Stroboskopisehe Untersuchungen über den zeitlichen Aufbau,die optische Absorption und das Nachleuchten gesteuerter Funkenentladungen

Zusammenfassung In elektrischen Funkenentladungen lassen sich Zündphase, Bogenphase und Abklingphase unterscheiden, die besondere charakteristische Eigenschaften aufweisen. Ihre Untersuchung wird durch ein neu entwickeltes Stroboskop ermöglicht, dessen Phasenlage beliebig gegenüber der periodischen Funkenfolge verstellt werden kann. Durch optische Absorption kann im abklingenden Funken nicht nur der atomare Metalldampf durch seine Grundlinien nachgewiesen werden, sondern auch seine molekularen Reaktionsprodukte mit der umgebenden Atmosphäre lassen sich durch Bandenabsorption feststellen. Das Nachleuchten abklingender Funkenentladungen wird im wesentlichen durch das Nachleuchten des aktiven Stickstoffs getragen, wenn der Metalldampfgehalt der Funkenstrecke gering gehalten wird. Gegen Ende der Nachleuchtphase lassen sich Sprüherscheinungen an den Elektroden feststellen, bei denen kleine Partikelchen mit unterschiedlichen, zum Teil spiralig verlaufenden Bahnkurven ausgeschleudert werden. Die Flugbahnen der Teilchen weisen auf starke Gasströmungen in der Funkenstrecke hin.

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Summary In electrical spark discharges it is possible to distinguish ignition phase, arc phase, and decay phase. These display special characteristic properties. It is possible to study them by means of a newly developed stroboscope, whose phase position can be adjusted at will against the periodic succession of sparks. Through optical absorption, not only the atomic metal vapor can be detected, through its ground lines, in the decaying sparks but also its molecular reaction products with the surrounding atmosphere can be established through the band spectrum. The phosphorescence of decaying spark discharges is essentially due to the afterglow of the active nitrogen, if the metal vapor of the spark gap is kept low. Toward the end of the phosphorescence phase, spray phenomena may be observed at the electrodes, in which tiny particles with distinctive, in part spiral, orbital curves are ejected. The flight paths of these particles indicate strong gas currents in the spark gap.

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Résumé On peut distinguer dans la décharge par étincelles, la phase d'ignition, la phase d'arc et la phase de décroissance. On explique ainsi certaines propriétés caractéristiques. On peut étudier ces diverses phases à l'aide d'un dispositif stroboscopique nouveau réglable à volonté pour observer la même phase d'étincelles qui se succèdent périodiquement. Grâce a l'absorption optique on peut détecter soit une vapeur atomique métallique par ses raies caractéristiques pendant la période de décroissance des étincelles, soit les réactions moléculaires qui se produisent dans les gaz environnants grâce aux spectres de bandes. La phosphorescence pendant la décroissance de l'étincelle est due essentiellement à la postluminescence de l'azote actif, si la tension de vapeur du métal entre les électrodes est suffisamment basse. Pendant la fin de la période de phosphorescence on observe sur les électrodes des phénomènes de pulvérisation avec formation de très petites particules qui sont éjectées en décrivant des trajectoires en spirales. Les trajectoires aériennes de ces particules révèlent l'existence de forts courants gazeux entre les électrodes.

     

Longitudinal acceptance computation for A 50 MeV race track microtron

The algorithm for analysing of longitudinal motion and for calculating phase trajectory in race track microtron (RTM) with small injection energy and small energy gain per turn is described. A longitudinal acceptance is calculated.We are indebted to E. A. Perelshtein and N. Ju. Kazarinov and A. Ju. Molodozhencev for stimulating advices. We thank M. Slodika for work with program coding.     

