
2. THERMODYNAMICS and ENSEMBLES (Part A) Introduction
... Statistical mechanics is concerned with the discussion of systems consisting of a very large number of particles such as gases, liquids, solids, electromagnetic radiation (photon) and most physical chemical or biological systems. A discussion of these would naturally involve the interaction between ...
... Statistical mechanics is concerned with the discussion of systems consisting of a very large number of particles such as gases, liquids, solids, electromagnetic radiation (photon) and most physical chemical or biological systems. A discussion of these would naturally involve the interaction between ...
Thermodynamics for Systems Biology
... The first law expresses the conservation of energy. The law was constructed from separate older conservation laws for mechanical energy in mechanics and for caloric in the theory of heat. It retrospect, the ability to rub two sticks together to produce heat flagrantly contradicts any conservation of ...
... The first law expresses the conservation of energy. The law was constructed from separate older conservation laws for mechanical energy in mechanics and for caloric in the theory of heat. It retrospect, the ability to rub two sticks together to produce heat flagrantly contradicts any conservation of ...
ONSAGER`S VARIATIONAL PRINCIPLE AND ITS APPLICATIONS
... is prescribed to be in the range δE at E0 , we may form a satisfactory ensemble by taking the density as equal to zero except in the selected narrow range δE at E0 : P (E) = constant for energy in δE at E0 and P (E) = 0 outside this range. This particular ensemble is known as the microcanonical ense ...
... is prescribed to be in the range δE at E0 , we may form a satisfactory ensemble by taking the density as equal to zero except in the selected narrow range δE at E0 : P (E) = constant for energy in δE at E0 and P (E) = 0 outside this range. This particular ensemble is known as the microcanonical ense ...
First Law of Thermodynamics Heat and Work done by a Gas
... 1.Will the change in internal energy be the same for the two cylinders? If not, which will be bigger? Ans. Since both systems undergo the same change in Temperature and they contain the same amount of gas, they have the same change in internal energy. ...
... 1.Will the change in internal energy be the same for the two cylinders? If not, which will be bigger? Ans. Since both systems undergo the same change in Temperature and they contain the same amount of gas, they have the same change in internal energy. ...
Thermodynamics
... the faster [Temperature = ave KE = ½ mv2] the molecules move, the more likely they are to collide and they collide with more “umph”. New stuff: ...
... the faster [Temperature = ave KE = ½ mv2] the molecules move, the more likely they are to collide and they collide with more “umph”. New stuff: ...
Free Energy Examples
... A. The average x-direction contribution to kinetic energy of a water molecule is greater than that of a copper atom. B. The average x-direction contribution to kinetic energy of a water molecule is less than that of a copper atom. C. The x-direction contribution kinetic energy of a water molecule is ...
... A. The average x-direction contribution to kinetic energy of a water molecule is greater than that of a copper atom. B. The average x-direction contribution to kinetic energy of a water molecule is less than that of a copper atom. C. The x-direction contribution kinetic energy of a water molecule is ...
Chapter 2. Entropy and Temperature
... where we have used the conservation of s (note the range of summation of s1 ). This assumes that the possible states of the 2 systems are independent of one another. Kittel & Kroemer refer to the set of all states of the combined system for a given s1 and s2 as a configuration. Thus we are intereste ...
... where we have used the conservation of s (note the range of summation of s1 ). This assumes that the possible states of the 2 systems are independent of one another. Kittel & Kroemer refer to the set of all states of the combined system for a given s1 and s2 as a configuration. Thus we are intereste ...
Nano Mechanics and Materials: Theory, Multiscale Methods
... 1) serves as an intrinsic characteristic of any equilibrium system (similar to V and P) 2) determines thermodynamic equilibrium between two systems in thermal contact Thus, it is postulated that: If two adiabatically isolated systems in equilibrium are brought into thermal contact with each other, t ...
... 1) serves as an intrinsic characteristic of any equilibrium system (similar to V and P) 2) determines thermodynamic equilibrium between two systems in thermal contact Thus, it is postulated that: If two adiabatically isolated systems in equilibrium are brought into thermal contact with each other, t ...
2. Laws of thermodynamics
... translational (straight-line) velocity, not rotational or vibrational…This course looks only at translational velocity when examining kinetic theory of gasses. ...
... translational (straight-line) velocity, not rotational or vibrational…This course looks only at translational velocity when examining kinetic theory of gasses. ...
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.