The Zeroth Law of Thermodynamics — Question 9

Section 18-2 · Physics pages 2848–2849

Question 9 A finite-time null result depends on thermal contact strength A passive contact test gives |P| < .030 W. Its independently verified conductance is in [.10, .30] W/K, and P = G(TA −TB) applies at the observation time. No other energy paths are present. A B weak contact: known or unknown G Schematic; labels, not drawing lengths, specify the data. (a) Find the strongest guaranteed upper bound on |TA −TB|. Why must the smallest possible conductance be used? (b) A second test constrains the conductance only to 0 < G ≤.30 W/K. Is any finite temperature-difference bound guaranteed by the same null result?
Show solutionHide solution
Question 9 - Solution A finite-time null result depends on thermal contact strength A B weak contact: known or unknown G (a) Method and calculation |∆T| = |P| G < .030 .10 = .30 K. Using G = .30 would give .10 K, but G = .10, |∆T| = .20 K =⇒|P| = .020 W, which is allowed and refutes that stronger bound. (b) Interpretation and further calculation For any proposed finite bound M > 0, choose |∆T| > M and sufficiently small positive G: 0 < G < min ( .30 W/K, .030 W |∆T| ) , so that |P| < .030 W despite the large temperature difference. No finite guarantee follows without a positive lower conductance bound. Physical check Failure to resolve transfer is evidence about temperature only when the comparison mechanism has established sensitivity.

Question 9

A finite-time null result depends on thermal contact strength

A passive contact test gives |P|<.030W|P|<.030\,\mathrm W. Its independently verified conductance is in [.10,.30]W/K[.10,.30]\,\mathrm{W/K}, and P=G(TA−TB)P=G(T_A-T_B) applies at the observation time. No other energy paths are present.

Diagram shown in the original SVG worksheet.

  1. Find the strongest guaranteed upper bound on |TA−TB||T_A-T_B|. Why must the smallest possible conductance be used?

  2. A second test constrains the conductance only to 0<G≤.30W/K0<G\le.30\,\mathrm{W/K}. Is any finite temperature-difference bound guaranteed by the same null result?

Question 9 - Solution

A finite-time null result depends on thermal contact strength

Diagram shown in the original SVG worksheet.

(a) Method and calculation

|ΔT|=|P|G<.030.10=.30K.|\Delta T|=\frac{|P|}{G}<\frac{.030}{.10}=.30\,\mathrm K.Using G=.30G=.30 would give .10.10 K, butG=.10,|ΔT|=.20K⇒|P|=.020W,G=.10,\quad |\Delta T|=.20\,\mathrm K\ \Longrightarrow\ |P|=.020\,\mathrm W,which is allowed and refutes that stronger bound.

(b) Interpretation and further calculation

For any proposed finite bound M>0M>0, choose |ΔT|>M|\Delta T|>M and sufficiently small positive GG:0<G<min⁡(.30W/K,.030W|ΔT|),0<G<\min\!\left(.30\,\mathrm{W/K},\frac{.030\,\mathrm W}{|\Delta T|}\right),so that |P|<.030W|P|<.030\,\mathrm W despite the large temperature difference. No finite guarantee follows without a positive lower conductance bound.

Physical check

Failure to resolve transfer is evidence about temperature only when the comparison mechanism has established sensitivity.