scholarly journals Absorption spectra of radicals of substrates for p-hydroxybenzoate hydroxylase following electrophilic attack of the .OH radical in the 3 position.

1987 ◽  
Vol 262 (36) ◽  
pp. 17475-17479 ◽  
Author(s):  
R F Anderson ◽  
K B Patel ◽  
M R Stratford
1971 ◽  
Vol 2 ◽  
pp. 402-403
Author(s):  
R. D. Davies

I have attempted to obtain an answer to the question “In which gas (neutral hydrogen) clouds do we find molecules?” By limiting the investigation to those clouds which might be considered normal (i.e. specifically excluding the class of clouds which emit by maser action) it is possible to obtain a definitive answer to the question namely, those clouds which have the highest gas concentration. Further data on the correlation between the distribution of neutral hydrogen and of different molecules can be found.The clouds which are seen in absorption against background radio sources are most ideally suited for this purpose and I have used the absorption spectra of neutral hydrogen (21 cm wavelength), of the OH radical (18 cm, the 1667 MHz line) and the formaldehyde molecule (6 cm). Only the absorption spectra of the three strongest non-thermal sources (Cas A, Cyg A, and Tau A) were used because only these have unambiguous neutral hydrogen absorption spectra and also because they, unlike the HII regions, do not have 1667 MHz OH spectra which may be confused by anomalous emission. In the absorption spectra of these three sources individual clouds at specific velocities can be recognized on the H, OH and H2CO spectra. We can then investigate the OH and H2CO content of each cloud relative to its neutral hydrogen content.


Methanolic solutions of I - , Br - , Cl - , SCN - and TMPD have been investigated by pulse radiolysis. Except for Cl - solutions oxidation of the solutes occurs and the transient products I 2 - , Br 2 - , (SCN) 2 - and TMPD + have been identified by their absorption spectra ( λ max = 380, 360, 470 and 565 nm respectively). For the Br - and SCN - cases the oxidation occurred only in acidified solution. These results are attributed to the occurrence of the reactions X - + CH 3 O → CH 3 O - + X, X + X - ⇌ X 2 - , where X - - I - , Br - , SCN - or TMPD. In pure methanol the methoxy radicals react to form the CH 2 OH radical. The dependences of the yields of I 2 - and TMPD + on the concentration of I - and TMPD respectively indicate that the yield of scavengable methoxy radicals G (CH 3 O) = 2.0 and that k (CH 3 O + X - )/ k (CH 3 O + CH 3 OH) = (1.4±0.1) x 10 4 . The presence of 0.1 mol HClO 4 /l or saturation of the solutions with N 2 O increases G (CH 3 O) by 0.5, an effect which is attributed to methoxy radicals which would otherwise react with electrons within the spurs. Solutions saturated with CO 2 do not show the increased yield presumably because of the occurrence of the back reaction: CO 2 - + CH 3 O → CH 3 O - + CO 2 . The yield of ethoxy radicals, G (C 2 H 5 O) derived from measurement of I 2 - formed in ethanolic KI solutions is estimated to be 1.5±0.1. Formate ion was found to have no effect on the yield of I 2 - from methanolic solutions of iodide and it is concluded that the reaction between methoxy radicals and formate ion is slow. The similar lack of effect of nitrite ion and iodide ion on the TMPD system is attributed to the reactions TMPD + NO 2 → TMPD + + NO 2 - , TMPD + I 2 - → TMPD + + 2I - .


1969 ◽  
Vol 24 (10) ◽  
pp. 1262-1267 ◽  
Author(s):  
A. Wigger ◽  
W. Grünbein ◽  
A. Henglein ◽  
E. J. Land

The OH radical rapidly reacts with CH3NH2 and C6H5NH2 but reacts slower with CH3NH3⊕, respectively C6H5NH3⊕. In the reaction with methylamine. the complex is formed which loses water with τ½=26 µs. The addition of OH to the aromatic ring of aniline occurs in 20% of the reactions. The hydroxy-amino-cyclohexadienyl radical has its absorption maximum at 3500 A. It decays by elimination of water to yield the anilino radical C6H5NH (τ½= 5.7µs at pH = 7), H⊕ and OH⊖ ions catalyse the decay. In 80% of the reactions. · OH adds to the amino group of aniline. The subsequent loss of water or of OH⊖ occurs rapidly (<1 µs). However, the basic form of the addition complex decays much more slowly (τ½=10 µs at pH= 13.7). The pK-value of the equilibriumis estimated to be equal to 11 — 12. The absorption spectra of C6H5NH2® and the pK-value of 7.0 of C6H5NH2⊕ first described by LAND and PORTER are confirmed.


1988 ◽  
Vol 102 ◽  
pp. 243-246
Author(s):  
J.T. Costello ◽  
W.G. Lynam ◽  
P.K. Carroll

AbstractThe dual laser-produced plasma technique for the study of ionic absorption spectra has been developed by the use of two Q-switched ruby lasers to enable independent generation of the absorbing and back-lighting plasmas. Optical pulse handling is used in the coupling cicuits to enable reproducible pulse delays from 250 nsec. to 10 msec, to be achieved. At delay times > 700 nsec. spectra of essentially pure neutral species are observed. The technique is valuable, not only for obtaining the neutral spectra of highly refractory and/or corrosive materials but also for studying behaviour of ionic species as a function of time. Typical spectra are shown in Fig. 1.


1988 ◽  
Vol 102 ◽  
pp. 71-73
Author(s):  
E. Jannitti ◽  
P. Nicolosi ◽  
G. Tondello

AbstractThe photoabsorption spectra of the carbon ions have been obtained by using two laser-produced plasmas. The photoionization cross-section of the CV has been absolutely measured and the value at threshold, σ=(4.7±0.5) × 10−19cm2, as well as its behaviour at higher energies agrees quite well with the theoretical calculations.


1996 ◽  
Vol 88 (1) ◽  
pp. 281-290 ◽  
Author(s):  
HAO WEN ◽  
TIANJING HE ◽  
CUNYI XU ◽  
JIAN ZUO ◽  
FAN-CHEN LIU

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