1
2.5 nm 2.5 nm Results Visualization of Systems: Rutile System Graphite System Bulk System Local Densities of Species: Mean Squared Displacements: Molecular Simula-on of a Deep Eutec-c Solvent Inside Nanoporous Materials Jasmine Chappell 1 , Yan Shen 2 , Francisco R. Hung 2 1 Department of Chemical Engineering, Tuskegee University, Tuskegee, AL 2 Cain Department of Chemical Engineering, Louisiana State University, Baton Rouge, LA Abstract Producers of solar energy utilize dye-synthesized solar cells (DSSCs), used to convert sunlight into energy. Within the cell, ionic liquids (ILs) act as electrolytes to move the charges which create energy. These ILs have properties negative for the environment, such as their toxicity, and are more costly than alternatives which are still in development. One such alternative is the deep eutectic solvent (DES) which is a mixture of two solids (an acceptor and a donor of hydrogen bonds) which, when mixed in a particular ratio, has a lower melting point than either of its components and forms a liquid at room temperature. DESs have been experimentally found to have similar chemical and physical properties as ILs while having a significantly lower cost and almost no toxicity. Here, molecular dynamics (MD) simulations were performed in order to understand fundamental and molecular properties of a choline iodide/glycerol DES in nanopores of different chemical composition, compared against that in bulk. Results of density profiles showed that the DES aggregated near the pore walls in both confined systems. Our results suggest that glycerol tends to form hydrogen bonds with the titania walls, and as a result, the dynamics of the DES in titania are much slower than that in graphite and in the bulk. Overall, results show a notable difference between the properties of the DES in pores of different chemical composition, and in bulk versus non-bulk samples. Acknowledgements This material is based upon work supported by the National Science Foundation under the NSF EPSCoR Cooperative Agreement No. EPS-1003897 with additional support from the Louisiana Board of Regents. In onrder to conduct my research, I utilized resources from HPC@LSU, and the Louisiana Optic Network Initiative (LONI). I thank my fellow REU students for their support. Conclusions Dynamic properties of all three species change when in confinement; particularly the density of hydrogen bonding properties of glycerol. Of the confined systems, the graphite system shows behavior more similar to that of the bulk system (e.g., subtler density peaks, non-linear ends to MSD within 20 ns, displacement). More study can be done to analyze the behavior of species among density layers All data can be used to further compare behavior of DESs to ILs in confinement and evaluate DESs as a substitute. Introduction DESs are used as alternative electrolytes in DSSCs. They share physical, chemical properties of ILs, but are less expensive and (mostly) nontoxic. The DES studied was a 1:3 mole ratio mixture of choline iodide and glycerol. Materials and Methods GROMACS and VMD (Visual Molecular Dynamics) software to run simulation: DES (1:3 mol ratio Choline Iodide and Glycerol) in 2.5 nm pore of titania or graphite and in bulk system under applied force field, general AMBER force field (GAFF) under initial temperature 500K Interpretation Local densities Partial densities reflect volume of planes 1/10 the height of the entire system, the length of the system’s pore wall, and the width of the system’s pore wall (2.5 nm) divided by the mass of solvent in that volume. No peaks (i.e., consistent density profiles) of all species in bulk proves effect of chemical interactivity with pore walls. High local density of glycerol near pore walls, more prominently in rutile system (titania pore walls) Glycerol can hydrogen bond to titania walls; no hydrogen bonds with graphitic walls. Mean Square Displacements MSD represents displacement of molecules of each species the 20 ns simulation of each system. Linear MSD plots reflect diffusive displacement (random). Exponential MSD plots (such as the final portions of those of the graphite and bulk systems) indicate a directionality of movement. Hydrogen Bonding Plots answer the question, “what fraction of this bond type appears this percentage of the 20 ns simulation?” This is important to consider because hydrogen bonds affect melting point, the characteristic which takes DES from solid to liquid when mixed; the bonds affect phase of solvent. All plots reflect high number of fleeting bonds and low number of enduring bonds. Plots reflect generally similar hydrogen bonding behavior in confined systems vs. bulk; especially the GLY-GLY bond. GLY-GLY bond behaves similarly regardless of system. GLY-IOD behaves differently in bulk than in confinement; higher fraction of this bond type exists at low percentage occupancy. Glycerol Choline Iodide Titania Graphite 0 500 1000 1500 2000 2500 0 0.5 1 1.5 2 2.5 Density (kg/m 3 ) z-coordinate (nm) 0 100 200 300 400 500 600 0 0.5 1 1.5 2 2.5 Density (kg/m 3 ) z-coordinate (nm) 0 200 400 600 800 1000 0 0.5 1 1.5 2 2.5 Density (kg/m 3 ) z-coordinate (nm) Rutile Graphite Bulk 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 0 5000 10000 15000 20000 MSD (nm 2 ) Time (ps) 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 0 5000 10000 15000 20000 MSD (nm 2 ) Time (ps) 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 0 5000 10000 15000 20000 MSD (nm 2 ) Time (ps) 0 0.03 0.06 0.09 0.12 0.15 0% 20% 40% 60% 80% 100% Fraction of Hydrogen Bonds Percentage Occupancy 0 0.03 0.06 0.09 0.12 0.15 0% 20% 40% 60% 80% 100% Fraction of Hydrogen Bond Percentage Occupancy 0 0.03 0.06 0.09 0.12 0.15 0% 20% 40% 60% 80% 100% Fraction of Hydrogen Bond Percentage Occupancy Rutile Graphite Bulk CHO-GLY CHO-IOD GLY-GLY GLY-IOD Scheme of a Dye- Synthesized Solar Cell Composition of DES studied Rutile Graphite Bulk Hydrogen Bonding of Systems Glycerol Choline Iodide Glycerol Choline Iodide

