
R eduction(12).pdf
... Nagel (1961) thought that thermodynamics reduces to the physics of molecular motions in the sense that thermodynamics is deducible from Newtonian mechanics with the help of ‘bridge’ laws that link terms such as ‘temperature’ to microphysical properties such as kinetic energy. Any deduction is, by de ...
... Nagel (1961) thought that thermodynamics reduces to the physics of molecular motions in the sense that thermodynamics is deducible from Newtonian mechanics with the help of ‘bridge’ laws that link terms such as ‘temperature’ to microphysical properties such as kinetic energy. Any deduction is, by de ...
Fundamentals of chemical thermodynamics and bioenergetics
... is located in a well-defined place and there is no spatial disorder either. In case of T = 0, the molecular motions in the substance are kept at a minimum and the number of microstates (W) is one (there is only one way to arrange the atoms or molecules to form a perfect crystal). Under these conditi ...
... is located in a well-defined place and there is no spatial disorder either. In case of T = 0, the molecular motions in the substance are kept at a minimum and the number of microstates (W) is one (there is only one way to arrange the atoms or molecules to form a perfect crystal). Under these conditi ...
Heat of Sublimation - Chemwiki
... for substances in the solid and liquid states. Note that ΔEthermal is divided between ΔPE and ΔKE for substances in the solid and liquid states. This is because the intermolecular and intramolecular forces that exist between the atoms of the substance (i.e. atomic bond, van der Waals forces, etc) ha ...
... for substances in the solid and liquid states. Note that ΔEthermal is divided between ΔPE and ΔKE for substances in the solid and liquid states. This is because the intermolecular and intramolecular forces that exist between the atoms of the substance (i.e. atomic bond, van der Waals forces, etc) ha ...
n - Purdue Physics
... • Mass of 1 mole of “stuff” in grams = molecular mass in u ▪ E.g. 1 mole of N2 has mass of 2 14 = 28 grams ...
... • Mass of 1 mole of “stuff” in grams = molecular mass in u ▪ E.g. 1 mole of N2 has mass of 2 14 = 28 grams ...
Thermodynamic system
... • Internal kinetic energy: sum of kinetic energies of all system parts – does not include motion of the whole system (center of mass) – includes translational, rotational, and vibrational kinetic energy of molecules – average kinetic energy of 1 molecule = n ½kBT ; v ~ 1 km/s (n = number of degrees ...
... • Internal kinetic energy: sum of kinetic energies of all system parts – does not include motion of the whole system (center of mass) – includes translational, rotational, and vibrational kinetic energy of molecules – average kinetic energy of 1 molecule = n ½kBT ; v ~ 1 km/s (n = number of degrees ...
More Thermodynamics
... temperature of a real gas will always decrease upon undergoing a free expansion. How much the temperature decreases depends upon the state point and the parameter a. Molecules having strong attractive interactions (a large a) should show the largest temperature decrease upon expansion. We can unders ...
... temperature of a real gas will always decrease upon undergoing a free expansion. How much the temperature decreases depends upon the state point and the parameter a. Molecules having strong attractive interactions (a large a) should show the largest temperature decrease upon expansion. We can unders ...
Thermodynamics Summary
... Let’s suppose we want to vaporize a liquid to its gas form. Initially the liquid is not about to vaporize. We say it is a compressed liquid or a subcooled liquid. We then add heat. After a while, the liquid will be about to vaporize. We now call it a saturated liquid. When part of the liquid has vap ...
... Let’s suppose we want to vaporize a liquid to its gas form. Initially the liquid is not about to vaporize. We say it is a compressed liquid or a subcooled liquid. We then add heat. After a while, the liquid will be about to vaporize. We now call it a saturated liquid. When part of the liquid has vap ...
Chapter 15
... a system; heat and work is not a system doesn’t have a given amount of heat or work; rather they are added or removed form the system by the change of state of the system so heat and work are part of a thermodynamic process that can change a system from one state to another not a characteristic of t ...
... a system; heat and work is not a system doesn’t have a given amount of heat or work; rather they are added or removed form the system by the change of state of the system so heat and work are part of a thermodynamic process that can change a system from one state to another not a characteristic of t ...
Equipartition theorem

In classical statistical mechanics, the equipartition theorem is a general formula that relates the temperature of a system with its average energies. The equipartition theorem is also known as the law of equipartition, equipartition of energy, or simply equipartition. The original idea of equipartition was that, in thermal equilibrium, energy is shared equally among all of its various forms; for example, the average kinetic energy per degree of freedom in the translational motion of a molecule should equal that of its rotational motions.The equipartition theorem makes quantitative predictions. Like the virial theorem, it gives the total average kinetic and potential energies for a system at a given temperature, from which the system's heat capacity can be computed. However, equipartition also gives the average values of individual components of the energy, such as the kinetic energy of a particular particle or the potential energy of a single spring. For example, it predicts that every atom in a monatomic ideal gas has an average kinetic energy of (3/2)kBT in thermal equilibrium, where kB is the Boltzmann constant and T is the (thermodynamic) temperature. More generally, it can be applied to any classical system in thermal equilibrium, no matter how complicated. The equipartition theorem can be used to derive the ideal gas law, and the Dulong–Petit law for the specific heat capacities of solids. It can also be used to predict the properties of stars, even white dwarfs and neutron stars, since it holds even when relativistic effects are considered.Although the equipartition theorem makes very accurate predictions in certain conditions, it becomes inaccurate when quantum effects are significant, such as at low temperatures. When the thermal energy kBT is smaller than the quantum energy spacing in a particular degree of freedom, the average energy and heat capacity of this degree of freedom are less than the values predicted by equipartition. Such a degree of freedom is said to be ""frozen out"" when the thermal energy is much smaller than this spacing. For example, the heat capacity of a solid decreases at low temperatures as various types of motion become frozen out, rather than remaining constant as predicted by equipartition. Such decreases in heat capacity were among the first signs to physicists of the 19th century that classical physics was incorrect and that a new, more subtle, scientific model was required. Along with other evidence, equipartition's failure to model black-body radiation—also known as the ultraviolet catastrophe—led Max Planck to suggest that energy in the oscillators in an object, which emit light, were quantized, a revolutionary hypothesis that spurred the development of quantum mechanics and quantum field theory.