On the detection of weak strain parallel to the bedding by magnetic anisotropy: A mathematical model study

Summary Five mathematical models of the superposition of deformational magnetic fabric on sedimentary magnetic fabric are presented. These models are represented by various combinations of pure shear and simple shear. The diagrams of the variations in the main magnetic anisotropy parameters with strain can help in recognizing weak ductile deformation in sedimentary rocks.

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Реэюме Пруво?rt;umся nяmь мamемamuческuх мо?rt;елеŭ суnерnозuцuu ?rt;еформaцuонноŭ мa?rt;нumноŭ mексmуры на осa?rt;очноŭ мa?rt;нumноŭ mексmуре. Мо?rt;елu ире?rt;сmвaлены в рaзных комбuнaцuях чuсmо?rt;о с?rt;вu?rt;а ц иросmо?rt;о с?rt;вu?rt;а. Дua?rt;раaммы вaрuaцuŭ в ?rt;лaвных naрaмеmрaх мa?rt;нumноŭ aнuзоmроnuu с ?rt;еформaцuеŭ мо?rt;уm nомочь nрu рaсnознaвaнuu слaбых nлaсmuчных ?rt;еформaцŭŭ в осa?rt;очных nоро?rt;aх.

     

Classification of landslides and other mass movements

Summary This paper presents a new universal classification of slope movements, destined for the purpose of engineering geological mapping. This classification was compiled after critical evaluation of the classifications used by now, on the basis of the experience gained by systematic study of slope movements in Czechoslovakia.The following 4 types of slope processes are recognized regarding to the geomechanical character and velocity of the movement: creep, sliding, flow and fall. Creep is a geologically long-term movement of non-increasing velocity without well-defined sliding surfaces. Sliding is a slope movement of coherent masses along one or more well-defined shear surfaces. Flow represents slope movements in rocks and soils, analogous to the movements in liquids. Fall is a sudden slope movement; the moving mass loses its coherence and, for a short time, also its contact with the underlying rock.The pictures show the elementary types of movements that are obvious in the European climatic conditions. Graphical representation of dimensions and velocity of the phenomena is included.

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Zusammenfassung Die vorgeschlagene Klassifikation geht zurück auf systematische Untersuchungen an Rutschgebieten in der SSR. Sie lehnt sich an die besten gebräuchlichen Klassifikationen an, wobei letztere einer kritischen Beurteilung unterzogen werden. Ziel des neuen Vorschlages ist die Erarbeitung von Kriterien für die ingenieurgeologische Kartierung.Auf Grund des geomechanischen Charakters der Bodenbewegungen werden folgende vier Vorgänge unterschieden: Kriechen — geologisch langandauernde, nicht beschleunigte Bewegungen ohne ausgeprägte Gleitflächen; Gleiten — Hangbewegungen zusammenhängender Massen längs einer oder mehrerer Gleitflächen; Fließen — Hangbewegungen von flüssigkeitsähnlichem Charakter; Fallen — plötzliche Hangbewegungen, wobei die bewegte Masse den inneren Zusammenhang und kurzfristig auch den Kontakt mit dem Liegenden verliert.Die Grundtypen werden an Hand europäischer Beispiele graphisch dargestellt und durch Angaben über Größenordnung der Massen und deren durchschnittliche Geschwindigkeit ergänzt.

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Résumé D'après les expériences acquises pendant les études de glissements en Tchécoslovaquie et d'après l'examen critique des classifications employées jusqu'ici, on a recommendé la classification suivante, destinée avant tout au levé de géologie de l'ingénieur.En relation avec le caractère géomécanique des mouvements de pente et de leur vitesse, quatre processus sont distingués: fluage, glissement, écoulement, écroulement. Le fluage — mouvements géologiquement de longue durée, sans accélération et sans surfaces de glissement exprimées. Le glissement — mouvements de pente de masses cohérentes, le long d'une ou de plusieurs surfaces de glissement. L'écoulement — mouvements de pente dans les roches et les sols, analogues aux mouvements dans les liquides. L'écroulement — mouvements de pente soudains, au cours desquelles les masses en mouvement perdent entièrement leur connexion intérieure et, pour un temps aussi, le contact avec le sous-sol.Les exemples sur les figures représentent les types principaux des mouvements courants dans les conditions climatiques de l'Europe. On indique aussi les dimensions et la vitesse moyenne des types individuels.

