<< < aco ang app are bar bir bre can clo com Com cor Cos cre dat deg dif dir dis eff exc ext fir for fre Fre gen Gre Gre her Hub imp inf ins int Jup Leg Lor Mag mat mix neu Nyq ore Par pic pre pre pre pre pro ram rea rea rec rec red red ref ref reg rel rel rel ren res res res res ret rev Rus sec sig spe squ ste str sur the tid tre ups wav > >>
Legendre transformation tarâdiseš-e Legendre Fr.: transformation de Legendre A mathematical operation that transforms one function into another. Two differentiable functions f and g are said to be Legendre transforms of each other if their first derivatives are inverse functions of each other: df(x)/dx = (dg(x)/dx)-1. The functions f and g are said to be related by a Legendre transformation. |
Lemaître Universe giti-ye Lemaître (#) Fr.: Univers de Lemaître A cosmological hypothesis, based on Einstein's relativity, in which the expanding Universe began from an exploding "primeval atom." In the Lemaître Universe the rate of expansion steadily decreases. Named after Monsignor Georges Edouard Lemaître (1894-1966), a Belgian Roman Catholic priest, honorary prelate, professor of physics and astronomer; → universe. |
light trespass tarâraft-e nuri Fr.: lumière intrusive A type of → light pollution which is light falling where it is not wanted or needed. Light trespass occurs when poorly shielded or poorly aimed fixtures cast light into unwanted areas, such as buildings, neighboring property, and homes. This light is a main contributor to → skyglow which interferes with astronomical instruments. |
Lindblad resonance bâzâvâyi-ye Lindblad Fr.: résonance de Lindblad A kinematic resonance hypothesized to explain the existence of galactic → spiral arms. It occurs when the frequency at which a star encounters the spiral → density wave is a multiple of its → epicyclic frequency. Orbital resonances occur at the location in the disk where Ωp = Ω ± κ/m, where Ωp is → pattern speed, κ → epicyclic frequency, and m an integer representing the number of spiral arms. The minus sign corresponds to the inner Lindblad resonance (ILR) and the plus sign to the outer Lindblad resonance (OLR). The corotation resonance corresponds to Ωp = Ω. In general, the Lindblad resonances are defined for two spiral arms (m = 2), and low order. There are other less important resonances corresponding to higher m values. These resonances tend to increase the object's orbital eccentricity and to cause its longitude of periapse to line up in phase with the perturbing force. Lindblad resonances drive spiral density waves both in galaxies (where stars are subject to forcing by the spiral arms themselves) and in Saturn's rings (where ring particles are subject to forcing by Saturn's moons). After the originator of the model, Bertil Lindblad (1895-1965), a Swedish astronomer, who made important contributions to the study of the rotation of the Galaxy; → resonance. |
line strength zur-e xatt Fr.: intensité de raie Same as → line intensity. |
linear correlation hambâzâneš-e xatti Fr.: corrélation linéaire A measure of how well data points fit a straight line. When all the points fall on the line it is called a perfect correlation. When the points are scattered all over the graph there is no correlation. → linear; → correlation. |
linear differential equation hamugeš-e degarsâne-yi-ye xatti Fr.: équation différentielle linéaire An equation in which the → dependent variable y
and all its differential coefficients occur only
in the first degree. A linear differential equation of → order
order n has the form: → linear; → differential; → equation. |
linear regression vâyâzi-ye xatti Fr.: regression linéaire In statistics, a regression method that establishes a linear relationship between two random variables. → linear; → regression. |
linearized differential equation hamugeš-e degarsâneyi-ye xatti Fr.: équation différentielle linéarisée A differential equation that has been derived from an original nonlinear equation. Linearized, p.p. of → linearize; → differential; → equation. |
Liouville's theorem farbin-e Liouville Fr.: théorème de Liouville A key theorem in statistical mechanics of classical systems which states that the motion of phase-space points defined by Hamilton's equations conserves phase-space volume. After Joseph Liouville (1809-1882), a French mathematician; → theorem. |
