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41.
Summary Phase velocities of Rayleigh and Love waves have been measured between the broadband seismic stations KHC (Kaperské Hory, South Bohemia) and KSP (Ksi, Lower Silesia), a profile that nearly coincides with the Interactional DSS Profile VII. The data for both wave types were separately inverted into models of shear-wave velocity versus depth. Novotný's model KHKS 82[1] for the DSS Profile VII was used as a start model. While the crustal section of Novotný's model is compatible with both of our data sets, our Rayleigh-wave data require smaller shear-wave velocities, on the average by 0.24 km/s, in the top 180 km of the mantle. The average difference between Novotný's model and our Love-wave model in that depth range is only 0.06 km/s. If our identification of the observed Love waves as the fundamental mode is correct, this result indicates the presence of polarization anisotropy in the uppermost mantle.
u a mu u a ¶rt; unu uuu mauu (an , a u) u S (, ua uu). u - S nuuum mmmm ¶rt;a¶rt; nu VII . a ¶rt; u mun m¶rt; umua ¶rt;u auumu mu nn mu. am mam¶rt;u a unaa ¶rt; S 82 m[1] ¶rt; nu VII . a am ¶rt;u m aua uu aau au ¶rt;a, ¶rt;a au ¶rt;a ¶rt; mm uu m nn — ¶rt; a 0,24 / 180 uma amuu. ¶rt;a aua ¶rt; ¶rt; m u a ¶rt; ¶rt; a m ¶rt;uanau n¶rt;mam 0,06 /. u aa u¶rt;muuau a¶rt;a a a ¶rt;ama ¶rt;a m nau, m mm mam u¶rt;ummm numuu nuau aumnuu amuu.
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42.
The Ivrea zone represents a tilted cross section through deep continental crust. Sm-Nd isotopic data for peridotites from Baldissero and Balmuccia and for a suite of gabbros from the mafic formation adjacent to the Balmuccia peridotite provide evidence for an event of partial melting 607±19 Ma ago in an extended mantle source with 607 Nd =+0.4±0.3. The peridotites are interpreted as the corresponding melt residue, the lower part of the mafic formation as the complementary melts which underwent further differentiation immediately after extraction. The Finero body represents a complex with layers of phlogopite peridotite, hornblende peridotite, and amphibole-rich gabbro. The isotopic signatures fall into two groups: (1) highly radiogenic Nd and low-radiogenic Sr characterize the phlogopite-free, amphibole-rich rocks, whereas (2) low-radiogenic Nd and highly radiogenic Sr is found in ultramafics affected by phlogopite metasomatism. Phlogopite metasomatism in the Ivrea zone is dated by a Rb-Sr whole rock isochron yielding 293±13 Ma. It was fed by K-rich fluids which were probably derived from metasediments. The high initial 293 Nd value of about +7.5 for phlogopite-free samples indicates a high time-integrated Sm/Nd ratio in the Finero protolith 293 Ma ago. Sm-Nd analyses of metapelites from the paragneiss series yield Proterozoic crustal residence ages of 1.2 to 1.8 Ga. Internal Sm-Nd isochrons for three garnetiferous rocks show that closure of garnet at temperatures around 600° C or even lower occurred about 250 Ma ago.  相似文献   
43.
Kohala revisited     
We present new isotopic data for Sr and Nd in basalts and alkalic volcanics from Kohala volcano, Hawaii, which had previously been described by Feigenson et al. (1983). These data complement our own isotopic data presented in that paper and those given in the companion paper by Lanphere and Frey (1986). We show that in spite of appearances to the contrary, there is no significant analytical bias in our previously published analyses. Accidental sampling bias and one erroneous value prevented us from recognizing the isotopic heterogeneity in our previously published data. The new data both confirm the Sr-isotopic distinction between Pololu and Hawi volcanics discovered by Lanphere and Frey and narrow the gap between them significantly. The two data sets agree for the Hawi samples, but the mean 87Sr/86Sr=0.703651±13 for our Pololu basalts is significantly lower than the mean 87Sr/86Sr= 0.703748±18 found by Lanphere and Frey. The Ndisotopic ratios are also heterogeneous, but they overlap for the two formations. We agree with the assessment of Lanphere and Frey that some of our samples originally classified as belonging to the Hawi Formation are actually derived from the uppermost Pololu Formation, but with some stratigraphic ambiguities remaining.We believe that our previous results of inverse modelling are valid for the tholeiitic and moderately alkalic Pololu Formation despite the isotopic heterogeneity because this heterogeneity does not correlate with the trace element chemistry of the Pololu samples.The severe depletion of Sc, which correlates with decreasing CaO/Al2O3 ratios and increasing Yb concentrations, confirms the importance of clinopyroxene fractionation in the evolved lavas of the Hawi Formation. In addition, apatite precipitation did fractionate the P/Ce ratios in the more evolved Hawi lavas, but its effect on the REE abundances is still uncertain and may not be significant.The MgO — P2O5 plot of Lanphere and Frey does not provide compelling evidence against a simple genetic relationship between Pololu and Hawi lavas. The internal consistency of the (fractionation corrected) trace element ratios such as Ba/Ce indicates that Ba is depleted in both the Hawi and the Pololu sources and that these sources do have similar chemistry.Finally, we show that contrary to the conclusions of Lanphere and Frey the REE patterns of Kohala volcanics can be generated from sources with only slightly negatively sloping REE patterns without involvement of garnet, as was indicated by the formal inversion analysis. Models which include garnet yield more highly anomalous source abundance patterns and calculated bulk-source partition coefficients which are inconsistent with the presence of garnet. The persistence of residual garnet is also inconsistent with the absence of significant heavy-REE fractionation among the Pololu basalts.  相似文献   
44.
