stellar feedback bâzxord-e setâre-yi Fr.: rétroaction stellaire The process whereby large quantities of → energy and → momentum are released into the gas surrounding → star formation regions in galaxies. More specifically, → massive stars inject → energy, → mass, and → metals back to the → interstellar medium through → stellar winds and → supernova explosions. Feedback inhibits further star formation either by removing gas from the galaxy, or by heating it to temperatures that are too high to form new stars. Observations reveal feedback in the form of → galactic-scale outflows of gas in galaxies with high → star formation rates, especially in the → early Universe. Feedback in faint, low-mass galaxies (→ low-mass galaxy) probably facilitated the escape of ionizing radiation from galaxies when the Universe was about 500 million years old, so that the hydrogen between galaxies changed from neutral to ionized, a process called → reionization (Dawn K. Erb, 2015, Nature, 9 July). |
stellar interior darune-ye setâré Fr.: intérieur stellaire That part of a star which lies below the photosphere. |
stellar luminosity tâbandegi-ye setâré Fr.: luminosité stellaire The total amount of energy emitted by a star per unit time. According to the → Stefan-Boltzmann law, the stellar luminosity is given by: L* = 4πR*2σTeff4, where R* is radius, σ is the → Stefan-Boltzmann constant, and Teff is → effective temperature. A star's luminosity depends, therefore, on two factors, its size and its surface temperature. Stellar luminosity is measured either in ergs per second or in units of → solar luminosity or in → absolute magnitude. See also → luminosity class. → stellar; → luminosity. |
stellar magnetic field meydân-e meqnâtisi-ye setâre-yi Fr.: champ magnétique stellaire The → magnetic field associated with a star. Magnetic fields are common among stars of solar and lower masses. So far definitive detections of fields in stars with masses ~1.5 Msun have, for the most part, been made for objects having anomalous chemical abundances (e.g., the → chemically peculiar A and B stars). Recently, however, observations of cyclic variability in the properties of → stellar winds from luminous → OB stars have been interpreted as evidence for the presence of large-scale magnetic fields in the surface layers and atmospheres of these objects (→ magnetic massive star). These inferences have been bolstered by the unambiguous measurement of a weak (~ 360 G) field in the chemically normal B1 IIIe star → Beta Cephei. These results suggest that magnetic fields of moderate strength might be more prevalent among → hot stars than had previously been thought. At the present time, the origin of magnetism in massive stars is not well understood. If the magnetic field of a hot star is produced by → dynamo effect in the → convective core, then a mechanism for transporting the field to the stellar surface must be identified. The finite electrical conductivity of the envelope leads to the outward diffusion of any fields contained therein, but only over an extended period of time. Estimates indicate that for stars more massive than a few solar masses, the resistive diffusion time across the radiative interior exceeds the → main sequence lifetime. Another possibility is that dynamo fields are advected from the core to the surface by rotation-induced → meridional circulation (MacGregor & Cassinelli, 2002, astro-ph/0212224). |
stellar mass jerm-e setâre-yi Fr.: masse stellaire 1) The quantity of mass contained in a star. It is usually
expressed in terms of the → solar mass
(Msun). |
stellar metallicity felezigi-ye setâre-yi Fr.: métallicité stellaire The metallicity derived from observations of stars in galaxies. It is mainly based on spectral → absorption lines in → ultraviolet (UV) and optical ranges. Stellar metallicity is a direct measure of the amount of metals in a galaxy, since large part of heavy elements lies in its stars. → stellar; → metallicity. |
stellar nucleosynthesis haste-handâyeš-e setâre-yi Fr.: nucléosynthèse stellaire The → nuclear reaction process taking place inside stars, whereby → chemical elements are produced from pre-existing nuclei heavier than → hydrogen and → helium. → stellar; → nucleosynthesis. |
stellar object barâxt-e setâre-yi Fr.: objet stellaire Any of a class of → astronomical objects which is thought to evolve into a → star or is a descendant of a star. |
stellar parallax didgašt-e setâré Fr.: parallaxe stellaire The apparent → difference in the → position
of a → celestial object as seen by an → observer
from two widely separated → locations.
