A molecular dynamics study of the evolution from the formation of the $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 -( $${\text {H}}_{2}{\text {O}})_{n}$$ H 2 O ) n small aggregates to the $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 solvation

Verfasser / Beitragende:
[M. Albertí, A. Amat, A. Aguilar, F. Huarte-Larrañaga, J. Lucas, F. Pirani]
Ort, Verlag, Jahr:
2015
Enthalten in:
Theoretical Chemistry Accounts, 134/5(2015-05-01), 1-12
Format:
Artikel (online)
ID: 605488215
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024 7 0 |a 10.1007/s00214-015-1662-2  |2 doi 
035 |a (NATIONALLICENCE)springer-10.1007/s00214-015-1662-2 
245 0 2 |a A molecular dynamics study of the evolution from the formation of the $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 -( $${\text {H}}_{2}{\text {O}})_{n}$$ H 2 O ) n small aggregates to the $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 solvation  |h [Elektronische Daten]  |c [M. Albertí, A. Amat, A. Aguilar, F. Huarte-Larrañaga, J. Lucas, F. Pirani] 
520 3 |a The interaction between hexafluorobenzene, $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 , and $${\text {H}}_{2}$$ H 2 O is investigated to construct a force field for molecular dynamics simulations. In order to construct the $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 - $${\text {H}}_{2}$$ H 2 O intermolecular interaction function, the nonpermanent charge contributions, grouped in the so-called nonelectrostatic term and described using an improved Lennard-Jones model, are combined with the electrostatic energy calculated in agreement with the permanent electric quadrupole and dipole moments of $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 and $${\text {H}}_{2}$$ H 2 O, respectively. Moreover, to test the potential energy function, BSSE-corrected energies at CCSD(T)/aug-cc-pVTZ level are calculated for three different approaches of $${\text {H}}_{2}{\text {O}}$$ H 2 O - $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 . By using the constructed force field, the structure and energetics of some small aggregates [ $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 -( $${\text {H}}_{2}{\text {O}})_{n}$$ H 2 O ) n ( $$n= 1{\text {--}}6$$ n = 1 -- 6 )], the formation of the first solvation shell [ $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 -( $${\text {H}}_{2}{\text {O}})_{n}$$ H 2 O ) n ( $$n = 9{\text {--}}36$$ n = 9 -- 36 )] and the solvation of $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 by 400 molecules of $${\text {H}}_{2}$$ H 2 O have been investigated. The $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 -( $${\text {H}}_{2}{\text {O}})_{n}$$ H 2 O ) n ( $$n= 1{\text {--}}6$$ n = 1 -- 6 ) small aggregates and the formation of the first solvation shell have been simulated using a microcanonical (NVE) ensemble of particles, while an isobaric-isothermal ensemble (NpT) has been used to investigate the solvation of $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 . Moreover, in order to approximate the system formed by one $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 and 400 $${\text {H}}_{2}$$ H 2 O molecules to a large (infinite) system, periodic boundary conditions have been imposed in the simulation of the solvation of $${\text {C}}_{6}{\text {F}}_{6}$$ C 6 F 6 . 
540 |a Springer-Verlag Berlin Heidelberg, 2015 
690 7 |a Weak interactions  |2 nationallicence 
690 7 |a Semi-empirical potential  |2 nationallicence 
690 7 |a Solvation shells  |2 nationallicence 
690 7 |a Hydration  |2 nationallicence 
700 1 |a Albertí  |D M.  |u IQTCUB, Departament de Química Física, Universitat de Barcelona, 08028, Barcelona, Spain  |4 aut 
700 1 |a Amat  |D A.  |u Computational Laboratory for Hybrid/Organic Photovoltaics (CLHYO), Istituto CNR di Scienze e Tecnologie Molecolari, Perugia, Italy  |4 aut 
700 1 |a Aguilar  |D A.  |u IQTCUB, Departament de Química Física, Universitat de Barcelona, 08028, Barcelona, Spain  |4 aut 
700 1 |a Huarte-Larrañaga  |D F.  |u IQTCUB, Departament de Química Física, Universitat de Barcelona, 08028, Barcelona, Spain  |4 aut 
700 1 |a Lucas  |D J.  |u IQTCUB, Departament de Química Física, Universitat de Barcelona, 08028, Barcelona, Spain  |4 aut 
700 1 |a Pirani  |D F.  |u Dipartimento di Chimica, Biologia e Biotecnologie, Università di Perugia, 06123, Perugia, Italy  |4 aut 
773 0 |t Theoretical Chemistry Accounts  |d Springer Berlin Heidelberg  |g 134/5(2015-05-01), 1-12  |x 1432-881X  |q 134:5<1  |1 2015  |2 134  |o 214 
856 4 0 |u https://doi.org/10.1007/s00214-015-1662-2  |q text/html  |z Onlinezugriff via DOI 
898 |a BK010053  |b XK010053  |c XK010000 
900 7 |a Metadata rights reserved  |b Springer special CC-BY-NC licence  |2 nationallicence 
908 |D 1  |a research-article  |2 jats 
949 |B NATIONALLICENCE  |F NATIONALLICENCE  |b NL-springer 
950 |B NATIONALLICENCE  |P 856  |E 40  |u https://doi.org/10.1007/s00214-015-1662-2  |q text/html  |z Onlinezugriff via DOI 
950 |B NATIONALLICENCE  |P 700  |E 1-  |a Albertí  |D M.  |u IQTCUB, Departament de Química Física, Universitat de Barcelona, 08028, Barcelona, Spain  |4 aut 
950 |B NATIONALLICENCE  |P 700  |E 1-  |a Amat  |D A.  |u Computational Laboratory for Hybrid/Organic Photovoltaics (CLHYO), Istituto CNR di Scienze e Tecnologie Molecolari, Perugia, Italy  |4 aut 
950 |B NATIONALLICENCE  |P 700  |E 1-  |a Aguilar  |D A.  |u IQTCUB, Departament de Química Física, Universitat de Barcelona, 08028, Barcelona, Spain  |4 aut 
950 |B NATIONALLICENCE  |P 700  |E 1-  |a Huarte-Larrañaga  |D F.  |u IQTCUB, Departament de Química Física, Universitat de Barcelona, 08028, Barcelona, Spain  |4 aut 
950 |B NATIONALLICENCE  |P 700  |E 1-  |a Lucas  |D J.  |u IQTCUB, Departament de Química Física, Universitat de Barcelona, 08028, Barcelona, Spain  |4 aut 
950 |B NATIONALLICENCE  |P 700  |E 1-  |a Pirani  |D F.  |u Dipartimento di Chimica, Biologia e Biotecnologie, Università di Perugia, 06123, Perugia, Italy  |4 aut 
950 |B NATIONALLICENCE  |P 773  |E 0-  |t Theoretical Chemistry Accounts  |d Springer Berlin Heidelberg  |g 134/5(2015-05-01), 1-12  |x 1432-881X  |q 134:5<1  |1 2015  |2 134  |o 214