The impacts of military activities in peacetime, military action and territorial changes on greenhouse gas emission commitments of nations under the Kyoto Protocol are analysed. We propose rules and institutional responsibilities to deal with the repercussions of such changes on markets in emission permits and national commitments aiming at prevention of serious distortions.  相似文献   
45.
46.
himu, em i andem ii are three of the main geochemical mantle components that give rise to oceanic island basalts [1]. They represent the end members that produce the extreme isotopic compositions measured on intraplate volcanics. In French Polynesia, all three mantle components are represented in volcanic rocks. The characteristichimu signature is found in Tubuai, Mangaia and Rurutu,em i is present in the source of Rarotonga and Pitcairn volcanics andem ii dominates the composition of most Society Islands. Intermediate values between the three end members are found on most islands.We suggest that the three components are not independent but are physically related in the mantle. Thehimu component is thought to be recycled oceanic crust that lost part of its Pb through hydrothermal processes prior to and during subduction.em i andem ii are believed to acquire their isotopic and trace element characteristics through entrainment of sediments that were subducted together with the oceanic crust.The trace element pattern and the isotopic composition ofhimu lavas can be quantitatively modelled using a mixture of 25% old recycledmorb crust and 75% mantle peridotite. The extreme Pb composition is modelled assuming that Pb was lost from oceanic crust when hydrothermal alteration at the ridge leached Pb from the basalt to redeposit it as sulphides on top of and throughout the crust, followed by preferential dissolution of sulphides during dehydration in the subduction zone. These processes led to a drastic increase of theU/Pb ratio of the subducted material which evolved over 2 Ga to very radiogenic Pb isotopic compositions. Pb isotopic compositions similar to those ofem i andem ii are modelled assuming that sediments with average crustal Pb isotopic compositions were subducted and recycled into the mantle together with the underlyingmorb oceanic crust. Pelagic sediments (μ 5 andκ 6) account for the Pb isotopic composition ofem i whereas terrigenous sediments (μ 10 andκ 4.5) evolve towards theem ii end member. A few percent of sediment in the recycled crust-sediment mixture will destroy the characteristic Pb isotopic signature of thehimu component. This, together with the low probability of isolating oceanic crust in the mantle for 2 Ga, explains why the extremehimu composition, as seen on Tubuai and St Helena, is sampled so rarely by oceanic volcanism.  相似文献   
47.
Lower and Upper Cretaceous sediments were investigated in the Peruvian Central Cordillera. As in the western facies of Central and Northern Peru, the Goyllarisquisga Group is subdivided into several lithologically different formations, in which sediments were transported from east to west. The area of investigation is situated west of the facies boundary between Marañon geanticline and West Peruvian trough; this indicates that the boundary continues south and does not follow the line Celendin-Rio Palanga as suggested byWilson. The limestones and dolomites of the Santa Formation were deposited in shallow water, possibly with intermittent subaerial exposure. The sandstone of the Farrat Formation are interpreted to be sediments of a west-east transgression; vertically they grade into the limestones of the Pariahuanca-Formation. Facies and thickness of the Chulec and Pariahuanca-Formation are little different from those in neighbouring areas. During deposition of the thick Jumasha Formation, the differences are much more significant, and only comparison with Northwest Peru shows some agreement.  相似文献   
48.
Приводится описание фотокомпенсационного усилителя на полупроводниках, предназначенного для усиления слабых выходных сигналов пассивных преобразователей геофизических величин. Шумовые помехи отнесенные к входу усилителя порядка 10?8 в или 10?10 а в диапазоне частот 0,01–20Гц. Описывается новый метод, который позволяет создать фотокомпенсационные усилители напряжения или тока с заранее заданными передаточными свойствами (заданной амплитудной или фазовой частотной характеристкой, заданным быстродействием и т.п.). Возможности использования этого метода демонстрируются на двух практических примерах.  相似文献   
49.
50.
