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- Table of Contents
Journal of Nanomaterials
Volume 2013 (2013), Article ID 871706, 6 pages
Methanol Adsorption on Graphene
Microtechnology and Nanoscience (MC2), Chalmers University of Technology, 412 96 Göteborg, Sweden
Received 14 March 2013; Accepted 11 August 2013
Academic Editor: Sulin Zhang
Copyright © 2013 Elsebeth Schröder. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
The adsorption energies and orientation of methanol on graphene are determined from first-principles density functional calculations. We employ the well-tested vdW-DF method that seamlessly includes dispersion interactions with all of the more close-ranged interactions that result in bonds like the covalent and hydrogen bonds. The adsorption of a single methanol molecule and small methanol clusters on graphene is studied at various coverages. Adsorption in clusters or at high coverages (less than a monolayer) is found to be preferable, with the methanol C-O axis approximately parallel to the plane of graphene. The adsorption energies calculated with vdW-DF are compared with previous DFT-D and MP2-based calculations for single methanol adsorption on flakes of graphene (polycyclic aromatic hydrocarbons). For the high coverage adsorption energies, we also find reasonably good agreement with previous desorption measurements.
Methanol (CH3OH) is the simplest of the alcohols, and it is used, for example, as a solvent, an alternative fuel, and as a source for producing other chemicals. Methanol is the second most abundant organic molecule in the atmosphere after methane (CH4), and along with other insoluble aerosol particles methanol is believed to play a role in the formation of ice in the atmosphere, as discussed and modeled, for example, in [1, 2]. Methanol is also found in the interstellar medium, as methanol ice dust grains.
In experiments where molecules are adsorbed on graphite, methanol is often used as a solvent for the larger molecules at target, and thus the adsorption properties of methanol affect the adsorption of the other molecule. Gaining access to detailed adsorption data for methanol on graphite, such as positions and energetics like those provided here, is thus valuable both directly and as input data for larger simulations of molecules on graphite embedded in the (methanol) solvent. For studies of atmospheric (water) ice formation and interstellar (methanol) ice formation the graphite surface is found to be a suitable model for the particles on which the ice forms [3, 4], further motivating our study of methanol adsorption on graphite.
In this paper, we calculate by first-principles density functional theory (DFT) the adsorption energy of methanol on graphite at various degrees of coverage (less than one molecular monolayer) and we determine the distance from and the optimal angle of the methanol molecule C-O axis with the plane of graphene. For the DFT calculations we use the method vdW-DF [5, 6].
Previously, the adsorption energies of methanol from graphene or flakes of graphene were calculated  by the semiempirical theory method DFT-D . In the study  the adsorption of methanol on to very small flakes of graphene—benzene and coronene—was also calculated by the higher-accuracy correlation method second-order Møller-Plesset perturbation theory (MP2). Desorption energies from highly oriented pyrolytic graphite (HOPG) or from various sizes of single-walled carbon nanotubes (SWCNTs) have also previously been measured in a number of desorption experiments [3, 9, 10].
The purpose of this study is to provide first-principles theory results of methanol interactions with graphite for larger-scale simulations and for interpretations of experiments. For this we determine basic information about adsorbed methanol on graphene, such as the optimal orientation the interaction (adsorption) energy at various coverages and distances from graphene. These data are then available as input to and/or for fine-tuning of molecular dynamics simulations of the methanol adsorption process.
In the following, we first introduce the methanol-graphene system, the vdW-DF method, and the setup of our calculations. Next, we describe our results both at low and high coverage of methanol on graphene and then discuss the relation to the theory results of  and some of the available experimental results.
2. Materials and Methods
On some surfaces methanol chemisorbs. When this is the case, traditional semilocal DFT methods, based on the generalized gradient expansion (GGA), may suffice for describing the adsorption. For instance, this is the case on the oxide surfaces -Al2O3 (0001) and -Cr2O3 (0001) on which we previously studied methanol adsorption [11, 12]. However, on graphene a number of small molecules physisorb, or at least owe a significant part of their adsorption energy to the dispersion interaction. Then GGA methods are inadequate.
