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Coccolithophores are an abundant phytoplankton group that exhibit remarkable diversity in their biology, ecology and calcitic exoskeletons (coccospheres). Their extensive fossil record is a testament to their important biogeochemical role and is a valuable archive of biotic responses to environmental change stretching back over 200 million years. However, to realise the full potential of this archive for (palaeo-)biology and biogeochemistry requires an understanding of the physiological processes that underpin coccosphere architecture. Using culturing experiments on four modern coccolithophore species (Calcidiscus leptoporus, Calcidiscus quadriperforatus, Helicosphaera carteri and Coccolithus braarudii) from three long-lived families, we investigate how coccosphere architecture responds to shifts from exponential (rapid cell division) to stationary (slowed cell division) growth phases as cell physiology reacts to nutrient depletion. These experiments reveal statistical differences in coccosphere size and the number of coccoliths per cell between these two growth phases, specifically that cells in exponential-phase growth are typically smaller with fewer coccoliths, whereas cells experiencing growth-limiting nutrient depletion have larger coccosphere sizes and greater numbers of coccoliths per cell. Although the exact numbers are species-specific, these growth-phase shifts in coccosphere geometry demonstrate that the core physiological responses of cells to nutrient depletion result in increased coccosphere sizes and coccoliths per cell across four different coccolithophore families (Calcidiscaceae, Coccolithaceae, Isochrysidaceae and Helicosphaeraceae), a representative diversity of this phytoplankton group. Building on this, the direct comparison of coccosphere geometries in modern and fossil coccolithophores enables a proxy for growth phase to be developed that can be used to investigate growth responses to environmental change throughout their long evolutionary history. Our data also show that changes in growth rate and coccoliths per cell associated with growth-phase shifts can substantially alter cellular calcite production. Coccosphere geometry is therefore a valuable tool for accessing growth information in the fossil record, providing unprecedented insights into the response of species to environmental change and the potential biogeochemical consequences.
In a joint enterprise, the ground water supplies in some Oases in UAR (namely El Kharga, El Dakhla, El Baharia and Siwa), in Wadi El Natrun (to the west of the Nile Delta), in Ayoun Mousa (West Sinai) and in some places along the Mediterranean Littoral, have been investigated. According to the dating of the water by the C14 method, the age of the artesian water from the Oases is between 25,000 and 40,000 years and the origin is obviously from rain water which fell and infiltrated within the "Nubian Sandstone" layers, occupying almost entirely the southern portion of the western Desert (the water underwent some evaporation before it disappeared in the subsurface as indicated from the loss of the 016). This process took place during one or more of the Pluvial periods which followed (and were not coincident with) the last "Würm" eustatic lowering of the Mediterranean. No infiltration water have presumably recharged the layers in question, so almost entirely fossil water reserves are tapped at present. The quantities of such reserves are unknown. More ancient waters, however, may be expected to the north of El Kharga and El Dakhla Oases. Such waters may- to their greater portions - enter these two oases from that direction. On the other hand, little or almost no water is expected to feed the reservoir from the opposite direction.
Mantle convection is the process by which heat from the Earth’s core is transferred upwards to the surface and it is accepted to explain the dynamics of the Earth’s interior. On geological time-scales, mantle material flows like a viscous fluid as a consequence of the buoyancy forces arising from thermal expansion. Indeed, mantel convection provides a framework which links together the major disciplines, such as seismology, mineral physics, geochemistry tectonic and geology. The numerical model has been applied to understand the dynamic, structure and evaluation of the Earth, and other terrestrial planets and the investigations continue to explore, different aspects of the mantle convection.
In fact, to model this phenomenon, two complementary approaches are possible. On the one hand, one can solve self-consistently the equations of thermal convection, including parameters and employing physical relationships derived from mineral physics. Our understanding of mantle convection depends ultimately upon the success of such fully self-consistent dynamic models in explaining observable features of the flow. Although, these models presently unable to predict the actual convection pattern of the Earth, they are extremely useful to investigate general characteristics of given physical systems. On the other hand, to permit comparison with specific observables associated with the flow, one can consider a more restricted problem. Instead of focusing on the time evolution of mantle flow, if we know a priori the temperature - and hence presumably the density - anomalies that drive the convection, we can try to build a snapshot of the present-day flow pattern, consistent with those anomalies, that can successfully predict the observables. As matter of fact, the aim of this study is to investigate both approaches in comparison with the main geophysical constraints on mantle structure. These constraints include the geoid anomalies, the dynamic surface and core-mantle boundary topography and tectonic plate motions.