Zusammenfassung Das Verformungsverhalten von Felshängen wird einmal durch die geologische Entwicklungsgeschichte, zum anderen durch die zum Zeitpunkt der Beobachtung herrschenden Randbedingungen (Höhe, Neigung des Hanges, eingeprägte Kräfte) und Gebirgseigenschaften bestimmt. Diese Gebirgseigenschaften sind einerseits von den Gesteinseigenschaften (Verformbarkeit und Festigkeit) und andererseits von der Klüftung abhängig.Mit Hilfe zweidimensionaler großmaßstäblicher Modelle, die in einer ersten Serie aus starren Kluftkörpern (Strukturmodelle) und in einer zweiten Serie aus äquivalentem Modellmaterial aufgebaut waren, wird der Versuch unternommen, die innere Kinematik eines ganzen Hangquerschnittes zu studieren. Während im ersten Fall der Einfluß des Trennflächengefüges allein untersucht werden kann, überlagern sich im zweiten Fall Material- und Gefügeparameter.Anhand der Strukturmodelle wird eine Einteilung in verschiedene typische Verformungsverhalten von Hängen in Abhängigkeit von der Kluftstellung und vom Kluftreibungswinkel vorgenommen.Der besonders interessante Fall eines Kluftkörperverbandes mit bergeinwärtsfallender Bankung — hier überlagern sich Rotations- und Translationsbewegungen — wird in seinem gesamten Verformungsablauf beschrieben und nach charakteristischen Verformungsstadien unterteilt. Dabei wird die Entwicklung der Verformungen vom Hakenwerfen der Böschungsfront bis zu einem tiefgreifenden Talzuschub mit der Ausbildung ausgeprägter Schwächezonen erfaßt.Die an den Versuchen durchgeführten Beobachtungen gestatten eine bessere Bewertung des Trennflächeneinflusses auf das Verformungsverhalten von Felsmassen mit regelmäßigem Gefügemuster (H-Typ) und geben Hinweise zur besseren Abschätzung des Verformungsablaufes im Inneren eines Hanges sowie der zu erwartenden Form des Böschungsbruchkörpers.
The deformation behaviour of rock slopes is influenced by the geological history, by the boundary conditions (height, inclination of the slope, additional forces) acting at the time of observation and the material properties of the rock mass. The properties depend on the rock parameters (deformability and strength) and on the joint patterns.With two-dimensional large scale models which consisted of rigid blocks in the first series of tests (structural models) and of equivalent model material in a second one, it was tried to study the kinematics of a whole slope section.In the first of those cases joint fabric is the only parameter to be investigated while in the second, series of test material and structural parameters have to be considered simultaneously. The structural models allow a classification into different types of deformation behaviour of the slopes. Criteria of classifications are the inclination of the strata and the friction angle.The especially interesting case of a jointed rock system with strata dipping into the mountain (in this case rotational and translational displacements are superposed) is described in its whole deformation history which is divided into characteristic stages of deformation. The development of displacements is studied from a first Hakenwerfen at the front of the slope to a deep Talzuschub with the formation of zones of weakness (latent sliding surfaces).Conclusions drawn from these tests allow a better assessment of the influence of joint sets on the deformation behaviour of a rock mass, the development of displacements in the interior of a slope and the shape of sliding surfaces.

Résumé Le processus de déformation des versants rocheux est déterminé d'abord par l'histoire géologique, ensuite par les conditions immédiates du milieu régnant au moment de l'observation (hauteur, inclinaison de la pente, forces emmagasinées) et par les propriétés à l'échelle de l'ensemble rocheux. Ces dernières dépendent d'une part des propriétés du matériau rocheux lui-même (déformabilité et résistance) et d'autre part de la fissuration.A l'aide de maquettes bidimensionelles à grande échelle composées, lors d'une première série, de blocs rigides (modèle structural) et lors d'une seconde série, de blocs faits d'un matériau équivalent, on a assayé d'étudier la cinématique interne d'une coupe transversale faite dans un versant. Tandis que dans le premier cas, c'est seulement l'influence de la disposition des plans de division qui a pu être recherchée, dans le second il y a eu superposition des paramètres propres à cette disposition et au matériau.En partant de ces modèles structuraux, on a pu classer les différents types de comportements à la déformation des versants en fonction de la position de fissures et de leur angle de frottement.Le cas particulièrement intéressant d'un complexe fissuré à stratification inclinant vers l'intérieur du versant (ici se superposent en effet les mouvements de rotation et de translation) est décrit intégralement dans le déroulement de sa déformation et subdivisé en stades caractéristiques de déformation. On a pu ainsi saisir le développement des déformations depuis le «Hakenwerfen» du front du talus jusqu'à la poussée en profondeur vers la vallée, avec formation de zones de faiblesse bien marquées.Les observations faites lors des essais permettent de mieux évaluer l'influence des plans de division sur le processus de déformation des masses rocheuses qui ont une structure régulière (type H). Elles donnent des indications pour apprécier plus justement le développement de la déformation dans un versant, et de la forme de la zone de rupture à laquelle il faut s'attendre.

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