
Phonons The Quantum Mechanics of Lattice Vibrations What is a
... the oscillators are taken quantum mechanically as ...
... the oscillators are taken quantum mechanically as ...
Systems and Surroundings
... Originally, 1 calorie cal was defined as the energy needed to raise the temperature of 1 g of water by 1oC. The modern definition is 1 cal = 4.184 J (exactly) It was postulated that the amount of heat lost by one object equaled exactly the amount gained by the object that received the heat. Heat is ...
... Originally, 1 calorie cal was defined as the energy needed to raise the temperature of 1 g of water by 1oC. The modern definition is 1 cal = 4.184 J (exactly) It was postulated that the amount of heat lost by one object equaled exactly the amount gained by the object that received the heat. Heat is ...
LECTURE 5 Temperature Scales The equation of state of any
... and is path independent. So we can pick a convenient path for doing the integral. In particular, we envision a quasi-static process in going from the initial to the final state. That way the system is always arbitrarily close to equilibrium and the temperature and heat capacity are well defined at a ...
... and is path independent. So we can pick a convenient path for doing the integral. In particular, we envision a quasi-static process in going from the initial to the final state. That way the system is always arbitrarily close to equilibrium and the temperature and heat capacity are well defined at a ...
Lecture 12
... pipes (down to 1K) by Joule-Thomson expansion # Lower temperatures (under 10 µK) can be achieved by adiabatic demagnetization - without a magnetic field, e- in paramagnetic materials are oriented randomly; however, in the presence of a magnetic field, the spin of the e- comes into play # There are m ...
... pipes (down to 1K) by Joule-Thomson expansion # Lower temperatures (under 10 µK) can be achieved by adiabatic demagnetization - without a magnetic field, e- in paramagnetic materials are oriented randomly; however, in the presence of a magnetic field, the spin of the e- comes into play # There are m ...
First Law of Thermodynamics
... Irreversible process is one in which thermal system’s changes cannot be retraced, such as gas expanding to fill a vacuum through an open stopcock. A thermodynamic system can transfer its internal energy by changing the temperature (or phase) of another system of it can use its internal energy to do ...
... Irreversible process is one in which thermal system’s changes cannot be retraced, such as gas expanding to fill a vacuum through an open stopcock. A thermodynamic system can transfer its internal energy by changing the temperature (or phase) of another system of it can use its internal energy to do ...
Thermodynamic functions - Phase Transformations Group
... The Helmholtz free energy F is the corresponding term at constant volume, when H is replaced by U in equation 9. A process can occur spontaneously if it leads to a reduction in the free energy. Quantities such as H, G and S are path independent and therefore are called functions of state. More About ...
... The Helmholtz free energy F is the corresponding term at constant volume, when H is replaced by U in equation 9. A process can occur spontaneously if it leads to a reduction in the free energy. Quantities such as H, G and S are path independent and therefore are called functions of state. More About ...
The Canonical Ensemble
... The study of thermodynamics is concerned with systems which can be described simply by a set of macroscopically observable variables. These systems can be described by statistical ensembles that depend on a few observable parameters, and which are in statistical equilibrium. Microcanonical ensemb ...
... The study of thermodynamics is concerned with systems which can be described simply by a set of macroscopically observable variables. These systems can be described by statistical ensembles that depend on a few observable parameters, and which are in statistical equilibrium. Microcanonical ensemb ...
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.