parabolically degenerate - translation to ρωσικά
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parabolically degenerate - translation to ρωσικά

COLLECTION OF FREE, NON-INTERACTING PARTICLES WITH A PRESSURE AND OTHER PHYSICAL CHARACTERISTICS DETERMINED BY QUANTUM MECHANICAL EFFECTS
Degeneracy pressure; Neutron degeneracy pressure; Degenerate gases; Degenerate gas; Degenerate pressure; Degenerancy Pressure; Degeneracy Pressure; Degenerate Gas; Neutron-degenerate matter; Electron-degenerate matter; Quark-degenerate matter; Preon-degenerate matter; Degenerate Fermi gas; Neutron degenerate matter; Neutron degeneracy; Fermion degeneracy pressure
  • Pressure vs temperature curves of classical and quantum ideal gases ([[Fermi gas]], [[Bose gas]]) in three dimensions.

parabolically degenerate      

математика

параболически вырожденный

non-degenerate         
POSSIBLE X & Y FOR X-E CONJUGATES
Non-degenerate bilinear form; Non-degenerate; Nondegeneracy; Nondegenerate bilinear form; Nondegenerate form; Nonsingular form; Degenerate form

математика

невырожденный

невырождающийся

degenerate form         
POSSIBLE X & Y FOR X-E CONJUGATES
Non-degenerate bilinear form; Non-degenerate; Nondegeneracy; Nondegenerate bilinear form; Nondegenerate form; Nonsingular form; Degenerate form

математика

вырожденная форма

Βικιπαίδεια

Degenerate matter

Degenerate matter is a highly dense state of fermionic matter in which the Pauli exclusion principle exerts significant pressure in addition to, or in lieu of, thermal pressure. The description applies to matter composed of electrons, protons, neutrons or other fermions. The term is mainly used in astrophysics to refer to dense stellar objects where gravitational pressure is so extreme that quantum mechanical effects are significant. This type of matter is naturally found in stars in their final evolutionary states, such as white dwarfs and neutron stars, where thermal pressure alone is not enough to avoid gravitational collapse.

Degenerate matter is usually modelled as an ideal Fermi gas, an ensemble of non-interacting fermions. In a quantum mechanical description, particles limited to a finite volume may take only a discrete set of energies, called quantum states. The Pauli exclusion principle prevents identical fermions from occupying the same quantum state. At lowest total energy (when the thermal energy of the particles is negligible), all the lowest energy quantum states are filled. This state is referred to as full degeneracy. This degeneracy pressure remains non-zero even at absolute zero temperature. Adding particles or reducing the volume forces the particles into higher-energy quantum states. In this situation, a compression force is required, and is made manifest as a resisting pressure. The key feature is that this degeneracy pressure does not depend on the temperature but only on the density of the fermions. Degeneracy pressure keeps dense stars in equilibrium, independent of the thermal structure of the star.

A degenerate mass whose fermions have velocities close to the speed of light (particle kinetic energy larger than its rest mass energy) is called relativistic degenerate matter.

The concept of degenerate stars, stellar objects composed of degenerate matter, was originally developed in a joint effort between Arthur Eddington, Ralph Fowler and Arthur Milne. Eddington had suggested that the atoms in Sirius B were almost completely ionised and closely packed. Fowler described white dwarfs as composed of a gas of particles that became degenerate at low temperature. Milne proposed that degenerate matter is found in most of the nuclei of stars, not only in compact stars.

Μετάφραση του &#39parabolically degenerate&#39 σε Ρωσικά