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SCIENCE · INVESTIGATE AND EXPLAIN

Distinguish useful conduction, leakage and a changed response law

A synthetic heater maintains a hot body while a cold calorimeter and ambient stay at 300 K. The first hot temperature is 400 K. In a linear model the useful path has conductance K and the leak has L, both in W/K. Heater power is 100(K+L); independent cold-side calorimetry reads 100K. The two measurements must have genuinely independent calibration premises.

Learning outcome: Fit useful and leak conductances with explicitly distinct records. Freeze both changed-temperature predictions, inspect the unused record, and propagate the direct prediction bound without double counting shared errors.

Starting recap

Review logarithmic integrals, equilibrium states, absolute temperature and the first-law work convention. State the domain and distinguish calibration data from unused validation.

All lessons are open directly. Your saved experiments remain when you leave and return.

Try

For K=2, L=1, first heater/cold records are 300/200 W. The linear fresh prediction is 600 W, while the fitted quadratic leak predicts 800 W. The supplied generator yields 600 W, supporting the linear family for this test but not independently proving calibration or real-device behavior.

Open the experiment

Predict

Which extra record separates K from L after one heater power reading?

Experiment

Fit useful and leak conductances with explicitly distinct records. Freeze both changed-temperature predictions, inspect the unused record, and propagate the direct prediction bound without double counting shared errors.

Separate a heat leak from useful conduction

Worked teaching model · synthetic values · Cold body and ambient both fixed300 K. Synthetic first records at hot400 K: heater power100(K+L), cold calorimeter100K. These independently calibrated readings identify K and L in the linear-leak model. A fresh hot500 K record tests it against a quadratic leak fitted at400 K. Controls reveal generators, not independent calibration evidence.

Reset keeps your prediction, captures and practice history.

Equal calibration record does not ensure equal extrapolation

heater power (W)hot temperature (K)05008000

Graph axes rescale independently; read units and values, not screen angles. 1: linear leak fitted at 400 K (solid).2: quadratic leak fitted at 400 K (dashed).3: unused 500 K heater record (open-circle marked location). Joined curves show the supplied model, not additional observations.

Equivalent numerical coordinates for Equal calibration record does not ensure equal extrapolation

linear leak fitted at 400 K

hot temperature (K)heater power (W)
3000
302.57.5
30515
307.522.5
31030
312.537.5
31545
317.552.5
32060
322.567.5
32575
327.582.5
33090
332.597.5
335105
337.5112.5
340120
342.5127.5
345135
347.5142.5
350150
352.5157.5
355165
357.5172.5
360180
362.5187.5
365195
367.5202.5
370210
372.5217.5
375225
377.5232.5
380240
382.5247.5
385255
387.5262.5
390270
392.5277.5
395285
397.5292.5
400300
402.5307.5
405315
407.5322.5
410330
412.5337.5
415345
417.5352.5
420360
422.5367.5
425375
427.5382.5
430390
432.5397.5
435405
437.5412.5
440420
442.5427.5
445435
447.5442.5
450450
452.5457.5
455465
457.5472.5
460480
462.5487.5
465495
467.5502.5
470510
472.5517.5
475525
477.5532.5
480540
482.5547.5
485555
487.5562.5
490570
492.5577.5
495585
497.5592.5
500600

At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.

quadratic leak fitted at 400 K

hot temperature (K)heater power (W)
3000
302.55.0625
30510.25
307.515.5625
31021
312.526.5625
31532.25
317.538.0625
32044
322.550.0625
32556.25
327.562.5625
33069
332.575.5625
33582.25
337.589.0625
34096
342.5103.0625
345110.25
347.5117.5625
350125
352.5132.5625
355140.25
357.5148.0625
360156
362.5164.0625
365172.25
367.5180.5625
370189
372.5197.5625
375206.25
377.5215.0625
380224
382.5233.0625
385242.25
387.5251.5625
390261
392.5270.5625
395280.25
397.5290.0625
400300
402.5310.0625
405320.25
407.5330.5625
410341
412.5351.5625
415362.25
417.5373.0625
420384
422.5395.0625
425406.25
427.5417.5625
430429
432.5440.5625
435452.25
437.5464.0625
440476
442.5488.0625
445500.25
447.5512.5625
450525
452.5537.5625
455550.25
457.5563.0625
460576
462.5589.0625
465602.25
467.5615.5625
470629
472.5642.5625
475656.25
477.5670.0625
480684
482.5698.0625
485712.25
487.5726.5625
490741
492.5755.5625
495770.25
497.5785.0625
500800

At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.

unused 500 K heater record

hot temperature (K)heater power (W)
500600

At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.

