On the accuracy of location of local shocks on the territory of Czechoslovakia and adjacent areas

Summary The calculation procedures for determining epicentre parameters of weak near shocks with foci in Poland are discussed and tested for explosions with known epicentres.

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m m¶rt; ¶rt; n¶rt;u num a uu m num nmua n auauu, u mu a mumuu u, n muu ¶rt;au uu mau. au mam nam (a. 4) nu nuuu na 71 u m ¶rt;u n¶rt; ¶rt; a auu ¶rt;a [11].

     

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.     

Earthquake distribution and volcanism in Kamchatka,Kurile Islands,and Hokkaido Part 3: Southern Kuriles and Hokkaido

Summary The morphology of the Wadati-Benioff zone in the region of Southern Kuriles and Hokkaido, based on the distribution of 4015 earthquake foci, verified the existence of an intermediate depth aseismic gap and its relation to active andesitic volcanism. A paleosubduction zone activated by an intermediate depth collision with the active subduction zone was found and described.

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u Wadati-Benioff amu uu - u a¶rt;, aa a an¶rt;uu 4015 a mu, nm¶rt;ua mau n¶rt; au u amu a¶rt;um au. a a¶rt;a u nuaa a na¶rt;uu, amuuuaa nmu mu amu ¶rt;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.     

Motion of particles in turbulent flow: Hyperbolicity,strange attractors and dynamic stochasticity of a system

¶rt;naa, m ma um uu maunuu m am muu ¶rt;uauu um. nua a mau ammama a, n¶rt; mnu ma u u au uu u¶rt;mu.     

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.     

Germanium in Icelandic geothermal systems

Germanium concentrations in geothermal waters in Iceland lie mostly in the range 2–30 ppb. There is an overall positive relation between the germanium content of the water and its temperature. Most of the germanium occurs as Ge(OH)^?₅in solution but Ge(OH)₄ may also be present in significant amounts in saline waters when above 200°C. Evidence indicates that aqueous germanium concentrations are controlled by exchange reactions where it substitutes for silica in silicates and iron in sulphides. It is the rate of dissolution and the relative abundance of the alteration minerals which take up germanium to a variable extent that ultimately fix Ge(OH)₄ concentrations in the water. This, together with water pH, fixes total dissolved germanium. It is mostly the primary rock composition that dictates the relative abundance of the alteration minerals. Conductive cooling in upflow zones favours removal of germanium from solution. During the initial stages of boiling of rising hot water dissolution is enhanced but precipitation at later stages.Thermodynamic data of various aqueous germanium species and several minerals are summarized and dissociation constants and solubilities estimated at elevated temperatures using available predictive methods.