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31.
Solar flare observations have been performed with the multichannel L.P.S.P. experiment on board OSO-8 NASA Satellite. Simultaneous H and K Caii, h and k Mgii, L and L Hi profiles have been recorded on the plage just before the flare, during the flare onset and relaxation phases. The different behaviour of line profiles and intensities during the flare is evidenced and indicates a downward propagation with relaxation times increasing from the upper part to the lower part of the chromosphere related to line formation processes. Using the H observed profile, an upper limit of 8 × 1013 cm-3 is derived for the electron density.  相似文献   
32.
A study of the variation of the spectral relative ratios of reflectivity of selected mare lunar grounds between wavelengths 4000 and 8000 Å is given in comparison with lunar craters. The intensities at different wavelengths of each lunar region are corrected for the angles of illumination and viewing, and they are scaled to unity at =5538Å. Distinct variety in the spectral reflectivity values of mare grounds at short wavelengths are confirmed. The Mare Tranquillitatis type grounds (similar to Apollo-11 site), have relative ratio of reflectivity at short wavelength at =4035 Å; larger than or equal to 1.03 in addition to a bigger difference in reflectivity between the short and the long wavelength. The Mare Serenitatis type grounds (similar to Apollo-12) are characterized to give relative ratio of reflectivity less than 1.03 at =4035 Å, and smaller difference in reflectivity between short and long wavelengths. This is due to the variation in the colour of the Mare Tranquillitatis and Mare Serenitatis type ground due to compositional differences. The mare type grounds are generally different in shape than that of lunar craters grounds.Presented at the IAU-COSPAR Julian Schmidt Symposium on 100 Years of Lunar Mapping held at Lagonissi, Greece, 25–27 May, 1978.  相似文献   
33.
An earlier paper gave solutions for the mean time rates of change of orbital elements of satellite atoms in an exosphere influenced by solar radiation pressure. Each element was assumet to beahve independently. Here the instantaneous rates of change for three elements (e, ω, and θ = ω + Ω) are integrated simultaneously for the case of the inclination i = 0. The results (a) confirm the validity of using mean rates when the orbits are tightly bound to the planet and (b) serve as examples to be reproduced by the complicated numerical solutions required for arbitrary inclination. Strongly bound hydrogen atoms perturbed in Earth orbit by radiation pressure do not seem a likely cause of the geotail extending in the anti-Sun direction. Instead, radiation pressure wil cause those particles' orbits to form a broad fan-shaped tail and to deteriorate into the Earth's atmosphere. Whether loosely bound H atoms are plentiful enough to create the geotail depends on their source function versusr; that question is beyond the scope of this paper.  相似文献   
34.
O vi ( = 1032 Å) profiles have been measured in and above a filament at the limb, previously analyzed in H i, Mg ii, Ca ii resonance lines (Vial et al., 1979). They are compared to profiles measured at the quiet Sun center and at the quiet Sun limb.Absolute intensities are found to be about 1.55 times larger than above the quiet limb at the same height (3); at the top of the prominence (15 above the limb) one finds a maximum blue shift and a minimum line width. The inferred non-thermal velocity (29 km s–1) is about the same as in cooler lines while the approaching line-of-sight velocity (8 km s–1) is lower than in Ca ii lines.The O vi profile recorded 30 above the limb outside the filament is wider (FWHM = 0.33 Å). It can be interpreted as a coronal emission of O vi ions with a temperature of about 106 K, and a non-thermal velocity (NTV) of 49 km s–1. This NTV is twice the NTV of quiet Sun center O vi profiles. Lower NTV require higher temperatures and densities (as suggested by K-coronameter measurements). Computed emission measures for this high temperature regime agree with determinations from disk intensities of euv lines.  相似文献   
35.
In isothermal models of the expanding solar corona there exists in general an exobase level where the collision mean free path becomes equal to the density scale height. At this level the hydrodynamic approximations of the transport equations fail to be justified and a kinetic approach is more appropriate. This exobase is located below the altitude of the critical point proper to the hydrodynamic solutions. The bulk velocity at the exobase is subsonic and smaller than the expansion velocity at the critical point. Therefore the transition to a supersonic solar wind velocity occurs in the collisionless ion-exosphere.  相似文献   
36.
