PRIMARY QUANTUM YIELD DETERMINATION BY INTERMITTENT ILLUMINATION IN THE REACTION OF METHANOL VAPOR WITH Hg 6(3P1) ATOMS

1961 ◽  
Vol 39 (11) ◽  
pp. 2251-2255 ◽  
Author(s):  
Arthur R. Knight ◽  
Harry E. Gunning

The decomposition of methanol vapor by Hg 6(3P1) atoms has been studied under intermittent illumination conditions, in a static system at 25 °C. The behavior of the NO-inhibited reaction under intermittent illumination has also been examined.For the pure substrate at a pressure of 50 mm, the quantum yield of hydrogen formation, Φ(H2), was found to rise steadily toward unity with decreasing light period (tL). The maximum value of Φ(H2) at a given tD could only be obtained if the dark period (tD) exceeded 100 mseconds. At the shortest tL studied, 0.156 msecond, Φ(H2) was 0.89 compared with the steady illumination value, at zero extent of reaction, of 0.46. A linear relation was found to obtain between Φ(H2) and log (tL) at a given tD Extrapolation showed that Φ(H2) would be unity at tL = 0.040 msecond.For a mixture of 4.8 mm of NO and 50 m of CH3OH, Φ(CH3ONO) was found to rise from its steady illumination value of 0.14 to 0.27 at a sector speed of 300 r.p.m., with a dark/light ratio of 20. At higher speeds the quantum yield decreased again.From the study it is concluded that the primary process of H atom detachment is at least 89% efficient, and that the primary quantum yield is likely unity. The fact that the quantum yield under steady illumination is only 0.46 is attributed to the consumption of H atoms by radical addition processes of which the most probable is the addition of H to CH2OH. For the inhibited reaction the low value of Φ(CH3ONO) under steady illumination is ascribed to the abstractive attack of CH3O on NOH.The kinetic effects of intermittent illumination are discussed, in the light of the results. It is concluded that the technique should be of considerable value in primary process studies in mercury photosensitization.

1971 ◽  
Vol 49 (12) ◽  
pp. 2125-2131 ◽  
Author(s):  
J. Castonguay ◽  
Y. Rousseau

The study of the mercury Hg6(3P1) photosensitized decomposition of methyl vinyl ether has been studied in a static system at substrate pressures from 10 to 800 Torr. The excited precursor proposed has a calculated lifetime of 1.18 × 10−10 s and its decomposition proceeds almost exclusively through the rupture of the O—CH3 bond. A second primary process is the intramolecular formation of ethylene but it accounts only for 2% of the total ether decomposition. The major products are shown to be formed by free radical reactions and the overall reactivity appears to be very similar to that of the olefins. The results obtained with CH3SH added to the system indicate that the primary radicals are formed with a quantum yield close to unity.


2021 ◽  
Author(s):  
Yining Ji ◽  
Daniel A. DiRocco ◽  
Cynthia M. Hong ◽  
Michael K. Wismer ◽  
Mikhail Reibarkh

1964 ◽  
Vol 42 (9) ◽  
pp. 2056-2064 ◽  
Author(s):  
J. K. S. Wan ◽  
O. P. Strausz ◽  
W. F. Allen ◽  
H. E. Gunning

The specific nature of the primary process in the reaction of 202Hg 6(3P1) atoms, photoexcited in natural mercury vapor by a cool 202Hg electrodeless discharge source, with CH3Cl has been examined in detail. Primary C–Cl bond scission occurs with unit efficiency. Quantum yields (φ) for the two primary modes of decomposition[Formula: see text]were found to have values of 0.71 (b) and 0.29 (a). The effect of various reaction parameters on the 202Hg enrichment in the calomel product has been investigated and the importance of isotopic mercury depletion in the reaction zone demonstrated by the use of intermittent illumination.A brief study of the reaction of ethyl, n-propyl, i-propyl, t-butyl, and n-amyl chlorides has revealed a relation between the molecular structure of the alleyl chloride and the efficiency of the monoisotopic route (a) to calomel formation. Thus, while the reactions of all the normal alkyl chlorides have φa values between 0.29 and 0.32, φa (isopropyl chloride) is only 0.22 and φa (t-butyl chloride) is 0.17.


1968 ◽  
Vol 46 (4) ◽  
pp. 527-530 ◽  
Author(s):  
N. J. Friswell ◽  
R. A. Back

The Hg(63P1)-sensitized decomposition of HNCO vapor has been briefly studied at 26 °C with HNCO pressures from about 3 to 30 Torr. The products detected were the same as in the direct photolysis, CO, N2, and H2. The quantum yield of CO was appreciably less than unity, compared with a value of 1.5 in the direct photolysis under similar conditions. From this and other observations it is tentatively concluded that a single primary process occurs:[Formula: see text]From a study of the mercury-photosensitized reactions in mixtures of HNCO with H2, it was concluded that hydrogen atoms react with HNCO to form CO but not N2. The initial step is probably addition to form NH2CO. From the competition between reaction [1] and the corresponding quenching by H2, the cross section for reaction [1] was estimated to be 2.3 times that of hydrogen.


2018 ◽  
Vol 28 (6) ◽  
pp. 1275-1280
Author(s):  
Kadhim Kh. Hashim ◽  
Shatha Y. Yahyaa ◽  
Asmaa A. Mohmmed Al-Rashidy

2019 ◽  
Vol 822 ◽  
pp. 871-877
Author(s):  
Victor Klinkov ◽  
Aleksander Semencha ◽  
Evgenia Tsimerman ◽  
Artem Osipov ◽  
Margarita G. Dronova

Fluoroaluminate glasses of the composition 2Ва (РО3)2–98MgCaSrBaYAl2F14-xErF3, where x=0, 0.1, 0.5, 1.0 mol. % have been prepared by melt quenching technique and characterized by optical absorption, emission spectra and decay curve analysis. Measured transmission spectra indicate the high practical relevance of the composition of glasses under investigation for photonics and optoelectronics products. In the region of 500–700 nm, luminescence spectra with peaks at about 522, 550, and 665 nm were obtained. The positions of the luminescence bands have been described using an erbium ion energy scheme. The concentration dependences of the absolute quantum yield values for the series of Er3+-doped fluoroaluminate glasses were also established. The maximum value of absolute quantum yield was found for a sample with Er3+ concentration 0.21∙1020 сm-3. The main reason for reducing the values of absolute quantum yield is concentration quenching.


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