Average Acceleration and Instantaneous Acceleration — Question 10

Section 4-3 · Physics pages 510–511

Question 10 A zero average can hide substantial acceleration A particle has⃗v(t) = [4 cos(ωt), 2 sin(ωt)] m/s with ω = π s−1. vx vy (4, 0) The velocity-space trajectory is an ellipse; it returns to its start after 2 s. (a) Find average acceleration from 0 to 2 s and instantaneous acceleration at zero. (b) Find the speed at 0 and 0.5 s. Is this a constant-speed motion? (c) Is acceleration ever the zero vector? Explain why its separate component zeros do not suffice.
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Question 10 - Solution A zero average can hide substantial acceleration vx vy (4, 0) (a) Distinguish a periodic endpoint difference from a derivative.⃗ aav =⃗v(2) −⃗v(0) 2 =⃗0,⃗ a(0) = (0, 2π) m/s2⃗ v(0) =⃗v(2 s) = (4, 0) m/s, so average acceleration over that interval is zero. Differentiation gives⃗ a = (−4π sin ωt, 2π cos ωt) m/s2, hence⃗a(0) = (0, 2π) m/s2. (b) Check the unequal velocity amplitudes. v2 = 16 cos2 ωt + 4 sin2 ωt : v(0) = 4, v(.5) = 2 m/s The two speeds are 4 m/s and 2 m/s. In general v2 = 16 cos2 ωt + 4 sin2 ωt, which is not constant. A periodic velocity is not automatically uniform-speed motion. (c) Require simultaneous sine and cosine zeros. a2 = 16π2 sin2 ωt + 4π2 cos2 ωt ≥4π2 m2/s4 > 0 Zero acceleration would require both sin ωt = 0 and cos ωt = 0, which never happens. Its direction and magnitude vary, but it is nonzero at every time. The zero full-period average represents cancellation of vector changes across the interval.

Question 10

A zero average can hide substantial acceleration

A particle has v→(t)=[4cos⁡(ωt),2sin⁡(ωt)]\vec v(t)=[4\cos(\omega t),2\sin(\omega t)] m/s with ω=πs−1\omega=\pi\ \mathrm{s^{-1}}.

Diagram shown in the original SVG worksheet.

  1. Find average acceleration from 0 to 2 s and instantaneous acceleration at zero.

  2. Find the speed at 0 and 0.5 s. Is this a constant-speed motion?

  3. Is acceleration ever the zero vector? Explain why its separate component zeros do not suffice.

Question 10 - Solution

A zero average can hide substantial acceleration

Diagram shown in the original SVG worksheet.

(a) Distinguish a periodic endpoint difference from a derivative.

a→av=v→(2)−v→(0)2=0→,a→(0)=(0,2π)m/s2\vec a_{\mathrm{av}}=\frac{\vec v(2)-\vec v(0)}2=\vec0,\quad\boxed{\vec a(0)=(0,2\pi)\,\mathrm{m/s^2}} v→(0)=v→(2s)=(4,0)\vec v(0)=\vec v(2\ \mathrm s)=(4,0) m/s, so average acceleration over that interval is zero. Differentiation gives a→=(−4πsin⁡ωt,2πcos⁡ωt)\vec a=(-4\pi\sin\omega t,2\pi\cos\omega t) m/s2^2, hence a→(0)=(0,2π)\vec a(0)=(0,2\pi) m/s2^2.

(b) Check the unequal velocity amplitudes.

v2=16cos⁡2ωt+4sin⁡2ωt:v(0)=4,v(.5)=2m/sv^2=16\cos^2\omega t+4\sin^2\omega t:\quad v(0)=4,\quad v(.5)=2\quad\mathrm{m/s} The two speeds are 4 m/s and 2 m/s. In general v2=16cos⁡2ωt+4sin⁡2ωtv^2=16\cos^2\omega t+4\sin^2\omega t, which is not constant. A periodic velocity is not automatically uniform-speed motion.

(c) Require simultaneous sine and cosine zeros.

a2=16π2sin⁡2ωt+4π2cos⁡2ωt≥4π2m2/s4>0a^2=16\pi^2\sin^2\omega t+4\pi^2\cos^2\omega t\ge4\pi^2\,\mathrm{m^2/s^4}>0 Zero acceleration would require both sin⁡ωt=0\sin\omega t=0 and cos⁡ωt=0\cos\omega t=0, which never happens. Its direction and magnitude vary, but it is nonzero at every time. The zero full-period average represents cancellation of vector changes across the interval.