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birefringent vacuum xala'-e došekastgar Fr.: vide biréfringent Empty space undergoing → vacuum birefringence. → birefringent; → vacuum. |
Birkhoff's theorem farbin-e Birkhoff Fr.: théorème de Birkhoff For a four dimensional → space-time, the → Schwarzschild metric is the only solution of → Einstein's field equations which describes the gravitational field created by a spherically symmetrical distribution of mass. The theorem implies that the gravitational field outside a sphere is necessarily static, and that the metric inside a spherical shell of matter is necessarily flat. The theorem was first demonstrated in 1923 by George David Birkhoff (1884-1944), an American mathematician; → theorem |
blackbody photosphere šidsepehr-e siyah-jesm Fr.: photosphère de corps noir The → blackbody surface of the → Universe defined at a → redshift of about z ≥ 2 × 106. This is distinct from the → last scattering surface, in other words the → cosmic microwave background radiation (CMBR), which refers to z = 1100. Prior to the epoch of the blackbody photosphere the distortions from the → Big Bang are exponentially suppressed. → blackbody; → atmosphere. |
blackbody temperature damâ-ye siyah-jesm (#) Fr.: température de corps noir The temperature at which a blackbody would emit the same radiation per unit area as that emitted by a given body at a given temperature. → blackbody; → temperature. |
blue region nâhiye-ye âbi Fr.: région bleue The portion of the → visible spectrum lying between 455 and 492 nm. |
blurred image vine-ye târ, ~ nâtig, tasvir-e ~ Fr.: image estompée, ~ floue An image which is dim, indistinct, or vague in appearance, for instance when the optics is not well-focused or when the seeing is poor. The same as → unsharp image, contrary to → sharp image. |
bolometric correction aršâyeš-e tafsanji, ~ tafsanjik Fr.: correction bolométrique The difference between the → visual magnitude and → bolometric magnitude. → bolometric; → correction. |
Boltzmann's relation bâzâneš-e Boltzmann Fr.: relation de Boltzmann A relation between the → entropy of a given → state of a → thermodynamic system and the → probability of the state: S = k . ln Ω where S is the entropy of the system, k is → Boltzmann's constant, and Ω the thermodynamic probability of the state. Boltzmann's relation connects → statistical mechanics and → thermodynamics. Ω is the number of possible → microstates of the system, and it represents the → randomness of the system. The relation also describes the statistical meaning of the → second law of thermodynamics. This expression has been carved above Boltzmann's name on his tombstone in Zentralfreihof in Vienna. Same as → Boltzmann's entropy formula. → Boltzmann's constant; → relation. |
Bondi-Hoyle accretion farbâl-e Bondi-Hoyle Fr.: accrétion de Bondi-Hoyle The → accretion of mass by a star (assumed as point particle) moving at a steady speed through an infinite, uniform gas cloud. It is directly proportional to the star mass (M) and the medium density (ρ) and inversely proportional to the relative star/gas velocity (v). In its classical expression: 4πρ(G M)2 / v3, where G is the → gravitational constant. See Bondi & Hoyle (1944, MNRAS 104, 273) and Bondi (1952, MNRAS 112, 195). For a recent treatment of accretion in a turbulent medium see Krumholtz et al. 2006 (ApJ 638, 369). Named after Hermann Bondi (1919-2005), an Anglo-Austrian mathematician and cosmologist and Fred Hoyle (1915-2001), British mathematician and astronomer best known as the foremost proponent and defender of the steady-state theory of the universe; → accretion. |
Bondi-Hoyle accretion radius šo'â'-e farbâl-e Bondi-Hoyle Fr.: rayon de l'accrétion de Bondi-Hoyle In the → Bondi-Hoyle accretion process, the radius where the gravitational energy owing to star is larger than the kinetic energy and, therefore, at which material is bound to star. The Bondi-Hoyle accretion radius is given by RBH = 2 GM / (v2 + cs2) where G is the gravitational constant, M is the stellar mass, v the gas/star relative velocity, and cs is the sound speed. → Bondi-Hoyle accretion; → radius. |
Bonnor-Ebert sphere epehr-e Bonnor-Ebert, kore-ye ~ Fr.: sphère de Bonnor-Ebert A sphere of interstellar gas at uniform temperature in equilibrium under its own gravitation and an external pressure. The pressure of a hotter surrounding medium causes the sphere to collapse. → Bonnor-Ebert mass. → Bonnor-Ebert mass; → sphere. |
bottom-up structure formation diseš-e sâxtâr az pâyin bé
bâlâ Fr.: formation des structures du bas vers le haut A → structure formation scenario in which small galaxies form first, and larger structures are then formed in due course. Contrary to → top-down structure formation. |
bound occurrence roxdâd-e bandidé Fr.: occurrence liée Any → occurrence of a → variable x in an x-bound part of a → wff. → bound; → occurrence. |
bound-free transition gozareš-e bandidé-âzâd Fr.: transition liée-libre A transition in which a bound electron is liberated. → free-bound emission; → free-free emission. |
Bowen fluorescence mechanism sâzokâr-e fluoresti-ye Bowen Fr.: mécanisme de fluorescence de Bowen A mechanism, made possible by certain chance coincidences between → spectral lines of He II, O III and N III in some → planetary nebulae , that explains the presence with a high intensity of a selected group of O III and N III lines while all other lines of these elements are missing. After I. S. Bowen who first discovered this mechanism in 1935; → fluorescence; → mechanism. |
break 1) šekastan; boridan; gosastan; 2) šekast; boreš, boré;
gosast Fr.: 1) couper, rompre; 2) brisure, coupure 1) To separate into parts or fragments violently; to become broken. From break, from M.E. breken, O.E. brecan, from P.Gmc. *brekan (cf. Du. breken, O.H.G. brehhan, Ger. brechen), from PIE base *bhreg- "to break" (see also → fraction). 1) Šekastan, škan- "to break, split;"
Mid.Pers. škastan "to break;" Av. scind-, scand
"to break, cleave;" Proto-Iranian *skand- "to break, cleave;"
PIE sken- "to cut off." |
break luminosity tâbandegi-ye boré Fr.: luminosité de coupure A characteristic luminosity around which the → luminosity function of a sample of galaxies changes to a steeper slope or exponentially declines. → break; → luminosity. |
break-up velocity tondâ-ye gosast Fr.: vitesse de rupture The velocity of a → rotating star at which the → centrifugal force equals the → gravitational force. Also known as → critical velocity. The simplest expression of the break-up velocity for an OB star, ignoring the → Eddington luminosity, is given by the relation: v = (GM / R)1/2, where M and R are the mass and radius of the star respectively, and G the → gravitational constant. A more realistic expression takes into account not only the → radiation pressure, but also the non-uniformity of the brightness over the stellar surface, as indicated by → von Zeipel theorem. With these conditions, the break-up velocity has a more complicated formula, corresponding to the velocity reached when somewhere on the star the → total gravity becomes zero. |
breakthrough tarâšekâft Fr.: percée 1) An act of overcoming or penetrating an obstacle or restriction. Tarâšekâft, from tarâ-, → trans-, + šekâft, past stem of šekâftan "to split, break, tear," → fission. |
breccia bereš (#) Fr.: brèche A rock composed of angular fragments (over two millimeter diameter) of older rocks melded together with a matrix of smaller particles or a mineral cement. From It. breccia "broken (rock)," from a Germanic source akin to O.H.G. brecha "a breaking," ultimately from PIE *bhreg- "to break," → fraction. Bereš, loan from Fr. |
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