ion pairing of li in water by classical and ab initio molecular … · 2015-08-23 · ion pairing...

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Ion pairing of Li + in water by classical and ab initio molecular dynamics, and neutron scattering Eva Pluhařová, Philip E. Mason, Pavel Jungwirth Institute of Organic Chemistry and Biochemistry, Academy of Sciences of the Czech Republic, Flemingovo nám. 2, 166 10 Prague 6 email: [email protected] 1. Motivation Lithium salts are of interest due their special physico-chemical properties compared to other salts. Li + differs from other alkali cations due to its small size resulting in high charge density. Lithium ion batteries are significant components of mobile electronic devices. In medicine, lithium ions are essential in the treatment of several psychiatric disorders. In all applications, lithium is active in the form of its ions, this is in contrast to much more complex organic compounds serving as drugs. Hydration is the most important type of solvation, therefore basic studies on the activity of lithium compounds have to start from hydration properties of the lithium ion in water. In simulations, the crucial step is to find reliable potentials including the essential many-body interactions. Results of classical MD simulations are sensitive to the details of the force field. Hence, there is a clear need for benchmarking and verification using ab initio based approaches. 4. Classical MD simulation of concentrated Li 2 SO 4 solution 5. Neutron scattering 2. Methods Acknowledgements Further reading 1. Petit, L.; Vuilleumier, R.; Maldivi, P.; Adamo, C. J. Chem. Theory Comput. 2008, 4, 1040. 2. Leontyev, I.; Stuchebrukhov, A. Phys. Chem. Chem. Phys. 2011, 13, 2612. 3. Fennell, C. J.; Bizjak, A.; Vlachy, V.; Dill, K. A. J. Phys. Chem. B 2009, 113, 6782. 4. Wernersson, E.; Jungwirth, P. J. Chem. Theory Comput. 2010, 6, 3233. 6. Conclusions and outlook Ab initio molecular dynamics Classical molecular dynamics Neutron scattering 3. Ab initio MD simulations of LiF ion pair CP2K program package BLYP functional with Grimmer correction GHT pseudopotential T = 300 K CSVR thermostat Short simulations 20-50 ps. Small system : 1 ion pair and 64 water molecules Evaluation of mean force Properties related to electron density. 1.5m solution, 36 Li 2 SO 4 and 1333 H 2 O in 3.45 nm box. In standard nonpolarizable simulations, Li 2 SO 4 precipitates from solution regardless of parametrization of water and ions. Effective accounting for polarization restores the solubility. Reparametrization of Li + (decreasing s from ~2.1 to ~1.8 Å) corrects radial distribution function of Li-water oxygen. First order 6/7 Li NDIS difference For several snapshots with ion-ion separations ranging from 1.9 to 3.7 Å , charges assigned to Li and F were calculated using the Bader scheme resulting in values of 0.9 and -0.8. Single ion pair Estimates of ionic charges, amount of charge transferred to solvent and distribution of water molecules around ion pair are accessible using ab initio methodology. The first step towards ab initio potential of mean force. Concentrated solution Electronic Continuum Correction (rescaling sulphate and lithium charges by 0.75) provides significantly better fit to neutron scattering data than regular force field. The displacement of the position of the first Li-water oxygen was corrected by reducing the size of Li + ion from ~2.1 to ~1.8 Å in the ECC simulations, which produced a much better agreement with the structural data. With careful parametrization, simulations are able to reproduce neutron scattering data. Experiments performed at ILL neutron reactor (France) Technique Neutron Diffraction with Isotopic Substitution (NDIS). 6/7 Li substitution in D 2 O solution Gromacs program package Empirical force field OPLS ions, Dang also tested TIP4P, SPC/E water Polarization effects are accounted for effectively within an electronic continuum correction (ECC) T = 300 K CSVR thermostat Long simulations tens of ns Finite concentrations Li F integral of mean force volume entropy correction Comparison of MD and Neutron scattering result Unscaled charges ECC ECC (reparametrized Li + ) Neutron scattering ) ( 003 . 0 ) ( 034 . 0 ) ( 88 . 2 ) ( 98 . 5 ) ( Q S Q S Q S Q S Q S LiLi LiS LiO LiH Li The constitution of the first order NDIS difference is: This was calculated from the MD simulations (red) and compared to the experimental data (black). Geometrically simple, but chemically complex lithium fluoride ion pair due to high charge density and possibility of charge transfer to solvent. NVT ensemble with fixed box size of 1.26 nm Mean force for constrained LiF distances. Potential of mean force (W): =− d 0 + 2 B ln + . Integration of the real space data NDIS function (arbitrary units)

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Page 1: Ion pairing of Li in water by classical and ab initio molecular … · 2015-08-23 · Ion pairing of Li+ in water by classical and ab initio molecular dynamics, and neutron scattering

Ion pairing of Li+ in water by classical and ab initio

molecular dynamics, and neutron scattering Eva Pluhařová, Philip E. Mason, Pavel Jungwirth

Institute of Organic Chemistry and Biochemistry, Academy of Sciences of the Czech Republic, Flemingovo nám. 2, 166 10 Prague 6

email: [email protected]

1. Motivation

• Lithium salts are of interest due their special physico-chemical properties compared to other

salts.

