<< < -me mac mag mag mag mag mag maj man Mar mas mas mat Max mea mec Meg Mer Mer met met met mic mic mil min min mis mne mod mol Mon moo mot mul mul mut > >>
magnetic pressure fešâr-e meqnâtisi (#) Fr.: pression magnétique The pressure exerted by a magnetic field on the material that contains the field. |
magnetic quantum number adad-e kuântomi-ye meqnâtisi (#) Fr.: nombre quantique magnétique In atomic physics, a quantum number that denotes the energy levels available within a subshell. Designated by the letter m, it is one of a set of quantum numbers which describe the unique quantum state of an electron. |
magnetic reconnection bâzhâband-e meqnâtisi Fr.: reconnexion magnétique In a → plasma, a change of → magnetic connectivity of plasma elements due to the presence of a localized → diffusion region. It allows charged particles to move from one → magnetic field line to another. Magnetic reconnection is an important process transforming magnetic energy into heat or/and kinetic energy. Magnetic reconnection events occur in the Earth's → magnetosphere. The process plays an important role in explosive phenomena in the Sun, such as → coronal mass ejections and → solar flares which heat the → solar corona. → magnetic; → re-; → connection. |
magnetic relaxation vâheleš meqnâtisi Fr.: relaxation magnétique The process by which a magnetic system relaxes to its minimum energy state over time. → magnetic; → relaxation. |
magnetic resonance bâzâvâyi-ye meqnâtisi (#) Fr.: résonance magnétique A phenomenon exhibited by certain atoms whereby they absorb energy at specific (resonant) frequencies when subjected to alternating magnetic fields. |
magnetic reversal vâruneš-e meqnâtisi Fr.: inversion magnétique A change in the Earth's → magnetic field in which the → magnetic north pole is transformed into a → magnetic south pole and the magnetic south pole becomes a magnetic north pole. There are geological proofs indicating that the Earth's magnetic field has undergone numerous reversals of → polarity in the past. In the last 10 million years, there have been, on average, 4 or 5 reversals per million years. At other times, for example during the → Cretaceous era, there have been much longer periods when no reversals occurred. Over the past two centuries, Earth's magnetic field has weakened by 15%. Risks of a weak magnetic field include more deaths from cancer due to increased radiation, electrical grid collapse from severe solar storms, climate change, and temporary ozone holes. See also → geomagnetic excursion. |
magnetic Reynolds number adad-e Reynolds-e meqnâtisi Fr.: nombre de Reynolds magnétique A → dimensionless quantity used in → magnetohydrodynamics to describe the relative balance of → magnetic advection to → magnetic diffusion. It is given by: Rm = σμ0νLU0, where σ is the → conductivity of the fluid, μ0 is the → magnetic permeability of the fluid, L is he characteristic length scale of the fluid flow, and U0 the characteristic velocity of the flow. A typical value for the Earth is Rm ~ 200. → magnetic; → Reynolds number. |
magnetic rigidity saxtpâyi-ye meqnâtisi Fr.: rigidité magnétique In → plasma physics, a → quantity that describes the → resistance of a → charged particle to change its direction of motion under the influence of a perpendicular → magnetic field. Rigidity is defined as: R = rLBc = (pc)/(Ze), where rL is the → Larmor radius, B is → magnetic induction, c is the → speed of light, p is the → momentum of the particle, Z is → atomic number, and e the → electron charge. Since pc has the dimensions of energy and e the dimensions of charge, rigidity has the dimensions of → volts (a 10 GeV proton has a rigidity of 10 GV). In → cosmic ray studies, the energies of cosmic rays are often quoted in terms of their rigidities, rather than their energies per nucleon. |
magnetic south pole qotab-e daštar-e meqnâtisi Fr.: pôle sud magnétique The → counterpart of the → magnetic north pole. It lies near the → geographic north pole. |
magnetic splitting fâqeš-e meqnâtisi Fr.: dédoublement magnétique A process whereby the (internal) → magnetic field of a star modifies the → pulsations by lifting some of its degeneracy. Instead of just one pulsation frequency, a multiplet of frequencies is then observed. This effect was proposed as a possible explanation for the observed frequency pattern of → Beta Cephei. In practice, the magnetic splitting is difficult to observe, because of the very small expected frequency difference between the peaks. However, when unaccounted for, it may lead to a wrong mode identification. The current best candidate to detect magnetic splitting is → HD 43317, since this star displays two close frequency patterns (Buysschaert et al., 2017, astro-ph/1709.02619). |
magnetic star setâre-ye meqnâtisi (#) Fr.: étoile magnétique A star whose → spectral lines show the → Zeeman effect. See also: → stellar magnetic field, → magnetic massive star, → Ap/Bp star. |
magnetic storm tufân-e meqnâtisi (#) Fr.: orage magnétique A temporary, worldwide disturbance of the Earth's magnetic field by streams of charged particles from the Sun. Magnetic storms are frequently characterized by a sudden onset, in which the magnetic field undergoes marked changes in the course of an hour or less, followed by a very gradual return to normalcy, which may take several days. |
magnetic susceptibility barxodgiri-ye meqnêtisi Fr.: susceptibilité magnétique A property of material defined by the ratio of the → magnetization to the → magnetic intensity. In other words, the magnetization per unit magnetic intensity. → magnetic; → susceptibility. |
magnetic tape navâr-e meqnâtisi Fr.: bande magnétique A continuous, flexible ribbon impregnated or coated with magnetic-sensitive material on which information (sound, images, data, etc.) may be recorded. |
magnetic tension taneš-e meqnâtisi Fr.: tension magnétique In → magnetohydrodynamic (MHD) treatment of → plasmas, that component of the → Lorentz force which is directed toward the centre of curvature of the → magnetic field lines and thus acts to straighten out the field lines. The Lorentz force can be decomposed into two components orthogonal to the magnetic field: j× B = (B . ∇) B / μ0 - ∇ (B2 / 2μ0), where j is the → current density, μ0 is the → magnetic permeability of free space, and B is the → magnetic flux density. The left side term is the Lorentz force, the first term on the right side is the magnetic tension and the second term the → magnetic pressure. |
magnetic vector potential tavand-e bordâri-ye meqnâtisi Fr.: vecteur potentiel magnétique A vector field A defined so that the → magnetic field B is given by its → curl: B = ∇ x A. |
magnetic-dipole radiation tâbeš-e doqotbe-ye meqnâtisi (#) Fr.: rayonnement du dipôle magnétique Radiation emitted by a rotating magnet. |
magnetics meqnâtik Fr.: magnétisme The study of magnetic phenomena, comprising magnetostatics and electromagnetism. |
magnetism meqnâtmandi Fr.: magnétisme The science of magnetic phenomena, including the fields and forces produced by magnets and, more generally, by moving electric charges. |
Magnetism in Massive Stars (MiMeS) MiMeS Fr.: MiMeS An international collaboration devoted to the study of the origin and physics of → magnetic fields in → massive stars. The project uses several observatories and a large number of telescopes equipped with → spectropolarimetric and → asteroseismologic instruments, including → HARPS, → HARPSpol, and → ESPaDOnS (Wade et al., 2016, MNRAS 456, 2). |
<< < -me mac mag mag mag mag mag maj man Mar mas mas mat Max mea mec Meg Mer Mer met met met mic mic mil min min mis mne mod mol Mon moo mot mul mul mut > >>