Temperature — Question 10

Section 18-1 · Physics pages 2830–2831

Question 10 A local temperature requires separation of time scales For a driven material, local microscopic equilibration takes τloc = .002 s. A sensor averages over time ∆t, while the macroscopic state changes appreciably in τdrive = .50 s. Adopt the explicit criteria ∆t ≥10τloc and ∆t ≤τdrive/10 for a meaningful time-resolved local-temperature report. ∆t admissible window 10τloc τdrive/10 Time-scale window; positions are schematic. (a) Find the allowed averaging-time interval. Assess choices .005, .030 and .20 s. (b) If the driving time falls to .10 s, is any averaging time admissible? Derive the general existence condition.
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Question 10 - Solution A local temperature requires separation of time scales ∆t admissible window 10τloc τdrive/10 (a) Method and calculation 10τloc = .020 s, τdrive/10 = .050 s. .020 ≤∆t ≤.050 s . Only .030 s passes: .005 s is too short for the specified equilibration criterion and .20 s blurs the changing state. (b) Interpretation and further calculation A nonempty interval requires 10τloc ≤τdrive/10 ⇐⇒ τdrive ≥100τloc. .10 s < 100(.002 s) = .20 s. No averaging choice works after the change. A numerical sensor output still exists but lacks the stipulated local-equilibrium interpretation. Physical check The factor of 100 follows from the two chosen factors of ten, not from a universal thermodynamic constant.

Question 10

A local temperature requires separation of time scales

For a driven material, local microscopic equilibration takes τloc=.002s\tau_{\mathrm{loc}}=.002\,\mathrm s. A sensor averages over time Δt\Delta t, while the macroscopic state changes appreciably in τdrive=.50s\tau_{\mathrm{drive}}=.50\,\mathrm s. Adopt the explicit criteria Δt≥10τloc\Delta t\ge10\tau_{\mathrm{loc}} and Δt≤τdrive/10\Delta t\le\tau_{\mathrm{drive}}/10 for a meaningful time-resolved local-temperature report.

Diagram shown in the original SVG worksheet.

  1. Find the allowed averaging-time interval. Assess choices .005.005, .030.030 and .20s.20\,\mathrm s.

  2. If the driving time falls to .10s.10\,\mathrm s, is any averaging time admissible? Derive the general existence condition.

Question 10 - Solution

A local temperature requires separation of time scales

Diagram shown in the original SVG worksheet.

(a) Method and calculation

10τloc=.020s,τdrive/10=.050s.10\tau_{\mathrm{loc}}=.020\,\mathrm s,\qquad\tau_{\mathrm{drive}}/10=.050\,\mathrm s..020≤Δt≤.050s.\boxed{.020\le\Delta t\le.050\,\mathrm s}.Only .030.030 s passes: .005.005 s is too short for the specified equilibration criterion and .20.20 s blurs the changing state.

(b) Interpretation and further calculation

A nonempty interval requires10τloc≤τdrive/10⇔τdrive≥100τloc.10\tau_{\mathrm{loc}}\le\tau_{\mathrm{drive}}/10\quad\Longleftrightarrow\quad\tau_{\mathrm{drive}}\ge100\tau_{\mathrm{loc}}..10s<100(.002s)=.20s..10\,\mathrm s<100(.002\,\mathrm s)=.20\,\mathrm s.No averaging choice works after the change. A numerical sensor output still exists but lacks the stipulated local-equilibrium interpretation.

Physical check

The factor of 100 follows from the two chosen factors of ten, not from a universal thermodynamic constant.