Photochemical degradation of blends of polystyrene and poly(2,6 -dimethyl-1,4-phenylene oxide)

Blends of polystyrene and poly(2,6-dimethyl-1,4-phenylene oxide) that cover the entire compositional range have been subjected to the action of singlet oxygen from microwave discharge, dye-sensitized reaction, and photochemical oxidation. With the applied analytical technique, which consisted of infrared (IR) analysis, including ATR technique and a spectroscopic method combined with chemical analysis for hydroperoxide groups, it was not possible to detect any effect of the singlet oxygen treatment. For that reason singlet oxygen does not appear to be important to the initiation of the photooxidation of these blends. In connection with photochemical oxidation the interaction observed between the two components probably involves energy transfer from PS to PPO. This interaction results in the enhancement of reactions in PPO that lead to greater carbonyl group formation and crosslinking. Simultaneously, the probability of chain scission in the PS is lowered with increased PPO content, found by determining the changes in the molecular weights.     

Theory-enforced Re-investigation of the Origin of the Large Metal–Carbon Bond Strength in PdCH2I+ and its reactions with unsaturated hydrocarbons

State-of-the-art ab initio studies demonstrate that the reaction Pd⁺ + CH₃I → PdCH₂I⁺ + H^. is endothermic by ca. 20 kcal/mol, which translates into a bond dissociation energy (BDE) of ca. 83 kcal/mol for the Pd⁺? CH₂I bond. This figure is in agreement with an experimental bracket of 68 kcal/mol < BDE(Pd⁺? CH₂I) < 92 kcal/mol. Based on these findings, the previously studied Pd⁺/CH₃I system was re-investigated, and double-resonance experiments demonstrate that the formation of PdCH₂I⁺ occurs stepwise via PdCH as a reactive intermediate. Further, ion/molecule reactions of PdCH₂I⁺ with unsaturated hydrocarbons are studied, which reveal the formation of carbon–carbon bonds in the gas phase.     

Application of sampled-d.c. anodic stripping voltammetry to metal/fulvic acid equilibria

The use of anodic stripping voltammetry (ASV) to determine the labile metal fraction in metal/ fulvic acid equilibrium systems is discussed. A method is described for distinguishing between the contributions of processes in the reduction and oxidation steps to the observed anodic (stripping) current. This method, which facilitates separate examination of the two processes, is based on timed addition of fulvic acids during the deposition step, on pH control, and on measurement of sampled-d.c. ASV peak areas (Faradaic charge) for metal/fulvic acid solutions. Results are presented for copper(Il) and lead(Il) complexes with six colloid-free soil-derived fulvic acids. In contrast to differential-pulse ASV, the stripping current measured by sampled-d.c. ASV showed no measurable contribution from ligand adsorption on the mercury drop. For heterogeneous ligand systems, such as fulvic acid, use of stripping peak heights over-estimates the fraction of non-labile metal complex because peak broadening results from the range of complexes formed in the anodic step.     

Contribution à la phytochimie du genre Gentiana. XXVI.. Identification d'une nouvelle di-O-glucosyl cinnamoyl-C-glucosylflavone extraite des feuilles de Gentiana X marcailhouana RY.

Phytochemistry of Genus Gentiana. XXVI. Identification of a New Di-O-glucosyl Cinnamoyl-C-glucosylflavone in the Leaves of Gentiana X marcailhouana RY . A new di-O-glucosyl cinnamoyl-C-glucosylflavone has been identified as 4′-O-β-D -glucosyl-2″-O-[2-O-β-D -glucosyl-2,4,5-trihydroxy-(E)-cinnamoyl]isoorientin ( 1 ).     

Derivatives and reactions of glutacondialdehyde V : The crystal and molecular structure of 5-hydroxy-trans-2, trans-4-pentadienal acetate. The charge distribution in the glutacondialdehyde anion

The structure of 5-hydroxy-trans-2, trans-4-pentadienal acetate has been determined, using three-dimensional diffractometercollected X-ray data. The compound has the all-trans configuration with the atoms C-1 to C-5 in a plane. The charge distribution in the acetate and in the glutacondialdehyde anion have been calculated using the CNDO/2 approximation. In both compounds higher negative charges were found on carbon atoms C-2 and C-4 than on C-1, C-3 and C-5.