4,666 research outputs found
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On the magnetospheric ULF wave counterpart of substorm onset
One nearâubiquitous signature of substorms observed on the ground is the azimuthal structuring of the onset auroral arc in the minutes prior to onset. Termed auroral beads, these optical signatures correspond to concurrent exponential increases in ground ultralow frequency (ULF) wave power and are likely the result of a plasma instability in the magnetosphere. Here, we present a case study showing the development of auroral beads from a Time History of Events and Macroscale Interactions during Substorms (THEMIS) allâsky camera with near simultaneous exponential increases in auroral brightness, ionospheric and conjugate magnetotail ULF wave power, evidencing their intrinsic link. We further present a survey of magnetic field fluctuations in the magnetotail around substorm onset. We find remarkably similar superposed epoch analyses of ULF power around substorm onset from space and conjugate ionospheric observations. Examining periods of exponential wave growth, we find the groundâ and spaceâbased observations to be consistent, with average growth rates of âŒ0.01 sâ1, lasting for âŒ4 min. Crossâcorrelation suggests that the spaceâbased observations lead those on the ground by approximately 1â1.5 min. Meanwhile, spacecraft located premidnight and âŒ10 RE downtail are more likely to observe enhanced wave power. These combined observations lead us to conclude that there is a magnetospheric counterpart of auroral beads and exponentially increasing ground ULF wave power. This is likely the result of the linear phase of a magnetospheric instability, active in the magnetotail for several minutes prior to auroral breakup
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DK-1D: a drift-kinetic simulation tool for modelling the shear Alfvén wave and its interaction with collisionless plasma
We present a highly accurate tool for the simulation of shear Alfven waves (SAW) in collisionless plasma. SAW are important in space plasma environments because for small perpendicular scale lengths they can support an electric field parallel to the ambient magnetic field. Electrons can be accelerated by the parallel electric field and these waves have been implicated as the source of vibrant auroral displays. However, the parallel electric field carried
by SAW is small in comparison to the perpendicular electric field of the wave, making it difficult to measure directly in the laboratory, or by satellites in the near-Earth plasma environment. In this paper, we present a simulation code that provides a means to study in detail the SAW-particle interaction in both space and laboratory
plasma. Using idealised, small-amplitude propagating waves with a single perpendicular wavenumber, the simulation code accurately reproduces the damping rates and parallel electric field amplitudes predicted by linear theory for varying temperatures and perpendicular scale lengths. We present a rigorous kinetic derivation of the parallel electric field strength for small-amplitude SAW and show that commonly-used inertial and kinetic approximations are valid except for where the ratio of thermal to Alfv\'{e}n speed is between 0.7 and 1.0. We also present nonlinear simulations of large-amplitude waves and show that in cases of strong damping, the damping rates and parallel electric field strength deviate from linear predictions when wave energies are greater than only a few percent of the plasma
kinetic energy, a situation which is often observed in the
magnetosphere. The drift-kinetic code provides reliable, testable predictions of the parallel electric field strength which can be investigated directly in the laboratory, and will help to bridge the gap between studies of SAW in man-made and naturally occuring plasma
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Comment on 'Role of dispersive AlfvĂ©n waves in generating parallel electric fields along the IoâJupiter fluxtube' by S. T. Jones and Y.âJ. Su
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Self-consistent wave-particle interactions in dispersive scale long-period field-line-resonances
Using 1D Vlasov drift-kinetic computer simulations, it
is shown that electron trapping in long period standing shear Alfven waves (SAWs) provides an efficient energy sink for wave energy that is much more effective than Landau
damping. It is also suggested that the plasma environment
of low altitude auroral-zone geomagnetic field lines is more
suited to electron acceleration by inertial or kinetic scale
Alfven waves. This is due to the self-consistent response of
the electron distribution function to SAWs, which must
accommodate the low altitude large-scale current system in
standing waves. We characterize these effects in terms of the relative magnitude of the wave phase and electron thermal velocities. While particle trapping is shown to be significant across a wide range of plasma temperatures and wave frequencies, we find that electron beam formation in long period waves is more effective in relatively cold plasma
Comportamento produtivo de feijão caupi no Amapå - ensaio avançado 3/1983.
O feijĂŁo caupi e um dos mais importantes componentes dos sistemas de produção de culturas alimentares, em uso no AmapĂĄ. Entretanto, sua produtividade media e muito baixa sendo que, em alguns municĂpios, nĂŁo chega a atingir a 500kg/ha. Esse fato motiva a pesquisa na busca de genotipos adaptaveis a esses sistemas e aos diversos ambientes ecolĂłgicos, atravĂ©s da seleção segundo dados de produtividade, ciclo e porte da planta, resistĂȘncia a doenças e pragas, alĂ©m da avaliação do potencial de aceitação do produto no mercado consumidor.bitstream/item/65011/1/AP-1984-comportamento-produtivo-feijao-amapa.pd
Comportamento produtivo de feijão caupi no Amapå - Ensaio avançado 1/1983.
