Effect of cofactors of adjusted and unadjusted quantities on their functions

aamuam uu am a (m u naamuu n) u u (a) uu a uu mu uu. mam (19), (28) naam, m amua am mau u m ¶rt; am amu: a) na ¶rt;um am, n n a uu am u uu a uu; ) ma ¶rt;um am, m aam uu a uu.     

Numerical modelling of time-harmonic seismic wave fields in simple structures by the Gaussian beam method. Part II

ma ama m n¶rt;u am[1]. u ama, m¶rt;au n unm ¶rt; uuauu ma m nau a¶rt;a. a uau ¶rt;m ma a muna . au mu mamau n [1], m m¶rt;au n ¶rt;am ¶rt;mam m mam ¶rt;a u amu aa mu. aumu amu, uauau n ma nuu ¶rt;a . m am ¶rt;am mumm mam a naama am, aa uu L ₀ au n. aa, m am mam namuu aum m L ₀ . amu aa mu u aumu amu, a m mam n ¶rt; u L ₀ . u uu L ₀ , anum¶rt; ma amu aa mu nuam, nu aua nam m, m uu L ₀ auum. aumu amu, u L ₀ um m uau m a uuu anum¶rt; u, mmmu a. uu L ₀ , uuu nam. ma uam mumm mam ¶rt;a ¶rt;u naama am. uau ¶rt;m ma anum¶rt; u ma muna S, S u SS.     

Magnetic susceptibility anisotropy of deformed rocks

¶rt;au uu aum nuuumu u aumnuu ¶rt; aa aam n¶rt; am amuu u namuu ¶rt;au. amu uu aumnuu nuuumu, a amu ¶rt;au, m ¶rt;mu au ma nma aaumu m¶rt; ¶rt;a, m a amu uu aum m mnu n¶rt;u ¶rt; mm uaum amua n¶rt; ¶rt;au. u aumnuu nu a namu ¶rt;auu(<1%) a uuu m nuuumu _i uaum amua. u aumnuu ¶rt;mu uu uum aauuau ¶rt;ua am m uu, m, m ¶rt; u au namu ¶rt;auu.     

Storm surge versus turbidite origin of the Coniacian to Santonian sediments in the eastern part of the Bohemian Cretaceous Basin

A flyschoid facies occurs in the Bezno Formation (Coniacian up to Santonian) of the eastern marginal part of the Bohemian Cretaceous Basin. According toJerzykiewicz (1970, 1971) this facies is of deep water, turbidite origin. He based his interpretation on the study of sedimentary structures. New palaeogeographic reconstruction of lithofacies relations, investigation of deep drillings and detailed sedimentological analysis, however, allowed new results concerning the sedimentary environments and depositional mechanism of this facies. According to the new model presented here, this flyschoid facies was deposited in a shallow marine environment. Clayey sedimentation was the natural response to normal environmental conditions, whereas sandstone intercalations reflect anomalous conditions during heavy storms. During these events, sands were transported basinwards up to distances of 25 km, with normal bottom currents, as well as turbidity currents, acted as transporting mechanisms. This flyschoid facies corresponds to other examples of clayey sequences with sandy storm layers.

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Zusammenfassung Die Bezno Schichtenfolge (Coniac bis Santon) enthält im östlichen Randteil des Böhmischen Kreidebeckens sogenannte flyschoide Fazies. NachJerzykiewicz (1970, 1971) entstand sie im tiefen Wasser wie echte Turbidite. Die paläogeographische Rekonstruktion von Faziesbeziehungen, ausführliche Bearbeitung der Schichtenfolge in Bohrungen, und vollständige Beckenanalyse ermöglichten eine Neudeutung von Transportmechanismen und Ablagerungsmilieu. Es werden Beweise für Flachwassersedimentation erbracht. Das Sedimentationsgebiet entsprach einem Bereich der Tonablagerung, der von Zeit zu Zeit während anomaler Bedingungen — seltenen, sehr schweren Sturmfluten durch Sandzufuhr gestört wurde. Während dieser Sturmfluten wurde Sand ins Becken geschüttet bis zu einer Entfernung von 25 km von der Küste. Die Funktion von Traktionströmen wird diskutiert im Verhältnis zum Einfluß von Trübeströmen. Die beschriebene flyschoide Fazies entspricht Schichtfolgen mit sandigen Sturmflutlagen.

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Résumé Dans la partie marginale du Bassin Crétacée de Bohême, la formation de Bezno (Coniacien à Santonien) est caractérisée par le développement du faciès flyschoide. Ce faciès a été étudié parJerzykiewicz (1970, 1971), qui a proposé son origine dans un bassin profond, sous l'activité de courants de turbidité. L'étude détaillée de la succession des couches dans les forages profonds, de nouvelles données sédimentologiques ainsi que la reconstruction paléogéographique ont amené l'auteur à établir un nouveau modèle de mécanisme de transport dans les milieux de sédimentation. Selon ce modèle le faciès flyschoid se déposerait dans la mer épicontinentale peu profonde. Les argiles marquent les conditions normales de ce milieu sédimentaire; les grès reflètent des conditions hydrodynamiques anomales au cours de tempêtes rares et très fortes. Durant ces tempêtes les sables côtiers ont été redéposés dans des fonds plus profonds jusqu' à une distance de 25 km. La fonction des courants de traction est discutée en rapport avec l'influence des courants de turbidité entant qu' agents de transport. Le faciès étudié est comparable avec les séquences des argiles à intercalations de grès.

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( ) . . . (jerzykiewicz 1970, 1971), . , , , . 25 . . .

