The photodissociation of ketene has been measured in the threshold region of the process CHaCOa 'Ar) t hv 4 CHa(Z 'A,) + CO betxeen 310 and 355 mu\_ The ketene has been dissociated by the tunable light from a frequency doubhxl dye laser. The singlet CHa(5'At) in its vibrational ground state (O,O,O)
Threshold energies for production of CH2(3B1) and CH2(1A1) from ketene photolysis. The CH2(3B1) ↔ CH2(1A1) energy splitting
✍ Scribed by J.W. Simons; Roberta Curry
- Publisher
- Elsevier Science
- Year
- 1976
- Tongue
- English
- Weight
- 438 KB
- Volume
- 38
- Category
- Article
- ISSN
- 0009-2614
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✦ Synopsis
measuring the relative CO qilantum yields from kctenc photolysis as a function of photolysis wavelength WC have determined the threshold energy at X0 for C112CO('AI) -+CHH(33~i) + CO(t -+ , ) to be 75.7 + 1.0 kcal/mole. This corrc-SpOl'ldS to a VdlC Of 40.7 f 1.0 kcal/molc for &Hpzss[ C112(3B,)]. By measuring the rclativc ratio of Cll~(1&t)/CII~(3Ut) from kctcnc photolysis as a function of photolysis wavelength WC have dctcrmincd the tbrcshold encrg at 25°C for CiI?CO(*A1) -CIl,('Al) + C!O('X+) to be 84.0 + 0.6 kcal/molc. This corresponds to a vJuc of 99.0 5 0.6 kcallmolc for Aff&fi[CH2(*At)]. 'IYIUS a VAJL for the Ctiz(313~) * CH~('AI) energy splitting 01~8.3 c 1 kcal/molc is dctcrmincd, whicir n$yxs wit11 three other recent indcpcndcnt experimental estimates and the most rcccnt quantum theoretical calcuhtions.
📜 SIMILAR VOLUMES
Excess molar enthalpies at the temperature 298.15 K were measured for CH2)nCH3} (n = 9, 12), and {x2CH3(CH2)4CH3 + (1-x2)CH3(CH2)n-2CH3} (n=9, 12), using a Calvet microcalorimeter. The experimental results were compared with those calculated by using the Nitta-and-Chao model.
The radiative lifetime Trad of the CH2(g 'BI) state has been determined using the CHz(g 'Bl +y lAl) emission produced by electrons incident on CH4. The value found for Trad is 1.90(%0.15) X lo\* s. A second lifetime component, 8.5(\* 1.0) X LO\* S, has been measured which is related to either cascad
Excess molar volumes V E m of the ternary mixture {x1CH3(CH2)3OH+x2CH3(CH2)4CH3 + (1-x1-x2)CH3(CH2)3NH2} at the temperatures 298.15 K and 313.15 K, and the binary mixtures {xCH3(CH2)3OH + (1-x)CH3(CH2)3NH2}, {xCH3(CH2)4CH3 + (1-x)CH3(CH2)3NH2} at T=313.15 K have been determined from density measurem