Average Velocity and Instantaneous Velocity — Question 9

Section 4-2 · Physics pages 488–489

Question 9 A half-circle average does not point along the local tangent A particle has⃗r(t) = [2 cos(ωt)ˆı + 2 sin(ωt)ˆȷ] m, with ω = π s−1. Consider 0 ≤t ≤1 s.⃗ v(0)⃗ v(1 s) Endpoint tangent velocities differ from the interval chord velocity. (a) Find the average velocity over the interval. (b) Differentiate to obtain instantaneous velocity at 0 and 1 s and the speed at every time. (c) Find the average speed over the interval and explain why it differs from the magnitude of average velocity.
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Question 9 - Solution A half-circle average does not point along the local tangent⃗ v(0)⃗ v(1 s) (a) Use the diameter displacement.⃗ vav = (−2, 0) −(2, 0) 1 = (−4, 0) m/s The positions are (2, 0) m and (−2, 0) m. Hence⃗vav = (−4, 0) m/s, magnitude 4 m/s. It points along the chord joining the endpoints. (b) Differentiate the trigonometric functions.⃗ v = 2π(−sin ωt, cos ωt) m/s, v = 2π √ sin2 ωt + cos2 ωt = 2π m/s⃗ v = 2π[−sin(πt/s)ˆı + cos(πt/s)ˆȷ] m/s. At the two endpoints it is (0, 2π) and (0, −2π) m/s. Its magnitude is always 2π m/s because the squared sine and cosine sum to one. (c) Use the actual arc traveled. ¯vspeed = πR ∆t = 2π m/s > |⃗vav| = 4 m/s The particle travels half a circumference, 2π m, in 1 s, so average speed is 2π ≈6.283 m/s. Constant speed does not imply constant vector velocity: the tangent direction changes throughout the half circle.

Question 9

A half-circle average does not point along the local tangent

A particle has r→(t)=[2cos⁡(ωt)ı̂+2sin⁡(ωt)ȷ̂]\vec r(t)=[2\cos(\omega t)\hat\imath+2\sin(\omega t)\hat\jmath] m, with ω=πs−1\omega=\pi\ \mathrm{s^{-1}}. Consider 0≤t≤10\leq t\leq1 s.

Diagram shown in the original SVG worksheet.

  1. Find the average velocity over the interval.

  2. Differentiate to obtain instantaneous velocity at 0 and 1 s and the speed at every time.

  3. Find the average speed over the interval and explain why it differs from the magnitude of average velocity.

Question 9 - Solution

A half-circle average does not point along the local tangent

Diagram shown in the original SVG worksheet.

(a) Use the diameter displacement.

v→av=(−2,0)−(2,0)1=(−4,0)m/s\boxed{\vec v_{\mathrm{av}}=\frac{(-2,0)-(2,0)}1=(-4,0)\,\mathrm{m/s}} The positions are (2,0)(2,0) m and (−2,0)(-2,0) m. Hence v→av=(−4,0)\vec v_{\mathrm{av}}=(-4,0) m/s, magnitude 4 m/s. It points along the chord joining the endpoints.

(b) Differentiate the trigonometric functions.

v→=2π(−sin⁡ωt,cos⁡ωt)m/s,v=2πsin⁡2ωt+cos⁡2ωt=2πm/s\vec v=2\pi(-\sin\omega t,\cos\omega t)\,\mathrm{m/s},\quad v=2\pi\sqrt{\sin^2\omega t+\cos^2\omega t}=2\pi\,\mathrm{m/s} v→=2π[−sin⁡(πt/s)ı̂+cos⁡(πt/s)ȷ̂]\vec v=2\pi[-\sin(\pi t/\mathrm s)\hat\imath+\cos(\pi t/\mathrm s)\hat\jmath] m/s. At the two endpoints it is (0,2π)(0,2\pi) and (0,−2π)(0,-2\pi) m/s. Its magnitude is always 2π2\pi m/s because the squared sine and cosine sum to one.

(c) Use the actual arc traveled.

v‾speed=πRΔt=2πm/s>|v→av|=4m/s\bar v_{\mathrm{speed}}=\frac{\pi R}{\Delta t}=2\pi\,\mathrm{m/s}>|\vec v_{\mathrm{av}}|=4\,\mathrm{m/s} The particle travels half a circumference, 2π2\pi m, in 1 s, so average speed is 2π≈6.2832\pi\approx6.283 m/s. Constant speed does not imply constant vector velocity: the tangent direction changes throughout the half circle.