Separate classical mode counts from a supplied activation law
Classical equipartition assigns mean energy kT/2 to each independent quadratic energy term. Three translational terms give molar Cv=3R/2. A diatomic molecule with two active rotational terms adds R, giving 5R/2 before vibrational and other contributions. Quantum level spacing can suppress a mode at low temperature, so a classical count is a regime statement rather than a universal constant.
Learning outcome: Compare two temperatures at fixed activation scale and two scales at fixed temperature. Differentiate the proposed energy function and retain a regime where classical mode counting is an approximation.
Starting recap
Review definite integrals, probability densities, mean versus mean square, temperature units and the first-law work convention. State the domain and distinguish calibration data from unused validation.
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At T=300 K and theta=200 K, Cv/R=1.5+90000/130000=57/26≈2.1923077. At T=theta it is exactly 2, halfway between the two limiting values. The energy change from 100 K follows the antiderivative, not Cv evaluated only at 300 K times the interval.
Open the experimentPredict
At T=theta, what is the supplied Cv/R?
Experiment
Compare two temperatures at fixed activation scale and two scales at fixed temperature. Differentiate the proposed energy function and retain a regime where classical mode counting is an approximation.
Audit a supplied mode-activation interpolation
Worked teaching model · synthetic values · Supplied molar Cv/R=3/2+T²/(T²+theta²), positive temperatures and fixed volume. This smooth interpolation illustrates one rotational contribution between classical limits; it is not an exact molecular quantum partition function or universal material heat capacity.
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Supplied mode-activation response
Graph axes rescale independently; read units and values, not screen angles. 1: smooth illustrative constitutive law (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Supplied mode-activation response
smooth illustrative constitutive law
| temperature (K) | molar Cv/R |
|---|---|
| 100 | 1.7 |
| 105 | 1.716071 |
| 110 | 1.732246 |
| 115 | 1.748473 |
| 120 | 1.764706 |
| 125 | 1.780899 |
| 130 | 1.797012 |
| 135 | 1.81301 |
| 140 | 1.828859 |
| 145 | 1.844531 |
| 150 | 1.86 |
| 155 | 1.875244 |
| 160 | 1.890244 |
| 165 | 1.904983 |
| 170 | 1.919448 |
| 175 | 1.933628 |
| 180 | 1.947514 |
| 185 | 1.961098 |
| 190 | 1.974376 |
| 195 | 1.987344 |
| 200 | 2 |
| 205 | 2.012344 |
| 210 | 2.024376 |
| 215 | 2.036097 |
| 220 | 2.047511 |
| 225 | 2.058621 |
| 230 | 2.069429 |
| 235 | 2.079942 |
| 240 | 2.090164 |
| 245 | 2.1001 |
| 250 | 2.109756 |
| 255 | 2.119138 |
| 260 | 2.128253 |
| 265 | 2.137106 |
| 270 | 2.145704 |
| 275 | 2.154054 |
| 280 | 2.162162 |
| 285 | 2.170035 |
| 290 | 2.177679 |
| 295 | 2.185101 |
| 300 | 2.192308 |
| 305 | 2.199305 |
| 310 | 2.206098 |
| 315 | 2.212695 |
| 320 | 2.219101 |
| 325 | 2.225322 |
| 330 | 2.231363 |
| 335 | 2.237231 |
| 340 | 2.242931 |
| 345 | 2.248467 |
| 350 | 2.253846 |
| 355 | 2.259072 |
| 360 | 2.264151 |
| 365 | 2.269086 |
| 370 | 2.273884 |
| 375 | 2.278547 |
| 380 | 2.28308 |
| 385 | 2.287488 |
| 390 | 2.291775 |
| 395 | 2.295944 |
| 400 | 2.3 |
| 405 | 2.303946 |
| 410 | 2.307785 |
| 415 | 2.311521 |
| 420 | 2.315157 |
| 425 | 2.318697 |
| 430 | 2.322143 |
| 435 | 2.325499 |
| 440 | 2.328767 |
| 445 | 2.33195 |
| 450 | 2.335052 |
| 455 | 2.338073 |
| 460 | 2.341017 |
| 465 | 2.343887 |
| 470 | 2.346685 |
| 475 | 2.349412 |
| 480 | 2.352071 |
| 485 | 2.354664 |
| 490 | 2.357194 |
| 495 | 2.359661 |
| 500 | 2.362069 |
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.
| Quantity | Value | Unit |
|---|---|---|
| Supplied molar Cv divided by R | 2.192308 | ratio |
| Energy difference from 100 K divided by R | 396.1708 | K |
| Low-temperature asymptote of Cv/R | 1.5 | ratio |
| High-temperature asymptote of Cv/R | 2.5 | ratio |
| Activated rotational contribution divided by R | 0.6923077 | ratio |
Mode counting is a classical limiting model, not a promise that every mode is active at every temperature.
Classical quadratic degrees of freedom each contribute R/2 per mole to Cv. Three translations give 3R/2; two activated rotations add R. The supplied interpolation tends toward those two limits. Integrating it gives U/R=2.5T−theta atan(T/theta)+constant. The reference constant cancels in differences. This is not a derived quantum rotor spectrum and does not model vibrations or dissociation.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Mode counting is a classical limiting model, not a promise that every mode is active at every temperature.
Classical quadratic degrees of freedom each contribute R/2 per mole to Cv. Three translations give 3R/2; two activated rotations add R. The supplied interpolation tends toward those two limits. Integrating it gives U/R=2.5T−theta atan(T/theta)+constant. The reference constant cancels in differences. This is not a derived quantum rotor spectrum and does not model vibrations or dissociation.
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