Bedform migration and bed-load transport in some rivers and tidal environments

Reliable field data obtained by directly measuring bed-load transport of fine- to coarse-grained bed material are extremely scarce, mainly because of the difficulty of sampling accurately. Therefore, the verification of bed-load transport formulae is largely based on flume experiments, which refer to unrealistic shallow-water conditions. In this study, some bed-load transport formulae were tested against data from natural environments. As an alternative to ascertaining the bed-load transport rate by sampling the bed-load, the transport rate was deduced from data on bedform height and bedform celerity. For this purpose, 43 sets of data from rivers, representing a wide range of bed material, bedform dimensions and hydraulic conditions were collected as were some sets of data from tidal settings. Two formulae were used for the prediction of the bed-load transport: the formula of Van Rijn (1981) and the Kalinske (1947) formula as approximated by Elzerman & Frijlink (1951) (and, in the present study, slightly modified for application to tidal waters). Both the bed-load function of Van Rijn and the modified formula of Kalinske-Frijlink require data which are easily obtained and that can be measured accurately. At those stages of the flow when bed-load transport was high the Van Rijn function tended to overestimate that transport. For flow stages when bed-load transport was low the opposite was true. The modified Kalinske-Frijlink function gave consistently good results: 86% of the transport rates predicted using the river data were within 0·5–2·0 times the values actually measured.     

THERMAL NEAR-SURFACE EXPRESSION OF SHALLOW GEOLOGICAL FEATURES*

It has been customary in geothermal studies to assume the surface to be an isothermal plane, though difficulties existed to explain the magnitude of thermal anomalies observed in the field under this assumption. Detailed investigations of temperatures at depths between 5 cm and 230 cm show that—after removal of the strong diurnal variations—sizeable anomalies persist right to the surface. Thus, the effective heat transfer (coefficient) at the surface might be lower than commonly assumed.     

INFLUENCE OF AMPLITUDE AND PHASE ERRORS ON MIGRATION RESULTS*

Random amplitude and phase errors in seismic input data introduce a coherent distribution of migration half-circles or “smiles”, the occurrence of which may cause a significant decrease of signal-to-noise ratio. In addition, the effect of quantization errors is discussed for different wordlengths, used both during acquisition and during data processing. Results of sign-bit recordings are shown.     

Microbiota of Salt Lakes as Food for the Brine Shrimp Artemia

正The brine shrimp Artemia is often abundantly found in hypersaline environments.The larvae(‘nauplii’)hatching from its dormant embryos(‘cysts’)are a crucial live food item for the larval stages of fish and shrimp in aquaculture     

Post-collision, Shoshonitic Volcanism on the Tibetan Plateau: Implications for Convective Thinning of the Lithosphere and the Source of Ocean Island Basalts