Mariner 9 ultraviolet spectra of the 1971 dust clouds were analyzed to obtain the phase function times single scattering albedo of the dust particles. The phase functions were matched with Mie scattering calculations for size distributions of spheres of homogeneous and isotropic material. The absorption index of the dust particles was found to increase with decreasing wavelenght from 350 nm down to about 210 nm, and drop off shortward of this wavelength. A structural shoulder occurs in the absorption spectrum between 240 and 250 nm. Titanium dioxide (anatase) has the correct transitions at 210 and 250 nm to match the absorption curve of Martian dust, and is proposed as a candidate constituent in Martian surface material. The spectral neutrality of TiO2 between 0.5 and 4 μm is consistent with visible and infrared observations of Mars. The high refractive index of TiO2 can explain the large refringence of Martian dust. The titanium dioxide content of the dust particles is estimated to be a few percent or less. Uncertainties in the results due to limitations in the model and data are discussed.  相似文献   
37.
Many applied dispersion models require the knowledge of boundary-layer parameters such as sensible heat flux,Q H , friction velocity,u *, and turbulent energy components, w and v . Formulas are suggested for calculating these parameters over a wide variety of types of ground surfaces, based on simple observations of wind speed near the ground and fractional cloud cover, and specification of constants such as roughness length, albedo, and soil moisture availability. Observations ofu *,Q H , w , and v during field experiments in St. Louis and Indianapolis are used to test the formulas for urban sites. Relative errors of about ±20% in the predictions are seen to occur whenu *,Q H , w , and v are large. However, when these quantities are small (e.g.,u * < 0.2 m/s), the errors in the predictions are as large as the mean value of the quantity itself.In addition, it is concluded from studies of available field data and theories that the magnitude of w is not well-known at elevations above about 100m during the late afternoon and night. Some simple parameterizations for w . are suggested that are consistent with the observed steady decrease in ground-level concentration in the afternoon and the sudden increase in concentration that can occur a few hours after sunset due to wind shears associated with a low-level jet, for continuous plumes emitted from moderate to tall stacks.  相似文献   
38.
In the Central Southern Alps (Feltre, Verona — Italy), a 750 m thick interval of Jurassic and Cretaceous pelagic limestones shows post-depositional partial brecciation and dolomitization. The overlying 500 m thick Tertiary sedimentary sequence is unaffected. Through the Paleogene, mostly submarine, mafic volcanism has been documented in the area. Small-scale extensional features were observed in the limestone near the contact with the dolomitized breccias. Their orientations measured in the field correspond to the tectonic framework of the area and give evidence for the contemporaneousness of the volcanic activity and the brecciation. The distribution and petrologic characteristics of the basalts, combined with the orientation of the extensional features observed in the field, allow a paleotectonic reconstruction. This tectonic scenario can be viewed as a back-arc extension, an eastward prolongation of the spreading that divided Southern France from the Sardinia-Corsica-Calabria block, generating the Ligurian-balearic basin in the Late Oligocene.The dolomite is fine-grained to sucrosic, with a microamygdaloidal porosity, partially filled with ankerite and calcite. The matrix shows a homogeneous, orange-red cathodoluminescence, indicating a single phase of iron-poor dolomite. The carbonate fraction consists of more than 90% dolomite. The dolomite is almost stoichiometric (Ca0.6Mg0.4 to Ca0.5Mg0.5). The 13C values of the dolomite are less than 1%. more negative than the unaffected limestone. The 18O values are between –5%. to –13%., with a depletion of 2–11%. relative to the undolomitized limestone. The depleted oxygen isotope ratios in the dolomitized rock can be derived either from fluids impoverished in the heavy isotopes (e.g. meteoric water) or high temperatures. The unvaried carbon isotopic ratios make the second interpretation the most acceptable. As the87Sr/86Sr values increase from a mean of 0.7077 in the unaffected limestones to 0.7085 in the dolomitized limestones, a derivation of the dolomitizing fluids from the volcanic rocks can be excluded. Comparing the obtained data with the Phanerozoic seawater isotope curve, however, the radiogenic Sr may be derived from marine waters of Late Oligocene-Early Miocene age. Microthermometric analyses of the fluid inclusions in the dolomite crystals from the bulk rocks and from the veins suggest a trapping temperature ranging from a minimum of 70°C (dolomite rock) to a maximum of 120°C (dolomite in veins). The solution contained in the inclusions is water with NaCl and MgCl2 with salinities of 46%. (dolomite bulk rock) and 17%. (dolomite in veins). The pressure correction calculated from the fluid inclusion data is about 250 bars, which roughly correspond to the lithostatic pressure over the Mesozoic limestones in the Early Miocene.These results point to a hydrothermal origin of the dolomitization during the Late Oligocene-Early Miocene, as ascertained from the strontium isotope and fluid inclusion data. The circulation of hot marine water through the brecciated limestones in convective cells, triggered by the geothermal gradient related to the volcanic activity, is the proposed hydrodynamic model. Hydrologie considerations demonstrate that the proposed model is feasible.
