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COLLEGE OF ENGINEERING Chemical, Biological &
Environmental Engineering
Introduction
As conventional energy sources begin to deplete, the need for alternative, renewable energy has
become necessary. Fuel cells have the potential to supply enough energy to power individual homes
and vehicles, as well as small, mobile devices in a cost effective and environmentally friendly manner.
Dimethyl ether (DME) is a promising fuel source that could fulfill these demands. Compared to other
well-known fuels, such as methanol or ethanol, a DME fuel cell is less toxic and stores hydrogen
more efficiently, the latter a great benefit with respect to employing fuel cells in smaller devices.
Surface Structure Sensitivity of Carbon-Oxygen
Bond Breakage within the Anode of a DME Fuel Cell
Yousif Almulla, Merissa Schneider-Coppolino and Líney Árnadóttir
School of Chemical, Biological, and Environmental Engineering
Oregon State University, Corvallis, Oregon
Methods
In conjunction with DFT, the Vienna Ab-initio Simulation Package (VASP) was used to model our
anode systems and to calculate system energies. DFT uses approximations of the Schrodinger equation
to model electron densities in atomic systems.
Different Surface Structures
Background
To produce the most efficient and effective
DME fuel cells, it is necessary to understand
the DME oxidation reaction on different
catalyst and catalyst structures. Experimental
studies have shown that the reaction rate of
dimethyl ether is different on Pt(100) and
Pt(111) surfaces. Here we use density
functional theory (DFT) to study the structural
sensitivity of the initial steps of DME
dissociation on platinum and nickel surfaces.
Different adsorption sites and configurations of
DME and C-O bond breaking dissociation
products (CH3O + CH3) are evaluated on two
different surface structures: fcc(100) and
fcc(111) for the two metals.
Figure 5: fcc (111) Adsorption Sites
Top Site
Bridge
Site
hcp
Hollow
fcc
Hollow
Figure 2: fcc (111) Side View
Figure 4: fcc (100) Side View
Figure 1: fcc (111) Top View
Figure 3: fcc (100) Top View
Results and Discussion
Platinum Nickel
fcc
(100)
fcc
(111)
Oxygen Down at Top Site
Adsorption Energy: -0.175 eV
Carbon Down at Bridge Site
Adsorption Energy: -0.113 eV
Carbon Down at Top Site
Adsorption Energy: -0.150 eV
Carbon Down at hcp Hollow
Adsorption Energy: -0.118 eV
Oxygen Down at Top Site
Adsorption Energy: -0.296 eV
Oxygen Down at Hollow Site
Adsorption Energy: -0.075 eV
a=3.976
a=3.514
-18.5
-18.0
-17.5
-17.0
-16.5
-16.0
-15.5
3.35 3.55 3.75 3.95 4.15
Energy(eV)
Lattice Constants (Å)
Platinum
Nickel
Acknowledgements
• Oregon State University Honors College
• Johnson Scholarship Program
• Dr. Liney Árnadóttir
• Graduate Students Lynza Halberstadt,
Dennis Petersen, and Qin Pang
Lattice Constants
Optimal lattice constants (a) were found, as
shown in the graph below, for both Platinum
and Nickel. These agree with experimentally
determined lattice constants, which were
found to be 3.912 and 3.499 for Platinum
and Nickel, respectively.
Adsorption
Energy
System
Energy
Surface
Energy
Adsorbate
Energy
Future Work
Next steps in this research include finding
the net change in energy after dissociation
of DME, and the activation energy of
dissociation for various surface
configurations, using the Nudged Elastic
Band (NEB) method. Both of these
energies are imperative to determining
the most promising material and material
structure for the anode catalyst. We would
also like to test more complex surfaces,
such as fcc(211) and fcc(355).
The final results will be useful for
determining potential surface structures
before conducting research within
experimental labs.
Different sites attract and repel
adsorbates differently based on the
relative proximity of electrons, and
electron density.
The adsorption energies were calculated for many different surface configurations. The
table below summarizes our initial findings for six different configurations. The Nickel
fcc(111) surface has shown the lowest adsorption energy, meaning that it has the most
favorable binding site.
References
Giustino, Feliciano. Material Modelling using Density
Functional Theory. United Kingdom: Oxford University Press,
2014. Print.
Richard, Masel I. Principles of Adsorption and Reaction on
Solid Surfaces. New York: John Wiley & Sons INC., n.d. 38-57.
Wiley Series in Chemical Engineering. Print.
Sholl, David S., and Janice A. Steckel. Density Functional
Theory A Practical Introduction. New Jersey: John Wiley &
Sons INC., 2009. Print.
