Protons in non-ionic aqueous reverse micelles

Using molecular dynamics techniques, we investigate the solvation of an excess proton within an aqueous reverse micelle in vacuo, with the neutral surfactant diethylene glycol monodecyl ether [CH3CH2) 11(OC2H4)2-OH]. The simulation experiments were performed using a multistate empirical valence bond...

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Publicado: 2007
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Acceso en línea:https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_15206106_v111_n17_p4432_Rodriguez
http://hdl.handle.net/20.500.12110/paper_15206106_v111_n17_p4432_Rodriguez
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spelling paper:paper_15206106_v111_n17_p4432_Rodriguez2023-06-08T16:18:56Z Protons in non-ionic aqueous reverse micelles Ethers Hamiltonians Hydrogen bonds Interfaces (materials) Molecular dynamics Protons Relaxation time Solvation Surface active agents Correlation functions Hamiltonian models Monodecyl ether Water surfactant interface Micelles Using molecular dynamics techniques, we investigate the solvation of an excess proton within an aqueous reverse micelle in vacuo, with the neutral surfactant diethylene glycol monodecyl ether [CH3CH2) 11(OC2H4)2-OH]. The simulation experiments were performed using a multistate empirical valence bond Hamiltonian model. Our results show that the stable solvation environments for the excess proton are located in the water-surfactant interface and that its first solvation shell is composed exclusively by water molecules. The relative prevalence of Eigen- versus Zundel-like solvation structures is investigated; compared to bulk results, Zundel-like structures in micelles become somewhat more stable. Characteristic times for the proton translocation jumps have been computed using population relaxation time correlation functions. The micellar rate for proton transfer is approximately 40x smaller than that found in bulk water at ambient conditions. Differences in the computed rates are examined in terms of the hydrogen-bond connectivity involving the first solvation shell of the excess charge with the rest of the micellar environment. Simulation results would indicate that proton transfers are correlated with rare episodes during which the HB connectivity between the first and second solvation shells suffers profound modifications. © 2007 American Chemical Society. 2007 https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_15206106_v111_n17_p4432_Rodriguez http://hdl.handle.net/20.500.12110/paper_15206106_v111_n17_p4432_Rodriguez
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
topic Ethers
Hamiltonians
Hydrogen bonds
Interfaces (materials)
Molecular dynamics
Protons
Relaxation time
Solvation
Surface active agents
Correlation functions
Hamiltonian models
Monodecyl ether
Water surfactant interface
Micelles
spellingShingle Ethers
Hamiltonians
Hydrogen bonds
Interfaces (materials)
Molecular dynamics
Protons
Relaxation time
Solvation
Surface active agents
Correlation functions
Hamiltonian models
Monodecyl ether
Water surfactant interface
Micelles
Protons in non-ionic aqueous reverse micelles
topic_facet Ethers
Hamiltonians
Hydrogen bonds
Interfaces (materials)
Molecular dynamics
Protons
Relaxation time
Solvation
Surface active agents
Correlation functions
Hamiltonian models
Monodecyl ether
Water surfactant interface
Micelles
description Using molecular dynamics techniques, we investigate the solvation of an excess proton within an aqueous reverse micelle in vacuo, with the neutral surfactant diethylene glycol monodecyl ether [CH3CH2) 11(OC2H4)2-OH]. The simulation experiments were performed using a multistate empirical valence bond Hamiltonian model. Our results show that the stable solvation environments for the excess proton are located in the water-surfactant interface and that its first solvation shell is composed exclusively by water molecules. The relative prevalence of Eigen- versus Zundel-like solvation structures is investigated; compared to bulk results, Zundel-like structures in micelles become somewhat more stable. Characteristic times for the proton translocation jumps have been computed using population relaxation time correlation functions. The micellar rate for proton transfer is approximately 40x smaller than that found in bulk water at ambient conditions. Differences in the computed rates are examined in terms of the hydrogen-bond connectivity involving the first solvation shell of the excess charge with the rest of the micellar environment. Simulation results would indicate that proton transfers are correlated with rare episodes during which the HB connectivity between the first and second solvation shells suffers profound modifications. © 2007 American Chemical Society.
title Protons in non-ionic aqueous reverse micelles
title_short Protons in non-ionic aqueous reverse micelles
title_full Protons in non-ionic aqueous reverse micelles
title_fullStr Protons in non-ionic aqueous reverse micelles
title_full_unstemmed Protons in non-ionic aqueous reverse micelles
title_sort protons in non-ionic aqueous reverse micelles
publishDate 2007
url https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_15206106_v111_n17_p4432_Rodriguez
http://hdl.handle.net/20.500.12110/paper_15206106_v111_n17_p4432_Rodriguez
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