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Lyot division šekâf-e Liyot (#) Fr.: division de Lyot In Saturn's rings, the gap between rings B and C. Named after Bernard Lyot (1897-1952), French astronomer who discovered the division. He was also a distinguished solar observer and invented (1930) the → coronagraph; → division. |
Mach cone maxrut-e Mach Fr.: cône de Mach The cone that confines the pressure disturbance created by a → supersonic object moving in a → compressible medium. → Mach number; → cone. |
macronova dorošt-novâ, dorošt-now-axtar Fr.: macronova A stellar → explosion with energies between those of a → nova and a → supernova and observationally distinguished by being brighter than a typical nova (MV ~ -8 mag) but fainter than a typical supernova (MV ~ -19 mag) (Kulkarni 2005; arXiv:astro-ph/0510256). |
magnetic advection pahnbaz-e meqnâtisi Fr.: advection magnétique The transport of the magnetic field by a fluid. It is given by the term ∇ x (v x B) in the → induction equation. |
magnetic connectivity hâbandandegi-ye meqnâtisi Fr.: connectivité magnétique Of magnetic field lines, the condition for them to be connected or the process whereby they become connected or connective. → magnetic;→ connectivity. |
magnetic constant pâyâ-ye meqnâtisi (#) Fr.: constante magnétique A physical constant relating mechanical and electromagnetic units of measurement. It has the value of 4π × 10-7 henry per meter. Also called the permeability of free space, or → absolute permeability. |
magnetic convection hambaz-e meqnâtisi Fr.: convection magnétique Thermal → convection modified by the presence of magnetic fields. → magnetic; → convection. |
magnetic declination vâkileš-e meqnâtisi Fr.: déclinaison magnétique In terrestrial magnetism, the difference between → true north (the axis around which the earth rotates) and magnetic north (the direction the needle of a compass will point,→ magnetic pole). → magnetic; → declination. |
magnetic diffusion paxš-e meqnâtisi Fr.: diffusion magnétique The process whereby the magnetic field tends to diffuse across the plasma and to smooth out any local inhomogeneities under the influence of a finite resistance in the plasma. For a stationary plasma the → induction equation becomes a pure → diffusion equation: ∂B/∂t = Dm∇2B, where Dm = (μ0σ0)-1 is the → magnetic diffusivity. |
magnetic inclination darkil-e meqnâtisi Fr.: inclinaison magnétique Same as → magnetic dip or → dip. → magnetic; → inclination. |
magnetic induction darhâzeš-e meqnâtisi Fr.: induction magnétique 1) Same as → magnetic flux density. |
magnetic monopole takqotbe-ye meqnâtisi (#) Fr.: monopôle magnétique A hypothetical particle that carries a single → magnetic pole, in contrast to magnets which are north-south pole pairs. These massive particles (billions of times heavier than the → proton) are required by grand unified theories(→ GUTs) to explain the actual matter content of the Universe, particularly the dominance of matter upon → antimatter. However, their existence contradicts → Gauss's law for magnetism. |
magnetic monopole problem parâse-ye takqotbe-ye meqnâtisi Fr.: problème du monopôle magnétique A problem concerning the compatibility of grand unified theories (→ GUTs) with standard cosmology. If standard cosmology was combined with grand unified theories, far too many → magnetic monopoles would have been produced in the early Universe. The → inflation hypothesis aims at explaining the observed scarcity of monopoles. The inflation has deceased their density by a huge factor. |
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 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-dipole radiation tâbeš-e doqotbe-ye meqnâtisi (#) Fr.: rayonnement du dipôle magnétique Radiation emitted by a rotating magnet. |
magnetization meqnâteš Fr.: magnétisation 1) General: The process of magnetizing or the state of being magnetized. Verbal noun of → magnetize. |
magnetocentrifugal acceleration šetâb-e meqnât-markazgoriz Fr.: accelération magnetocentrifuge The acceleration exerted on the plasma particles according to the → magnetocentrifugal model. |
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