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43277-B5
Better Understanding the Behavior of Hexane Deposited onto Graphite Using Improved Computer Simulations
Michael W. Roth, University of Northern Iowa
I. General Comments
We met
the proposed objectives regarding hexane on graphite (C6/gr) as well as
tetracosane on graphite (C24/gr) . Two papers have been published, and several
other studies are in progress which will lead to dissemination which credit PRF.
The work done has been disseminated in 5 conference presentations with student
co – authors.
In addition,
the funding over the last three yeas has allowed the PI to continue
collaborating with colleagues at UMC and at Penn State, to build collaborations
with scientists from Europe and, most importantly, to leverage the experience
to benefit local UNI undergraduate students. There will be publications and
presentations crediting this source of funding over the next year, and the
project will act as a seed for future work and proposals.
II. Hexane on
Graphite
A published paper is reported in the appropriate electronic location.
III. Tetracosane on Graphite
A paper in press is reported in the appropriate electronic location.
IV. Scaling
In studying C24/gr, adjustment of the nonbonded scaling
parameter in NAMD simulations is crucial in determining alkane flexibility and
hence phase transition temperatures and dynamics. The interplay between torsional
potential and the scaling of nonbonded interactions plays a crucial role in all
– atom NAMD simulations. Three alkanes (C6, C12, C24),
are simulated and the melting temperatures compared to accepted values. Thee scaling
parameter is not universal but changes with the molecular length. In fact we
are able to plot the optimal scaling factor as a function of backbone length, as
shown in Fig. 1. There is also a manuscript in preparation:
L. Firlej, B. Kuchta,
M.W. Roth, and C. Wexler, “Mechanism
of the melting transition in monolayers of alkanes adsorbed on graphite and the universality of energy
scaling”, in preparation
Figure 1. Optimal scaling factor (SF) as a function of the
inverse number of the carbons in the alkane backbone.
V. Alkane Percolation
A current percolation
study involves an extensive series of simulations of alkanes at submonolayer
coverages. Melting is directly related to lattice topology, and we concentrate
on where the adsorbate forms a connected (percolating) network. In this regime,
melting temperature is insensitive to density changes. We study four different
species (C5, C6, C12 and C24) with the intent of relating molecular flexibility
to the system’s behavior at percolation. We have completed the study for rigid
molecules (C5; C6, Fig. 2) and have moved on to more flexible species (C12;
C24).
Figure2. Low
– temperature snapshots for pentane (top row) and hexane (bottom row) layers on
graphite ant various coverages.
We continue to collaborate with Renee Diehl at Penn State
regarding fullerenes on graphite at various coverages.
Our fundamental results are not altered from those discussed last time but the
runs are being taken out much longer in order to ensure good statistics.
V. Tetracosane Bilayers
The PI and collaborators from Missouri
and Europe are currently studying C24/gr bilayer systems. The molecules in the second layer show
much more thermal agitation (gauche defects and tumbling) those in the lower
layer. The dynamics are very slow and the primary challenge is to run the
simulations out for ca. 10 ns in order to get good statistics. We expect the
results to be completed and published over the next year.
Figure3. Final snapshot side view of a C24 bilayer.
Note that the second layer shows considerably more gauche defects and signs of
thermal fluctuations than does the lower layer.
VI. Tetracosane Trilayers
The PI and the SUMR Scholar also simulated C24 trilayers this summer, with the third layer standing
perpendicular to the substrate and first two parallel layers. In addition, the
upper layer shows interesting concavity on it sides as temperature is increased
up to thermal collapse. The Scholar had some health issues this past summer and
the PI wants to involve him in as much of the science as possible so the
project will be completed and published over the next year. We are currently
running out our simulations for much longer times in order to get better
statistics.
VII. Hydrogen
The
PI conducted some NAMD hydrogen on graphite simulations and the results
are published; the paper is reported in the appropriate electronic
location.
VIII. Natural Gas / Crude
Oil
The PI and SUMR Scholar began simulating natural gas and
crude oil on graphite – the first such work to our knowledge. The crude oil is
a mixture of alkanes from C6 on up to C30, and
natural gas contains C1 – C5. We see selective adsorbtion
and interesting adsorbed molecule orientation. We are currently running
simulations out for a much longer time in order to get better statistics.
Figure4. Final snapshot of crude oil on graphite. Note the relatively
high abundance of lighter molecules in the gas phase in between the adsorbed
layers.
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