Jeans Fr.: Jeans Sir James Hopwood Jeans (1877-1946), English mathematical physicist, astrophysicist, and popularizer of science. He made important contributions to theoretical astrophysics, especially to the theory of stellar formation. → Jeans escape, → Jeans instability, → Jeans length, → Jeans mass, → Jeans scale, → Rayleigh-Jeans law, → Rayleigh-Jeans spectrum, → thermal Jeans mass, → turbulent Jeans mass, → Jeans escape. |
Jeans Fr.: Jeans Sir James Hopwood Jeans (1877-1946), English mathematical physicist, astrophysicist, and popularizer of science. He made important contributions to theoretical astrophysics, especially to the theory of stellar formation. → Jeans escape, → Jeans instability, → Jeans length, → Jeans mass, → Jeans scale, → Rayleigh-Jeans law, → Rayleigh-Jeans spectrum, → thermal Jeans mass, → turbulent Jeans mass, → Jeans escape. |
goriz-e Jeans Fr.: échappement de Jeans A → thermal escape process by which the atmosphere of a planet loses gases to outer space. This form of thermal escape occurs because some molecules, especially low mass ones, are within the higher-velocity end of the → Maxwell-Boltzmann distribution. The possibility for the gases to escape occurs when the thermal energy of air molecules becomes greater than the → gravitational potential energy of the planet: (3/2)kT = (1/2)mv2 > GmM/R where v is upward velocity of a molecule of mass m, M is the mass of the planet, and R is the radius of the planet at which thermal escape occurs. The minimum velocity for which this can work is called the → escape velocity is: ve = (2MG/R)1/2. Hydrogen molecules (H2) and helium, or their ions tend to have velocities high enough so that they are not bound by Earth’s gravitational field and are lost to space from the top of the atmosphere. This process is important for the loss of hydrogen, a low-mass species that more easily attains escape speed at a given temperature, because v ~ (2kT/m)1/2. As such, Jeans’ escape was likely influential in the atmospheric evolution of all the early terrestrial planets. Jeans' escape currently accounts for a non-negligible fraction of hydrogen escaping from Earth, Mars, and Titan, but it is negligible for Venus because of a cold upper atmosphere combined with relatively high gravity (see, e.g., Catling, D. C. and Kasting, J. F., 2017, Escape of Atmospheres to Space, pp. 129-167. Cambridge University Press). |
goriz-e Jeans Fr.: échappement de Jeans A → thermal escape process by which the atmosphere of a planet loses gases to outer space. This form of thermal escape occurs because some molecules, especially low mass ones, are within the higher-velocity end of the → Maxwell-Boltzmann distribution. The possibility for the gases to escape occurs when the thermal energy of air molecules becomes greater than the → gravitational potential energy of the planet: (3/2)kT = (1/2)mv2 > GmM/R where v is upward velocity of a molecule of mass m, M is the mass of the planet, and R is the radius of the planet at which thermal escape occurs. The minimum velocity for which this can work is called the → escape velocity is: ve = (2MG/R)1/2. Hydrogen molecules (H2) and helium, or their ions tend to have velocities high enough so that they are not bound by Earth’s gravitational field and are lost to space from the top of the atmosphere. This process is important for the loss of hydrogen, a low-mass species that more easily attains escape speed at a given temperature, because v ~ (2kT/m)1/2. As such, Jeans’ escape was likely influential in the atmospheric evolution of all the early terrestrial planets. Jeans' escape currently accounts for a non-negligible fraction of hydrogen escaping from Earth, Mars, and Titan, but it is negligible for Venus because of a cold upper atmosphere combined with relatively high gravity (see, e.g., Catling, D. C. and Kasting, J. F., 2017, Escape of Atmospheres to Space, pp. 129-167. Cambridge University Press). |
nâpâydâri-ye Jeans Fr.: instabilité de Jeans An instability that occurs in a → self-gravitating
→ interstellar cloud which is in
→ hydrostatic equilibrium.
Density fluctuations caused by a perturbation may condense the material See also: → Jeans; → instability. |
nâpâydâri-ye Jeans Fr.: instabilité de Jeans An instability that occurs in a → self-gravitating
→ interstellar cloud which is in
→ hydrostatic equilibrium.
