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State selective investigation of the reactions O(1D)+CH4 (C2H6)→OH (CH2OH)+CH3(ν1(ν),ν2(ν),J,K) using resonant multiphoton ionization detection of CH3

✍ Scribed by J. Schlütter; R. Schott; K. Kleinermanns

Publisher
Elsevier Science
Year
1993
Tongue
English
Weight
419 KB
Volume
213
Category
Article
ISSN
0009-2614

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📜 SIMILAR VOLUMES

Excess molar volumes of {xCH3(CH2)3OH +
Excess molar volumes of {xCH3(CH2)3OH + (1−x)H(CH2)ν(OCH2CH2)3OH} (ν= 1, 2, and 4) at the temperature 298.15 K
✍ A. Pal; W. Singh 📂 Article 📅 1996 🏛 Elsevier Science 🌐 English ⚖ 268 KB

The excess molar volumes V E m of {xCH3(CH2)3OH + (1x)H( CH2)n(OCH2CH2)3OH} for n = 1, 2, and 4 were determined as a function of mole fraction x using a continuous-dilution dilatometer at the temperature 298.15 K. The V E m values decreased as the alkyl chain length of the alkoxyethanol increased. E

Speeds of sound and isentropic compressi
Speeds of sound and isentropic compressibilities of {xCH3O(CH2)2OH+(1−x)H(CH2)ν(OCH2CH2)2OH} (ν=1, 2, and 4) at the temperature 298.15 K
✍ A. Pal; W. Singh 📂 Article 📅 1997 🏛 Elsevier Science 🌐 English ⚖ 209 KB

The speed of sound u has been obtained at a frequency of 4 MHz in 4xCH3O(CH2)2OH + (1 -x)H( CH2)n (OCH2CH2)2OH5 for n = 1, 2, and 4 over the whole range of x at T = 298.15 K and atmospheric pressure, using a NUSONIC velocimeter based on the sing-around technique. The excess molar volumes were taken

Excess molar volumes and excess partial
Excess molar volumes and excess partial molar volumes of {xCH3O(CH2)2OH +(1 −x)H(CH2)νO(CH2)2O(CH2)2OH}, (ν= 1, 2, and 4) at the temperature 298.15 K
✍ A. Pal; W. Singh 📂 Article 📅 1996 🏛 Elsevier Science 🌐 English ⚖ 375 KB

The excess molar volumes of {xCH3O(CH2)2OH+(1-x)H(CH2)nO(CH2)2O(CH2)2OH} for n = 1, 2, and 4 have been measured as a function of composition using a continuous-dilution dilatometer at the temperature T=298.15 K. The excess molar volumes are negative over the entire range of composition for the syste

OH (ν, J) distributions from the reactio
OH (ν, J) distributions from the reaction between CH4 and O (1D2), initiated in CH4·O3 clusters
✍ Roger D. van Zee; John C. Stephenson; Michael P. Casassa 📂 Article 📅 1994 🏛 Elsevier Science 🌐 English ⚖ 610 KB

## AbStlWt The nascent OH rovibrational distribution for the reaction CH4\*03+h~266,,,,, + CH3 + OH + Oz are reported. The population ratio betweenthevibrationallevelswasfound tobe u(O)/v( 1) = l.Of0.2 (2a), v( 1)/u(2) =0.67?0.26, and u(2)/u(3) = l.SkO.2; and significant rotational excitation was

Speeds of sound and isentropic compressi
Speeds of sound and isentropic compressibilities of {xH(CH2)νO(CH2)2O(CH2)2OH +(1 −x)H2O}, (ν= 1, 2, and 4) at the temperature 298.15 K
✍ A. Pal; Y.P. Singh 📂 Article 📅 1996 🏛 Elsevier Science 🌐 English ⚖ 434 KB

The speeds of sound in {xH(CH2)n O(CH2)2O(CH2)2OH + (1-x)H2O} for n=1, 2, and 4 have been measured over the whole range of x at the temperature T=298.15 K. The molar isentropic compressibilities KS, m of these solutions were estimated from the products of the molar volume and the isentropic compress

The speed of sound and isentropic functi
The speed of sound and isentropic functions of {xH(CH2)ν(OC2H4)2OH + (1−x)(C4H9)O} (ν = 1, 2, and 4) at the temperature 298.15 K
✍ A. Pal; Y.P. Singh 📂 Article 📅 1996 🏛 Elsevier Science 🌐 English ⚖ 216 KB

The speeds of sound have been measured in {xH(CH2)n(OC2H4)2OH + (1x)(C4H9)2O} for n = 1, 2, and 4 as a function of mole fraction x at the temperature 298.15 K, using a sing-around technique, and at a frequency of 4 MHz. The excess molar volumes were taken from the literature and combined with the me