Hydrocarbon rearrangements on Pt surfaces
Platinum catalysts and their alloys remain the catalyst of choice for
many hydrocarbon reforming and conversion
processes so important in chemical and petrochemical applications. In
addition, there is increased interest in improving Pt-based catalysts
for such critical applications as fuel cells. The chemistry of C1
and C2 hydrocarbons is important for many industrial
reactions
on Pt and these reactions serve as prototypes for many others.
Knowledge of the
structures, energetics, and barriers should be useful in characterizing
the mechanisms and improving the processes. Although many
experiments have characterized small hydrocarbon species on various
metal surfaces, there remains considerable uncertainty about the
structures and energetics of the chemisorbed intermediates and the role
they play in
various reaction pathways. To aid in developing improved catalysts, it
is
useful to know these quantities for a complete set of reaction
intermediates.
Using the B3LYP flavor of density functional theory (DFT) we
studied the chemisorption of all CHx and C2Hy
intermediates on the Pt(111) surface. The surface was modeled with the
35 atom Pt14.13.8 cluster, which was found to be reliable
for
describing all adsorption sites. We find that these hydrocarbons all
bind covalently
(σ-bonds) to the surface, in agreement with the studies by Kua and
Goddard on
small Pt-clusters. In nearly every case the structure of the adsorbed
hydrocarbon achieves a saturated configuration in which each C is
almost
tetrahedral with the missing H atoms replaced by covalent bonds to the
surface Pt atoms.
Thus, (Pt3)CH prefers a μ3 hollow site (fcc), (Pt2)CH2
prefers a μ2 bridge site, and PtCH3 prefers μ1
on-top sites (see Figure 1).
Figure 1: Different CHx species on Pt35.
Vinyl leads to (Pt2)CH–CH2 (Pt), which prefers a μ3
hollow site (fcc). The only exceptions to
this model are ethynyl (CCH), which binds as (Pt2)C=CH(Pt),
retaining a
CC π-bond while binding at an μ3 hollow site (fcc), and
HCCH, which binds as (Pt)HC=CH(Pt), retaining a π-bond that coordinates
to a third
atom of an μ3 hollow site (fcc) to form an off center
structure (see Figure
2). These structures are in good agreement with available experimental
data.

Figure 2: Different C2Hy species on Pt35.
For all species we calculated heats of formation ΔHf to be
used
for considering various reaction pathways on Pt(111). For conditions of
low
coverage, the most strongly bound CHx species is methylidyne
(CH, BE=146.61\,kcal/mol), and ethylidyne (CCH3,
BE=134.83\,kcal/mol)
among the C2Hy molecules. We find that the
net bond energy is nearly proportional to the number of C–Pt bonds
(48.80 kcal/mol per bond) with
the average bond energy decreasing slightly with the number of C
ligands.

Figure 3: Decomposition of ethylene with di-σ-ethylene as initial
compound.
Afterwards we used the heats of formation to analyze reactions such as
hydrogenation and decomposition of ethylene
(see Figure 3), but also the conversion of ethene to ethane (see Figure
4).
Both chemically important reactions are still under discussion
regarding the
different involved reaction steps. For the decomposition of ethylene we
were able to exclude CHCH2 and CCH2 as
intermediates.

Figure 4: Stepwise hydrogenation of ethylene.
Personnel: Dr. Timo Jacob