Lissajous figure xam-e Lissajous (#) Fr.: courbe de Lissajous, figure de ~ A curve traced out by a point which is oscillating simultaneously in two mutually perpendicular directions. In general, the amplitude and frequency may be different in the two directions, and the two oscillations may have an arbitrary initial phase difference. The simplest pattern is a straight line, being obtained from two oscillations of equal frequency in phase with each other. The patterns can become very involved if the ratio of the frequencies is not a simple one. After the French physicist Jules Antoine Lissajous (1822-1880), who first demonstrated such curves (Comptes-Rendus, 1857, 44, 727); → figure. Xam, → curve. |
literature neveštârgân (#) Fr.: littérature 1) Writings in which expression and form, in connection with ideas of
permanent and universal interest, are characteristic or essential
features, as poetry, novels, history, biography, and essays. From L. literatura/litteratura "writing, grammar, learning," from litera/littera "letter." Neveštârgân, from neveštâr, literally "written; writing," verbal noun from neveštan, nevis- "to write;" Mid.Pers. nibištan, nibes- "to write;" Av./O.Pers. nī- "down; in, into," → ni- (PIE), + paēs- "to paint; to adorn," paēsa- "adornment" (Mid.Pers. pēsīdan "to adorn"); O.Pers. pais- "to adorn, cut, engrave" (Mod.Pers. pisé "variegated"); cf. Skt. piśáti "adorns; cuts;" Gk. poikilos "multicolored;" L. pingit "embroiders, paints;" O.C.S. pisati "to write;" O.H.G. fēh "multicolored;" Lith. piēšti "to draw, adorn;" PIE base *peik- "colored, speckled," + -gân suffix of suffix forming plural entities, from Mid.Pers. -gânag. |
lithosphere sangsepehr (#), litosepehr Fr.: lithosphère The solid portion of the → Earth, as compared to the → atmosphere and the → hydrosphere. The lithosphere consists of semi-rigid plates that move relative to each other on the underlying → asthenosphere. The process is known as → plate tectonics and helps explain → continental drift. |
local Lorentz invariance nâvartâyi-ye Lorentz-e mahali Fr.: invariance de Lorentz locale → Einstein equivalence principle. → local; → Lorentz; → invariance. |
local sidereal time zamân-e axtari-ye mahali Fr.: temps sidéral local Local time measured by the apparent motion of the stars. It is the most useful form of sidereal time since it gives the right ascension of a transiting celestial object at a given location. |
local standard of rest estânde-ye mahali-ye âram Fr.: standard local de repos A frame of reference that turns around the Galactic center at a velocity and a distance which are the mean values for the stars in the solar neighborhood. In this reference system the stars belonging to the solar neighborhood are statistically at rest. The orbital velocity of the Local Standard of Rest around the Galaxy is about 220 km/sec. |
Lorentz Lorentz Fr.: Lorentz Contraction of the full name of Hendrik Antoon Lorentz (1853-1928), a Dutch physicist, who made important contribution to physics. He won (with Pieter Zeeman) the Nobel Prize for Physics in 1902 for his theory of electromagnetic radiation, which, confirmed by findings of Zeeman, gave rise to Albert Einstein's special theory of relativity. |
Lorentz contraction terengeš-e Lorentz Fr.: contraction de Lorentz The decrease in the length of a body moving in the direction of its length as measured by an observer situated in that direction. The shortening factor is [1 - (v/c)2]1/2, where v is the relative velocity and c light speed. → Lorentz; → contraction. |
Lorentz factor karvand-e Lorentz Fr.: facteur de Lorentz In → special relativity, an important parameter which appears in several equations, including → time dilation, → length contraction, and → relativistic mass. It is defined as γ = 1 / [1 - (v/c)2]1/2 = dt/dτ, where v is the velocity as observed in the reference frame where time t is measured, τ is the proper time, and c the → velocity of light. Same as Lorentz γ factor. |
Lorentz force niru-ye Lorentz (#) Fr.: force de Lorentz The force acting upon a → charged particle as it moves in a → magnetic field. It is expressed by F = q.v x B, where q is the → electric charge, v is its → velocity, and B the → magnetic induction of the field. This force is perpendicular both to the velocity of the charge and to the magnetic field. The magnitude of the force is F = qvB sinθ, where θ is the angle between the velocity and the magnetic field. This implies that the magnetic force on a stationary charge or a charge moving parallel to the magnetic field is zero. The direction of the force is given by the → right-hand rule. |
<< < aco ang app are bar bir bre can clo com Com cor Cos cre dat deg dif dir dis eff exc ext fir for fre Fre gen Gre Gre her Hub imp inf ins int Jup Leg Lor Mag mat mix neu Nyq ore Par pic pre pre pre pre pro ram rea rea rec rec red red ref ref reg rel rel rel ren res res res res ret rev Rus sec sig spe squ ste str sur the tid tre ups wav > >>