Editing Volumetric heat capacity (section)

==History==
[[Pierre Louis Dulong|Dulong]] and [[Alexis Thérèse Petit|Petit]] predicted in 1818 {{Citation needed|date=February 2010}} that the product of solid substance density and specific heat capacity (ρc<sub>p</sub>) would be constant for all solids. This amounted to a prediction that volumetric heat capacity in solids would be constant. In 1819 they found that volumetric heat capacities were not quite constant, but that the most constant quantity was the heat capacity of solids adjusted by the presumed weight of the atoms of the substance, as defined by Dalton (the [[Dulong–Petit law]]). This quantity was proportional to the heat capacity per [[atomic weight]] (or per [[molar mass]]), which suggested that it is the heat capacity ''per atom'' (not per unit of volume) which is closest to being a constant in solids.

Eventually it became clear that heat capacities per particle for all substances in all states are the same, to within a factor of two, so long as temperatures are not in the cryogenic range.<!-- TO MERGE:
For very cold temperatures, heat capacities fall drastically and eventually approach zero as temperature approaches zero.
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