Kinetic Energy — Question 8

Section 7-2 · Physics pages 886–887

Question 8 Equal endpoint kinetic energies can hide a complete stop Use classical translational kinetic energy K = 1 2m|⃗v|2. A 2 kg particle has v(t) = (2 −2t) m/s for numerical time 0 ≤t ≤2 in seconds. t (s) v (m/s) 2 −2 1 2 The signed velocity crosses zero halfway through the interval. (a) Find K(t) and the endpoint energies. (b) Find when kinetic energy is smallest and interpret the motion then. (c) Find the energy change over each one-second half and explain why the full-interval change does not describe the whole history.
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Question 8 - Solution Equal endpoint kinetic energies can hide a complete stop t (s) v (m/s) 2 −2 1 2 (a) Square the signed velocity. The governing relation is K(t) = 1 2m[v(t)]2, dK dt = mvdv dt K(t) = (2 −2t)2 J. Therefore K(0) = K(2) = 4 J. (b) Locate zero speed. v = 0 at t = 1 s, where K = 0. Velocity changes from positive to negative, so this is a stop and reversal. (c) Keep the interval information. ∆K0→1 = −4 J, ∆K1→2 = +4 J. Their sum is zero, but kinetic energy was not constant. A zero net change can conceal large intermediate changes.

Question 8

Equal endpoint kinetic energies can hide a complete stop

Use classical translational kinetic energy K=12m|v→|2K=\tfrac12 m|\vec v|^2. A 2 kg particle has v(t)=(2−2t)v(t)=(2-2t) m/s for numerical time 0≤t≤20\le t\le2 in seconds.

Diagram shown in the original SVG worksheet.

  1. Find K(t)K(t) and the endpoint energies.

  2. Find when kinetic energy is smallest and interpret the motion then.

  3. Find the energy change over each one-second half and explain why the full-interval change does not describe the whole history.

Question 8 - Solution

Equal endpoint kinetic energies can hide a complete stop

Diagram shown in the original SVG worksheet.

(a) Square the signed velocity.

The governing relation is K(t)=12m[v(t)]2,dKdt=mvdvdt\boxed{K(t)=\tfrac12m[v(t)]^2,\qquad\frac{dK}{dt}=mv\frac{dv}{dt}}

K(t)=(2−2t)2J.K(t)=(2-2t)^2\ \mathrm J. Therefore K(0)=K(2)=4J.K(0)=K(2)=4\ \mathrm J.

(b) Locate zero speed.

v=0v=0 at t=1s,t=1\ \mathrm s, where K=0K=0. Velocity changes from positive to negative, so this is a stop and reversal.

(c) Keep the interval information.

ΔK0→1=−4J,ΔK1→2=+4J.\Delta K_{0\to1}=-4\ \mathrm J,\qquad \Delta K_{1\to2}=+4\ \mathrm J. Their sum is zero, but kinetic energy was not constant. A zero net change can conceal large intermediate changes.