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==Volumetric heat capacity of gases== Large complex gas molecules may have high heat capacities per mole (of molecules), but their heat capacities per mole of '''atoms''' are very similar to those of liquids and solids, again differing by less than a factor of two per mole of atoms. This factor of two represents vibrational degrees of freedom available in solids vs. gas molecules of various complexities. In monatomic gases (like argon) at room temperature and constant volume, volumetric heat capacities are all very close to 0.5 kJβ K<sup>β1</sup>β m<sup>β3</sup>, which is the same as the theoretical value of {{sfrac|3|2}}RT per kelvin per mole of gas molecules (where '''R''' is the [[gas constant]] and T is temperature). As noted, the much lower values for gas heat capacity in terms of volume as compared with solids (although more comparable per mole, see below) results mostly from the fact that gases under standard conditions consist of mostly empty space (about 99.9% of volume), which is not filled by the atomic volumes of the atoms in the gas. Since the molar volume of gases is very roughly 1000 times that of solids and liquids, this results in a factor of about 1000 loss in volumetric heat capacity for gases, as compared with liquids and solids. Monatomic gas heat capacities per atom (not per molecule) are decreased by a factor of 2 with regard to solids, due to loss of half of the potential [[Degrees of freedom (mechanics)|degrees of freedom]] per atom for storing energy in a monatomic gas, as compared with regard to an ideal solid. There is some difference in the heat capacity of monatomic vs. polyatomic gasses, and also gas heat capacity is temperature-dependent in many ranges for polyatomic gases; these factors act to modestly (up to the discussed factor of 2) increase heat capacity per atom in polyatomic gases, as compared with monatomic gases. Volumetric heat capacities in polyatomic gases vary widely, however, since they are dependent largely on the number of atoms per molecule in the gas, which in turn determines the total number of atoms per volume in the gas. The volumetric heat capacity is defined as having [[SI]] units of [[joule|J]]/([[cubic metre|m<sup>3</sup>]]β [[Kelvin|K]]). It can also be described in Imperial units of [[British thermal unit|BTU]]/([[cubic foot|ft<sup>3</sup>]]β [[Fahrenheit|Β°F]]).
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