2015
DOI: 10.1021/acs.jpca.5b06638
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Characterization of the 1,1-HCl Elimination Reaction of Vibrationally Excited CD3CHFCl Molecules and Assignment of Threshold Energies for 1,1-HCl and 1,2-DCl plus 1,1-HF and 1,2-DF Elimination Reactions

Abstract: Vibrationally excited CD3CHFCl molecules with 96 kcal mol(-1) of energy were generated by the recombination of CD3 and CHFCl radicals in a room-temperature bath gas. The four competing unimolecular decomposition reactions, namely, 1,1-HCl and 1,2-DCl elimination and 1,1-HF and 1,2-DF elimination, were observed, and the individual rate constants were measured. The product branching fractions are 0.60, 0.27, 0.09, and 0.04 for 1,2-DCl, 1,1-HCl, 1,2-DF, and 1,1-HF elimination, respectively. Electronic structure c… Show more

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Cited by 10 publications
(55 citation statements)
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“…Adduct energies calculated by M06-2X relative to the molecules are usually within 1–2 kcal mol –1 of the energy given by Δ H 0 – D 0 (adduct). d M06-2X/aug-cc-pVTZ calculations for the threshold energy, E 0 , and for the normal mode associated with the HCl stretch vibration. For reference, ω e for HCl is 2991 cm –1 . e CCSD­(T) with M06-2X/aug–cc-pVTZ calculation of the threshold energy. f MP2 calculation from ref . g Since the geometry optimization in CBS-QB3 calculations failed for CH 3 (Cl)­C:HCl or for C 2 H 5 (Cl)­C:HCl, D 0 was obtained by subtracting the M06-2X adduct energy (CH 3 CHCl 2 ) or E 0 (1,1-HCl) energy (C 2 H 5 CHCl 2 ) from the enthalpy of reaction. We also reinvestigated the MP2/6-311+G­(2d,p) results for C 2 D 5 CHCl 2 ; convergence was obtained for both the transition state and the adduct, but the energies were nearly identical. h G3 calculations by Zhu and Bozzelli (they did not report a Cl 2 C:HCl adduct). …”
Section: Resultsmentioning
confidence: 99%
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“…Adduct energies calculated by M06-2X relative to the molecules are usually within 1–2 kcal mol –1 of the energy given by Δ H 0 – D 0 (adduct). d M06-2X/aug-cc-pVTZ calculations for the threshold energy, E 0 , and for the normal mode associated with the HCl stretch vibration. For reference, ω e for HCl is 2991 cm –1 . e CCSD­(T) with M06-2X/aug–cc-pVTZ calculation of the threshold energy. f MP2 calculation from ref . g Since the geometry optimization in CBS-QB3 calculations failed for CH 3 (Cl)­C:HCl or for C 2 H 5 (Cl)­C:HCl, D 0 was obtained by subtracting the M06-2X adduct energy (CH 3 CHCl 2 ) or E 0 (1,1-HCl) energy (C 2 H 5 CHCl 2 ) from the enthalpy of reaction. We also reinvestigated the MP2/6-311+G­(2d,p) results for C 2 D 5 CHCl 2 ; convergence was obtained for both the transition state and the adduct, but the energies were nearly identical. h G3 calculations by Zhu and Bozzelli (they did not report a Cl 2 C:HCl adduct). …”
Section: Resultsmentioning
confidence: 99%
“…The moments of inertia and vibrational frequencies of transition states, adducts, and the molecule are in Supporting Information. The lower frequencies of 1,1-HX transition states relative to 2,1-DX transition states has been discussed previously. , The statistical rate constant at energy E was obtained in the usual way from eq : …”
Section: Calculation Of Rrkm Rate Constants and Assignment Of E 0 Valuesmentioning
confidence: 99%
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