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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 2530-2536 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: HBr−2 has D∞h symmetry at both the second-order (MP2) and third-order (MP3) Møller–Plesset perturbation levels of theory with the extended basis sets, whereas the Hartree–Fock level of theory predicts that it has C∞v symmetry. A potential energy map is calculated with the MP2 method as a function of two parameters, i.e., the distance of two Br atoms and the displacement of H from the center of them. Two-dimensional vibration analysis is performed by using this potential energy map. The calculated ν1 is 200 cm−1 and the ν3 is 837 cm−1 in HBr−2, and those in DBr−2 are 199 and 569 cm−1, respectively. Thus the ratio of the asymmetric vibration (ν3)H/(ν3)D is 1.47, being somewhat greater than the value of (square root of)2 expected for a harmonic oscillator. The enthalpy changes (ΔH°) in the reaction of Br− with an HBr molecule are determined by both the MP3 total energy changes and the thermal energy changes between the reactants and the product. The calculated enthalpy change of −21.2 kcal/mol is in good agreement with the experimental one (−21 kcal/mol) recently observed by Caldwell and Kebarle. These calculated data on HBr−2, which will provide us with a useful guide for future measurements of gas-phase vibrational spectra, are compared with those on HCl−2 and HF−2.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 91 (1989), S. 3539-3548 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The geometry of ClHCl− has D∞h symmetry, [Cl–H–Cl]−, as opposed to C∞v symmetry [Cl–H...Cl−], which is predicted to be favored at the Hartree–Fock (HF) level of calculation with a basis set of [11s9p2d1f(Cl)/5s2p1d(H)]. The chemical bond of the D∞h structure is a nonclassical four-electron three-center bond, while the C∞v geometry corresponds to an ion–dipole complex. The energy difference between the two is small. Calculations with inclusion of configuration revealed that both have predominantly a HF configuration. D∞h is realized by excitations from σ molecular orbitals (MO) to their antibonding σ* MO, whereas excitations to π MO are ineffective. Normal vibrational frequencies were calculated as follows (units are cm−1): G82(MP2): (ν1,σg): 346; (ν3,σu ): 547; (ν2,πu): 854; 1D Analysis(MP4): (ν1,σg ): 338; (ν3,σu): 830; (ν2, πu ):...; 2D Analysis(MP4): (ν1,σg)@B: 310; (ν3,σu) : 709; (ν2,πu) : 877. The potential for the asymmetric vibration is shown to be quartic. The standard free energy (ΔG°), enthalpy (ΔH°), and entropy (ΔS°) changes (i.e., at 1 atm and 298.16 K) were evaluated from the reaction, HCl+Cl−→ClHCl−, to be as follows: ΔG°=−16.5 kcal/mol, ΔH°=−23.5 kcal/mol, and ΔS°=−23.5 cal/K/mol.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 3809-3814 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The molecular structure of various stationary points of HC2N has been studied using the quadratic configuration interaction including single and double substitutions with triples contributions (QCISD(T)). A Huzinaga–Dunning double-zeta plus polarization (D95**) basis set was used. A stability ladder of these species is calculated using the configuration interaction including single and double substitutions (SDCI) with the Davidson correction (SDCI+Q). The general contraction scheme of the [5s3p2d1f(C and N)/3s2p1d(H)] atomic natural orbital basis set was chosen. The natural orbitals obtained in the preceding complete active space self-consistent field (CASSCF) calculations were applied to the open-shell SDCI. The triplet cyanomethylene is bent, and the barrier to linearity is 1.4 kcal/mol at the single-reference SDCI+Q level of theory in accord with the Schaefer and Roos' values (0.8–1.0 kcal/mol). The nine-reference SDCI+Q calculation increases the energy separation by 0.7 kcal/mol. The thermal energy change between the two (1 and 2) including the calculated zero-point vibrational energies is 1.4 kcal/mol. The enthalpy barrier (ΔH≠) to linearize 1 to transition state 2 in a (hypothetical) reaction is predicted to be 0.0 kcal/mol using the single-reference SDCI+Q bent-linear energy separation. As a result, experiments might find no barrier to inversion of bent triplet 1. The most stable singlet species 6 (ring form of HC2N) lies 7.7 kcal/mol above the triplet bent cyanomethylene. Vertical excitation energies from the ground-state (3A‘) of triplet bent cyanomethylene to 1A' and 1A‘ are studied using the CASSCF and SDCI methods; the SDCI+Q energies are 0.93 and 1.11 eV, respectively. These excitation energies are compared with those in the methylene and oxygen molecules having a qualitatively similar electronic structure to the present HCCN species, where two electrons occupy near-degenerate π-like (or degenerate π) highest occupied molecular orbitals (HOMO) forming a triplet ground-state. The excitation energies of 0.93 and 1.11 eV are close to the relative energies of the 3, 8, and 9 to the most stable triplet bent cyanomethylene.