Discontinuous Nature of the Lower Part of the South American Wadati-Benioff Zone in The Arica Elbow Region

The Arica Elbow region represents that part of Andean South America where the azimuth of the strike of the Peru-Chile trench changes from 150° to 190°. The area under study is roughly bounded by latitudes 17 °S and 23 °S, The shape of the Wadati-Benioff zone was studied in terms of the distribution of ISC hypocentres dated between 1964 and 1993. A system of 22 vertical cross-sections, perpendicular to the trench axis, and a map of epicentres was used to derive the detailed shape of the Wadati-Benioff zone of the presently descending slab. The distribution of earthquake foci indicates a fingerlike shape of the lower part of the Wadati-Benioff zone beneath the aseismic gap. The slab length shows small changes around 350 km in the northern sections, pronounced length oscillations between 350 and 750 km in the neighbouring central sections and a constant value of 650 km in the southern sections. The dip and thickness of the Wadati-Benioff zone are practically constant in all sections. Fault plane solutions, separated spatially into three zones, were used to estimate the state of stress in the slab.     

Genetische Probleme der Zinn-Wolfram-Vererzung im Erzgebirge

Zusammenfassung Die Zinnvererzungen im Erzgebirge stehen in engen räumlichen Beziehungen zu den Granitkontakten. Dieses Merkmal wird durch eine strukturelle Rolle der konsolidierten Endokontaktpartien der Granite beim Aufstieg der Erzlösungen erklärt. Die Mineralisationslösungen stammen aus den tieferen Teilen der Erdkruste; die Lagerstätten stehenin einer paragenetischen Stellung zu den Graniten. Die Zinn-Wolfram Mineralisation verlief in mehreren Mineralisationsstadien. In den Quarzgängen konnte eine deutliche innere Gangmetasomatose beobachtet werden, bei der ine ältere Quarzgangfüllung verdrängt wurde. Die symmetrischen Salbänder mancher Mineralien um die Quarzgänge sind durch Verdrängung des Quarzes vom Gangkontakt aus gebildet worden. Die Abschnitte der Quarzgänge mit Feldspäten die den Pegmatiten sehr ähnlich sehen, sind durch Metasomatose nach der Greisenbildung entstanden. Die Granitbildung wurde von extensiven Nebengesteinsumwandlungen begleitet bei der Kalifeldspatbildung (I–II), Albitisierung, Vergreisung, Serizitisierung, Kaolinitisierung, und Hämatitisierung unterschieden werden. Die wichtigsten geologischen und mineralogischen Merkmale der Lagerstätten sind in Tabellen zusammengefaßt.

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The tin-tungsten mineralization in the Kruné hory Mts. /Erzgebirge shows a close spatial association with the granite contacts. This feature is explained by the structural control of solid endocontact part of the granite bodies for the import of postmagmatic solutions. The mineralizing solutions were derived from the deeper parts of the earth's crust, the ore deposits being thus in a paragenetic position to the granites. The tin-tungsten mineralization occurred during an interrupted process of metallization in the course of several stages. In the quartz veins a distinct intravenous metasomatism was observed with the replacement of earlier quartz vein fillings. The symmetrical selvages of some minerals around quartz veins originated by the replacement of quartz from the wall contact. The sections of the quartz veins with felspars resembling very closely the pegmatites were formed by the post-greisen metasomatism of the quartz veins. The emplacement of granites was accompanied by extensive wall- rock alterations of which potash- felspatization (I and II), albitization, greisenization, sericitization, kaolinization and hematitization were distinguished. The main geological and mineralogical features of the deposits are summarized in tables.

     

Optimization of determining the additional constant of an electronic distance meter

Summary The optimization of the method of determining the addition constant of an EDM is discussed. The advantages of the optimization procedure from the point of view of efficiency and improvement of accuracy are reported.

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Longitudinal distribution of PCA sources on the sun

For 181 PCA's recorded during the years 1956–1969 the association with flares is studied. Both the number of events which cannot be associated with any flare on the visible hemisphere, as well as the longitude distribution of identified proton flares, lead to the conclusion that 25–30% of PCA's are caused by flares behind the western solar limb. PCA's of this kind are mostly small. During the investigated years no PCA > 13 dB and possibly no PCA > 8.5 dB were caused by flares behind the limb, while hardly 60% of PCA's < l dB had their origin on the visible hemisphere. While the sources of GLE's and of PCA's in general, are centered around 50°W which corresponds to the average curvature of the magnetic field lines in interplanetary space, the strongest PCA's (> 8.5 dB) show an anomalous longitude distribution centered around ∼ 20°W. It is suggested that this anomaly may be a consequence of the fact that in strong PCA events the kinetic energy density of protons below 100 MeV becomes comparable to the magnetic energy density in space, thus leading to a ‘straightening’ of the magnetic field lines.     

Transequatorial loops interconnecting McMath regions 12472 and 12474

We discuss the life-story of a transequatorial loop system which interconnected the newly born active region McMath 12474 with the old region 12472. The loop system was probably born through reconnection accomplished 1.5 to 5 days after the birth of 12474 and the loops were observed in soft X-rays for at least 1.5 days. Transient sharpenings of the interconnection and a striking brightening of the whole loop system for about 6 hr appear to be caused by magnetic field variations in the region 12474. A flare might have been related to the brightening, but only in an indirect way: the same emerging flux could have triggered the flare and at the same time strengthened the magnetic field at the foot-points of the loops. Electron temperature in the loop system, equal to 2.1 × 10⁶ K in its quiet phase, increased to 3.1 × 10⁶ K during the brightening. Electron density in the loop system was 1.3 × 10⁹ cm^–3 and it could be estimated to 7 × 10⁸ cm^–3 prior to the brightening. During the brightening the loops became twisted. There was no obvious effect whatsoever of the activity in 12474 upon the in erconnected old region. The final decay of the loop system reflected the decay of magnetic field in the region 12474.     