     

Die Kristallstruktur des Minerals Eclarit, (Cu,Fe) Pb9Bi12S28

Zusammenfassung Die Kristallstruktur des zuerst vonPaar, Chen undMeixner beschriebenen neuen Minerals wurde an der Originalprobe bestimmt. Für die prinzipielle Lösung der Struktur war eine Kombination von direkten und Pattersonmethoden erforderlich. Anhand von 2774 kristallographisch unabhängigen Röntgenreflexen (davon 1828 beobachtet) wurde die Struktur bis zu einem gewichtetenR-Wert von 10.7% isotrop verfeinert. Das Mineral ist orthorhombisch, RaumgruppePnma mit den Gitterkonstantena ₀=54.76Å,b ₀=4.030 Å,c ₀=22.74 Å undZ=4. Die Kristallstruktur ist durch galenitähnliche Bereiche, deren [110] Richtung parallel zurb ₀-Achse verläuft, gekennzeichnet. Die gegenseitige Anordnung dieser Bereiche ist teils kobellit-, teils cosalitähnlich. Die galenitähnlichen Bereiche sind vorwiegend wismuthhaltig (Koordination 3+2+1), während die Ph-Atome in einer trigonal-prismatischen Koordination mit 2 zusätzlichen Schwefelatomen vorwiegend als Bindeglieder dazwischen liegen.

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The crystal structure of eclarite, (Cu,Fe)Pb₉Bi₁₂S₂₈

Summary The crystal structure of the new mineral eclarite, first described byPaar, Chen andMeixner was determined using the original material. It was necessary to apply a combination of direct and Patterson methods. The structure was refined for 2774 independent reflections (1828 observed) with isotropic temperature factors to a weightedR-value of 10.7%. Eclarite crystallizes in the orthorhombic space groupPnma with lattice parametersa ₀=54.76 Å,b ₀=4.030 Å,c ₀=22.75 Å,Z=4. The structure is characterized by galena-like building units with [110] (galena) parallel to theb-axis. These units are linked to each other partly as in kobellite, partly as in cosalite structures. Bi prefers to occupy the metal positions in the galena-like units, coordinated by 3+2+1S, whereas Pb occupies preferably the positions coordinated trigonal prismatic with two additional S. The latter groups serve to connect the galena-like units.

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Mit 3 Abbildungen

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Herrn Professor Dr.Josef Zemann zum 60. Geburtstag gewidmet.     

Mode of occurrence of Cu and Zn in till over three mineralized areas in Finland

The variation of Cu and Zn contents with grain size was studied in the size fractions: 2000-500 μm, 500-64 μm, 64-2 μm and minus 2 μm. The fixation to different minerals was investigated in the 500-64 μm and minus 64 μm fractions with microscope, microprobe, electron microscope and X-ray diffraction after heavy-liquid separation.The distribution of Cu and Zn between the four size fractions is very similar in all target areas. The contents tend to be highest in the minus 2 μm fraction, and to decrease with increasing grain size except for an increase in the coarsest material. This feature is typical in mineralized areas with till having anomalously high Cu and Zn contents.The anomalous Cu and Zn in the till of Talvivaara are mainly fixed to chalcopyrite and sphalerite, respectively, which indicates that the main part of the material originates from fresh bedrock and that postglacial alterations are slight. In the till of Outokumpu and Maaselkä sulphides are rare. We assume that in Outokumpu the reason for this is the postglacial weathering of sulphides and that in Maaselkä a great deal of till derives from highly weathered, sulphide-poor, preglacial regolith. In both target areas Cu in till seems to fix to limonite and also to clay minerals, particularly in Maaselkä. Zinc seems mainly to be hosted by limonite in Outokumpu.     

Eddy energy dissipation rate and puff diffusion during calms

The paper considers a puff diffusion in its inertial stage when particle separation obeys the laws of the inertial subrange and depends only on eddy energy dissipation rate . The can be determined in the surface layer by the turbulent kinetic energy equation. Similarity equations connect with diffusion measure .A simple analytical model has been deduced to estimate pollutants diffusion during calms.     

Some possibilities of predicting radio wave absorption in the lower ionosphere

Summary An attempt is made to show possible ways of predicting radio wave absorption in the midlatitude lower ionosphere using relations between absorption and the intensity of solar ionizing radiation and/or common solar activity indices, and between absorption and f₀F2.

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aa mu nuau nu a¶rt;u ¶rt;um u u a mu ¶rt; nu u umum uuu uu (uu uu u¶rt;au amumu) u ¶rt; nu u f₀F2.

     

Effects of the imf sector structure in the midlatitude troposphere and stratosphere

Summary The data on geopotential heights and temperatures at 7 pressure levels between 1000-10 hPa above Berlin(52.5 °N, 13.4 °E) are analysed for the winters of 1963–1973. No demonstrable effect of the interplanetary magnetic field sector boundary crossing (IMF SBC) is found in the lower and middle stratosphere, but there is a demonstrable effect in the middle troposphere at the 500 hPa level. This effect is less important than the IMF SBC effect in the tropospheric vorticity area index and seems to be of a different type.

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auum ¶rt;a nnmua m u mnam a 7 nm ¶rt;au ¶rt; 1000-10 a a¶rt; u(52,5 °.., 13,4 °.¶rt;.) ¶rt; u 1963–1973. ua ¶rt;aam m nu mau nam aum n( ) ¶rt;a amu u u ¶rt; mam, ma m a¶rt; ¶rt; mn a 500 a. mm m a, m u¶rt; na¶rt;u aumu am, u am m ¶rt; muna.