Potassic volcanism has been widespread and semi-continuous onthe Tibetan plateau since 13 Ma, post-dating the orogenic thickeningof the India-Asia collision. Volcanism may have commenced slightlyearlier (16–20 Ma) in the southern portion of the plateauand then ceased around 10 Ma. The dominant lavas are pyroxen-and plagioclase-phyric shoshonites with subordinate occurrencesof dacites and rhyolites. Their mineralogy reflects crystallizationfrom high-temperature (1100C) magmas which had elevated oxygenand water fugacities. Geochemically, they are characterizedby relatively low TiO², Al²O³ and Fe²O³, and high Na²O, coupledwith variable abundances of compatible trace elements and veryhigh contents of incompatible trace elements. Normalized incompatibleelement patterns have marked negative Nb, Ta and Ti anomalieswhereas K²O appears to be buffered at 4% over a wide range ofSiO². Isotope data show a relatively broad and enriched rangeof ⁸⁷Sr/⁸⁶ Sr (0.7076–0.7106) at more restricted ENd (–5.2to –8.1). Pb isotopes are characterized by a range of²⁰⁷Pb/²⁰⁴ Pb (15.51–15.72) and ²⁰⁸ Pb/²⁰⁴Pb (38.67–39.30) at very uniform ²⁰⁶Pb/²⁰⁴ Pb (18.39–18.83), leadingto vertical arrays. Volcanics from the southern parts of theplateau have more primitive isotopic compositions: ⁸⁷Sr/⁸⁶ Sr0.7048–0.7080, _Nd 1.4 to –3.3, ²⁰⁶Pb/²⁰⁴ Pb 18.48–18.67,²⁰⁷Pb/²⁰⁴ Pb 15.59–15.68 and ²⁰⁸Pb/²⁰⁴ Pb 38. 73–38.98. In general, the geochemical and isotopic data most closely approximatepartial melting arrays, although fractionation processes haveclearly operated. The isotopic ratios and the enrichment ofincompatible elements and LREE/HREE cannot be derived from adepleted mantle source via a single-stage melting process. Instead,a metasomatized, garnet peridotite source containing 6% phlogopiteis required and this is inferred to lie within the lithosphericmantle. The enrichment in incompatible elements in this sourcemust have been sufficiently ancient to generate the observedisotopic ratios, and Nd depleted mantle model ages suggest thiswas Proterozoic in age (1.2 Ga), whereas Pb model ages recordan Archaean event, suggesting the source had a multi-stage enrichmenthistory. The negative Ta, Nb and Ti anomalies and low Rb/Basuggest that metasomatism may have occurred during an ancientsubduction episode. The high ²⁰⁸Pb/²⁰⁴Pb, ²⁰⁷Pb/²⁰⁴ Pb and lowNb/U, Ce/Pb of the Tibetan shoshonites are distinct from oceanisland basalts. Thus, if convectively removed lithospheric mantleprovides a source for ocean island basalts, it must differ significantlyfrom the source of the Tibetan shoshonites. A lithospheric mantle source for the volcanism places importantconstraints on geodynamic models for the evolution of the Tibetanplateau and the India-Asia collision. For likely thermal structuresbeneath the plateau, the temperatures required to trigger meltingwithin the lithospheric mantle can only be plausibly obtainedif the lower parts of the lithospheric mantle were removed byconvective thinning. This is consistent with recent models whichinvoke the same process to explain the current elevation andextensional deformation of the plateau. The age data suggestthis occurred at 13 Ma and the duration of volcanism may beexplained by continued conductive heating since that time. Poorlysampled but slightly older volcanics from the southern portionsof the plateau may indicate that convective thinning began inthe south and migrated northwards. Rapid uplift of the plateaumay have resulted in increased rates of chemical weathering,which led to global cooling, as indicated by oxygen isotopedata from Atlantic sediments. KEY WORDS: Climate; lithospheric mantle; OIB; Tibet; volcanism ^*Corresponding author.     

Siliceous Cementation of Chlorite-Coated Grains in the Permian Sandstone Gas Reservoirs, Ordos Basin

<正>Objective It has long been controversial that whether authigenic chlorite coatings in sandstone reservoirs can prevent precipitation of siliceous cements.It is commonly believed that chlorite coatings(also called chlorite films,chlorite linings,or chlorite rims)may prevent quartz overgrowth,and thus help the preservation of original pores in sandstone reservoirs.Recently,however,this assumption has been challenged by reservoir geologists.This dispute cannot be solved by mere analysis of thin sections,nor by chemical equations and diagenesis analysis.The main objective of the present contribution is to shed light on this     

Accurate Determination of Gallium in South African Primary and Secondary Reference Samples by Ion Exchange Chromatography and Atomic Absorption Spectrometry

Results are presented for gallium in six South African primary rock standards (NIMROCS) and in twelve secondary rock standards (SAROCS). A selective ion exchange procedure is used to separate gallium completely from all other elements, except remaining traces of thorium. It is followed by a determination of gallium with flame atomic absorption spectrometry using the nitrous oxide-acetylene flame, after the addition of 2000 ppm lanthanum as ionization suppressor.