Apply part (b) to each supplied rotational sum. Multiplying the odd sum by its constant nuclear-spin factor three does not change or . At the specified temperature the dimensionless rotational contributions areThus the rotational heat capacities are for parahydrogen and for orthohydrogen. For the total gas heat capacities, including translation and neglecting vibration,The difference is substantial because the permitted rotational ladders differ. The para ladder starts at and next reaches , separated by ; its excited population is changing appreciably here. The ortho ladder starts at and next reaches , a larger separation of , so much of the ortho population remains in its lowest rotational manifold. A rotational contribution greater than is possible in the intermediate quantum regime and is not a violation of high-temperature equipartition.
For a frozen ortho-para mixture, the mole fractions do not change during the heat measurement, and the molar heat capacity is the composition-weighted average. A high-temperature composition retained on cooling has , , soFor a mixture that continues to interconvert and remain in equilibrium near the specified temperature, use the combined rotational sum and differentiate that sum:ConsequentlyThe equilibrium composition itself is , giving . Its changing composition supplies a further positive heat capacity: warming converts some lower-energy para molecules into higher-energy ortho molecules. One can isolate this term asFor clarity, if a mixture is first equilibrated at this temperature and then its composition is frozen during measurement, the conversion term is absent: its rotational value is and its total value is . This is distinct from the equilibrium heat capacity of interconverting states even though the instantaneous composition is the same. An experiment must specify conversion activity and equilibration time; compare sufficiently slow temperature steps with a conversion catalyst against a composition-preserving sample, while keeping the same thermal background and checking that the sample has reached the stated temperature.
Original ideal-rotor heat capacities showing the difference between frozen normal hydrogen and continuously equilibrating hydrogen
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