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With 4 Figures     

Hazard distribution and risk assessment in the network systems

In the age when transport flows in the railway and road systems, information flows in the internet channels, etc. intensify, hazard distribution in the network systems becomes a more relevant and important issue. In the paper various theoretical hazard type distributions in the network systems are analysed. Conditions and assumptions that hazard in the network system cells would settle and became steady are defined. Cases are analysed, when hazard is initiated in one or several network nodes, while in other nodes hazard is decreased, i.e. they have immunity to the hazard. In all cases hazard distribution equilibrium equations are constructed and their solutions‘ existence conditions are defined. Theoretical results are illustrated by simulation of hazard fuel transportation in the Lithuanian roads. It is shown that using this methodology it is possible to construct an algorithm, which enables to operate and decrease fuel transportation hazard and risk. The novelty of the work is associated with employing Markov process to describe hazard distribution mechanism and to determine limited hazard distribution in the nodes of networks. The hazard of tank trucks in the network of Lithuanian roads has been assessed for the first time.     

Gravity potential of the normal body in the outer and inner space

Summary The level rotational ellipsoid, best fitting the actual Earth, rotating with the same angular velocity around a common axis of rotation, is assumed to be a mathematical model of the real Earth. The gravity potential of this body and its derivatives in the outer space are derived by means of the generalized Pizzetti method[1]. For some analyses of the structure of the Earth we need to know the gravity anomaly and thus the gravity potential and its derivatives inside the mathematical model. These values are not defined in the classical conception. In this paper, the normal potential and its derivatives in the inner space are derived up to a certain depth, which is still of significance for gravimetric research.Dedicated to RNDr Jan Pícha, CSc., on his 60th Birthday     

Cs137 gamma-ray absorption in eclogites

Summary The coefficient of the gamma-ray absorption _Cs ¹³⁷ investigated in eclogites of the Bohemian Massif varies with fresh samples from0.2477 cm ^–1 to 0.2804 cm ^–1 . Symplectite is the main factor decreasing the value of down to0.242 cm ^–1 . On the contrary, the coefficient increases with the increasing content of clinopyroxene and especially of garnet. The linear dependence of the coefficient on the density may be expressed by the equation =0.0682+0.028.     

Sur le magmatisme et les minéralisations hydrothermales du Massif de Bohême

Résumé Après un bref aperçu sur les types intrusifs de roches plutoniques, sont décrits les divers types d'associations min7'erales isogénétiques d'origine hydrothermale du Massif de bohême, sur le territoire de la Tchécoslovaquie. L'étude de la répartition spatiale de certaines associations minérales conduit à la différenciation de 2 zones et de 7 sous-provinces, dans la province du Massif de Bohême. Du point de vue chronologique, trois époques de minéralisation sont distinguées: antéhercynienne, hercynienne et posthercynienne, qui comportent plusieurs sous-époques distinctes de minéralisation. En conclusion, une distinction est faite entre: 1°) des associations hydrothermales montrant des relations chronologiques et spatiales nettes avec des granitoïdes voisins; 2°) des associations ne montrant que des relations spatiales; 3°) des associations, les plus nombreuses, qui sont sans aucun rapport évident avec les massifs connus de granitoïdes.