• Li+ differs from other alkali cations due to its small size resulting in high charge density.

• Lithium ion batteries are significant components of mobile electronic devices.

• In medicine, lithium ions are essential in the treatment of several psychiatric disorders. In all

applications, lithium is active in the form of its ions, this is in contrast to much more complex

organic compounds serving as drugs.

• Hydration is the most important type of solvation, therefore basic studies on the activity of

lithium compounds have to start from hydration properties of the lithium ion in water.

• In simulations, the crucial step is to find reliable potentials including the essential many-body

interactions.

• Results of classical MD simulations are sensitive to the details of the force field. Hence, there

is a clear need for benchmarking and verification using ab initio based approaches.

4. Classical MD simulation of concentrated Li2SO4 solution

5. Neutron scattering

2. Methods

Acknowledgements Further reading

1. Petit, L.; Vuilleumier, R.; Maldivi, P.; Adamo, C. J. Chem. Theory Comput. 2008, 4, 1040.

2. Leontyev, I.; Stuchebrukhov, A. Phys. Chem. Chem. Phys. 2011, 13, 2612.

3. Fennell, C. J.; Bizjak, A.; Vlachy, V.; Dill, K. A. J. Phys. Chem. B 2009, 113, 6782.

4. Wernersson, E.; Jungwirth, P. J. Chem. Theory Comput. 2010, 6, 3233.

6. Conclusions and outlook

Ab initio molecular dynamics Classical molecular dynamics Neutron scattering

3. Ab initio MD simulations of LiF ion pair

• CP2K program package

• BLYP functional with

Grimmer correction

• GHT pseudopotential

• T = 300 K

• CSVR thermostat

• Short simulations 20-50 ps.

• Small system : 1 ion pair

and 64 water molecules

• Evaluation of mean force

• Properties related to

electron density.

• 1.5m solution, 36 Li2SO4 and 1333 H2O in 3.45 nm box.

• In standard nonpolarizable simulations, Li2SO4 precipitates from solution regardless of

parametrization of water and ions.

• Effective accounting for polarization restores the solubility.

• Reparametrization of Li+ (decreasing s from ~2.1 to ~1.8 Å) corrects radial distribution

function of Li-water oxygen.

First order 6/7Li NDIS difference

• For several snapshots with ion-ion separations

ranging from 1.9 to 3.7 Å , charges assigned to

Li and F were calculated using the Bader

scheme resulting in values of 0.9 and -0.8.

Single ion pair

• Estimates of ionic charges, amount of charge transferred to solvent and distribution of water

molecules around ion pair are accessible using ab initio methodology.

• The first step towards ab initio potential of mean force.

Concentrated solution

• Electronic Continuum Correction (rescaling sulphate and lithium charges by 0.75) provides

significantly better fit to neutron scattering data than regular force field.

• The displacement of the position of the first Li-water oxygen was corrected by reducing the size

of Li+ ion from ~2.1 to ~1.8 Å in the ECC simulations, which produced a much better

agreement with the structural data.

• With careful parametrization, simulations are able to reproduce neutron scattering data.

• Experiments

performed at ILL

neutron reactor

(France)

• Technique Neutron

Diffraction with

Isotopic Substitution

(NDIS).

• 6/7Li substitution in

D2O solution

• Gromacs program package

• Empirical force field

• OPLS ions, Dang also tested

• TIP4P, SPC/E water

• Polarization effects are

accounted for effectively

within an electronic

continuum correction (ECC)

• T = 300 K

• CSVR thermostat

• Long simulations tens of ns

• Finite concentrations

Li F

integral of mean force volume entropy correction

Comparison of MD and Neutron scattering result

Unscaled charges

ECC

ECC (reparametrized Li+)

Neutron scattering

)(003.0)(034.0)(88.2)(98.5)( QSQSQSQSQS LiLiLiSLiOLiHLi

The constitution of the first order NDIS difference is:

This was calculated from the MD simulations (red) and compared to the experimental data (black).

• Geometrically simple, but chemically complex

lithium fluoride ion pair due to high charge density

and possibility of charge transfer to solvent.

• NVT ensemble with fixed box size of 1.26 nm

• Mean force 𝐹 for constrained LiF distances.

• Potential of mean force (W):

𝑊 𝑟 = − 𝐹 𝑟′ d𝑟′𝑟

𝑟0

+ 2𝑘B𝑇ln 𝑟 + 𝑐𝑜𝑛𝑠𝑡.

Integration of the real space data NDIS function (arbitrary units)