Molecular)Simula-on)of)a)Deep)Eutec-c)Solvent)Inside ... · 2.5 nm 2.5 nm Results Visualization of Systems: Rutile System Graphite System Bulk System Local Densities of Species: Mean

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Page 1: Molecular)Simula-on)of)a)Deep)Eutec-c)Solvent)Inside ... · 2.5 nm 2.5 nm Results Visualization of Systems: Rutile System Graphite System Bulk System Local Densities of Species: Mean

2.5 nm 2.5 nm

Results

Visualization of Systems:

Rutile System Graphite System Bulk System

Local Densities of Species: Mean Squared Displacements:

Molecular  Simula-on  of  a  Deep  Eutec-c  Solvent  Inside  Nanoporous  Materials  Jasmine  Chappell1,  Yan  Shen2,  Francisco  R.  Hung2  1Department  of  Chemical  Engineering,  Tuskegee  University,  Tuskegee,  AL  2Cain  Department  of  Chemical  Engineering,  Louisiana  State  University,  Baton  Rouge,  LA  

Abstract

Producers of solar energy utilize dye-synthesized solar cells (DSSCs), used to convert sunlight into energy. Within the cell, ionic liquids (ILs) act as electrolytes to move the charges which create energy. These ILs have properties negative for the environment, such as their toxicity, and are more costly than alternatives which are still in development. One such alternative is the deep eutectic solvent (DES) which is a mixture of two solids (an acceptor and a donor of hydrogen bonds) which, when mixed in a particular ratio, has a lower melting point than either of its components and forms a liquid at room temperature. DESs have been experimentally found to have similar chemical and physical properties as ILs while having a significantly lower cost and almost no toxicity. Here, molecular dynamics (MD) simulations were performed in order to understand fundamental and molecular properties of a choline iodide/glycerol DES in nanopores of different chemical composition, compared against that in bulk. Results of density profiles showed that the DES aggregated near the pore walls in both confined systems. Our results suggest that glycerol tends to form hydrogen bonds with the titania walls, and as a result, the dynamics of the DES in titania are much slower than that in graphite and in the bulk. Overall, results show a notable difference between the properties of the DES in pores of different chemical composition, and in bulk versus non-bulk samples.

