pressure mode tarz-e fešÃ¢r, mod-e ~ Fr.: mode pression Same as → p mode |
pressure scale height bolandi-ye marpel-e fešâr Fr.: hauteur d'échelle de pression A basic ingredient of the → mixing length theory that scales with the → mixing length. It is defined by the relation: HP = -dr/dln P = -Pdr/dP , where r is the height and P the pressure. See also → scale height. |
radiation pressure fešâr-e tâbeš Fr.: pression de radiation The → momentum carried by → photons to a surface exposed to → electromagnetic radiation. Stellar radiation pressure on big and massive objects is insignificant, but it has considerable effects on → gas and → dust particles. Radiation pressure is particularly important for → massive stars. See, for example, → Eddington limit, → radiation-driven wind , and → radiation-driven implosion. The → solar radiation pressure is also at the origin of various physical phenomena, e.g. → gas tails in → comets and → Poynting-Robertson effect. |
ram pressure fešâr-e qucvâr Fr.: pression dynamique The pressure exerted on a body moving through a → fluid medium. For example, a → meteor traveling through the Earth's atmosphere produces a → shock wave generated by the extremely rapid → compression of air in front of the → meteoroid. It is primarily this ram pressure (rather than → friction) that heats the air which in turn heats the meteoroid as it flows around the meteoroid. The ram pressure increases with → velocity according to the relation P = (1/2)ρv2, where ρ is the density of the medium and v the relative velocity between the body and the medium. Similarly, → ram pressure stripping produces → jellyfish galaxies. Same as → dynamic pressure. |
ram pressure stripping loxtâneš bâ fešâr-e qucvâr Fr.: balayage par la pression dynamique A process proposed to explain the observed absence of gas-rich galaxies in → galaxy clusters whereby a galaxy loses its gas when it falls into a cluster. There is a tremendous amount of hot (~ 107 K) and tenuous (~ 10-4 cm-3) gas (several 1013 → solar masses) in the → intracluster medium (ICM). Ram pressure stripping was first proposed by Gunn & Gott (1972) who noted that galaxies falling into clusters feel an ICM wind. If this wind can overcome the → gravitational attraction between the stellar and gas disks, then the gas disk will be blown away. The mapping of the gas content of spiral galaxies in the → Virgo cluster showed that the → neutral hydrogen (H I) disks of cluster spiral galaxies are disturbed and considerably reduced. Their molecular gas, more bound to the galaxy, is less perturbed, but still may be swept out in case of very strong ram pressure. These observational results indicate that the gas removal due to the rapid motion of the galaxy within the intracluster medium is responsible for the H I deficiency and the disturbed gas disks of the cluster spirals (e.g., J. A. Hester, 2006, ApJ 647:910). |
solar depression nešib-e xoršid Fr.: dépression solaire The → angle between the → sea horizon, the → center of → Earth, and the center of the → solar disk. → solar; → depression. |
solar radiation pressure fešâr-e tâbeš xoršid (#) Fr.: pression du rayonnement solaire The → radiation pressure of solar photons, which pushes a comet's dust outward to form a → dust tail. |
sound pressure fešâr-e sedâ Fr.: pression de son The periodic fluctuation above and below atmospheric pressure created by an oscillating body which provides the → sound power. Instantaneous sound pressure is the peak value of air pressure. |
stagnation pressure fešâr-e nâravâni Fr.: pression de stagnation The sum of → static pressure and → dynamic pressure in the → Bernoulli equation. → stagnation; → pressure. |
standard temperature and pressure (STP) damâ o fešâr-e estândé Fr.: conditions normales de température et de pression 1) The most commonly used definition is temperature of 273.15 K (0 °C) and
pressure of 1 → atmosphere. → standard; → temperature; → pressure. |
static pressure fešâr-e istâ Fr.: pression statique In → fluid mechanics, the → pressure felt by an object suspended in a → fluid and moving with it. This pressure is called static because the object is not moving relative to the fluid. See also → dynamic pressure. |
suppress nehâvidan Fr.: supprimer 1) To put down by authority or force. L. suppressus, p.p. of supprimere "to press down, stop, stifle," from → sub- "down, under" + premere "to press, push against," → express. Nehâvidan, from ne-, → ni- "down, below," + hâvidan "to press," → express. |
suppression nehâveš Fr.: suppression The act of suppressing; the state of being suppressed. → Compton suppression, → zero suppression. |
thermal pressure fešâr-e garmâyi (#) Fr.: pression thermale The ordinary pressure in a gas that is due to motions of particles and can be attributed to the object's → temperature. |
total pressure fešâr-e hamâk Fr.: pression totale The sum of → static pressure, → dynamic pressure, and → hydrostatic pressure in the → Bernoulli equation. |
vapor pressure fešâr-e boxâr Fr.: pression de vapeur The equilibrium pressure of a vapor above its condensed phases (liquid or solid). In other words, the pressure of the vapor resulting from evaporation of a liquid (or solid) above a sample of the liquid (or solid) in a closed container. The vapor pressure varies with the temperature. As the temperature increases its the vapor pressure also increases, and conversely. The temperature at which the vapor pressure is equal to the atmospheric pressure is called the → boiling point. For example, at 20 °C, water would boil at a pressure of about 0.023 atm, or about a fortieth of atmospheric pressure. |
velocity pressure fešâr-e tavânik Fr.: pression dynamique |
Wilson depression našib-e Wilson Fr.: dépression de Wilson The depression on the → Sun's → photosphere associated with → sunspots and involving the → Wilson effect. The measured depression values vary between about 700 and 2,000 km. → Wilson effect; → depression. |
zero suppression nehâveš-e sefr Fr.: suppression de zéro The removal of non-significant zeroes from a number. For example, replacing 531.2300 by 531.23. → zero; → suppression. |