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After a brief survey of intrusive types of plutonic rocks, the present paper contains a review of isogenetic mineral associations of hydrothermal origin occurring in the Bohemian Massif in the territory of Czechoslovakia; further, the distribution of some mineral associations is discussed; the result is the differentiation of 2 zones and 7 subprovinces of the province of the Bohemian Massif. From the chronological point of view three epochs can be distinguished: pre-Variscan, Variscan and post-Variscan which include marked mineralisation subepochs. In conclusion the authors discern: 1°) hydrothermal associations showing spatial and chronological relations to the surrounding granitoids; 2°) associations displaying spatial relations only; 3°) those — the most numerous — which do not show any distinct relations to the known massifs of granitoids.

     

Testing for nonlinearity in European climatic time series by the method of surrogate data

Summary Using temperature and pressure records from Czech meteorological stations and NCEP/NCAR reanalysis series, we tested for the presence of detectable nonlinearity in univariate and multivariate climatic time series. The method of surrogate data was utilized for nonlinearity detection – results of nonlinear prediction for the original series were compared to the results for series whose nonlinear structure was randomized. The prediction was done by means of local linear models in the reconstructed phase space. None or very weak nonlinearity was found in the single (univariate) series, and pressure series generally exhibited stronger nonlinearity than series of temperature (daily mean, minimum or maximum). Distinct nonlinearity was found in all tested multivariate systems, especially when both temperatures and pressures were used simultaneously to form the phase space. Nonlinearity tests were carried out for 30-year and 10-year-long datasets and nonlinear behavior was generally more apparent in the longer versions. In addition, the tested systems showed more substantial nonlinearity when the success of short-range prediction was used as the discriminating statistic; with an increase of the prediction time, detectable nonlinearity became weaker and it disappeared completely for long-term prediction.     

Solar Activity Effects on Gravity Wave Activity Inferred from Radio Wave Absorption in the Lower Ionosphere

The low frequency (LF) nighttime radio-wave absorption in the lower ionosphere has been measured at Prhonice (50°N, 15°E) in central Europe for over 35 years. Digital measurements, performed since summer 1988, allow absorption oscillations in the period range 10 – 180 mins, which are believed to reflect gravity wave activity, to be derived. Unfortunately, problems with the transmitter in recent years terminated the evaluation of gravity wave activity. The analysis of the available information (6 years of data) allows two conclusions to be drawn as to the effects of the solar activity on gravity wave activity: (1) there is no detectable effect of the solar 27-day variation on gravity wave activity; (2) there is an indication that the positive effect of the 11-year solar cycle on gravity wave activity in the winter half of the year is remarkable (lack of data in summer). The result concerning the solar cycle effect is, to a certain extent, preliminary, because the available data do not cover a complete solar cycle. A comparison with results from other stations and an interpretation of results are presented.     

Long-period fluctuations observed in the ionospheric absorption variations

Summary By subsequent application of power spectrum analysis, autocorrelation analysis and fast Fourier transform (FFT) of the day- and night-time absorption values of five LF radio-paths (164 kHz, 155 kHz, 185 kHz, 218 kHz and 272 kHz) in Europe during the interval 1 June 1979–30 June 1980, fluctuations with the following basic (fundamental), commonly recurrent periods were found: 3.5–5 days and 10.5–12 days. They exist in all investigated time series, while 6- and 9-day fluctuations are observed on the northern radio-paths (185 kHz and 272 kHz). Shorterperiod oscillations are most active during autumn and especially during winter, while the longerperiod oscillation (10.5–12-day) has significant amplitudes also in summer.

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n n¶rt;am nuu aaua nma mu, amu aaua u m maauu () ¶rt; u ¶rt;a n nu u nmu a¶rt;u ma (164 , 155 , 185 , 218 u 272 ) a¶rt; n nu¶rt; 1 u 1979–30 u 1980. u a¶rt; ¶rt;u (¶rt;ama) nmu nu¶rt;: 3.5–5 ¶rt; u 10.5–12 ¶rt. u nummm u¶rt;a ¶rt;a. 6- u 9-m au a¶rt;am m a¶rt;umaa (185 u 272 ). ama au a amu u u u. ¶rt;nu¶rt; (10.5–12 ¶rt;) um aum anum¶rt; u m.