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1.
Suspended sediment plays an important role in the distribution and transport of many pollutants (such as radionuclides) in rivers. Pollutants may adsorb on fine suspended particles (e.g. clay) and spread according to the suspended sediment movement. Hence, the simulation of the suspended sediment mechanism is indispensable for realistic transport modelling. This paper presents and tests a simple mathematical model for predicting the suspended sediment transport in river networks. The model is based on the van Rijn suspended load formula and the advection–diffusion equation with a source or sink term that represents the erosion or deposition fluxes. The transport equation is solved numerically with the discontinuous finite element method. The model evaluation was performed in two steps, first by comparing model simulations with the measured suspended sediment concentrations in the Grote Nete–Molse Nete River in Belgium, and second by a model intercomparison with the sediment transport model NST MIKE 11. The simulations reflect the measurements with a Nash‐Sutcliffe model efficiency of 0.6, while the efficiency between the proposed model and the NST MIKE 11 simulations is 0.96. Both evaluations indicate that the proposed sediment transport model, that is sufficiently simple to be practical, is providing realistic results.  相似文献   
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Pollen‐based quantitative estimates of seasonal precipitation from Lake Pergusa and lake‐level data from Lake Preola in Sicily (southern Italy) allow three successive periods to be distinguished within the Holocene: an early Holocene period before ca. 9800 cal a BP with rather dry climate conditions in winter and summer, a mid‐Holocene period between ca. 9800 and 4500 cal a BP with maximum winter and summer wetness, and a late Holocene period after 4500 cal a BP with declining winter and summer wetness. This evolution observed in the south‐central Mediterranean shows strong similarities to that recognized in the eastern Mediterranean. But, it contrasts with that reconstructed in north‐central Italy, where the mid‐Holocene appears to be characterized by a winter (summer) precipitation maximum (minimum), while the late Holocene coincided with a decrease (increase) in winter (summer) precipitation. Maximum precipitation at ca. 10 000–4500 cal a BP may have resulted from (i) increased local convection in response to a Holocene insolation maximum at 10 000 cal a BP and then (ii) the gradual weakening of the Hadley cell activity, which allowed the winter rainy westerlies to reach the Mediterranean area more frequently. After 4500 cal a BP, changes in precipitation seasonality may reflect non‐linear responses to orbitally driven insolation decrease in addition to seasonal and inter‐hemispheric changes of insolation. Copyright © 2011 John Wiley & Sons, Ltd.  相似文献   
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We present results from the generation of 10-year-long continuous time series of the Earth’s polar motion at 15-min temporal resolution using Global Positioning System ground data. From our results, we infer an overall noise level in our high-rate polar motion time series of 60 \(\upmu \hbox {as}\) (RMS). However, a spectral decomposition of our estimates indicates a noise floor of 4 \(\upmu \hbox {as}\) at periods shorter than 2 days, which enables recovery of diurnal and semidiurnal tidally induced polar motion. We deliberately place no constraints on retrograde diurnal polar motion despite its inherent ambiguity with long-period nutation. With this approach, we are able to resolve damped manifestations of the effects of the diurnal ocean tides on retrograde polar motion. As such, our approach is at least capable of discriminating between a historical background nutation model that excludes the effects of the diurnal ocean tides and modern models that include those effects. To assess the quality of our polar motion solution outside of the retrograde diurnal frequency band, we focus on its capability to recover tidally driven and non-tidal variations manifesting at the ultra-rapid (intra-daily) and rapid (characterized by periods ranging from 2 to 20 days) periods. We find that our best estimates of diurnal and semidiurnal tidally induced polar motion result from an approach that adopts, at the observation level, a reasonable background model of these effects. We also demonstrate that our high-rate polar motion estimates yield similar results to daily-resolved polar motion estimates, and therefore do not compromise the ability to resolve polar motion at periods of 2–20 days.  相似文献   
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Individual aerosol particles collected in the Negev desert in Israel during a summer and winter campaign in 1996–1997 were analysed by scanning electron microscopy with energy-dispersive X-ray analysis. Hierarchical cluster analysis was performed to interpret the data on the basis of particle diameter and composition. Eleven particle classes (groups) provided clues on sources and/or particle formation. The summer samples were enriched in sulphates and mineral dusts; the winter samples contained more sea salts, aged sea salts, and industrial particles. The fine size fraction below 1 m diameter was enriched in secondary particles and showed evidence of atmospheric processing. The secondary sulphate particles were mainly attributed to long-range transport. A regional conversion from calcite to calcium sulphate occurred during summer. Industrial particles originating from local pollution appeared during winter.  相似文献   