The parallax of an object can be used to derive its → distance.
The relationship between the → parallax angle
p (measured in seconds of arc) and the distance d (measured in
→ astronomical units)
is given by d = 206,264 / p.
For a parallax angle p = 1'', the distance to the
star would correspond to 206,264 AU. By convention, the distance unit
→ parsec is defined to be equivalent to 206,264
AU. Therefore, the parallax relation takes the much
simpler form: d (in pc) = 1/p (in seconds of arc).
The first star whose parallax was measured was → 61 Cygni
(Bessel, 1838). |
stellar photometry nursanji-ye setâre-yi Fr.: photométrie stellaire The precise measurement of a star's brightness, usually through several specific wavelength bands. → stellar; → photometry. |
stellar physics fizik-e setâre-yi (#) Fr.: physique stellaire Same as → stellar astrophysics. |
stellar population porineš-e setâre-yi Fr.: population stellaire → Population I star; → Population II star. → stellar; → population. |
stellar population synthesis handâyeš-e porinešhâ-ye setâre-yi Fr.: synthèse de poupulations stellaires A theoretical model that reconstructs the integrated spectrum of → stellar populations from an empirical library of stellar spectra containing the range of types expected to be present in the sample. The light received from a given galaxy is emitted by a large number of stars that may have different masses, ages, and metallicities. Stellar population synthesis models are tools for interpreting the integrated light that we observe from the galaxies. → stellar; → population; → model. |
stellar pulsation tapeš-e setâré, ~ setâre-yi Fr.: pulsation stellaire The expansion of a star followed by contraction so that its → surface temperature and → luminosity undergo periodic variation. Pulsation starts with a loss of → hydrostatic equilibrium, when, for example, a layer contracts. This layer heats up and becomes more opaque to radiation. Therefore, radiative diffusion slows down through the layer because of its increased → opacity and heat increases beneath it. Hence pressure rises below the layer. Eventually this increase in pressure starts to push the layer out. The layer expands, cools and becomes more transparent to radiation. Energy now escapes from below the layer and the pressure beneath the layer drops. The layer falls inward and the cycle starts over. See also → kappa mechanism; → gamma mechanism; → partial ionization zone; → pulsating star; → valve mechanism. |
stellar rotation carxeš-e setâré, é setêre-yi Fr.: rotation stellaire The spinning of a star about its axis, due to its angular momentum. Stars do not necessarily rotate as solid bodies, and their angular momentum may be distributed non-uniformly, depending on radius or latitude.Thus the equator of the star can rotate at a different angular velocity than the higher latitudes. These differences in the rate of rotation within a star may have a significant role in the generation of a stellar magnetic field. |
stellar structure sâxtâr-e setâré, ~ setêre-yi Fr.: structure stellaire A physical model that describes the internal arrangement of a star in detail and makes detailed predictions about the luminosity, the color, and the future evolution of the star. |
stellar structure equation hamugeš-e sâxtâr-e setâré Fr.: équation de structure stellaire A set of → differential equations describing the physical properties of stars based on two main assumptions: a star is a perfect sphere and the net force on a macroscopic mass element is zero. If the effects of rotation and magnetism are ignored, these assumptions lead to a set of five differential equations. |
stellar system râžmân-e setâre-yi Fr.: système stellaire A system comprised of a group of stars bound by → gravitational attraction. Same as → star system. |
stellar wind bâd-e setâre-yi Fr.: vent stellaire The steady flow of gas away from a star resulting in → mass loss. They range from gentle solar wind (2 x 10-14 solar masses per year) to violent winds some 10 billions times stronger (10-4 solar masses per year) for hot, massive stars. |
stellar-mass black hole siyah câl bâ jerm-e setâre-y Fr.: trou noir de masse stellaire Same as → stellar black hole. |