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Abstract— Clasts of alkaline (the second find in meteorites) and subalkaline rocks were found in the Kaidun meteorite. One of them (#d4A) is a large crystal of albite with inclusions of fluorapatite, arfvedsonite, aenigmatite, and wilkinsonite. The two latter minerals were previously unknown in meteorites. Another clast (#d[3–5]D) has a melt crystallization texture of mainly feldspar (oligoclase) composition and contains relict grains of both high‐Ca and low‐Ca pyroxene and fluorapatite. The mineralogical characteristics of these clasts suggest a genetic relationship and an origin from the same parent body. The textural and mineralogical characteristics of the clasts indicate origin by extensive igneous differentiation. Such processes most likely took place in a rather large differentiated body. The material of clast #d(3–5)D is similar in some mineralogical respects to basaltic shergottites.  相似文献   
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We present the results of extensive thermal-infrared observations of the C-type near-Earth Asteroid (1580) Betulia obtained in June 2002 with the 3-m NASA Infrared Telescope Facility (IRTF) on Mauna Kea, Hawaii. Betulia is a highly unusual object for which earlier radiometric observations, interpreted on the basis of simple thermal models, indicated a surface of high thermal inertia. A high thermal inertia implies a lack of thermally insulating regolith. Radiometric observations of other asteroids of comparable size indicate that regolith is present in nearly all cases. Knowledge of the surface thermal properties of small near-Earth asteroids is crucial for meaningful calculations of the Yarkovsky effect, which is invoked to explain the delivery of collisional fragments from the main belt into near-Earth orbits, and apparently has a significant influence on the orbital evolution of potentially hazardous near-Earth asteroids. Furthermore, apart from being an indicator of the presence of thermally insulating regolith on the surface of an asteroid, the thermal inertia determines the magnitude of the diurnal temperature variation and is therefore of great importance in the design of instrumentation for lander missions to small asteroids. In the case of Betulia our database is sufficiently broad to allow the use of more sophisticated thermal models than were available for earlier radiometric observations. The measured fluxes have been fitted with thermal-model emission continua to determine the asteroid's size and geometric albedo, pv. Fits obtained with a new thermophysical model imply an effective diameter of 4.57±0.46 km and an albedo of 0.077±0.015 and indicate a moderate surface thermal inertia of around 180 J m−2 s−0.5 K−1. It is difficult to reconcile our results with earlier work, which indicate a larger diameter for Betulia and a high-thermal-inertia surface of bare rock.  相似文献   
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We carry out numerical simulations of dissipationless major mergers of elliptical galaxies using initial galaxy models that consist of a dark matter haloes and a stellar bulge with properties consistent with the observed fundamental plane. By varying the density profile of the dark matter haloes [standard Navarro, Frenk & White (NFW) profile versus adiabatically contracted NFW profile], the global stellar to dark matter mass ratio and the orbit of the merging galaxies, we are able to assess the impact of each of these factors on the structure of the merger remnant. Our results indicate that the properties of the remnant bulge depend primarily on the angular momentum and energy of the orbit; for a cosmologically motivated orbit, the effective radius and velocity dispersion of the remnant bulge remain approximately on the fundamental plane. This indicates that the observed properties of elliptical galaxies are consistent with significant growth via late dissipationless mergers. We also find that the dark matter fraction within the effective radius of our remnants increases after the merger, consistent with the hypothesis that the tilt of the fundamental plane from the virial theorem is due to a varying dark matter fraction as a function of galaxy mass.  相似文献   
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A simulation of the atmospheric state under ice age conditions (18,000 years before present) is presented. The T21 Atmospheric General Circulation Model (AGCM), originally developed at the European Centre for Medium-Range Weather Forecasts, was used for the calculation of six annual cycles. Results of the near-surface climatology (2 m-temperature, 10 m-wind, and precipitation), averaged over the last five model years, are presented. The presentation is restricted to January and July means in order to demonstrate the glacial changes in summer and winter. The model's response to ice age boundary conditions was quite consistent with paleogeological data on land and with AGCM experiments of other studies. Although the differences between the mean climate states of the model atmosphere under glacial and modern boundary conditions were statistically significant, the basic structure of the simulated atmospheric circulation was not altered substantially.