The most appropriate mathematical basis functions for describing a bounded and continuous function on a spherical surface are spherical harmonics. We may therefore expand the geodynamic observables in terms of spherical harmonics. We have investigated two methods of the global spherical harmonic analysis by specific attention to the dynamic geoid computation of the geodynamic models. The first method is the quadrature method in which the loss of the orthogonality of the Legendre functions in transition from continues to discrete case is the major drawback to the method. Particularly, we showed that in the absence of the tesseral harmonics, quadrature formulation leads to obtain inaccurate results. The second method is the least-squares which can be considered as the best linear unbiased estimator that provides the exact results. We showed that even with a low resolution grid data it is possible to reconstruct the data and achieve an accurate result by using this method, which is extremely remarkable in three-dimensional global convection studies. However, special care has to be taken since there is some source of errors that might influence the efficiency of this method.
In general, to better understanding of the properties of the mantle, it is useful to assess observable characteristics of plumes in the mantle, including geoid, topography and heat flow anomalies. However, only few studies exist on geoid and topography for axi-symmetric convection and their models were restricted to isoviscous (or stratified) mantle and low Rayleigh numbers. We studied fully coupled depth and temperature dependent Arrhenius type of viscosity in axi-symmetric spherical shell geometry in order to investigate the shape of geoid anomalies and dynamic topography above a plume. Indeed, the topography and geoid anomalies produced from plumes are sensitive to rheology of the mantle and rheology of the plume; both have effects on shape and amplitude of the geoid anomalies. As results we are able to define different classes of plumes by their geoid signals.
Mainly depth-dependent viscosity models show a geoid with negative sign above the plume which can turn to the positive sign by decrease the viscosity contrast. This can be considered as a transition between the strongly depth dependent and the constant viscosity case. Our results basically support the idea by Morgan [1965] and McKenzie [1977]. They have shown the magnitude and even the sign of the total gravity anomaly depend on the spatial variation in effective viscosity. In addition, Hager [1984] has concluded that the total gravity field is depend on the radial distribution of effective viscosity, and a small change in viscosity contrast leads to varying sign of the response function.
In the case of temperature-dependent viscosity, the formation of an immobile lithosphere is a natural result, and the flow as well as the total geoid becomes strongly time dependent. When we increase the activation energy, all geoids associated with the first arriving plumes look like bell shaped whereas for typical plumes, after reaching a statistical steady state, bell-shaped geoids with decreasing amplitude as well as linear flank shaped geoids are observed. It is surprising that in spite of large differences in lateral and depth varying viscosities, the shapes of the geoid anomalies remained rather similar. We also identified different behaviors in the combined model with temperature-and pressure-dependent viscosity. In fact, in spite of the strongly different rheology, the geoid anomalies in all cases were surprisingly similar. Furthermore, we proposed a scaling law for the geoid which makes our results directly applicable to other planets. Moreover, we can apply the results of our calculation to find relations between different rheology and sub-lid temperature, since we know that the mantle temperature can change significantly with variation in pressure-temperature dependent viscosity. It is also possible to define a range of stagnant lid thickness related to the amplitude of the geoid which can be reasonable for study of the lid thickness in Venus or Mars.
Nevertheless, in these series of models, we simplified a number of complexities within the Earth. One of the most important of such simplification is the Boussinesq approximation. This approximation is valid if the temperature scale height (i.e. the depth over which temperature increases by a factor of “ ” due to adiabatic compression) is much greater than the convection depth. However, a temperature scale height in the Earth’s mantle is at best only slightly greater than the mantle depth. Hence, the Boussinesq approximation could mask some very important stratification and compressibility effects that influence both the spatial and temporal structure of the convection. Therefore, in more advance models we considered compressibility in our mantle convection models, assuming that density vary both radially and laterally, being determined as a function of pressure and temperature through an appropriate equation of the state. Moreover, thermodynamic properties assumed to be a function of depth.
