statistical decryption - translation to ρωσικά
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statistical decryption - translation to ρωσικά

PHYSICS OF LARGE NUMBER OF PARTICLES' STATISTICAL BEHAVIOR
Statistical Mechanics; Statistical thermodynamics; Non-equilibrium statistical mechanics; Stat mech; Probabilistic mechanics; Statistical dynamics; Fundamental postulate of statistical mechanics; Fundamental assumption of statistical mechanics; Equilibrium statistical mechanics; Classical statistical mechanics; Nonequilibrium statistical mechanics; History of statistical mechanics; Statistical-mechanical

statistical decryption      
статистическое дешифрование
statistical ensemble         
  • classical]] systems in [[phase space]] (top). Each system consists of one massive particle in a one-dimensional [[potential well]] (red curve, lower figure). The initially compact ensemble becomes swirled up over time.
  • Visual representation of five statistical ensembles (from left to right): [[microcanonical ensemble]], [[canonical ensemble]], [[grand canonical ensemble]], [[isobaric-isothermal ensemble]], [[isoenthalpic-isobaric ensemble]]
SET OF POSSIBLE STATES
Using statistical ensembles; Using Statistical Ensembles; Ensemble average; Statistical ensemble; Thermodynamic ensemble; Gibbsian ensemble; Statistical Ensemble; Ensemble averaging (statistical mechanics); Ensemble average (statistical mechanics); Statistical ensemble (mathematical physics)

математика

статистическая совокупность

статистический ансамбль

statistical law         
STATISTICAL TENDENCY THAT OCCURS IN A BROAD RANGE OF DATASETS
Statistical law; Law of statistics
закон распределения

Ορισμός

statistical mechanics
¦ plural noun [treated as sing.] the description of physical phenomena in terms of a statistical treatment of the behaviour of large numbers of atoms or molecules, especially as regards the distribution of energy among them.

Βικιπαίδεια

Statistical mechanics

In physics, statistical mechanics is a mathematical framework that applies statistical methods and probability theory to large assemblies of microscopic entities. It does not assume or postulate any natural laws, but explains the macroscopic behavior of nature from the behavior of such ensembles.

Statistical mechanics arose out of the development of classical thermodynamics, a field for which it was successful in explaining macroscopic physical properties—such as temperature, pressure, and heat capacity—in terms of microscopic parameters that fluctuate about average values and are characterized by probability distributions. This established the fields of statistical thermodynamics and statistical physics.

The founding of the field of statistical mechanics is generally credited to three physicists:

  • Ludwig Boltzmann, who developed the fundamental interpretation of entropy in terms of a collection of microstates
  • James Clerk Maxwell, who developed models of probability distribution of such states
  • Josiah Willard Gibbs, who coined the name of the field in 1884

While classical thermodynamics is primarily concerned with thermodynamic equilibrium, statistical mechanics has been applied in non-equilibrium statistical mechanics to the issues of microscopically modeling the speed of irreversible processes that are driven by imbalances. Examples of such processes include chemical reactions and flows of particles and heat. The fluctuation–dissipation theorem is the basic knowledge obtained from applying non-equilibrium statistical mechanics to study the simplest non-equilibrium situation of a steady state current flow in a system of many particles.

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