Density fluctuations caused by a perturbation may condense the material See also: → Jeans; → instability. |
derâzâ-ye Jeans (#) Fr.: longueur de Jeans The critical size of a homogeneous and isothermal interstellar cloud above which the cloud is unstable and must collapse under its own gravity. Below this size the cloud’s internal pressure is sufficient to resist collapse. The Jeans length is defined by: λJ = (π cs2/Gρ)1/2
= 0.2 pc (T/10 K)1/2(nH2/104
cm-3)-1/2,
where cs is the → sound speed, G is the
→ gravitational constant, ρ is the gas density, |
derâzâ-ye Jeans (#) Fr.: longueur de Jeans The critical size of a homogeneous and isothermal interstellar cloud above which the cloud is unstable and must collapse under its own gravity. Below this size the cloud’s internal pressure is sufficient to resist collapse. The Jeans length is defined by: λJ = (π cs2/Gρ)1/2
= 0.2 pc (T/10 K)1/2(nH2/104
cm-3)-1/2,
where cs is the → sound speed, G is the
→ gravitational constant, ρ is the gas density, |
jerm-e Jeans (#) Fr.: masse de Jeans The → minimum mass for an → interstellar cloud below which the → thermal pressure of the gas prevents its → collapse under the force of its own → gravity. It is given by the formula MJ = (π5/2 / 6) G -3/2ρ0-1/2cs3, where G is the → gravitational constant, ρ0 the initial → density, and cs the isothermal → sound speed. It can be approximated to MJ |
jerm-e Jeans (#) Fr.: masse de Jeans The → minimum mass for an → interstellar cloud below which the → thermal pressure of the gas prevents its → collapse under the force of its own → gravity. It is given by the formula MJ = (π5/2 / 6) G -3/2ρ0-1/2cs3, where G is the → gravitational constant, ρ0 the initial → density, and cs the isothermal → sound speed. It can be approximated to MJ |
marpel-e Jeans Fr.: échelle de Jeans Same as → Jeans length. |
marpel-e Jeans Fr.: échelle de Jeans Same as → Jeans length. |
želé (#) Fr.: gelée
Etymology (EN): M.E. gely, from O.Fr. gelee “a jelly,” from L. gelare “to freeze, congeal, stiffen,” from PIE *gel- “cold; to freeze.” Etymology (PE): Želeh, loan from Fr., as above. |
želé (#) Fr.: gelée
Etymology (EN): M.E. gely, from O.Fr. gelee “a jelly,” from L. gelare “to freeze, congeal, stiffen,” from PIE *gel- “cold; to freeze.” Etymology (PE): Želeh, loan from Fr., as above. |
medusâ, arus-e daryâyi Fr.: méduse |
medusâ, arus-e daryâyi Fr.: méduse |
kahkešên-e medusâ Fr.: galaxie méduse A type of galaxy exhibiting “tentacles” (tails) of material that appear to be stripped from the main body of the galaxy, making it resemble a jellyfish. Such type of galaxies occur in → galaxy clusters and are produced by a process called → ram pressure stripping. The mutual → gravitational attraction between galaxies causes them to fall at high speed into the clusters, where they encounter a hot → intracluster medium (ICM) with dense gas. The falling galaxy feels a powerful wind, forcing tails of gas out of the galaxy’s disk and triggering → starbursts within it. Jellyfish galaxies have mainly been observed in nearby clusters (e.g., Virgo, Coma, A1367, A3627, Shapley). A few examples have been identified in clusters at → redshifts z ~ 0.2-0.4, and there is accumulating evidence for a correlation between the efficiency of the stripping phenomenon and the presence of shocks and strong gradients in the X-ray → intergalactic medium (Poggianti et al., 2016, AJ 151, 78). |
kahkešên-e medusâ Fr.: galaxie méduse A type of galaxy exhibiting “tentacles” (tails) of material that appear to be stripped from the main body of the galaxy, making it resemble a jellyfish. Such type of galaxies occur in → galaxy clusters and are produced by a process called → ram pressure stripping. The mutual → gravitational attraction between galaxies causes them to fall at high speed into the clusters, where they encounter a hot → intracluster medium (ICM) with dense gas. The falling galaxy feels a powerful wind, forcing tails of gas out of the galaxy’s disk and triggering → starbursts within it. Jellyfish galaxies have mainly been observed in nearby clusters (e.g., Virgo, Coma, A1367, A3627, Shapley). A few examples have been identified in clusters at → redshifts z ~ 0.2-0.4, and there is accumulating evidence for a correlation between the efficiency of the stripping phenomenon and the presence of shocks and strong gradients in the X-ray → intergalactic medium (Poggianti et al., 2016, AJ 151, 78). |
1, 2, 3) ešân, šân; 4) jet Fr.: jet
Etymology (EN): Jet, from M.Fr. jeter “to throw,” from V.L. *jectare, alter. of L. jactare, from jac- “throw” + -t- frequentative suffix + -are infinitive suffix; PIE base *ye- “to do” (cf. Gk. hienai “to send, throw;” Hittite ijami “I make”). Etymology (PE): Ešân, from ešândan, → eject; šân contraction of ešân. |
1, 2, 3) ešân, šân; 4) jet Fr.: jet
Etymology (EN): Jet, from M.Fr. jeter “to throw,” from V.L. *jectare, alter. of L. jactare, from jac- “throw” + -t- frequentative suffix + -are infinitive suffix; PIE base *ye- “to do” (cf. Gk. hienai “to send, throw;” Hittite ijami “I make”). Etymology (PE): Ešân, from ešândan, → eject; šân contraction of ešân. |