We examined the details of the structure of the spherical axi-symmetric Anelastic Liquid Approximation model (ALA) with special attention to the Arrhenius rheology, and compare it to the cases of compressible convection without depth dependent thermodynamical properties, and to cases of the extended Boussinesq approximation. At the same time, the effects of the interaction between temperature and pressure-dependent viscosity and thermodynamic parameters in the compressible mantle convection on the geoid and topography have been studied. We showed that assuming compressible convection with depth-dependent thermodynamic properties strongly influence the geoid undulations. Using compressible convection with constant thermodynamic properties is physically inconsistent and may lead to spurious results for the geoid and convection pattern. Indeed, by a systematic study of different approaches of compressibility in the spherical shell convection for different Arrhenius viscosity laws we proved that only in the unrealistic case of zero activation energy the different compressibility modes result in comparable convection and geoid patterns. In all other rheological cases, large differences have been obtained, that stressing the important role of consistent compressible thermodynamic properties for mantle convection.
In addition, we examine the impact of compressibility as well as different rheologies on the power law relation that connects the Nusselt number to the Rayleigh number. We have discovered that the power law index of the relationship is controlled by the rheology, independent of which approximation is used. Instead, the bound of this relation is controlled by a combination of different approximation and rheology.
Next, instead of focusing on the time evolution of mantle flow, we have carried out three-dimensional spherical shell models of mantle circulation to investigate the effects of joint radial and lateral viscosity variations on the Earth’s non-hydrostatic geoid, surface and core-mantle boundary topographies. These models include realistic lateral viscosity variations (LVV) in the lithosphere, upper mantle and lower mantle in combination with different stratified viscosity structures. We have demonstrated that the contradictory results concerning the effects of LVV can be clarified by the most straight-forward problem in geoid modeling; namely, rather poorly known stratified viscosity structure. We explored three classes of dynamic geoid models due to lateral viscosity variations. In the first class, the LVV strongly improved the fit to the observed geoid. Indeed, when the viscosity contrast between lower and upper mantles is not large enough to produce a good fit to geoid the LVVs are able to perform this action by adjusting amplitudes, so that it becomes comparable with observation. In the second class, inducing the LVV moderately improved the fit. Actually, when the geoid induced by a stratified viscosity structure already has a good correlation with observation, then the LVV causes its amplitude to further improve. In the last class, if the viscosity contrast between upper and lower mantle would be high enough, inducing LVV deteriorate the fit to the observed geoid.. Indeed, depending on the stratified viscosity, inducing the LVV may take place in one of these categories.
We also quantified the effects of LVV in the mantle and lithosphere individually. We found that the presence of LVV in the mantle (upper and lower) improves the fit to the observed geoid regardless of stratified viscosity. While LVV in the lithosphere is a crucial parameter, and dependent of the stratified viscosity, may increase or decrease the geoid fit. In fact, when the lower mantle considers being viscous enough, it would support the negative buoyancy of subducting slabs. Thus, it transmits some of the stress back to the top boundary and causes a weak coupling between slab and surface. Therefore, by including the low viscous plate boundaries in this model, the slabs and overriding plates decouples and the fit to the observed geoid degrades. In contrast, when the lower mantle viscosity is not sufficiently stiff, the presence of the low viscous plate boundaries assists to weaken the strong mechanical coupling between slab and surface. Hence, a better fit achieved.
