A numerically calibrated reference level (MP28) for the terrestrial mammal-based biozonation of the European Upper Oligocene

The fauna of the Enspel (Westerwald) and the neighbouring Kärlich (Neuwied basin) fossil deposits correspond to the Upper Oligocene Mammal Paleogene (MP) reference level 28 and 28–30, respectively. Basaltic flows and a trachyte tuff terminating and predating the fossil deposit sedimentation allow to numerically calibrate the MP reference levels by radioisotope dating. Laser fusion ⁴⁰Ar/³⁹Ar step heating on volcanic feldspars yield a time interval of 24.9–24.5 Ma for reference level MP28 at Enspel and a maximum age of 25.5 Ma for the time interval MP28–MP30 at Kärlich. Interpolation between the time intervals determined for the Enspel reference level MP28 and the age of the global Oligocene/Miocene boundary of 24.0 ± 0.1 Ma taken from literature results in time intervals of 24.5–24.2 Ma and 24.2–23.9 Ma for the younger reference levels MP29 and MP30, respectively. These intervals of ≤ 0.4 m.y. for MP reference levels of the latest Oligocene are short relative to older Oligocene MP reference levels 21–27 between 34 and 25 Ma. Since subdivision into MP reference levels essentially is based on assemblages of mammal taxa and on evolutionary changes in tooth morphology of mammals short MP time intervals during the latest Oligocene indicate a rapid evolutionary change relative to the early Oligocene.     

Equilibrium and disequilibrium degassing of a phonolitic melt (Vesuvius AD 79 “white pumice”) simulated by decompression experiments

Equilibrium and disequilibrium degassing of a volatile phase from a magma of K-phonolitic composition was investigated to assess its behavior upon ascent. Decompression experiments were conducted in Ar-pressurized externally heated pressure vessels at superliquidus temperature (1050 °C), in the pressure range 10–200 MPa using pure water as fluid phase. All experiments were equilibrated at 200 MPa and then decompressed to lower pressures with rates varying from 0.0028 to 4.8 MPa/s. Isobaric saturation experiments were performed at the same temperature and at 900–950 °C to determine the equilibrium water solubility in the pressure range 30–250 MPa. The glasses obtained from decompression experiments were analyzed for their dissolved water content, vesicularity and bubble size distribution. All decompressed samples presented a first event of bubble nucleation at the capsule–melt interface. Homogeneous bubble nucleation in the melt only occurred in fast-decompressed experiments (4.8 and 1.7 MPa/s), for ΔP ≅ 100 MPa. For these decompression rates high water over-saturations were maintained until a rapid exsolution was triggered at ΔP > 150 MPa. For slower rates (0.0028, 0.024, 0.17 MPa/s) the degassing of the melt took place by diffusive growth of the bubbles nucleating at the capsule–melt interface. This process sensibly reduced water over-saturation in the melt, preventing homogeneous nucleation to occur. For decompression rates of 0.024 and 0.17 MPa/s low water over-saturations were attained in the melt, gradually declining toward equilibrium concentrations at low pressures. A near-equilibrium degassing path was observed for a decompression rate of 0.0028 MPa/s. Experimental data combined with natural pumice textures suggest that both homogeneous and heterogeneous bubble nucleations occurred in the phonolitic magma during the AD 79 Vesuvius plinian event. Homogeneous bubble nucleation probably occurred at a depth of ∼ 3 km, in response to a fast decompression of the magma during the ascent.     

Phosphorus oxynitride PON, a silica analogue: structure and compression of the cristobalite-like phase; P –T phase diagram

 The structure of the cristobalite-like polymorph of phosphorus oxynitride PON has been refined using neutron powder diffraction data. It is tetragonal, space group I&4macr;2d, Z=4. The four P–(O,N) distances are equal but the tetrahedron is compressed along c. In AX₂ or ABX₄ compounds, the tetragonal I&4macr;2d or I&4macr; structure is obtained when the average ratio of the cation to anion radius is below 1.186, whereas the tetragonal P4₁2₁2 or orthorhombic C222₁ structure is obtained at low temperatures for larger ratios. The cell parameters of this PON polymorph have been determined as a function of hydrostatic pressure by in situ angle dispersive X-ray powder diffraction in a diamond-anvil cell. Under truly hydrostatic pressure, a strong anisotropic behavior is observed with the c parameter being nearly incompressible. Very slight anisotropic stress strongly modifies the high-pressure behavior. According to the pressure-temperature conditions of treatment, three phases, cristobalite-, moganite-, and quartz-like, have been obtained by quenching experiments, and the P–T phase diagram of PON was derived. The high-pressure behavior of the α-quartz, moganite, and cristobalite-like polymorphs of PON and SiO₂ is discussed. Received: 7 August 2000 / Accepted: 21 January 2001     

