Why can a bundle of wires warm the coldest sample stage? Wires conduct heat from warmer stages to the sample, adding to the heat the refrigerator must remove. A clamp on an intermediate cold plate intercepts much of that heat. Poor thermal contact can also leave the sample warmer than the mixing chamber.
Watch helium-3 cross a liquid phase boundary and carry heat from the mixing chamber. Drag the wire clamp to compare heat interception, weak exchange and poor sample contact.
Interactive modelDilution Refrigerator
Already precooled. The apparatus replays the first heater step at four times physical time. Surface tint follows model temperature; pipes and markers are enlarged.
Temperature reconstructed from reversed sensor observations
Mixing chamberSample
t/s · T/mK
Recorded heater steps and conditional mixing-chamber cooling
Measured heater powerEnthalpy model with measured flow and temperature
t/s · P/μW
Raw observations, standards and uncertainty
Each sensor has three fitted reference baths, two withheld temperatures, a second excitation and an actual bath-step response check. Flow, current and voltage each carry separate fit and withheld standards. Reference baths and uncertainties are declared synthetic inputs.
Scroll the table sideways to see every column.
First eight raw observations; full channels and references are exported
The 1971 NBS cooling coefficients are 94 and 12; the equal-temperature difference is 82. The dilute exchanger stream uses heat capacity 107.2 times temperature. The finite junction sends wire heat into the fixed cold plate, whose external cooler removes that heat. Wire conductivity, thermal masses and contact coefficients are synthetic. Quantitative integration covers the two lowest nodes from 20 to 40 millikelvin.
Three settled heater steps test a differential cooling slope. The absolute cooling curve uses the stated enthalpy law with calibrated flow and temperature. A single temperature does not determine the unknown parasitic heat.
Physics tutorial
Follow heat into the coldest stage
BackgroundHelium-3 absorbs heat as it crosses from the upper concentrated liquid into the lower dilute liquid. Circulation removes helium-3 from the dilute side and returns it to the concentrated side.
Why it mattersThe sample still needs wiring and a thermometer. Each connection adds a possible route for heat.
Start with the essentials
Focus question
Why can a bundle of wires warm the coldest sample stage?
One-sentence intuition
A thermal anchor diverts wire heat to an intermediate plate; the sample also needs good contact with the mixing chamber.
Core mathematical model
Heat absorbed in the mixing chamber
Q˙m=n˙3(94Tm2−12Ti2)
This 1971 NBS approximation is used only in the selected 20–40 millikelvin window. Temperatures are kelvin and flow is moles per second. The coefficients have units of joules per mole per kelvin squared. Warmer incoming liquid reduces cooling.
Heat conducted along a wire
Q˙u→v=LA∫TvTuκ(T)dT,κ(T)=k1T
Larger area and shorter length carry more heat. The synthetic effective alloy is used from 20 millikelvin to four kelvin. A finite anchor junction must send away exactly the heat that arrives.
Energy stored in two nodes
Ui=21γiTi2,U˙m+U˙s=Pin+Q˙wire−Q˙m
Sample-to-mixing heat cancels when the nodes are added. Electrical heat, parasitic heat and thermometer dissipation enter; helium circulation removes energy.
Resistance from reversed excitation
R=I+−I−V+−V−
Current reversal removes a stable thermoelectric offset. Each sensor has its own reference baths. Held-out temperatures and a second excitation check must pass before resistance is reported as a platform temperature.
Common difficulties
The sample temperature
Typical misconceptionA cold mixing chamber guarantees an equally cold sample.
Better mental modelA heated sample passes heat back through a finite contact. That heat needs a temperature difference, so the sample can remain warmer.
What heater steps determine
Typical misconceptionOne temperature determines every heat leak.
Better mental modelSettled heater steps show how an added heat load changes temperature. An absolute heat leak also needs independent background and conductance measurements.
Run the experiment
01
Loosen the wire clamp
Hold the gold clamp and drag left, or focus the canvas and press the left arrow.
What to observe: Weaker anchor contact warms the junction and sends more wire heat to the mixing chamber. The thermal graph and newly acquired curve change before release.
02
Stop circulation
Choose Circulation stops and follow the end of the temperature trace.
What to observe: Positive heat input keeps warming the nodes. The run stops at the 40-millikelvin boundary and withholds a cooling inference.
03
Compare the sample and mixing chamber
Choose Weak sample contact and inspect the sample mount.
What to observe: The same sample heater needs a larger temperature difference to pass its heat through weaker contact.
04
Check thermometer excitation
Choose Thermometer self-heating and open the raw observations and standards.
What to observe: The sensor warms itself and fails the independent high-excitation bath check. Raw resistance remains available; platform thermometry is withheld.
05
Keep a cooling scan
Keep the run, change the anchor, select the old record and export CSV or JSON.
What to observe: The three heater steps, unsettled observations, reversed currents and references remain fixed and support independent replay.
Related experiments and articles
How physics instruments measure · Reading path
How physics instruments measure
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