Zusammenfassung In den zentralen Südalpen (Feltre, Verona — Italien) findet sich eine etwa 750 m dicke Abfolge jurassischer und kretazischer pelagischer Kalke, die nach der Ablagerung zum Teil breckziert und dolomitisiert wurde, während die darüberliegenden 500 m mächtigen tertiären Sedimente keine Dolomitisierung zeigen. Im Paläogen ist im Gebiet ein mafischer, überwiegend mariner Vulkanismus dokumentiert. Kleinmaßstäbliche listrische Brüche in Kalken am Kontakt mit der dolomitisierten Breckzie entsprechen geometrisch einem großräumigen extensiven Regime im Paläogen. Sie beweisen die Gleichzeitigkeit der vulkanischen Aktivität und der Breckzierung. Die Verteilung und petrographischen Eigenschaften der Basalte, mit der Geometrie der Extensionsstrukturen, erlauben eine paläotektonische Rekonstruktion. Diese tektonische Situation entspricht einem Back-arc-basin und stellt die östliche Verlängerung des ligurisch-balearischen Beckens dar, das Südfrankreich vom Sardisch-Korsisch-Kalabrischen-Block im späten Oligozän getrennt hat.Die 13C Werte der Dolomite sind weniger als 1%. negativer als die entsprechender nicht dolomitisierter Kalke. Die 18O-Werte (relativ zum PDB Standard) variieren zwischen –5%. und –13%., das ist 2 bis 11%. negativer als die nicht dolomitisierter Kalke. Dies wird auf erhöhte Bildungstemperaturen zurückgeführt. Ein Anstieg der87Sr/86Sr-Signaturen im Mittel von 0.7077 in den nicht dolomitisierten Kalken auf 0.7085 in den dolomitisierten Kalken schließt eine Herkunft der dolomitisierenden Fluide von den vulkanischen Gesteinen aus. Beim Vergleich der Isotopensignaturen mit der phanerozoischen Meerwasser-Isotopenkurve, könnte aber das radiogene Strontium von spät oligozänem — früh miozänem Meerwasser kommen. Mikrothermometrische Analysen flüssiger Einschlüsse in Dolomitkristallen im Gestein und in Adern deutet auf eine Einschlußtemperatur von 70°C (Dolomitgestein) bzw. 120°C (Dolomit in Adern) hin. Die Lösung in den Einschlüssen ist Wasser mit NaCl und MgCl2, mit einer Salinität von 46%. (Dolomitgestein) bzw. 17%. (Adern). Die aus den Einschlüssen berechnete Druckkorrektur ist etwa 250 bar. Dies entspricht ungefähr der früh miozänen Gesteinssäule über den mesozoischen Kalken.Aufgrund dieser Daten wird eine hydrothermale Bildung der Dolomite im späten Oligozän - frühen Miozän postuliert. Es wird ein hydrodynamisches Modell vorgeschlagen, in dem aufgeheiztes Meerwasser konvektiv durch die breckzierte mesozoische Abfolge zirkuliert. Als Motor wirkt ein vulkanischer geothermischer Gradient. Dieses Modell läßt sich mit hydrologischen Betrachtungen testen und stützen.

Résumé Dans la partie sud des Alpes Centrales (Feltre, Verone: Italie) il existe une succession, épaisse de 750 m, de calcaires pélagiques jurassiques et crétacés, qui ont subi après leur sédimentation une bréchification et une dolomitisation partielles. Les sédiments tertiaires surincombants, épais de 500 m, ne sont pas affectés par ces phénomènes. Un volcanisme paléogène mafique, essentiellement sousmarin, a été reconnu dans la région. Dans les calcaires, au contact de la brèche dolomitisée, existent des cassures listriques de petite échelle dont la géométrie témoigne d'un régime extensif général au Paléogène. Leurs orientations, mesurées sur le terrain, indiquent la contemporanéité de l'activité volcanique et de la bréchification. La distribution et les caractères pétrologiques des basaltes, combinés à la géometrie des structures extensives, permet une reconstitution paléotectonique. Celle-ci montre une extension dans un bassin d'arrière-arc, prolongement oriental de l'expansion qui, à l'Oligocène supérieur, a séparé du sud de la France le bloc corsico-sardo-calabrais en créant le bassin liguro-baléare.La dolomie, finement grenue à saccharoïde, possède une porosité à vides micro-amygdaloïdes, partiellement occupés par de l'ankérite et de la calcite. La matrice présente une cathodoluminescence homogène rouge-orange, indiquant la présence d'une seule phase constituée de dolomite pauvre en Fe. La fraction carbonatée consiste en dolomite pour plus de 90%. Cette dolomite est à peu près stoechiométrique (Ca0,6Mg0,4 à Ca0,5Mg0,5). Les rapports 13C de la dolomie sont inférieurs de moins de 1%. à ceux du calcaire intact. Les rapports 18O sont compris entre –5%. et –13%., soit 2 à 