) m/s and its speed is 1 m/s. A vanishing component alone indicates alignment of the velocity with the other axis.

(c) Use the endpoint difference.

v→av=(0,−4/3)−(0,0)2=(0,−2/3)m/s\vec v_{\mathrm{av}}=\frac{(0,-4/3)-(0,0)}2=(0,-2/3)\,\mathrm{m/s} r→(0)=(0,0)\vec r(0)=(0,0) m and r→(2s)=(0,−4/3)\vec r(2\ \mathrm s)=(0,-4/3) m. Average velocity is (0,−2/3)(0,-2/3) m/s. The horizontal motion reverses and cancels in displacement; it is not absent throughout the interval.