Zusammenfassung Eine Simulation des Zustands der eiszeitlichen Atmosphäre (18000 Jahre vor heute) wird vorgestellt. Das T21-Modell (allgemeines Zirkulationsmodell der Atmosphäre), entwickelt am Europäischen Zentrum für Mittelfrist-Wettervorhersage, wurde zur Berechnung von sechs Jahresgängen verwendet. Die Ergebnisse der oberflächennahen Klimatologie (2 m-Temperatur, 10 m-Wind und Niederschlag) werden präsentiert als Mittel über die letzten fünf Modelljahre. Die Darstellung ist eingeschränkt auf Januar- und Julimittel, um die eiszeitlichen Änderungen im Sommer und Winter deutlich zu machen. Die Antwort des Modells auf die eiszeitlichen Randbedingungen stimmt recht gut überein mit paläogeologischen Landdaten und mit anderen Simulationsrechnungen. Obgleich die Klimaunterschiede in der eiszeitlichen und der heutigen Modellatmosphäre statistisch signifikant sind, wurde die Grundstruktur der atmosphärischen Zirkulation vom T21-Modell nur wenig verändert.

Résumé Cette note présente une simulation de l'état de l'atmosphère dans les conditions de l'âge glaciaire, il y a 18.000 ans. Le calcul de 6 cycles annuels a été effectué au moyen du modèle T 21 de la circulation atmosphérique générale développé au Centre Européen de prévision du temps à moyen terme. Les éléments du climat proche de la surface (température à 2 m, vent à 10 m, précipitations) sont présentés en moyenne des cinq dernières années du modèle. Ces éléments sont limités aux moyennes de janvier et de juillet, de manière à mettre en évidence les changements hiver/été. La réponse du modèle aux conditions aux limites de l'âge glaciaire est en bon accord avec les données paléontologiques de terrain ainsi qu'avec d'autres calculs de simulation. Bien qu'il existe d'importantes différences climatiques entre les modèles d'atmosphère de l'âge glaciaire et d'aujourd'hui, la structure de base de la circulation atmosphérique du modèle T 21 est peu modifiée.

, 18000 . 21 = , = , 6 . , — 2 10 , 5 . , , , . . , 21 .
  相似文献   
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For the conservative, two degree-of-freedom system with autonomous potential functionV(x,y) in rotating coordinates; $$\dot u - 2n\upsilon = V_x , \dot \upsilon + 2nu = V_y $$ , vorticity (v x -u y ) is constant along the orbit when the relative velocity field is divergence-free such that: $$u(x,y,t) = \psi _y , \upsilon (x,y,t) = - \psi _x $$ . Unlike isoenergetic reduction using the Jacobi, integral and eliminating the time,non-singular reduction from fourth to second-order occurs when (u,v) are determined explicitly as functions of their arguments by solving for ψ (x, y, t). The orbit function ψ satisfies a second-order, non-linear partial differential equation of the Monge Ampere type: $$2(\psi _{xx} \psi _{yy} - \psi _{xy}^2 ) - 2(\psi _{xx} + \psi _{yy} ) + V_{xx} + V_{yy} = 0$$ . Isovortical orbits in the rotating frame arenot level curves of ψ because it contains time explicitly due to coriolis effects. Rather, (x, y) coordinates along the orbit are obtained, from (u, v) either by numerical integration of the kinematic equations, or by partial differentiation of the Legendre transform ? of ψ. In the latter case, ? is shown to satisfy a non-linear, second-order partial differential equation in three independent variables, derived from the Monge-Ampere Equation. Complete reduction to quadrature is possible when space-time symmetries exist, as in the case of central force motion.  相似文献   
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A nonpolytropic model of a polar coronal hole at 2 R R 5 R is constructed. Our main assumptions are: (1) the magnetic structure of the Sun can be described by a combination of dipole-like and radial fields; (2) in the magnetically dominated region [(v 2/2) < (B 2/8)] the influence of the outflow on the magnetic structure is negligible. The magnetic and thermodynamic structures are obtained by solving the force balance equation for plasma with the observationally derived electron density. Profiles of velocities in the acceleration regime are presented and the influence of the outflow on the thermodynamic structure of the solar corona above the polar region is discussed.This paper is the first part of a joint project of the Space Environment Laboratory, the Joint Institute for Laboratory Astrophysics, and the High Altitude Observatory, NCAR. The second paper by Munro and Tzur is in preparation.Work done while at the Space Environment Laboratory, NOAA, ERL, Boulder, CO 80303, U.S.A.1982–83 Visiting Fellow at the Joint Institute for Laboratory Astrophysics, National Bureau of Standards and University of Colorado.The National Center for Atmospheric Research is sponsored by the National Science Foundation.Visitor at NCAR.  相似文献   
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