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Theoretical gas and dielectric second virial coefficients of CO-Ar (Articolo in rivista)
- Type
- Label
- Theoretical gas and dielectric second virial coefficients of CO-Ar (Articolo in rivista) (literal)
- Anno
- 2008-01-01T00:00:00+01:00 (literal)
- Alternative label
Cacheiro, J.L.; Fernandez, B.; Rizzo, A.; Jansík, B.; Pedersen, T. B. (2008)
Theoretical gas and dielectric second virial coefficients of CO-Ar
in Molecular physics (Print)
(literal)
- Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#autori
- Cacheiro, J.L.; Fernandez, B.; Rizzo, A.; Jansík, B.; Pedersen, T. B. (literal)
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- Note
- ISI Web of Science (WOS) (literal)
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- J. L. C., B. F.: Faculty of Chemistry, Department of Physical Chemistry, University of Santiago de Compostela, Santiago de Compostela, Spain
A. R.: Istituto per i Processi Chimico-Fisici del Consiglio Nazionale delle Ricerche, Area della Ricerca, Pisa, Italy
B. J.: Teoretisk Kemi, Kemisk Institut, Aarhus Universitet, Aarhus, Denmark
T. B. P.: Department of Theoretical Chemistry, Chemical Center, University of Lund, Lund, Sweden (literal)
- Titolo
- Theoretical gas and dielectric second virial coefficients of CO-Ar (literal)
- Abstract
- Using coupled cluster singles and doubles linear response theory and the d-aug-cc-pVTZ basis set extended with a
3s3p2d1f1g set of midbond functions, the interaction induced electric dipole polarisability surface of the COAr
van der Waals complex is computed. Combining this surface with accurate intermolecular potential energy and
electric dipole surfaces, the pressure and dielectric second virial coefficients of the complex are calculated by a
classical statistical approach. Excellent agreement with experimental results (to within the experimental error
bars) is obtained for the pressure second virial coefficient over a range of temperatures. No previous experimental
or theoretical investigations have been carried out for the dielectric second virial coefficient, B_epsilon(T), which is
estimated to be about 1.9 cm^6 mol-1 at room temperature. This value results from a balance of terms due to the
interaction induced electric dipole polarisability (predominant at high temperatures) and orientational electric
dipole contributions. (literal)
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