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Shapley concentration dabzeš-e Shapley Fr.: concentration de Shapley Same as the → Shapley supercluster. |
shellular rotation carxeš-e puste-yi Fr.: rotation coquillaire A rotation mode in which internal rotation of a star depends essentially on depth and little on latitude: Ω(r,θ) = Ω(r), where r is the mean distance to the stellar center of the considered level surface (or → isobar). This particular mode was introduced by J.-P. Zahn (1992, A&A 265, 115) to simplify the treatment of rotational → mixing, but also on more physical grounds. Indeed differential rotation tends to be smoothed out in latitude through → shear turbulence. See also → von Zeipel theorem; → meridional circulation . Shellular, the structure of this term is not clear; it may be a combination of → shell (referring to star's assumed division in differentially rotating concentric shells) + (circ)ular, → circular. The first bibliographic occurrence of shellular is seemingly in Ghosal & Spiegel (1991, On the Thermonuclear Convection: I. Shellular Instability, Geophys. Astrophys. Fluid Dyn. 61, 161). However, surprisingly the term appears only in the title, and nowhere in the body of the article; → rotation. |
sidereal revolution period dowre-ye gardeš-e axtari (#) Fr.: période de révolution sidérale The time taken by a planet or satellite to complete one revolution about its primary with respect to stars. For Earth, same as → sidereal year. Sidereal periods of the solar system planets, interms of the sidereal year, are as follows: Mercury 0.240846 (87.9691 days); Venus 0.615 (225 days); Earth 1 (365.25636 solar days); Mars 1.881; Jupiter 11.86; Satrurn 29.46; Uranus 84.01; and Neptune 164.8. That of the Moon is 0.0748 (27.32 days) and for → Sedna 12050. → sidereal; → revolution; → period. |
sidereal rotation period dowre-ye carxeš-e axtari Fr.: période de rotation sidérale The rotation period of a celestial body with respect to fixed stars. For Earth, same as → sidereal day. |
signification nešânâreš Fr.: signification 1) Something that is signified, → meaning, sense. Verbal noun of → signify. |
similarity transformation tarâdiseš-e hamânandi Fr.: transformation de similarité 1) A transformation that preserves angles and changes all distances in the same ratio. → similarity; → transformation. |
simple fraction barxe-ye sâdé Fr.: fraction simple A fraction in which the → numerator and → denominator are positive → integer numbers. Compare → compound fraction. |
simple harmonic motion jonbeš-e hamâhang-e sâdé Fr.: mouvement harmonique The motion of a body subjected to a restraining force which is directly proportional to the displacement from a fixed point in the line of motion. The equation of simple harmonic motion is given by x = A sin(ωt + θ0), where x is the body's displacement from equilibrium position, A is the → amplitude, or the magnitude of harmonic oscillations, ω is the → angular frequency, t is the time elapsed, and θ0 is the → initial phase angle. |
simple population porineš-e sâdé Fr.: population simple A set of stars resulting from a spatially (≤ few pc) and temporally (≤ Myr) correlated star formation event. → simple; → population. |
simplification sâde-kard, sâde-šod Fr.: simplification The act of simplifying, or the fact of being simplified. Verbal noun of → simplify. |
simulation mânandeš, hamânand sâzi Fr.: simulation The construction of a mathematical model to reproduce the characteristics of a phenomenon, system, or process, often using a computer, in order to infer information or solve problems. Verbal noun of → simulate. |
single-dish observation nepâhešè-e tak-jâm Fr.: observation avec antenne uinique A radio astronomical observation which uses only one antenna, in contrast to interferometric observations. → single; → dish; → observation. |
singly ionized atom atom-e yekbâr yonidé Fr.: atome une fois ionisé An atom that has lost one electron and has become a positive ion. |
singly ionized carbon Fr.: carbone une fois ionié A carbon atom → singly ionized by a photon of energy 11.3 eV. The ion C+ emits a → fine-structure line (2P3/2→ 2P1/2) at 157.7 μm when excitation conditions are satisfied (critical density ~ 3 x 103 cm-3). In → photodissociation regions, [C II] 157.7 μm is a major cooling line for regions exposed to significant → far ultraviolet (FUV) photon fluxes. In Galactic → H II regions, as well as in the central regions of external galaxies, the luminosity of the [C II] line is typically ~ 0.05-0.5% of the FUV luminosity and correlates well with → carbon monoxide (CO) line intensities. |
singular solution luyeš-e takin Fr.: solution singulière, ~ particulière Of partial differential equations, the solution which cannot be obtained from the general solution by particular choice of arbitrary functions. → general solution; → particular solution. |
site selection gozineš-e sit Fr.: sélection de site The process of choosing a site for an astronomical observatory based on meteorology, seeing conditions, and access to the site. → site; → selection. |
situation siteš Fr.: situation 1) The manner of being placed with respect to surroundings. Verbal noun of → situate. |
sky subtraction zirkaršeš-e âsmân Fr.: soustraction de ciel The act or instance of removing the contribution of non-related, intervening foreground light to the object. → sky; → subtraction. |
SMASS classification radebandi-ye SMASS Fr.: classification SMASS An asteroid taxonomy built on the → Tholen classification but based on the presence or absence of → absorption features in the visible part of the spectrum. In many cases the two classifications are the same, but the Tholen C and S classes are subdivided in the SMASS classification. SMASS stands for the Small Main-belt Asteroid Spectroscopic Survey, → small; → main belt; → asteroid; → spectroscopic; → survey; → classification. |
Sobolev approximation nazdineš-e Sobolev Fr.: approximation de Sobolev A method allowing for a simplified solution to the → radiative transfer equation at frequencies of spectral lines in media moving with a high velocity gradient. This method assumes that the macroscopic velocity gradients are more important than local random variations of thermal line width: dv/dr > vth/l, where dv/dr is the velocity gradient, vth is the thermal broadening of the line, and l the length scale. The Sobolev approximation is only valid if the conditions of the gas do not change over the → Sobolev length. Under the Sobolev approximation, each point in the medium is isolated from other points, and the → radiative transfer problem becomes a local one and therefore much easier to solve. Named after the Russian astronomer Viktor Viktorovich Sobolev, Moving Envelopes of Stars [in Russian], Leningr. Gos. Univ., Leningrad (1947) [translated by S. Gaposchkin, Harvard Univ. Press, Cambridge, Mass. (1960)]; → approximation. |
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