A novel ozone sensor for direct eddy flux measurements

A small, lightweight (1.5 kg) and fast-response ozone sensor for direct eddy flux measurements has been built. The basis for detection is the chemiluminescence of an organic dye adsorbed on dry silica gel in the reaction with ozone. The chemiluminescence is monitored with a cheap and small blue-sensitive photomultiplier. At a flow rate of 100 l min^-1 the ozone sensor has a 90% response time of significantly better than 0.1 s with a detection limit lower than 50 ppt at S/N=3. There are no interferences from other atmospheric trace gases like NO_x, H₂O₂ and PAN. Water vapour and SO₂ enhance the chemiluminescence efficiency of the ozone sensor. Since their response times are 22 seconds and 30 minutes, respectively, no correlation between rapid ozone fluctuations and those of these two trace gases is noticed by the ozone sensor when operating at a frequency of 10 Hz.The ozone sensor was tested for several weeks in continuous measurements of ozone fluxes and deposition velocities over different croplands using the eddy correlation technique. Good agreement was found between ozone dry deposition velocities derived from profile measurements and by eddy correlation.     

Zur Baugeschichte der Ardennen I

Zusammenfassung Die bereits kaledonisch gefalteten Massive in den Ardennen wurden von der variscisdien Tektogenese (asturische Phase) mehr oder weniger überprägt. Vorstellungen über diese Überprägung älterer Strukturen und deren Vergitterung mit jüngeren Verformungsrichtungen sowie über den Einfluß der kaledonischen Kerne (Unterstockwerk) auf das Faltenstreichen der devonischen Mantel-Schichten (Oberstockwerk) lassen sich vor allem in der Antiklinalzone der Hochardennen im Massiv von Rocroi, im Massiv von Serpont und im Massiv von Stavelot gewinnen.

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Résumé Les massifs des Ardennes, déjà plissés à l'ère caledonienne furent plus ou moins remaniés par la tectogénèse hercynienne (phase asturienne). C'est surtout dans la zone anticlinale des hautes Ardennes, dans le massif de Rocroi, dans le massif de Serpont et dans le massif de Stavelot qu'on peut se faire une idée en bons affleurements de ce remaniement de structures plus anciennes et de leurs interférences avec des directions de déformation plus jeunes ainsi que de l'influence des anciens massifs calédoniens (étage inférieur) sur la direction du plissement des couches de revêtement dévoniennes (étage supérieur).Dans ces massifs, les couches du dévonien sont plus ou moins fortement plissés ou disposés par écailles avec le socle calédonien. Dans le massif de Rocroi, dans le massif de Serpont et dans la partie ouest du massif des Stavelot les couches du socle présentent des structures qui sont totalement différentes des couches de revêtement dévoniennes et coupé de façon discordante des couches gedinniennes inférieures.Dans le massif de Rocroi et surtout dans le massif de Serpont, la tectogénèse hercynienne a exercé le même effet que l'orogénèse calédonienne plus ancienne sous l'influence d'un plan d'efforts semblable orienté Nord-Sud. L'auteur, à l'aide d'un exemple, celui du massif de Serpont, essaye d'analyser la structure du plissement calédonien originel déroulement des plis des couches gedinniennes et reformation constructive de la déformation conditionnée par le clivage hercynien.A la différence des deux massifs occidentaux, dans le massif de Stavelot, les structures de plissement calédoniens orientées d'est en ouest furent remaniées sous angle oblique par la tectogénèse hercynienne. Ce mouvement a entraîné, à différents endroits, le déplacement des axes calédoniens en direction hercynienne. C'est ce qui a produit un style de mouvement et de structure étranger aux autres massifs. Le fort rétrécissement hercynien eut pour conséquence des charriages à différents endroits.

     

Zur Deckentektonik des Hochbalkans

Zusammenfassung Im Botewgebiet der Stara Planina (Hochbalkan) liegt inmitten paläozoischer, mesozoischer und tertiärer Schichten ein 30 km langer und 12 km breiter Granitkomplex, der als autochthone Einheit, aber auch als Deckscholle gedeutet worden ist. Die Deckennatur des Komplexes wird durch die großtektonischen Verhältnisse eindeutig belegt. Der Bewegungsplan besitzt meridionale Symmetrie, die tektonischen Haupttransporte erfolgten von S nach N. Groß- und Kleingefüge entsprechen einander. Das Liegende der Decke besitzt keine einheitliche Prägung. Diskordante Lagerungsverhältnisse lassen variszische, kimmerische, kretazische, laramische und pyrenäische Bewegungen erkennen.     

A meteorological 80-m tower near Rotterdam

Construction, observation site and instrumentation are described of an 80-m meteorological observation tower, erected in Vlaardingen, The Netherlands, for studies in connection with air pollution problems along the Nieuwe Waterweg. From measurements made regularly in the period April 1967–April 1968 summaries are given of wind profile parameters and gustiness averages. Case histories are presented of an air pollution episode lasting several days, and of an hourly average wind direction difference of 120 ° over 70 m.