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In honour of Prof. Mario Capitelli On the occasion of his 70th ... - CNR

In honour of Prof. Mario Capitelli On the occasion of his 70th ... - CNR

In honour of Prof. Mario Capitelli On the occasion of his 70th ... - CNR

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F. Pirani et al. PCCP 10, 5489 (2008)


EXPERIMENTAL DATA


The analysis <strong>of</strong> several experimental data allowed:-­‐The proper formula(on <strong>of</strong> an Improved Lennard Jones (IL J) modelwhere-­‐The proper descrip(on <strong>of</strong> <strong>the</strong> V dependence on <strong>the</strong> molecular orienta8on;-­‐The discovery <strong>of</strong> scaling laws (correla8on formulas): ma<strong>the</strong>ma(cal rela(ons binding well depth and its loca(on with fundamental physical proper8es <strong>of</strong> <strong>the</strong> interac(ng partners (polarizability, total charge , charge distribu8on….)


Results <strong>of</strong> <strong>the</strong> analysis <strong>of</strong> <strong>the</strong> experimental data Scaling laws + ILJThe phenomenological method-­‐Predicts <strong>the</strong> behavior <strong>of</strong> complex systems-­‐Suggests new experiments -­‐Aims relevant <strong>the</strong>ore(cal calcula(ons -­‐Helps to understand <strong>the</strong> nature <strong>of</strong> <strong>the</strong> intermolecular interac(on and to develop-­‐extend modeling


The inves(ga(on <strong>of</strong> complex systemsandThe Perugia–Bari join8ng ac8vity1) <strong>On</strong> <strong>the</strong> possibility <strong>of</strong> using model poten(als for collision integral calcula(ons <strong>of</strong> interest for planetary atmospheres (M. <strong>Capitelli</strong> et al. Chem. Phys. 338 (2007) 62);2) Classical transport collision integrals for a Lennard-­‐Jones like phenomenological model poten(al (A. Laricchiuta et al. Chem. Phys. Le+. 445 (2007) 133);3) Transport proper(es <strong>of</strong> high-­‐temperature Mars-­‐atmosphere components (A. Laricchiuta et al. Thermophysics Conference 39 th AIAA(2007) 1);4) From microscopic to macroscopic modeling <strong>of</strong> supersonic seeded atomic beam(S. Longo et al. Lecture Notes in Computer Sciences 5072 (2008) 1131);5) The role <strong>of</strong> electronically excited states on transport proper(es <strong>of</strong> air plasmas(A. Laricchiuta et al. Thermophysics Conference 40 th AIAA (2008) 127308);6) Transport proper(es <strong>of</strong> high-­‐temperature Jupiter-­‐atmosphere components(A. Laricchiuta et al. Thermophysics Conference 41 th AIAA (2009) 4257); 7) High temperature Mars atmosphere. Part I : transport cross sec(ons(A. Laricchiuta et al. Eur. Phys. J. D 54 (2009) 607);8) Collision integrals for interac(ons involving atoms in electronically excited states(A. Laricchiuta et al. J. Phys. Chem. A 113 (2009) 15250);9) Transport proper(es <strong>of</strong> high-­‐temperature Jupiter-­‐atmosphere components(A. Laricchiuta et . al. Physics <strong>of</strong> Plasmas 17 (2010) 112315).


<strong>On</strong> <strong>the</strong> role <strong>of</strong> charge transfer in <strong>the</strong> stabiliza(on <strong>of</strong> weakly bound complexes involving water and hydrogen sulphide moleculesF. Pirani, P. Candori, M.S. Pedrosa Mundim, L. Belpassi,F. Tarantelli, D. CappelleSiUniversità degli studi di Perugia ItalyThe mee(ng in <strong>honour</strong> <strong>of</strong> <strong>Mario</strong> <strong>Capitelli</strong>-­‐ Bari 31/01-­‐01/02 2011


Å 3Å 3


Å 3 Å 3Å 3Å 3


2/5


Ra(o <strong>of</strong> <strong>the</strong> well deptsRa(o <strong>of</strong> <strong>the</strong> long range a:rac(on coefficients


Ab ini(o calcula(on <strong>of</strong> <strong>the</strong> op(mized energy at <strong>the</strong>equilibrium distanceAb ini(o calcula(on <strong>of</strong> <strong>the</strong> CCSD(T)/aug-­‐ccpVQZ op(mized distance Kr-­‐X as a func(on <strong>of</strong> <strong>the</strong> orienta(on angle


=electron density change


=electron density changeSee also JACS (2010) 13046132


<strong>In</strong> <strong>the</strong> water complex <strong>the</strong> C.T. is 50-­‐150% larger providing a more effec(ve stabiliza(on


CO 2 dimer poten(al energy surface: rigid monomersThe bond-­‐bond approach -­‐ PCCP, 10, 4281 (2008) **** JCP, 130, 034110 (2009)** present calcula(ons: aug-­‐cc-­‐pVTZ basis set + bond func(ons


CO 2 dimer poten(al energy surface: rigid monomersTest on second virial coefficient data


CO 2 dimer poten(al energy surface: flexible monomers<strong>On</strong>e monomer symmetric stretchingR, Å


CO 2 dimer poten(al energy surface: flexible monomers<strong>On</strong>e monomer asymmetric stretchingR, Å


CO 2 dimer poten(al energy surface: flexible monomers<strong>On</strong>e monomer bending: averaging over monomer rota(onαR, Å

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