We here use the vdW-DF method [5, 6]. It includes the van der Waals (vdW) interactions (also termed the London dispersion interactions), that are especially important on intermediate to long ranges, along with all the traits of GGA for short-range interactions. Thus, vdW-DF delivers a description of the system that takes care of both the vdW interaction between the fragments (and within the fragments) and the short-ranged interaction within the molecules, like the covalent bonding, hydrogen bonding, possible ionic interactions, and so forth, all from first principles.
Over the past few years, our group has carried out a series of physisorption studies of relatively small molecules on graphene: n-alkanes (of length 1 to 10 C atoms) , phenol , small polycyclic aromatic hydrocarbons (PAHs) [15, 16], trihalomethanes , adenine , and with somewhat different computational details, all of the five nucleobases of DNA and RNA . General considerations of use of the vdW-DF method for such systems, as well as further method discussions, can be found in [13–18] mentioned above.
We use periodic orthorhombic unit cells as detailed in Table 1, with 8–60 graphene C-atoms per unit cell. The unit cell side lengths in the plane of graphene range from 4.29 to 12.87 Å with one, three, or five methanol molecules per unit cell, as illustrated for one molecule in Figure 1 and for three and five molecules in Figure 2.
The wave functions are sampled on a regular grid with points 0.12 Å apart (the charge density is sampled at points half that distance apart) to obtain sufficient accuracy for high-quality results from the vdW-DF calculations [13, 25]. The reciprocal space -point sampling is for the largest and for the smallest unit cell, except for the calculation of isolated methanol where only the -point is used.
In all calculations, the atomic positions are allowed to relax. We use the molecular-dynamics optimization method “fast inertial relaxation engine” (FIRE)  and require that the remaining force on each atom has a size of less than 0.01 eV/Å.
We determine the adsorption energy per adsorbate, , as the difference in total energies of the full system and each fragment isolated, where is the number of molecules in the cluster (here 1, 3, or 5). The first two terms in (1) are found using the unit cell size of the full system (Table 1), whereas the last term is calculated in a Å unit cell with only -point sampling.
The data points of the potential energy curve in Figure 3 are obtained with a slightly longer unit cell than the other calculations: because we need to calculate the methanol-graphene interaction at up to relatively large separations (11 Å) the unit cell height is increased to 23 Å, all other settings remaining the same.
3. Results and Discussion
In Table 1, we list the adsorption energies for the various methanol-graphene systems that we consider. Also shown for each calculation is the coverage of methanol on graphene in units of molecular monolayers (ML), derived from the estimated area per molecule 17.6 Å2 at 1 ML obtained by Morishige et al.  from X-ray diffraction studies of a methanol film on graphite.
In the unit cell, we test starting the calculations with methanol oriented such that the C-O axis is either parallel or perpendicular to graphene (with the O atom pointing away from or towards graphene). As evident from Table 1, the almost-parallel orientation, after relaxation of the atomic positions, is energetically more favorable than the two perpendicular orientations (“O up” and “O down”). While the parallel orientation gives rise to a 219 meV (21.1 kJ/mol) binding, the perpendicular orientations only bind with 160 and 151 meV (15.5 and 14.6 kJ/mol). For the remaining calculations, we therefore start methanol oriented parallel to graphene (We did check starting with the “O down” orientation in the small unit cell, but after full relaxation of the atomic positions methanol ended up with an orientation parallel to graphene).
Ignoring the of the two perpendicular orientations (“O up” and “O down”) we see that grows with increasing coverage, from 214 meV at 0.11 ML to 361 meV at 0.92 ML, the exception being the single molecule in the unit cell. We also find that the methanol-graphene distance, here measured as the distance to O in methanol, , slightly increases with coverage, although the trend is not clear for the cluster calculations.
As seen by the growth in with coverage, the methanol molecules interact attractively, across unit cell boundaries (due to periodic boundary conditions) and for the cluster calculations also within the unit cell. The nearest-neighbor adsorbate-adsorbate distance in our single-molecule calculations varies from 12.4 Å in the largest unit cell to 4.3 Å in the smallest unit cell. In the cluster calculations, the O-to-O nearest-neighbor separation is 3.0 Å in the three-adsorbate cluster (one such interaction per unit cell) and 2.9 Å in the five-adsorbate cluster (two such nearest neighbors per unit cell).