motor-e šâni Fr.: turboréacteur |
motor-e šâni Fr.: turboréacteur |
partâb-e šân Fr.: lancement de jet The mechanism whereby → astrophysical jets are thrown out of → accretion disks . Observed correlations between emission from the accretion disk and from the jet provide evidence that the jets are launched from the disks directly. As the energy emitted from the jets is a → synchrotron radiation, the presence of a → magnetic field is deduced for the ejection. The most promising model for such “accretion-ejection” structures is based on a scenario where a large-scale magnetic field threads an accretion disk. This model, using a → magnetohydrodynamic (MHD) approach, shows that the magnetic field can azimuthally brake the matter inside the disk (carrying off → angular momentum allowing accretion) and accelerate matter above the disk surface. The → collimation of the flow is achieved via → magnetic tension due to the presence of a → toroidal component of the magnetic field. The magnetic field provides an effective alternative to the radially outward transport of disk angular momentum by → viscosity. The interaction of the magnetic structure with the disk plasma can create a MHD → Poynting flux leaving the disk along the magnetic surface. This energy flux can then be converted into → kinetic energy of the matter within the jet. Because the → mass density in the jet is smaller than in the disk, it is thereby possible to reach high → terminal velocities for a given amount of angular momentum removed from the disk (Casse & Keppens, 2002, ApJ 581, 988, and references therein). |
partâb-e šân Fr.: lancement de jet The mechanism whereby → astrophysical jets are thrown out of → accretion disks . Observed correlations between emission from the accretion disk and from the jet provide evidence that the jets are launched from the disks directly. As the energy emitted from the jets is a → synchrotron radiation, the presence of a → magnetic field is deduced for the ejection. The most promising model for such “accretion-ejection” structures is based on a scenario where a large-scale magnetic field threads an accretion disk. This model, using a → magnetohydrodynamic (MHD) approach, shows that the magnetic field can azimuthally brake the matter inside the disk (carrying off → angular momentum allowing accretion) and accelerate matter above the disk surface. The → collimation of the flow is achieved via → magnetic tension due to the presence of a → toroidal component of the magnetic field. The magnetic field provides an effective alternative to the radially outward transport of disk angular momentum by → viscosity. The interaction of the magnetic structure with the disk plasma can create a MHD → Poynting flux leaving the disk along the magnetic surface. This energy flux can then be converted into → kinetic energy of the matter within the jet. Because the → mass density in the jet is smaller than in the disk, it is thereby possible to reach high → terminal velocities for a given amount of angular momentum removed from the disk (Casse & Keppens, 2002, ApJ 581, 988, and references therein). |
jet (#), havâpeymâ-ye ~ (#) Fr.: avion à réaction An airplane moved by → jet propulsion. Etymology (EN): → jet; plane, short for airplane, from Fr. aeroplane, from aero-, → air, + plane feminine of plan “flat, level,” from L. planus, perhaps by association with forme plane; apparently coined and first used by Fr. sculptor and inventor Joseph Pline in 1855. Etymology (PE): → jet;
havâpeymâ “airplane,” from havâ, → air, + peymâ
“travelling; traveller,” from peymudan, peymâyidan “to travel, traverse, pass over,” |
jet (#), havâpeymâ-ye ~ (#) Fr.: avion à réaction An airplane moved by → jet propulsion. Etymology (EN): → jet; plane, short for airplane, from Fr. aeroplane, from aero-, → air, + plane feminine of plan “flat, level,” from L. planus, perhaps by association with forme plane; apparently coined and first used by Fr. sculptor and inventor Joseph Pline in 1855. Etymology (PE): → jet;
havâpeymâ “airplane,” from havâ, → air, + peymâ
“travelling; traveller,” from peymudan, peymâyidan “to travel, traverse, pass over,” |
pišrâneš-e šâni Fr.: propulsion par réaction Powerful, forward thrust that results from the rearward expulsion of a jet of fluid, especially propulsion by jet engines. See also: → jet; → propulsion. |
pišrâneš-e šâni Fr.: propulsion par réaction Powerful, forward thrust that results from the rearward expulsion of a jet of fluid, especially propulsion by jet engines. See also: → jet; → propulsion. |
râbe-ye šâni Fr.: jet stream |
râbe-ye šâni Fr.: jet stream |
gâhšomâr-e yahud (#) Fr.: calendrier juif Same as → Hebrew calendar Etymology (EN): Jewish, adj. of jew, from
M.E. jewe, giu, gyu, ju, from O.Fr. juiu, juieu, gyu, Etymology (PE): Gâhšomâr→ calendar; yahud, from Ar., from Heb., as above. |
gâhšomâr-e yahud (#) Fr.: calendrier juif Same as → Hebrew calendar Etymology (EN): Jewish, adj. of jew, from
M.E. jewe, giu, gyu, ju, from O.Fr. juiu, juieu, gyu, Etymology (PE): Gâhšomâr→ calendar; yahud, from Ar., from Heb., as above. |