Range, Strength
and Anisotropy of Intermolecular Forces in Atom-Molecule Systems: an Atom-Bond
Pairwise Additivity Approach
F. Pirani, D. Cappelletti and G. Liuti
INFM
and Dipartimento di Chimica and Dipartimento di Ingegneria Civile ed Ambientale
Universita’
di Perugia, 060123-Perugia, Italy
A new method is
proposed for calculations of intermolecular interactions in van der Waals complexes which is of general
applicability and gives accurate results with a negligible effort in terms of
computing time. The method is based on correlation formulas between the
polarizability of the interacting partners and the main interaction
parameters. Our attention was
originally addressed to spherical atom--closed shell atom systems [1,2,3] bound
by typical van der Waals forces, where the attractive and repulsive component
of the interaction were modeled in terms only of the polarizabilities of the
interacting partners. This represented the foundation for a proper description
of ion--atom [4] ion--ion [5], and open shell atom--closed shell particle
systems [6,7],
where in addition to van der Waals forces, additional interaction components
operate.
The present work
[8] is concerned with the extension of the method to systems involving diatoms
or polyatomic molecules interacting with a closed shell atom. The basic idea is
to consider the molecular size as determined by the bonds nearest to the approaching atom and to delocalize
the dispersion centers on the molecule by using additively bond
polarizabilities. The method, tested mainly on homonuclear diatomics-rare gas
and simple hydrocarbon-rare gas complexes for which experimental and
theoretical information is available, is used to make predictions for systems
of higher complexity up to a graphite plane. Tables 1-4 below illustrate the
quality of the agreement and some example of the applications. This effort is
worthwhile for an advanced and systematic study of phenomena like collisional
alignment, broadening and shift of spectral lines of molecules in very
different environments, steric effects
in elementary processes, chemistry and physics of aggregates, transport
properties in gas phase and physical absorption on surfaces. Moreover, as for
atom--atom cases, the results of this work could be crucial for a proper rapresentation
of systems with increasing complexity where in addition to typical van der
Waals forces, induction, electrostatic and chemical contributions can operate.
Table 1
– Interaction features for some homonuclear diatom-Ar systems in the two
limiting parallel and perpendicular configurations.
|
|
parallel |
|
|
perpendicular |
|
|
|
|
Rm(Ĺ) |
e (meV) |
|
Rm(Ĺ) |
e (meV) |
|
|
H2-Ar |
3.32 |
3.32 |
|
3.35 |
3.24 |
present |
|
|
3.35 |
3.08 |
|
3.28 |
2.78 |
Exp. (LeRoy) |
|
O2-Ar |
4.11 |
9.07 |
|
3.61 |
13.6 |
|
|
|
4.00 |
9.50 |
|
3.56 |
14.0 |
Exp. (Pirani) |
|
N2-Ar |
4.07 |
9.27 |
|
3.68 |
13.0 |
|
|
|
4.28 |
7.6 |
|
3.68 |
13.2 |
Exp. (Casavecchia) |
Table 2
– Interaction features for benzene-rare gas systems in the perpendicular
configurations.
|
|
Rm(Ĺ) |
e (meV) |
|
|
C6H6-He |
3.24 |
10.3 |
present |
|
|
3.17 |
|
Exp. (Smalley) |
|
|
3.3 |
8.4 |
Calc. (Hobza) |
|
|
|
|
|
|
C6H6-Ne |
3.28 |
21.0 |
|
|
|
3.30 |
|
Exp. (Bauder) |
|
|
3.32 |
19.8 |
Calc. (Bauder) |
|
|
|
|
|
|
C6H6-Ar |
3.55 |
46.0 |
|
|
|
|
<46.4 |
Exp. (Meijer) |
|
|
3.50 |
|
Exp. (Bauder) |
|
|
3.55 |
47.9 |
Calc. (Makarewitz) |
|
|
|
|
|
|
C6H6-Kr |
3.69 |
55.9 |
|
|
|
3.68 |
<57 |
Exp. (Neusser) |
|
|
3.66 |
|
Exp. (Gutowski) |
|
|
3.7 |
60 |
Calc. (Hobza) |
|
|
|
|
|
|
C6H6-Xe |
3.89 |
63.3 |
|
|
|
3.77 |
|
Exp. (Bauder) |
|
|
3.9 |
75 |
Calc. (Hobza) |
|
|
|
|
|
Table 3
– Interaction features for coronene-rare gas, N2 and O2
systems.
|
|
Rm(Ĺ) |
e (meV) |
|
C23H12-He |
3.43 |
13 |
|
C23H12-Ne |
3.43 |
29 |
|
C23H12-Ar |
3.61 |
75 |
|
C23H12-Kr |
3.73 |
96 |
|
C23H12-Xe |
3.90 |
116 |
|
C23H12-N2 |
3.63 |
75 |
|
C23H12-O2 |
3.60 |
76 |
Table 4
– Interaction energy (in meV) for rare gas atoms interacting with a single
layer of graphite (G).
|
|
present
|
experiment |
|
G-He |
15 |
17 |
|
G-Ne |
31 |
33 |
|
G-Ar |
74 |
96 |
|
G-Kr |
93 |
125 |
|
G-Xe |
112 |
162 |
References
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F.Pirani, Chem. Phys. Lett., 122 (1985) 245.
[2] V.Aquilanti,
G.Liuti, F.Pirani and F.Vecchiocattivi, J.Chem.Soc.Faraday Trans., 2 85 (1989)
955.
[3] R.Cambi, D.Cappelletti, G.Liuti, and F.Pirani, J. Chem. Phys., 95, 1852
(1991).
[4] D.Cappelletti, G.Liuti and F.Pirani, Chem. Phys. Lett., 183
(1991) 297.
[5] V. Aquilanti, D. Cappelletti, F.Pirani, Chem. Phys, 209, 299
(1996).
[6] V. Aquilanti, D. Cappelletti, F.Pirani, Chem. Phys. Lett., 271, 216 (1997).
[7] F.Pirani, A. Giulivi,
D. Cappelletti, and V. Aquilanti, Mol. Phys., 98, 1749 (2000).
[8] F. Pirani,
D.Cappelletti, G. Liuti, submitted for
publication (2001).