Stand und Entwicklungsmöglichkeiten der absoluten Schweremessungen

Summary The chief object treated here relates to the proposals of the author, to modify the wellknown thread-pendulum apparatus (FP), constructed byBessel 1826 at Königsberg, aiming at the introduction of modern physical methods and materials. This method seems to be the single one comparable in exactitude with reversion pendulum (RP). Further more the free fall method (FF) has been shortly discussed with regard to the expectable mean errors, for purpose of comparison with the two others. The FF-method seems not to be able to control the RP-measurements.

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Résumé L'objet principal de l'article se rapporte à des propositions de l'auteur ayant le but de modifier le bienconnu appareil à fil (FP), construit parBessel en 1826 à Königsberg. Les propositions tendent à l'introduction de méthodes et de matériaux physiques modernes. La méthode est probablement la seule comparable en exactitude aux pendules de reversion (RP). En outre la méthode de la chute libre (FF) a été discutée relativement aux erreurs moyennes expectables, au but de la comparaison avec les deux autres. La méthode FF est trouvée incapable à contrôler les mesures RP.

     

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Der künstliche Mond als Hilfsmittel für Geodäsie und Astronomie

Summary The artificial moon, projected from serious scientists, presents, whenever previously without reality, a field of interesting theoretical problems. At first the figure of movement of the body itself within the varying gravity field, further more its observation by angles and distances relative to earth's body and to sky and the possible reconclusions to earth's figure and to natural moons movement. The latter beeing in a too far distance from the earth, the former surely will help to solve different problems of geodesy and astronomy.

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Résumé La Lune artificielle, comme projet d'une science sérieuse moderne, présente, quand même préalablement sans réalité, un grand nombre de problèmes théoriques intéressantes. Avant tout la figure elle même de sa route dans le champs variant de la gravité et de la force centrifuge, de plus l'observation par angles et distances relatives à la terre et au ciel, et les reconclusions à la figure de la terre et au mouvement de la Lune naturelle. Cette dernière se trouvant perpétuellement dans une position de distance trop grande, la première peut aider sans doute la solution de problèmes différents de géodésie et astronomie.

     

Geodynamic evolution of crust accretion at the axis of the Reykjanes Ridge,Atlantic Ocean

The results of analysis of the anomalous magnetic field of the Reykjanes Ridge and the adjacent basins are presented, including a new series of detailed reconstructions for magnetic anomalies 1–6 in combination with a summary of the previous geological and geophysical investigations. We furnish evidence for three stages of evolution of the Reykjanes Ridge, each characterized by a special regime of crustal accretion related to the effect of the Iceland hotspot. The time interval of each stage and the causes of the variation in the accretion regime are considered. During the first, Eocene stage (54–40 Ma) and the third, Miocene-Holocene stage (24 Ma-present time at the northern Reykjanes Ridge north of 59° N and 17–11 Ma-present time at the southern Reykjanes Ridge south of 59° N), the spreading axis of the Reykjanes Ridge resembled the present-day configuration, without segmentation, with oblique orientation relative to the direction of ocean floor opening (at the third stage), and directed toward the hotspot. These attributes are consistent with a model that assumes asthenospheric flow from the hotspot toward the ridge axis. Decompression beneath the spreading axis facilitates this flow. Thus, the crustal accretion during the first and the third stages was markedly affected by interaction of the spreading axis with the hotspot. During the second, late Eocene-Oligocene to early Miocene stage (40–24 Ma at the northern Reykjanes Ridge and 40 to 17–11 Ma at the southern Reykjanes Ridge), the ridge axis was broken by numerous transform fracture zones and nontransform offsets into segments 30–80 km long, which were oriented orthogonal to the direction of ocean floor opening, as is typical of many slow-spreading ridges. The plate-tectonic reconstructions of the oceanic floor accommodating magnetic anomalies of the second stage testify to recurrent rearrangements of the ridge axis geometry related to changing kinematics of the adjacent plates. The obvious contrast in the mode of crustal accretion during the second stage in comparison with the first and the third stages is interpreted as evidence for the decreasing effect of the Iceland hotspot on the Reykjanes Ridge, or the complete cessation of this effect. The detailed geochronology of magnetic anomalies 1–6 (from 20 Ma to present) has allowed us to depict with a high accuracy the isochrons of the oceanic bottom spaced at 1 Ma. The variable effect of the hotspot on the accretion of oceanic crust along the axes of the Reykjanes Ridge and the Kolbeinsey and Mid-Atlantic ridges adjoining the former in the north and the south was estimated from the changing obliquity of spreading. The spreading rate tends to increase with reinforcing of the effect of the Iceland hotspot on the Reykjanes Ridge.     

Seismotectonic deformations related to the 2010 Maule earthquake at different stages of the seismic cycle from satellite geodetic observations

Doklady Earth Sciences - The interpretation of multiannual satellite geodetic observations after the 2010 Maule earthquake is given on the basis of the keyboard concept of the subduction region...     

Intermittent chaos in nonlinear wave–wave interactions in space plasmas

There is increasing observational evidence of nonlinear wave–wave interactions in space and astrophysical plasmas. We first review a number of theoretical models of nonlinear wave–wave interactions which our group has developed in the past years. We next describe a nonlinear three-mode truncated model of Alfvén waves, involving resonant interactions of one linearly unstable mode and two linearly damped modes. We construct a bifurcation diagram for this three-wave model and investigate the phenomenon of intermittent chaos. The theoretical results presented in this paper can improve our understanding of intermittent time series frequently observed in space and astrophysical plasmas.     

Wind sedimentation in the Jafurah sand sea, Saudi Arabia

The Jafurah sand sea of the Eastern Province of Saudi Arabia extends along the Arabian Gulf coastline from Kuwait in the north to the Rub Al Khali in the south, a distance of about 800 km. Sand drifts southward to south-eastward from regions of high wind energy in the north to low wind energy in the south. The aeolian landscape is zoned, with areas of deflation, transport and deposition from north to south. Drift rates in the zone of transport, near Abqaiq, range from 2 m³ m-w^-1 yr^-1 on sabkhas, to 29 m³ m-w^-1 yr^-1 on the crests of dunes. Average drift rates of approximately 18 m³ m-w^-1 yr^-1 observed during the study can cause about 1 m of accumulation per 5500 yr in a 100 km zone of deposition downwind, not including the bulk transport represented by the forward advance of dunes. Dune advance ranged from 23 m (2.9 m high dune) to 3 m (23 m high dune) during April-October 1980. The study area consists of dune, interdune, sand sheet and siliciclastic sabkha terrains, each of which is characterized by differing drift rates, and differing rates of erosion or deposition. Sedimentation occurs by lateral movement of dunes and interdunes, and vertical accretion by sand sheets and sabkhas.