Seismic Moment Tensor Resolution on a Local Scale: Simulated Rockburst and Mine-induced Seismic Events in the Kopanang Gold Mine, South Africa

Seismic records contain information about the effect of the source as well as the effect of wave propagation through the rock mass. The effect of wave propagation is usually not well known as only simplified models of geological structures are available. Therefore, the information about the source retrieved by inverting seismograms may include errors due to incomplete knowledge of the rock mass along the propagation path, which in turn cause a distortion in the calculated moment tensor (MT). The distortion of the MT on a local scale was observed by inverting records of a simulated rockburst conducted at the Kopanang gold mine in South Africa. A dominant isotropic component of the explosive characteristics was found from the inversion. The deviatoric components retrieved from the blast are spurious. A test of their stability indicated that they are not significant, assuming an uncertainty above 5% for velocities and 10% for attenuation within the homogeneous model available for the mine. Thus, the retrieval of the MT from records of local networks in mines using a homogeneous model of the rock mass seems to be feasible. However, the homogeneous model of the rock mass can only be applied to close stations, within a few kilometers of the source. The seismic records from distant stations were too complex to be modelled by a homogeneous rock mass. Records of six mine-induced seismic events recorded at the Kopanang gold mine were also inverted. A vertical linear dipole along the pressure (P) axis was found for three of the events, suggesting a pillar burst. The mechanism of two events contains an isotropic implosion together with a nearly vertical dip-slip, and seems to indicate a combination of a cavity collapse with a down dip-slip along a nearly vertical fault. One event corresponds to a dipole along the tensional (T) axis. However, it is vertical, thus its association with tensile faulting of the hangingwall is uncertain.     

The iron-tungsten-sulphur system and its geological application

The subsolidus region of the Fe-W-S system was studied by experiments performed in evacuated silica tubes. Ternary phases were not encountered. Tungsten disulphide WS₂ is stable with the iron sulphides but not with metallic iron. The major tie-line pyrrhotite-tungsten differentiates this system from the analogous Fe-Mo-S system. Experiments on the Fe-W-O-S system demonstrate that WS₂ (tungstenite) is not stable in the presence of iron oxides. Molybdenum and tungsten show different affinities to sulphur which is manifested in nature in abundant molybdenite as contrasted with rare tungstenite. Sulphur fugacity data in the literature differ on WS₂. There data are compared with the present experimental results.

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Zusammenfassung Das ternäre System Fe-W-S wird durch Abschreckungsexperimente in evakuierten Quarzglasampullen sowie durch Differential-Thermoanalyse untersucht, die Phasengleichgewichtsbeziehungen sind in einem isothermen Digramm T<743 °C veranschaulicht. Unterhalb 743±2 °C liegt der Stabilitätsbereich des Pyrits, FeS₂, welcher mit Tungstenit, WS₂, koexistiert. Konodenscharen erstrecken sich ferner von WS₂ zu Pyrrhotin und zwar über einen weiten Bereich der Fe_1-xS-Mischkristallreihe. Von FeS, oder annähernd stöchiometrischem FeS verlaufen Konoden zum metallischen Wolfram und zu den intermetallischen Phasen Fe₂W und Fe₃W₂. Eine ternäre Phase wurde nicht gefunden. Experimente im ternären sowie im quaternären System Fe-W-O-S demonstrieren, daß WS₂ weder mit metallischem Eisen noch mit Eisenoxiden stabil ist. Molybdän und Wolfram zeichnen sich durch unterschiedliche Affinität zu Schwefel aus, und daraus resultierende Schlußfolgerungen werden in bezug auf natürliche Mineralvergesellschaftungen diskutiert. Die in der einschlägigen Literatur gemachten Angaben über die Schwefelfugazität von Fe, Mo und W werden kritisch untersucht. Dominierende Unterschiede hinsichtlich der Phasengleichgewichtsbeziehungen des Fe-W-S-Diagrammes zu anderen Fe-beinhaltenden Sulfidsystemen, wie Fe-Mo-S, Fe-Sn-S und Fe-Bi-S, werden aufgezeigt.

     

Frequency modified fourier transform and its application to asteroids

Recently a method has been suggested to analyze the chaotic behaviour of a conservative dynamical system by numerical analysis of the fundamental frequencies. Frequencies and amplitudes are determined step by step. As the frequencies are not generally orthogonal, a Gramm-Schmidt orthogonalization is made and for each new frequency the old amplitudes of previously determined frequencies are corrected. For a chaotic trajectory variations of the frequencies and amplitudes determined over different time periods are expected. The change of frequencies in such a calculation is a measure of the chaoticity of the trajectory. While amplitudes are corrected, the frequencies (once determined) are constant. We suggest here simple linear corrections of frequencies for the effect of other close frequencies. The improvement of frequency determination is demonstrated on a model case. This method is applied to the first fifty numbered asteroids.