11%. inférieurs à ceux du calcaire non dolomitisé. Cette baisse du rapport isotopique peut provenir soit de fluides appauvris en isotopes lourds (p. ex. l'eau météorique), soit d'une température élevée; la constance des rapports isotopiques du C rend cette deuxième explication la plus plausible. Le rapport87Sr/86Sr passe d'une valeur moyenne de 0,7077 dans les calcaires non affectés à 0,7085 dans les calcaires dolomitisés; cet accroissement exclut une origine volcanique pour les fluides dolomitisants. En comparant ces valeurs à la courbe isotopique du Sr de l'eau de mer au Phanérozoïque, on peut déduire que le Sr radiogénique est dérivé d'eaux marines d'âge oligocène tardif à miocène inférieur. L'analyse microthermométrique des inclusions fluides contenues dans les cristaux de dolomite suggère une température de formation qui va de 70°C (dans la roche) à 120° (dans les veines). Le contenu de ces inclusions est une solution aqueuse de NaCl et MgCl2 avec une salinité de 44%. (dans la roche) et de 17%. (dans les veines). La correction de pression calculée à partir des inclusions fluides est d'environ 250 bars, ce qui correspond grosso modo à la pression lithostatique qui s'exerçait au Miocène inférieur sur les calcaires mésozoïques.Sur la base de ces données, on conclut à une origine hydrothermale de la dolomie au cours de l'Oligocène supérieur - Miocène inférieur. Le modèle hydrodynamique proposé fait appel à la circulation convective, à travers le calcaire bréchié, d'eau marine échauffée grâce au gradient géothermique élevé dû à l'activité volcanique. Ce modèle est en accord avec des considérations hydrologiques.

(, — ) , 750 , , , , 500 , . , . , . , . . - , - . 13 , 1%. 18, PDB –5 –13%, .. 2 11% . , , . 87Sr/86Sr 0.7077 0,7085 . , - . 70° , 120° . , , 44%, 17%. , , 250 . - . , - . , . , . .
  相似文献   
39.
Observations with the French (L.P.S.P.) experiment on board OSO-8 of a sunspot and nearby plage region are described. The behaviour of the emission cores of the Ca II H and K and Mg II h and k resonance lines is very similar and the correspondence in intensity between the four lines persists in all observed features. In contrast, the Lyman lines show little correlation with the other lines. Their emission regions appear broader in the spectroheliograms than the underlying sunspot structure and must not necessarily possess a counterpart in lower layers. From the central intensity of L above the umbra an electron density of 4.3 × 1010 cm-3 n e * 2.3 × 1011 cm-3 at 20 000 K is estimated.Mitteilungen aus dem Kiepenheuer-Institut Nr. 186.Stockholm Observatorium, S-13300 Saltsjöbaden, Sweden.Laboratoire de Physique Stellaire et Planétaire, CNRS, P.O. Box 10, F-91370 Verrières-le-Buisson, France.  相似文献   
40.
Ion microprobe U–Pb dating of zircons from Neoproterozoic volcano-sedimentary sequences in Cameroon north of the Congo craton is presented. For the Poli basin, the depositional age is constrained between 700–665 Ma; detrital sources comprise ca. 920, 830, 780 and 736 Ma magmatic zircons. In the Lom basin, the depositional age is constrained between 613 and 600 Ma, and detrital sources include Archaean to Palaeoproterozoic, late Mesoproterozoic to early Neoproterozoic (1100–950 Ma), and Neoproterozoic (735, 644 and 613 Ma) zircons. The Yaoundé Group is probably younger than 625 Ma, and detrital sources include Palaeoproterozoic and Neoproterozoic zircons. The depositional age of the Mahan metavolcano-sedimentary sequence is post-820 Ma, and detrital sources include late Mesoproterozoic (1070 Ma) and early Neoproterozoic volcanic rocks (824 Ma). The following conclusions can be made from these data. (1) The three basins evolved during the Pan-African event but are significantly different in age and tectonic setting; the Poli is a pre- to syn-collisional basin developed upon, or in the vicinity of young magmatic arcs; the Lom basin is post-collisional and intracontinental and developed on old crust; the tectono-metamorphic evolution of the Yaoundé Group resulted from rapid tectonic burial and subsequent collision between the Congo craton and the Adamawa–Yade block. (2) Late Mesoproterozoic to early Neoproterozoic inheritance reflects the presence of magmatic event(s) of this age in west–central Africa.  相似文献   
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