Thursday, December 31, 2015

bec If the available thermal energy is not much bigger than this energy gap kBT ≲ △ε, KE = 3/2 kT (or kBT) (kB: boltzmann constant)

Einstein's Physics: Atoms, Quanta, and Relativity - ...

https://books.google.com/books?isbn=0199669910
Ta-Pei Cheng - 2013 - ‎Science
If the available thermal energy is not much bigger than this energy gap kBT ≲ △ε, ... On the other hand, Bose–Einstein condensation (BEC) is the phenomenon ..

 KE = 3/2 kT (or kBT) (kB: boltzmann constant)

kT is the product of the Boltzmann constantk, and the temperatureT. This product is used in physics as a scaling factor for energy values in molecular-scale systems (sometimes it is used as a unit of energy), as the rates and frequencies of many processes and phenomena depend not on their energy alone, but on the ratio of that energy andkT, that is, on E / kT (see Arrhenius equationBoltzmann factor). For a system in equilibrium in canonical ensemble, the probability of the system being in state with energy E is proportional to e−ΔE / kT. More fundamentally, kT is the amount of heat required to increase the thermodynamic entropy of a system, in natural units, by one nat.
In macroscopic scale systems, with large numbers of molecules, RT value is commonly used; its SI units are joules per mole (J/mol): (RT = kT ⋅ NA).


In statistical mechanics and mathematics, a Boltzmann distribution (also called Gibbs distribution[1]) is a probability distributionprobability measure, or frequency distribution of particles in a system over various possible states. The distribution is expressed in the form
F({\rm {state}})\propto e^{-{\frac {E}{kT}}}
where E is state energy (which varies from state to state), and kT

No comments:

Post a Comment