Increases in water demand often result in unsustainable water use, leaving insufficient amounts of water for the environment. Therefore, water-saving strategies have been introduced to the environmental policy agenda in many (semi)-arid regions. As many such interventions failed to reach their objectives, a comprehensive tool is needed to assess them. We introduced a constructive framework to assess the proposed strategies by estimating five key components of the water balance in an area: (1) Demand; (2) Availability; (3) Withdrawal; (4) Depletion and (5) Outflow. The framework was applied to assess the Urmia Lake Restoration Program (ULRP) which aimed to increase the basin outflow to the lake to reach 3.1 × 109 m3 yr−1. Results suggested that ULRP could help to increase the Outflow by up to 57%. However, successful implementation of the ULRP was foreseen to be impeded because of three main reasons: (i) decreasing return flows; (ii) increased Depletion; (iii) the impact of climate change. Decreasing return flows and increasing Depletion were expected due to the introduction of technologies that increase irrigation efficiency, while climate change could decrease future water availability by an estimated 3–15%. We suggest that to reach the intervention target, strategies need to focus on reducing water depletion rather than water withdrawals. The framework can be used to comprehensively assess water-saving strategies, particularly in water-stressed basins.
A realistic simulation of the atmospheric boundary layer (ABL) depends on an accurate representation of the land–atmosphere coupling. Land surface temperature (LST) plays an important role in this context and the assimilation of LST can lead to improved estimates of the boundary layer and its processes. We assimilated synthetic satellite LST retrievals derived from a nature run as truth into a fully coupled, state‐of‐the‐art land–atmosphere numeric weather prediction model. As assimilation system a local ensemble transform Kalman filter was used and the control vector was augmented by the soil temperature and humidity. To evaluate the concept of the augmented control vector, two‐day case‐studies with different control vector settings were conducted for clear‐sky periods in March and August 2017. These experiments with hourly LST assimilation were validated against the nature run and overall, the RMSE of atmospheric and soil temperature of the first‐guess (and analysis) were reduced. The temperature estimate of the ABL was particularly improved during daytime as was the estimate of the soil temperature during the whole diurnal cycle. The best impact of LST assimilation on the soil and the ABL was achieved with the augmented control vector. Through the coupling between the soil and the atmosphere, the assimilation of LST can have a positive impact on the temperature forecast of the ABL even after 15 hr because of the memory of the soil. These encouraging results motivate further work towards the assimilation of real satellite LST retrievals.
The weather of the atmospheric boundary layer significantly affects our life on Earth. Thus, a realistic modelling of the atmospheric boundary layer is crucial. Hereby, the processes of the atmospheric boundary layer depend on an accurate representation of the land-atmosphere coupling in the model. In this context the land surface temperature (LST) plays an important role. In this thesis, it is examined if the assimilation of LST can lead to improved estimates of the boundary layer and its processes.
To properly assimilate the LST retrievals, a suitable model equivalent in the weather prediction model is necessary. In the weather forecast model of the German Weather Service used here, the LST is modelled without a vegetation temperature. To compensate for this deficit, two different vegetation parameterizations were investigated and the better one, a conductivity scheme, was implemented. In order to make optimal use of the influence of the assimilation of the LST observation on the model system, it is useful to pass on the information of the observation to land and atmosphere already in the assimilation step. For that reason, a fully coupled land-atmosphere prediction model was used. Therefore, the existing control vector of the assimilation system, a local ensemble transform Kalman filter, was extended by the soil temperature and moisture. In two-day case studies in March and August 2017, different configurations of the augmented assimilation system were evaluated based on observing system simulation experiments (OSSE).
LST was assimilated hourly over two days in the weakly and strongly coupled assimilation system. In addition, every six hours a free 24-hour forecast was simulated. The experiments were validated with the simulated truth (a high-resolution model run) and compared against an experiment without assimilation. It was shown that the prediction of the boundary layer temperature, especially during the day, and the prediction of the soil temperature, during the whole day and night, could be improved.
The best impact of LST assimilation was achieved with the fully coupled system. The humidity variables of the model benefited only partially from the LST assimilation. For this reason, covariances in the model ensemble were investigated in more detail. To check their compatibility with the high-resolution model run the ensemble consistency score was introduced. It was found that the covariances between the LST and the temperatures of the high-resolution model run were better represented in the ensemble than those between the LST and the humidity variables.
