Kinetic Energy — Question 10

Section 7-2 · Physics pages 890–891

Question 10 Averaging speed before squaring loses kinetic-energy information Use classical translational kinetic energy K = 1 2m|⃗v|2. A 2 kg cart spends 3 s at speed 2 m/s and 1 s at speed 6 m/s. Ignore the durations of transitions when taking time averages over this idealized record. t (s) v (m/s) 2 6 3 4 The durations are the averaging weights; the transition is idealized as negligible. (a) Find the mean speed and the kinetic energy evaluated at that speed. (b) Find the actual time-average kinetic energy. (c) Derive the difference between these two expressions in terms of the speed variance ⟨(v −⟨v⟩)2⟩.
Show solutionHide solution
Question 10 - Solution Averaging speed before squaring loses kinetic-energy information t (s) v (m/s) 2 6 3 4 (a) Weight the speed by time. The governing relation is ⟨K⟩= 1 2m⟨v2⟩, K(⟨v⟩) = 1 2m⟨v⟩2 ⟨v⟩= (3 · 2 + 1 · 6)/4 = 3 m/s. Kinetic energy at that speed is 1 2(2)32 = 9 J. (b) Average the squared speeds instead. ⟨K⟩= [3(4) + 1(36)]/4 = 12 J. This is 3 J larger. (c) Expand the nonnegative square. ⟨(v −⟨v⟩)2⟩= ⟨v2⟩−⟨v⟩2. Thus ⟨K⟩−K(⟨v⟩) = 1 2m Var(v) ≥0. Equality requires constant speed almost everywhere in the averaging interval.

Question 10

Averaging speed before squaring loses kinetic-energy information

Use classical translational kinetic energy K=12m|v→|2K=\tfrac12 m|\vec v|^2. A 2 kg cart spends 3 s at speed 2 m/s and 1 s at speed 6 m/s. Ignore the durations of transitions when taking time averages over this idealized record.

Diagram shown in the original SVG worksheet.

  1. Find the mean speed and the kinetic energy evaluated at that speed.

  2. Find the actual time-average kinetic energy.

  3. Derive the difference between these two expressions in terms of the speed variance ⟨(v−⟨v⟩)2⟩\langle(v-\langle v\rangle)^2\rangle.

Question 10 - Solution

Averaging speed before squaring loses kinetic-energy information

Diagram shown in the original SVG worksheet.

(a) Weight the speed by time.

The governing relation is ⟨K⟩=12m⟨v2⟩,K(⟨v⟩)=12m⟨v⟩2\boxed{\langle K\rangle=\tfrac12m\langle v^2\rangle,\qquad K(\langle v\rangle)=\tfrac12m\langle v\rangle^2}

⟨v⟩=(3⋅2+1⋅6)/4=3m/s.\langle v\rangle=(3\cdot2+1\cdot6)/4=3\ \mathrm{m/s}. Kinetic energy at that speed is 12(2)32=9J.\tfrac12(2)3^2=9\ \mathrm J.

(b) Average the squared speeds instead.

⟨K⟩=[3(4)+1(36)]/4=12J.\langle K\rangle=[3(4)+1(36)]/4=12\ \mathrm J. This is 3 J larger.

(c) Expand the nonnegative square.

⟨(v−⟨v⟩)2⟩=⟨v2⟩−⟨v⟩2.\langle(v-\langle v\rangle)^2\rangle=\langle v^2\rangle-\langle v\rangle^2. Thus ⟨K⟩−K(⟨v⟩)=12mVar(v)≥0.\langle K\rangle-K(\langle v\rangle)=\tfrac12m\,\mathrm{Var}(v)\ge0. Equality requires constant speed almost everywhere in the averaging interval.