A high resolving power ion selector for post-source decay measurements in a reflecting time-of-flight mass spectrometer

An electrostatic deflector has been designed and constructed that can be used in a reflecting time-of-flight mass spectrometer for either single-deflector or dual-deflector velocity selection in post-source decay measurements. The deflector consists of an interleaved set of parallel deflection electrodes as in a Loeb/Cravath/Bradbury device, but thin metal ribbon instead of wire is used for the deflection electrodes. The time for reversing the electric field, which depends on various factors such as the electronics for pulsing the voltage and the time constant of a particular electrode geometry, is about 19 ns for the deflectors used in this study. By properly timing the reversal of the electric field, the time-window for ion transmission can be made substantially less than the switching time of each individual deflector. In conjunction with matrix-assisted laser desorption/ionization, the single-deflector's resolving power and transmission are robust with respect to laser fluence, i.e. they remain high even when the fluence is raised well above threshold. By contrast the operational features of the dual-deflector gate offer more versatility in locating and sizing the selection window. Operating the ion selector in a single-deflector mode, we have achieved a resolving power of approximately 710 full width at half maximum (FWHM) for different isotopes of protonated, sodiated, and potassiated substance-P (m/z 1348.6, 1370.6 and 1386.6 respectively; 10.073 keV). Operating it in the dual-deflector mode under two different sets of conditions, we have succeeded in obtaining resolving powers of approximately 1100 (FWHM) for protonated substance-P (m/z 1348.6; 10.8 keV) and approximately 5200 (FWHM) for an isotopomer of PEG 6000 (approximately m/z 6000; 10.04 keV). This accomplishment implies that high-resolution ion selection can be coupled to post-source decay analyses.     

Effects of oily contamination and decontamination on the flame resistance of thermal protective textiles

This paper reports an experimental study wherein flame resistance and limiting oxygen index of protective fabrics were determined before and after contamination with oil and after decontamination. Experimental variables were presence of contamination, laundry treatment, number of contamination/decontamination cycles, and fabric type. Although laundering with pre‐wash products alone was the most effective in removing oil, some product residues may have contributed to the increased flammability of some fabrics. Thus, use of that product was truly effective only if combined with detergent. For two fabrics higher flammability was noted after five contamination/decontamination cycles than after one. Of the three fabrics studied, aramid specimens retained the least oil, and although they had the highest flammability both before and after contamination, it increased the least with contamination. The FR cotton/nylon fabric retained the most oil after decontamination, but had better flame resistance than aramid. Much of the oil remained in the interior of cotton fibres making it difficult to remove but also less accessible for vaporization and combustion. For the aramid/FR viscose, energy from combustion of residual oil activated the FR additive, thereby reducing apparent fabric flammability, but this FR transference effect occurred only up to an optimum quantity of oil. Copyright © 2010 John Wiley & Sons, Ltd.     

Photon diffusion in a homogeneous medium bounded externally or internally by an infinitely long circular cylindrical applicator. II. Quantitative examinations of the steady-state theory

This is Part II of the work that examines photon diffusion in a homogenous medium enclosed by a concave circular cylindrical applicator or enclosing a convex circular cylindrical applicator. Part I of this work [J. Opt. Soc. Am. A 27, 648 (2010)] analytically examined the steady-state photon diffusion between a source and a detector for two specific cases: (1) the detector is placed only azimuthally with respect to the source, and (2) the detector is placed only longitudinally with respect to the source, in the infinitely long concave and convex applicator geometries. For the first case, it was predicted that the decay rate of photon fluence would become smaller in the concave geometry and greater in the convex geometry than that in the semi-infinite geometry for the same source-detector distance. For the second case, it was projected that the decay rate of photon fluence would be greater in the concave geometry and smaller in the convex geometry than that in the semi-infinite geometry for the same source-detector distance. This Part II of the work quantitatively examines these predictions from Part I through several approaches, including (a) the finite-element method, (b) the Monte Carlo simulation, and (c) experimental measurement. Despite that the quantitative examinations have to be conducted for finite cylinder applicators with large length-to-radius ratio to approximate the infinite-length condition modeled in Part I, the results obtained by these quantitative methods for two concave and three convex applicator dimensions validated the qualitative trend predicted by Part I and verified the quantitative accuracy of the analytic treatment of Part I in the diffusion regime of the measurement, at a given set of absorption and reduced scattering coefficients of the medium.     

Influence of heat and pH on structure and conformation of whey proteins

The aim of this study was to understand the fundamental interactions responsible for aggregation of whey proteins (WPs) at pH 6 and 3 during heating at 140 °C for 30 s in the presence of different acidulants. The conformational changes in the various heat-treated WP dispersions were studied using chemical bond blockers and analysed using differential scanning calorimeter thermograms, polyacrylamide gel electrophoresis and turbidity measurements. Overall, the results indicated that WPs were denatured mainly by disruption of hydrophobic interactions, and that the extent of WP denaturation at pH 3 was affected by the type of acidulant used. The type of acidulant affected the extent of formation of additional high or medium molecular weight aggregates during heating at pH 3, while the types of interactions involved in the formation of such aggregates were affected by the pH at heating.