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Design of a groundwater pumping and treatment system for a wood-treatment facility adjacent to the tidally influenced Fraser River estuary required the development of methodologies to account for cyclic variations in hydraulic gradients. Design of such systems must consider the effects of these cyclic fluctuations on the capture of dissolved-phase contaminants. When the period of the cyclic fluctuation is much less than the travel time of the dissolved contaminant from the source to the discharge point, the hydraulic-gradient variations resulting from these cycles can be ignored. Capture zones are then designed based on the average hydraulic gradient determined using filter techniques on continuous groundwater-level measurements. When the period of cyclic fluctuation in hydraulic gradient is near to or greater than the contaminant travel time, the resulting hydraulic-gradient variations cannot be ignored. In these instances, procedures are developed to account for these fluctuations in the capture-zone design. These include proper characterization of the groundwater regime, assessment of the average travel time and period of the cyclic fluctuations, and numerical techniques which allow accounting for the cyclic fluctuations in the design of the capture zone. Electronic Publication  相似文献   
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On the basis of geomorphological and sedimentological data, we believe that the entire Barents Sea was covered by grounded ice during the last glacial maximum. 14C dates on shells embedded in tills suggest marine conditions in the Barents Sea as late as 22 ka BP; and models of the deglaciation history based on uplift data from the northern Norwegian coast suggest that significant parts of the Barents Sea Ice Sheet calved off as early as 15 ka BP. The growth of the ice sheet is related to glacioeustatic fall and the exposure of shallow banks in the central Barents Sea, where ice caps may develop and expand to finally coalesce with the expanding ice masses from Svalbard and Fennoscandia.The outlined model for growth and decay of the Barents Sea Ice Sheet suggests a system which developed and existed under periods of maximum climatic deterioration, and where its growth and decay were strongly related to the fall and rise of sea level.  相似文献   
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Zusammenfassung Die Änderung der Sterntaglänge schwankt im Rhythmus des Luftdruckgefälles zwischen 45 und 65° Süd sowohl im mittleren Jahresgang als auch im Ablauf der sechzig Monate der Jahre 1957–1961. Dieser überzufällige Gleichgang in Phase und Amplitude läßt sich so erklären, daß die Schwankungen der Tageslänge direkt durch den Schub oder die Bremsung der Lithosphäre, auf welche die Atmosphäre mit ihren Monsunen oder Passaten wirkt, erzeugt werden. Die den schwankenden Tropenwinden parallel gehenden außertropischen Westwinde würden voll die schiebende oder bremsende Wirkung der Tropenwinde kompensieren, wenn sie auch direkt die Lithosphäre erfaßten. Da nun aber im Gebiet der braven Westwinde die Hydrosphäre den gesamten Drehimpuls übernimmt und ihn wohl erst mit großer Verzögerung an die Lithosphäre weiterreicht, tritt die Änderung der Tageslänge auf, die sich im wesentlichen harmonisch aus einer halbjährlichen und einer jährlichen Welle zusammensetzt.
Geophysical effects on the length of the sideral day
Summary The variations in the length of the day are found to be equal in phase to the oscillation of the atmospheric pressure gradient occurring between 45 and 65 degrees south. This rhythm manifests itself in the annual mean as well as in the course of the 60 months of the years 1957 to 1961. The rhythm that seems to be overaccidental may be explained with regard to phase and amplitude in the following way:The variations in the length of the day are produced by the pushing or braking of the lithosphere on which the atmosphere is acting by its monsoons or trade winds. The outertropical westerlies that are blowing parallel to the tropical wind would be able to compensate the pushing and braking effects if they, too, were directly acting on the lithosphere. As, however, in the region of the westerlies the hydrosphere assumes all angular momentum and apparently passes it on to the lithosphere after considerable delay, the variations in the length of the day are caused which essentially consist of the second and first harmonics.

Effets géophysiques sur la longueur du jour sidéral
Résumé Les variations de la longueur du jour sidéral suivent le rythme du gradient de pression atmosphérique rencontré entre le 45e et 65e degré de latitude Sud. Elles se manifestent dans la moyenne annuelle aussi bien que dans la période des soixants mois des années de 1957 à 1961. Cette homogénéité super-aléatoire du rythme qui se montre également dans la phase et dans l'amplitude pourrait être expliquée par le fait que les variations de la longueur du jour sidéral sont directement produites par la poussée et le freinage de la lithosphère sur lequel agit l'atmosphère par ses moussons et ses vents alizés.Les vents extra-tropicaux d'ouest qui soufflent parallèlement aux vents tropicaux seraient à même de compenser les effets de la poussée et du freinage des vents tropicaux pourvu qu'ils agissent de même immédiatement sur la lithosphère. Comme, cependant, dans la région des braves vents d'ouest l'hydrosphère attire tout le moment angulaire et le passe, probablement après un long délai, au lithosphère, il se produit les variations de longueur du jour sidéral, qui se composent essentiellement d'une oscillation harmonique semestrielle et annuelle.


Nach einem Vortrag Über Erddrehung und atmosphärische Globalzirkulation vor dem Geophysikalischen Kolloquium der Universität Hamburg am 8. Juni 1961, erweitert um die neuen Daten der Tageslänge und des Luftdruckgefälles zwischen 45° und 65° S.  相似文献   
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