Os sistemas de produção com culturas alimentares de ciclo curto em uso no AmapĂĄ, tem no feijĂŁo caupi um dos seus componentes mais importantes, muito embora a produtividade media alcançada seja quase sempre muito baixa, sendo em algumas zonas produtoras, inferior a 500kg/ha. Dessa forma, as açÔes de pesquisa voltadas para esta cultura entĂŁo, em grande parte, dando enfase a seleção de genotipos adaptaveis a esses sistemas, levando-se em consideração a produtividade e a resistĂȘncia a pragas e doenças.bitstream/item/65010/1/AP-1984-comportamento-produtivo-feijao-caupi-amapa.pd
Confinement of knotted polymers in a slit
We investigate the effect of knot type on the properties of a ring polymer
confined to a slit. For relatively wide slits, the more complex the knot, the
more the force exerted by the polymer on the walls is decreased compared to an
unknotted polymer of the same length. For more narrow slits the opposite is
true. The crossover between these two regimes is, to first order, at smaller
slit width for more complex knots. However, knot topology can affect these
trends in subtle ways. Besides the force exerted by the polymers, we also study
other quantities such as the monomer-density distribution across the slit and
the anisotropic radius of gyration.Comment: 9 pages, 6 figures, submitted for publicatio
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Statistical azimuthal structuring of the substorm onset arc: implications for the onset mechanism
The onset of an auroral substorm is generally thought to occur on a quiet, homogeneous auroral arc. We present a statistical study of independently-selected substorm onset arcs and find that over 90% of the arcs studied have resolvable characteristic spatial scales in the form of auroral beads. We find that the vast majority (~88%) of auroral beads have small amplitudes relative to the background, making them invisible without quantitative analysis. This confirms that auroral beads are highly likely to be ubiquitous to all onset arcs, rather than a special case phenomena as previously thought. Moreover, as these auroral beads grow exponentially through onset, we conclude that a magnetospheric plasma instability is fundamental to substorm onset itself
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What effect do substorms have on the content of the radiation belts?
Substorms are fundamental and dynamic processes in the magnetosphere, converting captured solar wind magnetic energy into plasma energy. These substorms have been suggested to be a key driver of energetic electron enhancements in the outer radiation belts. Substorms inject a keV âseedâ population into the inner magnetosphere which is subsequently energized through wave-particle interactions up to relativistic energies; however, the extent to which substorms enhance the radiation belts, either directly or indirectly, has never before been quantified. In this study, we examine increases and decreases in the total radiation belt electron content (TRBEC) following substorms and geomagnetically quiet intervals. Our results show that the radiation belts are inherently lossy, shown by a negative median change in TRBEC at all intervals following substorms and quiet intervals. However, there are up to 3 times as many increases in TRBEC following substorm intervals. There is a lag of 1â3âdays between the substorm or quiet intervals and their greatest effect on radiation belt content, shown in the difference between the occurrence of increases and losses in TRBEC following substorms and quiet intervals, the mean change in TRBEC following substorms or quiet intervals, and the cross correlation between SuperMAG AL (SML) and TRBEC. However, there is a statistically significant effect on the occurrence of increases and decreases in TRBEC up to a lag of 6âdays. Increases in radiation belt content show a significant correlation with SML and SYM-H, but decreases in the radiation belt show no apparent link with magnetospheric activity levels
The Globular Cluster Systems in the Coma Ellipticals. II: Metallicity Distribution and Radial Structure in NGC 4874, and Implications for Galaxy Formation
Deep HST/WFPC2 (V,I) photometry is used to investigate the globular cluster
system (GCS) in NGC 4874, the central cD galaxy of the Coma cluster. The
luminosity function of the clusters displays its normal Gaussian-like shape and
turnover level. Other features of the system are surprising: the GCS is (a)
spatially extended, with core radius r_c = 22 kpc, (b) entirely metal-poor (a
narrow, unimodal metallicity distribution with mean [Fe/H] = -1.5), and (c)
modestly populated, with specific frequency S_N = 3.7 +- 0.5. We suggest on the
basis of some simple models that as much as half of this galaxy might have
accreted from low-mass satellites, but no single one of the three classic modes
of galaxy formation (accretion, disk mergers, in situ formation) can supply a
fully satisfactory formation picture. Even when they are used in combination,
strong challenges to these models remain. The principal anomaly in this GCS is
essentially the complete lack of metal-rich clusters. If these were present in
normal (M87-like) numbers in addition to the metal-poor ones that are already
there, then the GCS in total would more closely resemble what we see in many
other giant E galaxies.Comment: 27 pp. with 9 Figures. Astrophys.J. 533, in press (April 10, 2000
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