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101.
John Inge Svendsen Lars Martin B. Frseth Richard Gyllencreutz Haflidi Haflidason Mona Henriksen Morten N. Hovland
ystein S. Lohne Jan Mangerud Dmitry Nazarov Carl Regnll Joerg M. Schaefer 《Boreas: An International Journal of Quaternary Research》2019,48(2):407-431
Our knowledge about the glaciation history in the Russian Arctic has to a large extent been based on geomorphological mapping supplemented by studies of short stratigraphical sequences found in exposed sections. Here we present new geochronological data from the Polar Ural Mountains along with a high‐resolution sediment record from Bolshoye Shchuchye, the largest and deepest lake in the mountain range. Seismic profiles show that the lake contains a 160‐m‐thick sequence of unconsolidated lacustrine sediments. A well‐dated 24‐m‐long core from the southern end of the lake spans the last 24 cal. ka. From downward extrapolation of sedimentation rates we estimate that sedimentation started about 50–60 ka ago, most likely just after a large glacier had eroded older sediments from the basin. Terrestrial cosmogenic nuclide (TCN) exposure dating (10Be) of boulders and Optically Stimulated Luminescence (OSL) dating of sediments indicate that this part of the Ural Mountains was last covered by a coherent ice‐field complex during Marine Isotope Stage (MIS) 4. A regrowth of the glaciers took place during a late stage of MIS 3, but the central valleys remained ice free until the present. The presence of small‐ and medium‐sized glaciers during MIS 2 is reflected by a sequence of glacial varves and a high sedimentation rate in the lake basin and likewise from 10Be dating of glacial boulders. The maximum extent of the mountain glaciers during MIS 2 was attained prior to 24 cal. ka BP. Some small present‐day glaciers, which are now disappearing completely due to climate warming, were only slightly larger during the Last Glacial Maximum (LGM) as compared to AD 1953. A marked decrease in sedimentation rate around 18–17 cal. ka BP indicates that the glaciers then became smaller and probably disappeared altogether around 15–14 cal. ka BP. 相似文献
102.
Joseph veverka Michael Noland Carl Sagan James Pollack Lynn Quam Robert Tucker Botand Eross Thomas Duxbury William Green 《Icarus》1974,23(2):206-289
This paper contains a complete set of the best enhancements of Mariner 9 high resolution television pictures of Phobos and Deimos, consisting of 27 different views of Phobos, and 9 of Deimos. Pertinent data about the pictures are arranged in convenient tabular and graphical form. 相似文献
103.
Zusammenfassung Es wird unterschieden zwischen Einschlüssen, auf dieSorbys Grundannahme zutrifft, daß eine homogene Phase, wie Wasser, Salzlösung oder CO2, eingeschlossen wurde, die Blasen also von dem Gas der eingeschlossenen Flüssigkeit gebildet werden, und solchen Einschlüssen, in denen fremdes Gas mit eingeschlossen wurde.Sorby-Einschlüsse können zur Temperaturbestimmung herangezogen werden, wenn entweder der Druck am Bildungsort bekannt ist oder sein Einfluß vernachlässigt werden kann, weil der Füllungsgrad so hoch ist, daß die Libelle schon bei niederen Temperaturen verschwindet. Ist fremdes Gas in der Flüssigkeit gelöst eingeschlossen worden und erst beim Abkühlen frei geworden, so ist der Schluß von der Füllungstemperatur auf die Bildungstemperatur noch unsicherer als bei Sorby-Einschlüssen, weil über den zu erwartenden großen Einfluß des Druckes noch nichts bekannt ist.Ist fremdes Gas als Gasblase eingeschlossen worden, so kann die Füllungstemperatur sehr weit von der Bildungstemperatur abweichen und beim Erwärmen sogar zuerst größer werden. Solche Nicht-Sorby-Einschlüsse sind zu erkennen durch Messung des Füllungsgrades und Vergleich der zugehörigen Füllungstemperatur mit der von Wasser bzw. CO2 bei gleichem Füllungsgrad.Die Frage, aus was die Einschlüsse bestehen, ist nicht nur für die Temperaturbestimmung von Wert, sondern auch für viele Fragen der Gesteinsbildung und -umbildung. Es wird auf die schon vonBrewster 1826 angegebene Methode der Bestimmung der Brechungszahl mit Hilfe der Totalreflexion hingewiesen.Alle diese Bemerkungen gelten sowohl für primäre wie für sekundäre Einschlüsse.Die Dekrepitationsmethode kann weder primäre und sekundäre Einschlüsse unterscheiden noch die Natur des Einschlusses, noch auch den Füllungsgrad berücksichtigen. 相似文献
104.
105.
Dr. phil. Carl Renz 《International Journal of Earth Sciences》1911,2(8):455-463
Ohne Zusammenfassung 相似文献
106.
107.