Acknowledgements

§  This material is based upon work supported by the National Science Foundation under the NSF EPSCoR Cooperative Agreement No. EPS-1003897 with additional support from the Louisiana Board of Regents. In onrder to conduct my research, I utilized resources from HPC@LSU, and the Louisiana Optic Network Initiative (LONI).

§  I thank my fellow REU students for their support.

Conclusions

•  Dynamic properties of all three species change when in confinement; particularly the density of hydrogen bonding properties of glycerol.

•  Of the confined systems, the graphite system shows behavior more similar to that of the bulk system (e.g., subtler density peaks, non-linear ends to MSD within 20 ns, displacement).

•  More study can be done to analyze the behavior of species among density layers

•  All data can be used to further compare behavior of DESs to ILs in confinement and evaluate DESs as a substitute.

Introduction

DESs are used as alternative electrolytes in DSSCs. They share physical, chemical properties of ILs, but are less expensive and (mostly) nontoxic.

The DES studied was a 1:3 mole ratio mixture of choline iodide and glycerol.

Materials and Methods

•  GROMACS and VMD (Visual Molecular Dynamics) software to run simulation: •  DES (1:3 mol ratio Choline Iodide and Glycerol) •  in 2.5 nm pore of titania or graphite •  and in bulk system •  under applied force field, general AMBER force field (GAFF) •  under initial temperature 500K

Interpretation

Local densities •  Partial densities reflect volume of planes 1/10 the height of the entire

system, the length of the system’s pore wall, and the width of the system’s pore wall (2.5 nm) divided by the mass of solvent in that volume.

•  No peaks (i.e., consistent density profiles) of all species in bulk proves effect of chemical interactivity with pore walls.

•  High local density of glycerol near pore walls, more prominently in rutile system (titania pore walls) •  Glycerol can hydrogen bond to titania walls; no hydrogen bonds with

graphitic walls.

Mean Square Displacements •  MSD represents displacement of molecules of each species the 20 ns

simulation of each system. •  Linear MSD plots reflect diffusive displacement (random). •  Exponential MSD plots (such as the final portions of those of the graphite

and bulk systems) indicate a directionality of movement.

Hydrogen Bonding •  Plots answer the question, “what fraction of this bond type appears this

percentage of the 20 ns simulation?” •  This is important to consider because hydrogen bonds affect melting

point, the characteristic which takes DES from solid to liquid when mixed; the bonds affect phase of solvent.

•  All plots reflect high number of fleeting bonds and low number of enduring bonds.

•  Plots reflect generally similar hydrogen bonding behavior in confined systems vs. bulk; especially the GLY-GLY bond.

•  GLY-GLY bond behaves similarly regardless of system. •  GLY-IOD behaves differently in bulk than in confinement; higher fraction of

this bond type exists at low percentage occupancy.

Glycerol Choline Iodide Titania Graphite

0

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0 0.5 1 1.5 2 2.5

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0 0.5 1 1.5 2 2.5

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Rutile Graphite Bulk

0 0.2 0.4 0.6 0.8

1 1.2 1.4 1.6 1.8

2

0 5000 10000 15000 20000

MS

D (n

m2 )

Time (ps)

0 0.2 0.4 0.6 0.8

1 1.2 1.4 1.6 1.8

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0 5000 10000 15000 20000

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D (n

m2 )

Time (ps)

0 0.2 0.4 0.6 0.8

1 1.2 1.4 1.6 1.8

0 5000 10000 15000 20000 M

SD

(nm

2 )

Time (ps)

0

0.03

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0% 20% 40% 60% 80% 100% Frac

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Rutile Graphite Bulk

CHO-GLY

CHO-IOD

GLY-GLY

GLY-IOD

Scheme of a Dye-Synthesized Solar Cell

Composition of DES studied

Rutile Graphite

Bulk

Hydrogen Bonding of Systems

Glycerol

Choline

Iodide

Glycerol

Choline

Iodide