Kinetic Energy — Question 4

Section 7-2 · Physics pages 878–879

Question 4 A speed uncertainty produces asymmetric energy bounds Use classical translational kinetic energy K = 1 2m|⃗v|2. A particle has mass in [1.9, 2.1] kg and speed in [4.9, 5.1] m/s. Every combination is allowed. A report gives the central estimate 25 J. m ∈[1.9, 2.1] kg v ∈[4.9, 5.1] m/s Independent mass and speed bounds define the allowed kinetic-energy range. (a) Find the exact allowed kinetic-energy interval. (b) Compare the upper and lower deviations from 25 J. (c) Could a separately reported energy of 28 J agree with the stated hard bounds?
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Question 4 - Solution A speed uncertainty produces asymmetric energy bounds m ∈[1.9, 2.1] kg v ∈[4.9, 5.1] m/s (a) Use monotonicity for positive mass and speed. The governing relation is ∂K ∂m = 1 2v2 > 0, ∂K ∂v = mv > 0 Kmin = 1 2(1.9)(4.9)2 = 22.8095 J, Kmax = 1 2(2.1)(5.1)2 = 27.3105 J. (b) Subtract the central estimate. 25 −Kmin = 2.1905 J, Kmax −25 = 2.3105 J. The quadratic speed dependence produces unequal downward and upward deviations; independent bounds do not define a statistical error. (c) Test intersection, not plausibility. No. An exact 28 J lies above 27.3105 J. At least one bound, measurement or modeling assumption would need revision. The intervals are not probabilistic error bars.

Question 4

A speed uncertainty produces asymmetric energy bounds

Use classical translational kinetic energy K=12m|v→|2K=\tfrac12 m|\vec v|^2. A particle has mass in [1.9,2.1][1.9,2.1] kg and speed in [4.9,5.1][4.9,5.1] m/s. Every combination is allowed. A report gives the central estimate 25 J.

Diagram shown in the original SVG worksheet.

  1. Find the exact allowed kinetic-energy interval.

  2. Compare the upper and lower deviations from 25 J.

  3. Could a separately reported energy of 28 J agree with the stated hard bounds?

Question 4 - Solution

A speed uncertainty produces asymmetric energy bounds

Diagram shown in the original SVG worksheet.

(a) Use monotonicity for positive mass and speed.

The governing relation is ∂K∂m=12v2>0,∂K∂v=mv>0\boxed{\frac{\partial K}{\partial m}=\tfrac12v^2>0,\qquad\frac{\partial K}{\partial v}=mv>0}

Kmin=12(1.9)(4.9)2=22.8095J,Kmax=12(2.1)(5.1)2=27.3105J.K_{\min}=\tfrac12(1.9)(4.9)^2=22.8095\ \mathrm J,\qquad K_{\max}=\tfrac12(2.1)(5.1)^2=27.3105\ \mathrm J.

(b) Subtract the central estimate.

25−Kmin=2.1905J,Kmax−25=2.3105J.25-K_{\min}=2.1905\ \mathrm J,\qquad K_{\max}-25=2.3105\ \mathrm J. The quadratic speed dependence produces unequal downward and upward deviations; independent bounds do not define a statistical error.

(c) Test intersection, not plausibility.

No. An exact 28 J lies above 27.3105 J. At least one bound, measurement or modeling assumption would need revision. The intervals are not probabilistic error bars.