5 research outputs found

    MICROWAVE SPECTROSCOPIC INVESTIGATIONS OF THE C--H⋯π\cdots\pi CONTAINING COMPLEXES CH2_2F2⋯_2\cdotsPROPYNE AND CH2_2ClF⋯\cdotsPROPYNE

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    Author Institution: Department of Chemistry, Eastern Illinois University, 600; Lincoln Ave., Charleston, IL 61920The spectra of the CH2_2F2⋯_2\cdotspropyne and CH2_2ClF⋯\cdotspropyne complexes have been studied by chirped-pulse and resonant cavity Fourier-transform microwave spectroscopy and by {\em ab initio} calculations at the MP2/6-311++G(2d,2p) level. Both complexes contain C--H⋯π\cdots\pi contacts, with the halogen atoms angled towards the methyl group end of the propyne. While CH2_2F2⋯_2\cdotspropyne has CsC_s symmetry, CH2_2ClF⋯\cdotspropyne has C1C_1 symmetry, with the fluorine and chlorine atoms straddling the propyne. \vspace{1em} Investigation of four single 13^{13}C and the DC≡\equivCCH3_3 isotopologues in CH2_2F2⋯_2\cdotspropyne has allowed a detailed structural determination, while only the 35^{35}Cl and 37^{37}Cl isotopologues have so far been assigned for CH2_2ClF⋯\cdotspropyne. Experimental data will be compared with {\em ab initio} results and with the analogous acetylene complexes, both of which have CsC_s symmetry structures, with double C--H⋯π\cdots\pi interactions

    Rotational Spectroscopic Studies of C–H···F Interactions in the Vinyl Fluoride···Difluoromethane Complex

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    Rotational spectra of the normal isotopic species and three <sup>13</sup>C isotopologues of the 1:1 complex between vinyl fluoride (CH<sub>2</sub>CHF) and difluoromethane (CH<sub>2</sub>F<sub>2</sub>) have been measured using 480 MHz bandwidth chirped-pulse Fourier-transform microwave spectroscopy in the 6.5–20 GHz region. A structure for this dimer has been determined by fitting the moments of inertia of all isotopologues and confirmed by calculation of Kraitchman single isotopic substitution coordinates. The structure is consistent with that determined by ab initio geometry optimization at the MP2/6-311++G­(2d,2p) level and has the difluoromethane subunit located on the CHF side of the vinyl fluoride subunit with three C–H···F contacts and with the hydrogen atoms of the CH<sub>2</sub>F<sub>2</sub> straddling the vinyl fluoride symmetry plane

    Characterization of Two Isomers of the Vinyl Fluoride···Carbon Dioxide Dimer by Rotational Spectroscopy

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    Rotational spectra of two different structural forms of the 1:1 weak complex between vinyl fluoride (C<sub>2</sub>H<sub>3</sub>F) and carbon dioxide were measured using 480 MHz bandwidth chirped-pulse and resonant cavity Fourier-transform microwave spectroscopy in the 5–17 GHz region. Both structures have the CO<sub>2</sub> molecule situated in the plane of the vinyl fluoride, such that the CO<sub>2</sub> is interacting either with a CHF side or with a HCCF edge of the vinyl fluoride subunit. Both observed structures are close to those predicted by <i>ab initio</i> geometry optimizations (corrected for basis set superposition error) at the MP2/6-311++G­(2d,2p) level. Dipole moment measurements and structural fits, including determinations of principal axis coordinates for all three carbon atoms, confirm the geometries of the assigned species

    Alkynes as CH/π Acceptors: Microwave Spectra and Structures of the CH<sub>2</sub>F<sub>2</sub>···Propyne and CH<sub>2</sub>ClF···Propyne Dimers

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    Rotational spectra of weakly bound complexes of chlorofluoromethane (CH<sub>2</sub>ClF) and difluoromethane (CH<sub>2</sub>F<sub>2</sub>) with propyne (HCCCH<sub>3</sub>) have been measured using chirped-pulse and resonant-cavity Fourier-transform microwave spectroscopy, adding to a relatively small body of high resolution spectroscopic data on propyne complexes. Both dimers contain CH/π contacts, as well as secondary contacts between one or both halogen atoms and the methyl group of propyne. A detailed structural determination for CH<sub>2</sub>F<sub>2</sub>···propyne has been made by study of the normal, one deuterated and four <sup>13</sup>C substituted isotopologues, with the second lowest energy configuration predicted from <i>ab initio</i> calculations agreeing well with the observed structure. Experimental rotational constants for the most abundant isotopologue of CH<sub>2</sub>F<sub>2</sub>···propyne are <i>A</i><sub>00</sub> = 5815.5858(15) MHz, <i>B</i><sub>00</sub> = 1341.1191(5) MHz, <i>C</i><sub>00</sub> = 1099.2040(4) MHz (uncorrected for internal rotation effects), and the dipole moment components, determined by Stark effect measurements, are μ<sub><i>a</i></sub> = 1.568(2) D, μ<sub><i>b</i></sub> = 0.587(2) D, and μ<sub>tot</sub> = 1.674(3) D. For CH<sub>2</sub>ClF···propyne, only <sup>35</sup>Cl and <sup>37</sup>Cl isotopologues have been assigned, providing rotational constants and chlorine atom coordinates consistent with the lowest energy structure from a series of <i>ab initio</i> predictions. Rotational constants for the <sup>35</sup>Cl isotopologue are <i>A</i> = 3423.639(7) MHz, <i>B</i> = 1253.7562(20) MHz, and <i>C</i> = 1200.4828(15) MHz and the diagonal and two off diagonal components of the quadrupole coupling tensor have also been determined
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