Am Rande der Westfälischen Bucht liegen bei Versmold und Gütersloh zwei Drumlinfelder. Die zusammen über 60 Rücken, die aus Sand und Geschiebelehm bestehen, wurden durch einen Gletscher des Inlandeises geformt, der aus der Westfälischen Bucht gegen die Randhöhen des Teutoburger Waldes vordrang. Es handelt sich um die Erstbeschreibung von Drumlins im Altmoränengebiet Nordwestdeutschlands.
The exchange of heat, momentum, and mass in the atmosphere over mountainous terrain is controlled by synoptic-scale dynamics, thermally driven mesoscale circulations, and turbulence. This article reviews the key challenges relevant to the understanding of exchange processes in the mountain boundary layer and outlines possible research priorities for the future. The review describes the limitations of the experimental study of turbulent exchange over complex terrain, the impact of slope and valley breezes on the structure of the convective boundary layer, and the role of intermittent mixing and wave–turbulence interaction in the stable boundary layer. The interplay between exchange processes at different spatial scales is discussed in depth, emphasizing the role of elevated and ground-based stable layers in controlling multi-scale interactions in the atmosphere over and near mountains. Implications of the current understanding of exchange processes over mountains towards the improvement of numerical weather prediction and climate models are discussed, considering in particular the representation of surface boundary conditions, the parameterization of sub-grid-scale exchange, and the development of stochastic perturbation schemes.
Die Wechselwirkung zwischen zwei verschiedenartigen Wellenphänomenen in einer Höhe von ca. 10 bis 100 km, der mittleren Atmosphäre, ist das zentrale Thema der vorliegenden Arbeit. Schwerewellen entstehen durch Oszillationen der Luft in einer stabil geschichteten Atmosphäre. Durch die Vielzahl von Schwerewellen-Paketen, die in der Troposphäre durch Gebirge, Gewitter, Fronten und andere dynamische Prozesse angeregt werden, wird Energie und Impuls in die mittleren Atmosphäre transportiert. Durch den turbulenten Zerfall von brechenden Schwerewellen wird auf die mittlere Strömung eine Kraft ausgeübt, welche im Bereich der Mesopause bei ca. 90 km maximal wird. Daraus resultiert die sogenannte interhemispherische residuelle Zirkulation, die in der Mesosphäre den Sommer- mit dem Winterpol verbindet und die beeindruckend kalte Sommer-Mesopause mit Temperaturen von unter −140°C verursacht. Thermische Gezeiten sind ein weiterer wichtiger Teil in der Dynamik der mittleren Atmosphäre. Sie werden durch die Erwärmung der Tagseite der Erde angeregt und sind globale Schwingungen mit Perioden von 24 Stunden und harmonischen Vielfachen. Mit Wind- und Temperatur-Amplituden von bis zu 50 m/s und 30 K dominieren sie die Tagesvariabilität im Mesopausen-Bereich.
In der Mesosphäre wird die Wechselwirkung zwischen Schwerewellen und thermischen Gezeiten wichtig. Dort wird durch die Gezeitenwinde das Brechen von Schwerewellen zeitlich moduliert und eine periodische Kraft erzeugt, welche auf die Gezeiten rückwirkt. Doch selbst unter Zuhilfenahme modernster Hochleistungsrechner kann in komplexen Zirkulationsmodellen nur ein Bruchteil des turbulenten sowie des Wellen-Spektrums aufgelöst werden. Der Effekt der nichtaufgelösten Skalen, wie Turbulenz und Schwerewellen, muss somit in effizienter Weise parametrisiert werden. Üblicherweise wird in Schwerewellen-Parametrisierungen die horizontale und zeitliche Variation des Hintergrundmediums vernachlässigt. Es entsteht eine vertikale Säule, in der sich stationäre Schwerewellen-Züge instantan nach oben ausbreiten. Es ist jedoch äußerst fraglich, inwieweit eine solche Beschreibung, auf der ein Großteil früherer Untersuchungen basiert, für das Ergründen der Schwerewellen-Gezeiten-Wechselwirkung hinreicht. Für diese Arbeit wurde deswegen das Ziel gesetzt, die Defizite der konventionellen Beschreibung der Schwerewellen-Ausbreitung in realistischen Gezeiten zu quantifizieren.