A batch sorption technique for the determination of particle–water interactions of hydrophobic organic micropollutants under simulated estuarine conditions is described. Results are presented for the behaviour of 2,2′,5,5′-tetrachlorobiphenyl (2,2′,5,5′-TCB) in river and sea waters, both in the presence and absence of estuarine suspended particles. Adsorption onto particles in sea water was enhanced compared with adsorption in river water owing to salting out of the compound, and possibly of the particulate organic matter, in the presence of high concentrations of dissolved ions. The particle–water distribution coefficient, KD, decreased from about 120×103 to 10×103 ml g−1, and from about 150×103 to 20×103 ml g−1, in river water and sea water, respectively, over a particle concentration range of 10–1000 mg l−1. Incomplete recovery of compound from the reactor walls is partly responsible for a particle concentration effect, while artefacts relating to inadequate sediment and water phase separation were ruled out following further experiments. The particle concentration effect, which is replicated in many field studies of hydrophobic organic micropollutants, including 2,2′,5,5′-TCB, is incorporated into a simple partitioning model and is discussed in the context of the likely estuarine behaviour of such compounds. 相似文献
108.
Carl Keller 《Ground water》2017,55(2):244-254
This study describes a new technique for measuring the head profile in a geologic formation. The technique provides rapid, low cost information on the depth of water‐producing zones and aquitards in heterogeneous aquifers, yielding estimates of hydraulic heads in each zone while identifying any potential for cross contamination between zones. The measurements can be performed in a typical borehole in just a few hours. The procedure uses both the continuous transmissivity profile obtained by the installation (eversion) of a flexible borehole liner into an open borehole and the subsequent removal (inversion) of the same liner from the borehole. The method is possible because of the continuous transmissivity profile (T profile described by Keller et al. 2014) obtained by measuring the rate of liner eversion under a constant driving head. The hydraulic heads of producing zones are measured using the reverse head profile (RHP) method (patent no. 9,008,971) based on a stepwise inversion of the borehole liner. As each interval of the borehole is uncovered by inversion of the liner, the head beneath the liner is allowed to equilibrate to a steady‐state value. The individual hydraulic heads contributing to each measurement are calculated using the measured transmissivity for each zone. Application of the RHP method to a sedimentary bedrock borehole in New Jersey verified that it reproduced the head distribution obtained the same day in the same borehole instrumented with a multilevel sampling system. 相似文献
109.
Image-based methods have compelling, demonstrated potential for characterizing flow fields in rivers, but algorithms like particle image velocimetry (PIV) must be further tested and improved to enable more effective use of these techniques. This paper presents a framework designed for this exact purpose: Simulating Hydraulics and Images for Velocimetry Evaluation and Refinement (SHIVER). The approach involves coupling a hydrodynamic model with a synthetic particle generator to advect particles between frames, as dictated by local velocity vectors and thus construct a plausible image sequence specific to the reach of interest. The resulting time series can then be used as input to a velocimetry algorithm to compare image-derived estimates with known (modelled) velocities to perform an exhaustive, spatially distributed accuracy assessment. As an example application of SHIVER, we examined the effects of interrogation area (IA) size, frame rate, flow velocity, and image sequence duration on the performance of a standard PIV algorithm. This analysis indicated that image-derived velocities were generally in close agreement with those from the flow model (root mean square error <10% and mean bias <3%), except when small IAs were coupled with low frame rates. Velocity estimates were most accurate for the lowest modelled discharge ( at baseflow) and became less reliable as the mean flow velocity increased ( for an intermediate discharge and at bankfull). Accuracy was essentially independent of image sequence duration, implying that long occupations might not be necessary. Errors were concentrated along channel margins, where PIV-based velocities tended to be greater than those from the flow model. Small IAs led to underpredictions of velocity, while larger IAs led to overpredictions. SHIVER is highly modular and could be updated to make use of different hydrodynamic models or image simulators. The framework could also facilitate more thorough sensitivity analyses and comparison of various velocimetry algorithms. 相似文献
110.
Larry Lines Joe Wong Kris Innanen Fereidoon Vasheghani Carl Sondergeld Sven Treitel Tadeusz Ulrych 《Geophysical Prospecting》2014,62(1):190-195
While seismic reflection amplitudes are generally determined by real acoustical impedance contrasts, there has been recent interest in reflections due to contrasts in seismic‐Q. Herein we compare theoretical and modelled seismic reflection amplitudes for two different cases of material contrasts. In case A, we examine reflections from material interfaces that have a large contrast in real‐valued impedance () with virtually no contrast in seismic‐Q. In case B, we examine reflections from material interfaces that have virtually no contrast in but that have very large seismic‐Q contrasts. The complex‐valued reflection coefficient formula predicts non‐zero seismic reflection amplitudes for both cases. We choose physical materials that typify the physics of both case A and case B. Physical modelling experiments show significantly large reflections for both cases – with the reflections in the two cases being phase shifted with respect to each other, as predicted theoretically. While these modelling experiments show the existence of reflections that are predicted by theory, there are still intriguing questions regarding the size of the Q‐contrast reflections, the existence of large Q‐contrast reflections in reservoir rocks and the possible application of Q‐reflection analysis to viscosity estimation in heavy oilfields. 相似文献