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  2. Gas constant - Wikipedia

    en.wikipedia.org/wiki/Gas_constant

    The molar gas constant (also known as the gas constant, universal gas constant, or ideal gas constant) is denoted by the symbol R or R. It is the molar equivalent to the Boltzmann constant, expressed in units of energy per temperature increment per amount of substance, rather than energy per temperature increment per particle.

  3. Molar heat capacity - Wikipedia

    en.wikipedia.org/wiki/Molar_heat_capacity

    where R is the ideal gas constant, about 8.31446 J⋅K −1 ⋅mol −1 (which is the product of the Boltzmann constant k B and the Avogadro constant). And, indeed, the experimental values of c V ,m for the noble gases helium , neon , argon , krypton , and xenon (at 1 atm and 25 °C) are all 12.5 J⋅K −1 ⋅mol −1 , which is ⁠ 3 / 2 ...

  4. Table of specific heat capacities - Wikipedia

    en.wikipedia.org/wiki/Table_of_specific_heat...

    The specific heat of the human body calculated from the measured values of individual tissues is 2.98 kJ · kg−1 · °C−1. This is 17% lower than the earlier wider used one based on non measured values of 3.47 kJ · kg−1· °C−1. The contribution of the muscle to the specific heat of the body is approximately 47%, and the contribution ...

  5. Dulong–Petit law - Wikipedia

    en.wikipedia.org/wiki/Dulong–Petit_law

    An equivalent statement of the Dulong–Petit law in modern terms is that, regardless of the nature of the substance, the specific heat capacity c of a solid element (measured in joule per kelvin per kilogram) is equal to 3R/M, where R is the gas constant (measured in joule per kelvin per mole) and M is the molar mass (measured in kilogram per mole).

  6. Ideal gas law - Wikipedia

    en.wikipedia.org/wiki/Ideal_gas_law

    Isotherms of an ideal gas for different temperatures. The curved lines are rectangular hyperbolae of the form y = a/x. They represent the relationship between pressure (on the vertical axis) and volume (on the horizontal axis) for an ideal gas at different temperatures: lines that are farther away from the origin (that is, lines that are nearer to the top right-hand corner of the diagram ...

  7. Equipartition theorem - Wikipedia

    en.wikipedia.org/wiki/Equipartition_theorem

    It follows that the heat capacity of the gas is ⁠ 3 / 2 ⁠ N k B and hence, in particular, the heat capacity of a mole of such gas particles is ⁠ 3 / 2 ⁠ N A k B = ⁠ 3 / 2 ⁠ R, where N A is the Avogadro constant and R is the gas constant. Since R ≈ 2 cal/(mol·K), equipartition predicts that the molar heat capacity of an ideal gas ...

  8. Specific heat capacity - Wikipedia

    en.wikipedia.org/wiki/Specific_heat_capacity

    R is the gas constant (J⋅K −1 ⋅mol −1) N is the number of molecules in the body. (dimensionless) k B is the Boltzmann constant (J⋅K −1) Again, SI units shown for example. Read more about the quantities of dimension one [28] at BIPM In the Ideal gas article, dimensionless heat capacity is expressed as ^

  9. Conformational isomerism - Wikipedia

    en.wikipedia.org/wiki/Conformational_isomerism

    where K is the equilibrium constant, ΔG° is the difference in standard free energy between the two conformers in kcal/mol, R is the universal gas constant (1.987×10 −3 kcal/mol K), and T is the system's temperature in kelvins. In units of kcal/mol at 298 K,