Die "Ray Tracing"-Methode wird auf die Problemstellung der Schwerewellen-Gezeiten-Wechselwirkung angewendet. In der "Ray Tracing"-Methode werden Schwerewellen-Pakete entlang ihrer Ausbreitungspfade explizit verfolgt und Veränderungen der Schwerewellen-Eigenschaften durch den Einfluss der Hintergrundströmung berücksichtigt. Vom Autor wurde das globale "Ray Tracing"-Modell RAPAGI (RAy PArameterization of Gravity-wave Impacts) entwickelt und mit realistischen Gezeitenfeldern aus dem Zirkulationsmodell HAMMONIA (HAmburg MOdel of the Neutral and Ionized Atmosphere) betrieben. In verschiedenen "Ray Tracing"-Experimenten wird für ein einfaches Schwerewellen-Ensemble gezeigt, wie horizontale Gradienten des Hintergrundmediums sowie dessen Zeitabhängigkeit wesentlichen Einfluss auf die Ausbreitung und Dissipation von Schwerewellen nehmen. Zum einen führt die durch Gezeitenwellen hervorgerufene Transienz zu einer tageszeitlichen Modulation der absoluten Schwerewellen-Frequenz.
Die dadurch induzierten Variationen der horizontalen Phasengeschwindigkeit der Schwerewellen können die anfängliche Phasengeschwindigkeit um bis zu eine Größenordnung übertreffen und folgen dem Verlauf des Hintergrundwindes. Die kritische Filterung von Schwerewellen wird durch diese Modulation abgeschwächt, was im Vergleich zu konventionellen Schwerewellen-Parametrisierungen zu einer im Mittel um 30 % geringeren Kraftwirkung auf die Gezeiten führt. Zum anderen werden durch horizontale Gradienten in der gesamten Hintergrundströmung Schwerewellen-Pakete horizontal abgelenkt. Wellen, die gegen die Hintergrundströmung laufen, werden in der Stratosphäre in die Maxima der Wind-Jets hineingeführt. Durch dieses Verhalten wird analog zum Fermatschen Prinzip der geometrischen Optik die Laufzeit der Schwerewellen in der mittleren Atmosphäre minimiert. Es entsteht eine Fokussierung von Schwerewellen-Feldern, bei gleichzeitiger Zunahme der horizontalen Wellenzahl in den Experimenten im Mittel um ca. 10 %. Dadurch reduziert sich der Schwerewellen-Impulsfluss und die mittlere und ebenfalls die periodische Kraft auf die Hintergrundströmung im Mittel um weitere 20 % bis 30 %. Konventionelle Schwerewellen-Parametrisierungen scheinen somit die Kraftwirkung von brechenden Schwerewellen zu uberschätzen. Aus den Ergebnissen der Arbeit wird klar, dass Schwerewellen-Parametrisierungen nicht "blind" für jede Untersuchung genutzt werden können. Alle Annahmen und Näherungen in Parametrisierungen müssen je nach Zielstellung neu getestet werden.
Aus Franken wird die Entwicklung quartärer Hohlformen beschrieben, deren Rekonstruktion mit Hilfe lößstratigraphischer Methoden (fossile Böden, Tuffbänder, Umlagerungszonen etc.) möglich ist. Bei vielen Formen zeigt sich, daß sie bereits größere Vorläuferformen präwürmzeitlichen Alters hatten. Die Entwicklung während des Würms läßt sich an manchen Beispielen in besonders instruktiver Weise verfolgen. Zu Beginn des Würms, im unteren Mittelwürm und im unteren Jungwürm dominierte zeitweise die Abtragung und Verlagerung. Im oberen Mittelwürm sowie im oberen Jungwürm herrschte äolische Lößsedimentation vor. Diese Ergebnisse stimmen gut mit den bereits aus anderen mitteleuropäischen Lößgebieten bekannten Befunden überein. Mit dem Trockental-System von Helmstadt wird die Entwicklung von Hohlformen beschrieben, deren Anlage bis in das ältere Pleistozän zurückreicht.