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 105 (1983), S. 1907-1912 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 87 (1987), S. 3701-3702 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    Theoretical chemistry accounts 11 (1968), S. 369-376 
    ISSN: 1432-2234
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology
    Description / Table of Contents: Zusammenfassung Die konventionelle ASMO-Theorie liefert bekanntlich eine viel zu große Differenz der Terme 3Σ u − und 3Σ u + von O2, weswegen der Vorschlag gemacht wird, die üblicherweise vorgenommene Äquivalenz-Einschränkung fallen zu lassen. Der Orbital-Exponent eines lockernden MO's kann von dem der übrigen π g's abweichen. Rechnungen zeigen, daß das äußerste MO viel diffuser als die anderen ist und daß die Energie des 3Σ u − -Zustandes beträchtlich erniedrigt wird.
    Abstract: Résumé La séparation entre les états 3Σ u − 3Σ u + de O2 donnée par la méthode ASMO conventionnelle est connue pour être trop grande. Afin de résoudre cette difficulté la levée des restrictions d'équivalence ordinairement utilisées est proposée. Ainsi l'exposant orbital d'une des orbitales moléculaires antiliantes π g peut prendre une valeur différente de celui de l'autre orbitale antiliante π g. Des calculs variationnels montrent que l'orbitale la plus haute ainsi obtenue est beaucoup plus diffuse que les autres. Ceci a pour effet de diminuer considérablement l'énergie de l'état 3Σ u − , améliorant la séparation entre les états 3Σ u − et 3Σ u + .
    Notes: Abstract It is well known that the energy interval separating 3Σ u − and 3Σ u + states of O2, as given by the conventional ASMO method, is too large. In order to resolve this difficulty, removal of the equivalence restrictions usually employed in the orbital theory is proposed. Thus the orbital exponent of one antibonding πg MO is allowed to take a different value from the other πg's. Variational calculations show that the resulting outermost orbital is much more diffuse than the others. This model of a single diffuse orbital brings about a considerable energy lowering for the 3Σ u − state and thus the agreement of the 3Σ u − - 3Σ u + interval with experiment is improved.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    Plasma chemistry and plasma processing 6 (1986), S. 179-193 
    ISSN: 1572-8986
    Keywords: Ammonia synthesis ; catalysis in plasma ; MgO ; CaO ; Al2O3 ; WO3 ; metal catalysts
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Technology
    Notes: Abstract Ammonia synthesis from H2-N2 mixed gas was studied at room temperature in a glow-discharge plasma in the presence of metals or metal oxides. Magnesia (MgO) and calcia (CaO), which are oxides with solid basicity, revealed catalytic activity in the plasma synthesis of ammonia, although they are catalytically inactive in industrial ammonia synthesis. The acidic oxides (Al2O3, WO3, and SiO2-Al2O3) lead to the consumption of the reactant, i.e., the H2-N2 mixed gas. No ammonia was isolated. Metal catalysts showed higher activity than the above basic oxides. They have, however, different activities. The reaction was faster over the active materials than over sodium chloride (NaCl) or glass wool or in a blank reactor without any catalyst.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    New York, NY : Wiley-Blackwell
    International Journal of Quantum Chemistry 18 (1980), S. 143-150 
    ISSN: 0020-7608
    Keywords: Computational Chemistry and Molecular Modeling ; Atomic, Molecular and Optical Physics
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: Global features of potential-energy curves are drawn using minimal basis SCF-CI method. Potential-energy surfaces are drawn at points of interest. The mechanism of the chemiluminescence is discussed along with the measurement of a rate constant exploiting the phenomena.
    Additional Material: 5 Ill.
    Type of Medium: Electronic Resource
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