Combined use of atomic spectrometric methods in the analysis of rocks

Standard reference materials of limestone, granite and argillite were analyzed by X-ray fluorescence spectrometry (XFS), flame and graphite furnace atomic absorption spectrometry (F-AAS and G-AAS), and inductively coupled plasma atomic emission spectrometry (ICP-AES). The major elements Al, Ca, Fe, Si and Ti were determined by XFS and ICP-AES. The relative standard deviations (RSD) of the concentrations of the corresponding oxides obtained by XFS and ICP-AES were (1.36±0.51)% (n=18) and (1.30±0.70)% (n=17), respectively, on the average. The relative deviations (RD) from the certified values were (1.29±3.01)% (n=18) and (–0.69±5.48)% (n=14), respectively, on the average. The numbers in parentheses are the numbers of the single RSD- and RD-values used for the calculation of the averages and the relative standard deviations. Some minor and trace elements of the standard reference materials were determined by G-AAS and ICP-AES. The precision (RSD) was markedly better in the case of ICP-AES. On the other hand, the accuracy (RD) of both methods was about the same (7%). Apparently, the precision and the accuracy are primarily determined by the measuring technique and the sample pretreatment procedure, respectively. The analytical power of the combined use of atomic spectrometric methods is also discussed.     

NMR investigation of guest–host complex between chloroform and cryptophane C

Guest–host complex between cryptophane C, possessing two non‐equivalent caps, and chloroform is investigated by NMR spectroscopy. The kinetics of the chloroform exchange between the bound and free sites is determined by ¹H exchange spectroscopy. Moreover, the preferential orientation of chloroform molecule with respect to the cryptophane C frame is examined by the NOESY and ROESY experiments. The experimental findings are compared to the results of quantum chemical calculations. Copyright © 2010 John Wiley & Sons, Ltd.     

Single enantiomer, chiral donor-acceptor metal complexes from bisoxazoline pseudoracemates

[structure: see text] Single enantiomer, chiral donor-acceptor metal complexes were synthesized via the self-discriminating zinc(II) complexation of a pseudoracemic mixture of donor/acceptor-substituted bisoxazoline derivatives.     

Differential non-destructive image current detection in a fourier transform quadrupole ion trap

Dual-detector differential non-destructive Fourier transform detection in a quadrupole ion trap is shown to improve signal intensity and reduce noise compared with spectra recorded using a single detector. A larger area detector in each end-cap electrode is machined to fit its hyperbolic shape and so minimize field imperfections on the z-axis. Argon, acetophenone and bromobenzene spectra were recorded to allow a comparison between single- and dual-detector (differential) modes of detection and to demonstrate the improvement achieved with differential detection. Copyright 1999 John Wiley & Sons, Ltd.     

Controlling mode selectivity in palladium-catalyzed bisdiene carbocyclizations: optimizing for cyclization-trapping over cycloisomerization

[reaction: see text] Screening combinations of five catalyst precursors with 13 phosphorus ligands identified cyclization catalysts that favor carbocyclization-trapping with N-hydroxyphthalimide over a competing cycloisomerization mode.     

Pseudo-steady-state solutions for solidification in a wedge

Polubarinova-Kochina's analytical differential equation methodis used to determine the pseudo-steady-state solution to problemsinvolving the freezing (solidification) of wedges of liquidwhich are initially at their fusion temperature. In particular,we consider four distinct problems for wedges which are: freezingwith the same constant boundary temperature, freezing with thesame constant boundary heat fluxes, freezing with distinct constantboundary temperatures and freezing with distinct constant fluxesat the boundaries. For the last two problems, a Heun's differentialequation with an unknown singularity is derived, which in bothcases admits a particularly elegant simple solution for thespecial case when the wedge angle is . The moving boundariesobtained are shown pictorially.