Calculated quantities under the declared measurement model
QuantityValueUnit
Calibration heater power at 400 K300W
Independent cold calorimeter at 400 K200W
Inferred useful conductance2W/K
Inferred linear leak conductance1W/K
Frozen linear prediction at 500 K600W
Quadratic-leak alternative prediction at 500 K800W
Fresh generated heater power600W
Useful-conductance error bound for ±2 W calorimetry0.02W/K
Leak-conductance error bound for each reading ±2 W0.04W/K
Direct heater prediction bound from ±2 W first heater record4W

An independent cold-side record separates useful conduction from leak, and a new temperature tests the leak law.

A single heater record constrains K+L only. Independent cold-side calorimetry gives K; subtraction yields L. The quadratic alternative L deltaT²/(100 K) shares the first calibration but differs at the fresh temperature. For independent absolute errors ε in each first record, K error≤ε/100 and L error≤2ε/100; the direct total heater prediction is twice the first heater record, so its bound is 2ε, not a sum treating fitted K and L errors as independent. Add fresh-record error when judging residuals. Shared calibration gain remains unidentifiable without independent calibration.

Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.

An independent cold-side record separates useful conduction from leak, and a new temperature tests the leak law.

A single heater record constrains K+L only. Independent cold-side calorimetry gives K; subtraction yields L. The quadratic alternative L deltaT²/(100 K) shares the first calibration but differs at the fresh temperature. For independent absolute errors ε in each first record, K error≤ε/100 and L error≤2ε/100; the direct total heater prediction is twice the first heater record, so its bound is 2ε, not a sum treating fitted K and L errors as independent. Add fresh-record error when judging residuals. Shared calibration gain remains unidentifiable without independent calibration.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

Declare the system and evidence

A synthetic heater maintains a hot body while a cold calorimeter and ambient stay at 300 K. The first hot temperature is 400 K. In a linear model the useful path has conductance K and the leak has L, both in W/K. Heater power is 100(K+L); independent cold-side calorimetry reads 100K. The two measurements must have genuinely independent calibration premises.

Derive the state or rate account

One heater record alone identifies only K+L. Adding the cold-side record gives K=Pcold/100 and L=(Pheater−Pcold)/100. A small heater residual cannot prove that the inferred useful conductance equals the total. A negative fitted leak outside the stated nonnegative family should prompt a calibration/model check, not silent clipping.

Audit the constraint and model

After fitting, freeze a prediction at hot 500 K. The linear model predicts 200(K+L). A competing leak law L(deltaT)²/(100 K), chosen to agree at the 400 K calibration, predicts 200K+400L. The unused heater record therefore tests response shape when L is nonzero. At zero leak both models coincide; no experiment can discriminate hypotheses that predict the same record.

Predict a changed boundary

If each first power reading has independent absolute error at most 2 W, K error is at most 0.02 W/K and L error at most 0.04 W/K. These fitted errors are correlated through the reused cold record. The direct 500 K heater prediction is 2Pheater, so its bound is 4 W, not a larger bound formed by pretending K and L errors are independent. Add fresh measurement error for a residual threshold. Shared gain cannot be resolved by simply collecting more readings from the same uncalibrated system.

Worked original case

For K=2, L=1, first heater/cold records are 300/200 W. The linear fresh prediction is 600 W, while the fitted quadratic leak predicts 800 W. The supplied generator yields 600 W, supporting the linear family for this test but not independently proving calibration or real-device behavior.

Investigation

Fit useful and leak conductances with explicitly distinct records. Freeze both changed-temperature predictions, inspect the unused record, and propagate the direct prediction bound without double counting shared errors.

Changed-case practice

Try the changed case before feedback

First heater and cold readings at 400 K are 450 W and 300 W. Under the linear family predict heater power at 500 K in watts.

This practice is public and unsaved. A matching number does not verify understanding. Retain your explanation, assumptions and changed-case evidence in the separate course workspace.

Sources and boundaries

Original derivations and synthetic cases checked 31 October 2026 against the primary teaching reference. No source exercises or diagrams are reproduced. All thermal operations are mathematical proposals or supplied records, not physical heating, pressure-vessel or exposure instructions. Public feedback and retained prose do not certify independent reasoning or actual practical participation. Preserve first work, critique, revision and a new assigned response in the separate course workspace.

Apply

Which extra record separates K from L after one heater power reading?

Public practice checks a specific claim. It does not establish independent mastery.

Which system boundary, reference path, constitutive law or independently calibrated record supports this entropy inference?

Continue

Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.

Skipping retains experiments and awards no mastery.

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