Wheeler, Davey P. "Precision Measurements of the Lattice
Constants of Twelve Common Metals." Physical
Reviews 25.753 (1925). Web. 2015.

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Yousif+Merissa's Research Poster 2.0

  • 1. COLLEGE OF ENGINEERING Chemical, Biological & Environmental Engineering Introduction As conventional energy sources begin to deplete, the need for alternative, renewable energy has become necessary. Fuel cells have the potential to supply enough energy to power individual homes and vehicles, as well as small, mobile devices in a cost effective and environmentally friendly manner. Dimethyl ether (DME) is a promising fuel source that could fulfill these demands. Compared to other well-known fuels, such as methanol or ethanol, a DME fuel cell is less toxic and stores hydrogen more efficiently, the latter a great benefit with respect to employing fuel cells in smaller devices. Surface Structure Sensitivity of Carbon-Oxygen Bond Breakage within the Anode of a DME Fuel Cell Yousif Almulla, Merissa Schneider-Coppolino and Líney Árnadóttir School of Chemical, Biological, and Environmental Engineering Oregon State University, Corvallis, Oregon Methods In conjunction with DFT, the Vienna Ab-initio Simulation Package (VASP) was used to model our anode systems and to calculate system energies. DFT uses approximations of the Schrodinger equation to model electron densities in atomic systems. Different Surface Structures Background To produce the most efficient and effective DME fuel cells, it is necessary to understand the DME oxidation reaction on different catalyst and catalyst structures. Experimental studies have shown that the reaction rate of dimethyl ether is different on Pt(100) and Pt(111) surfaces. Here we use density functional theory (DFT) to study the structural sensitivity of the initial steps of DME dissociation on platinum and nickel surfaces. Different adsorption sites and configurations of DME and C-O bond breaking dissociation products (CH3O + CH3) are evaluated on two different surface structures: fcc(100) and fcc(111) for the two metals. Figure 5: fcc (111) Adsorption Sites Top Site Bridge Site hcp Hollow fcc Hollow Figure 2: fcc (111) Side View Figure 4: fcc (100) Side View Figure 1: fcc (111) Top View Figure 3: fcc (100) Top View Results and Discussion Platinum Nickel fcc (100) fcc (111) Oxygen Down at Top Site Adsorption Energy: -0.175 eV Carbon Down at Bridge Site Adsorption Energy: -0.113 eV Carbon Down at Top Site Adsorption Energy: -0.150 eV Carbon Down at hcp Hollow Adsorption Energy: -0.118 eV Oxygen Down at Top Site Adsorption Energy: -0.296 eV Oxygen Down at Hollow Site Adsorption Energy: -0.075 eV a=3.976 a=3.514 -18.5 -18.0 -17.5 -17.0 -16.5 -16.0 -15.5 3.35 3.55 3.75 3.95 4.15 Energy(eV) Lattice Constants (Å) Platinum Nickel Acknowledgements • Oregon State University Honors College • Johnson Scholarship Program • Dr. Liney Árnadóttir • Graduate Students Lynza Halberstadt, Dennis Petersen, and Qin Pang Lattice Constants Optimal lattice constants (a) were found, as shown in the graph below, for both Platinum and Nickel. These agree with experimentally determined lattice constants, which were found to be 3.912 and 3.499 for Platinum and Nickel, respectively. Adsorption Energy System Energy Surface Energy Adsorbate Energy Future Work Next steps in this research include finding the net change in energy after dissociation of DME, and the activation energy of dissociation for various surface configurations, using the Nudged Elastic Band (NEB) method. Both of these energies are imperative to determining the most promising material and material structure for the anode catalyst. We would also like to test more complex surfaces, such as fcc(211) and fcc(355). The final results will be useful for determining potential surface structures before conducting research within experimental labs. Different sites attract and repel adsorbates differently based on the relative proximity of electrons, and electron density. The adsorption energies were calculated for many different surface configurations. The table below summarizes our initial findings for six different configurations. The Nickel fcc(111) surface has shown the lowest adsorption energy, meaning that it has the most favorable binding site. References Giustino, Feliciano. Material Modelling using Density Functional Theory. United Kingdom: Oxford University Press, 2014. Print. Richard, Masel I. Principles of Adsorption and Reaction on Solid Surfaces. New York: John Wiley & Sons INC., n.d. 38-57. Wiley Series in Chemical Engineering. Print. Sholl, David S., and Janice A. Steckel. Density Functional Theory A Practical Introduction. New Jersey: John Wiley & Sons INC., 2009. Print. Wheeler, Davey P. "Precision Measurements of the Lattice Constants of Twelve Common Metals." Physical Reviews 25.753 (1925). Web. 2015.