Modelling magnetization processes in single-and multi-domain rock samples using the preisach diagram

Summary The paper presents the results of identifying a model of the Preisach type for haematite grains of the single-domain as well as multi-domain size. Due to the phenomenological conception of the model, the relations between the parameters of the model and actual parameters are very complex, however, impressive accuracy and stability of the modified model indicate the need to resume studies of this problem. The model parameters also confirm the adequate properties of the vibrating-sample magnetometr (VSM) used and developed in our laboratories.     

Radioactive and trace element distribution in basaltic rocks of Lower Silesia

Summary The distribution of radioactive(Th, U, K) and selected trace(Rb, Sr, Ba, Y, Zr, V, Cr, Ni) elements in volcanic rocks from the Opole and Jawor regions of the Lower Silesia has been studied. The behaviour of these elements in the studied rocks indicates that the Lower Silesian volcanic rocks are characterized by less differentiated type than other volcanic rocks of the Bohemian Massif, the Opole rock types probably having a less differentiated character than the Jawor rock types.

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¶rt;a an¶rt;u a¶rt;uamu(Th, U, K) u m ¶rt;u(Rb, Sr, Ba, Y, Zr, V, Cr, Ni) m auu n¶rt;a am n u u uuu. a n mam n¶rt;num, m aum u uuu n¶rt;mam ¶rt; aamuu n¶rt; u ¶rt;uuau, aum u ana¶rt; uu. au a n¶rt;num, m auu n¶rt; amu n ¶rt;uuau ma ua n¶rt; u amu .

     

Expansions of the double product of the global gravity field

Summary Four fundamental forms of expansion of the double product of the gravity function into an infinite series are derived. Two isotropic parts are separated, one is expressed by Legendre polynomials and the other by invariants of Wigner's D-matrices.

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¶rt; m n¶rt;mau ¶rt; au ¶rt; nu¶rt;uaumau uu ¶rt;. ¶rt; ¶rt; umn amu, na aam n nu a¶rt;a u ma n uauam amu ua.

     

Effects of the IMF pro- and anti-sectors in the winter midlatitude ionosphere

Summary On the basis of the 1966–73 data, the effect of the difference between pro- and anti-sectors of the IMF is found to be negligible in the winter midlatitude (Central Europe) ionosphere contrary to the dominant effect of this difference in the high-latitude ionosphere found earlier.

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a ¶rt;a a 1966–73. u¶rt;m u m amu ¶rt; pro- u anti- mau . na a u ¶rt;um (¶rt; na) u, , a naa a, naum um u.

     

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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