What Is Energy? — Question 6

Section 7-1 · Physics pages 862–863

Question 6 Hard measurement bounds can expose a missing transfer For this introductory problem use the supplied accounting rule ∆E = Ein −Eout, with all quantities in joules. Independent measurements give input in [98, 102] J, output in [58, 62] J and stored-energy increase in [43, 45] J. These are hard bounds, not standard deviations. ∆E ∈[43, 45] J [98, 102] J [58, 62] J Input, output and stored-change intervals are independent hard bounds. (a) Find the energy-increase interval predicted from input and output alone. (b) Can the three observations agree if all transfers are listed? (c) If an omitted input q is the only missing term, find all possible q values compatible with the bounds.
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Question 6 - Solution Hard measurement bounds can expose a missing transfer ∆E ∈[43, 45] J [98, 102] J [58, 62] J (a) Combine the extreme admissible readings. The governing relation is ∆Epredicted ∈[Imin −Omax, Imax −Omin] ∆Epredicted ∈[98 −62, 102 −58] = [36, 44] J. (b) Intersect the intervals. Yes. The common interval is [43, 44] J, so no missing transfer is compelled by these bounds. Central values give 40 J and 44 J, but a central-value mismatch alone is not proof. (c) Solve for the omitted term. q = ∆E −Ein + Eout ∈[43 −102 + 58, 45 −98 + 62] = [−1, 9] J. Requiring an input, q ≥0, gives [0, 9] J. Zero remains feasible.

Question 6

Hard measurement bounds can expose a missing transfer

For this introductory problem use the supplied accounting rule ΔE=Ein−Eout\Delta E=E_{\mathrm{in}}-E_{\mathrm{out}}, with all quantities in joules. Independent measurements give input in [98,102][98,102] J, output in [58,62][58,62] J and stored-energy increase in [43,45][43,45] J. These are hard bounds, not standard deviations.

Diagram shown in the original SVG worksheet.

  1. Find the energy-increase interval predicted from input and output alone.

  2. Can the three observations agree if all transfers are listed?

  3. If an omitted input q is the only missing term, find all possible q values compatible with the bounds.

Question 6 - Solution

Hard measurement bounds can expose a missing transfer

Diagram shown in the original SVG worksheet.

(a) Combine the extreme admissible readings.

The governing relation is ΔEpredicted∈[Imin−Omax,Imax−Omin]\boxed{\Delta E_{\mathrm{predicted}}\in[I_{\min}-O_{\max},I_{\max}-O_{\min}]}

ΔEpredicted∈[98−62,102−58]=[36,44]J.\Delta E_{\mathrm{predicted}}\in[98-62,102-58]=[36,44]\ \mathrm J.

(b) Intersect the intervals.

Yes. The common interval is [43,44]J[43,44]\ \mathrm J, so no missing transfer is compelled by these bounds. Central values give 40 J and 44 J, but a central-value mismatch alone is not proof.

(c) Solve for the omitted term.

q=ΔE−Ein+Eout∈[43−102+58,45−98+62]=[−1,9]J.q=\Delta E-E_{\mathrm{in}}+E_{\mathrm{out}}\in[43-102+58,45-98+62]=[-1,9]\ \mathrm J. Requiring an input, q≥0q\ge0, gives [0,9]J[0,9]\ \mathrm J. Zero remains feasible.