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HAL Id: cea-02491621

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Submitted on 26 Feb 2020

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Specificity of ionic adsorption in silicas studied with

molecular dynamics and potential of mean force

S. Hocine, Bertrand Siboulet, M. Duvail, B. Coasne, P. Turq, Jean-François

Dufrêche

To cite this version:

S. Hocine, Bertrand Siboulet, M. Duvail, B. Coasne, P. Turq, et al.. Specificity of ionic adsorption in

silicas studied with molecular dynamics and potential of mean force. LowPerm 2015 - Low permeability

media and nanoporous materials from characterisation to modelling, Jun 2015, Rueil Malmaison,

France. �cea-02491621�

(2)

S. Hocine,

1

B. Siboulet,

1

M. Duvail,

1

B. Coasne,

2

P. Turq,

3

J.-F. Dufrêche

1

1Institut de Chimie Séparative de Marcoule (ICSM), UMR 5257, CEA – CNRS – UM2 – ENSCM

Site de Marcoule, Bât. 426, BP 17171, F-30207 Bagnols-sur-Cèze Cedex, France

2Department of Civil and Environmental Engineering, Massachusetts Institute of Technology,

77 Massachusetts Avenue, Cambridge, MA 02139, USA

3Université Pierre et Marie Curie Paris VI, UMR 8234, PHENIX, F-75005 Paris, France

Specificity of ionic adsorption in silicas studied with molecular

dynamics and potential of mean force

Références

[1] S. Hocine et al., J. Chem. Phys (en préparation)

[2] B. Siboulet et al., Hydrophobic transition in porous amorphous silica, J. Phys. Chem. B, 2011, 115, 7881–7886 [3] A. Grossfield, WHAM : an implementation of the weighted histogram analysis me- thod, 2008. http :// membrane.urmc.rochester.edu/content/wham

Context

ü  Radionuclides retention in glasses

ü  Decontamination of polluted soils and water

ü  Ion exchange in mesoporous oxydes

Objectives

Objectives

ü  Analyse the role of the cation on adsorption ü  Determinate

thermodynamic and kinetics properties of ions in contact with charged surfaces

ü DL_POLY

ü Water model: SPC/E

ü Simulation box: 2.8 × 2.8 × 5.0 nm3

ü Simulation time: 2 ns

ü A single net charge on the surface (oxygen atom)

ü Free energy profile vs. interatomic distance (PMF)

ü Varying hydrophilicity: 1, 29 and 57 silanols

ü Harmonic constraint at varying distances [3]

H

Si

Os

Sic

Oc

Os

Fig.1:  Snapshot  from  molecular  dynamics  showing  the  silica  surface  

with  atom  types.  [2]   Fig.3:  Histogram  of  probabili@es  vs.  distance  and  free  energy  profile  as  produced  by  WHAM.  

2,

8

nm

M

+

O

c

2,8 nm

5 nm

Fig.2:  Snapshot  of  a   molecular  dynamic  box   showing  ion  interac@on  in   wate.  The  solvated  ion  is   monitored  on  top  of  the   oxygen.  

Potential of Mean Force (PMF)

Stable configuration Activation barrier Coordonnée de réaction F re e en erg y WHAM

Association constants: two models for silica

The association constant can be calculated out of the free energy profile:

K

D

(d) = 2π

Rmax

0

exp(

−βU

eff

)r

2

dr

We consider the following adsorption reaction:

ü The interaction is much stronger with Li+ than with Cs+. ü Increasing hydrophilicity increases Li+ adsorption.

M

+

= Li

+

ou Cs

+

Mean residence time :

τ

Li

+

aq

+ O

x−

c

K

D

� Li–O

1−x

c

V =

1

2

k(r

− r

0

)

2 Average distance Stiffness constant

INTRODUCTION

BIASED MOLECULAR DYNAMICS

ynamique moléculaire

01

02

RESULTS

Fig.4 : Potential of Mean Force (PMF) for various surfaces (1 OH, 29 OH et 57 OH for 2.82 nm2) in the case of Li+ ion, vs. distance r and withε

r = 78.4 for the solvant.

vs.

Fig.5  :  Poten@al  of  Mean  Force  ,  for  the  Li+     and  Cs+,  vs.  the  distance  r,  with  

εr  =  78.4  for  le  solvant.  

Ion

Charge

on O

c

 

τ  

1  (ns)    

τ  

2  (ns)  

 

     log K

(L/mol) D

Li

-1,0

-1,5

1.6 ×10

-7

1.1×10

-6

2.7×10

-8

1,8×10

-10

0.15

4.7

ü We developped a method which provides a quantitative analysis of solvated ion to charged surface analysis.

ü PMF show oscillations similar to those observed between ions. The Lithium ion is more strongly bonded than the Cesium ion.

ü Surface hydrophilicity increases Li+ binding.

ü Association constants are very high. This shows that moddeling equilibria of such systems at the atomic level is problematic. [1]

03

CONCLUSIONS

Remerciements

In tribute to Professor Pierre Turq, deceased on 21st mai 2015.

We thank “L’Ecole Doctorale Sciences Chimiques Balard N° 459” for the grant of Sarah Hocine.

0 0,5 1 Distance / nm -30 -20 -10 0 10 20 ! Ueffectif Li+, 29 OH Cs+, 29 OH 0 0,5 1 Distance / nm -30 -20 -10 0 10 20 ! Ueffectif 0 0,5 1 Distance / nm -30 -20 -10 0 10 20 ! Ueffectif

q

Silice

= -1,0 e

q

Silice

= -1,5 e

1 OH 29 OH 57 OH Coulomb 1 OH 29 OH 57 OH Coulomb Solvant Separated Ion Pair (SSIP)

Contact Ion Pair (CIP)

Fig.6  :  In  a  Solvant  Separated  Ion  pair,  a   single  molecule  is  intercalated.    This  is  the  

second  minimum  posi@on.    

0 5 10 15 Distance / nm 0 10000 20000 30000 40000 Pro ba bi lit y

τ

1

: Average mean time for the ion to leave the bonded position.

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