It should be noted that the cluster calculations are started with methanol distributed at “reasonable” intermolecular separations, of 3–5 Å O-O separation for the closest molecules, not specifically in any expected cluster-configuration, and the relative orientations are not optimized for the orientations at for, example, a full ML .
It is possible to partition the adsorption energy into the contributions from the substrate-adsorbate interaction and the adsorbate-adsorbate interaction. The adsorbate-adsorbate interaction energy is found from the total energy of the system with the graphene substrate removed, all other atom positions unchanged, and subtracting the total energy of an isolated molecule (times three or five for the clusters).
For the unit cell this attractive interaction across cell boundaries amounts to a mere 2 meV per molecule (0.2 kJ/mol), it increases to 7 meV (0.7 kJ/mol) for the unit cell, and to 125 meV (12.1 kJ/mol) for the much more dense phase in the unit cell. For the three-cluster system the sum of adsorbate-adsorbate interactions per unit cell is 366 meV, thus, in average 122 meV per molecule (11.8 kJ/mol). However, as noted above and seen also in the top panel of Figure 2, one pair of molecules per unit cell is closer together than the other pair interactions, and this pair interaction is, thus, expected to dominate the sum of interaction energies. This explains why the three-cluster system yields an adsorbate-adsorbate energy at only 0.55 ML that is almost the same as the evenly distributed molecules in the unit cell at 0.83 ML.
In the five-cluster calculations, the adsorbates are in reality almost uniformly distributed within the unit cell and can hardly be considered a “cluster”. The coverage is close to a full ML and all molecules are relatively close to each other, although two O-O separations stand out as being smaller. We find the sum of adsorbate-adsorbate interactions per unit cell 909 meV, which yields an average 182 meV per adsorbate (17.5 kJ/mol), which is the largest adsorbate-adsorbate interaction energy of this study.
Thus, the methanol-methanol interactions are important as they contribute to a large fraction of the adsorption energy, but the methanol-graphene interaction is stronger. As discussed for example, in  this facilitates the formation of a full methanol monolayer prior to forming multilayers because the energy gain for the methanol molecule is larger when binding to graphene than to other methanol molecules.
In Figure 3, the potential-energy curve of various graphene-methanol separations is shown. In this figure, each data point (circle) is found by keeping the center of mass of methanol relative to the plane of graphene at the distance , shown on the bottom axis of the figure. The atoms of the molecule are allowed to move in all directions, as long as remains unchanged. Thus, the orientation of the C-O axis changes with distance from graphene, as shown by the filled circles of Figure 3. When methanol is squeezed close to graphene ( Å) the angle is smallest (the orientation is closest to being parallel), as a way for methanol to “avoid” a too close contact to graphene of any of its atoms. At the adsorption distance, the angle is approximately 10.6∘. As the fragments are further separated, the angle grows a bit until the distance Å, where the vdW interaction is too weak to change the angle from the initial angle 10.6∘ (each calculation is started with methanol in the adsorption configuration, translated towards or away from graphene).
Pankewitz and Klopper  carried out nonperiodic DFT-D calculations of methanol adsorbed on SWCNTs and PAH-models of graphene of size from benzene up to a PAH with 112 C atoms. Although the DFT-D calculations are semiempirical and, thus, can be less accurate (depending on the choice of empirical parameters for each type of calculation) the adsorption energies on PAH (Table 1) agree reasonably with the present results, when the smaller substrate size in the DFT-D calculations (due to lack of periodicity) is taken into account [18, 27]. For adsorption on to benzene and the PAH coronene (24 C) they also carried out spin-component-scaled MP2 (SCS-MP2). Their SCS-MP2 result for methanol on coronene is in good agreement with the present results. From the DFT-D calculations, we can estimate that approximately 1.3 kJ/mol of the methanol-substrate interaction is missing on coronene compared to graphene or a rather large (112-C) PAH molecule. Their SCS-MP2 coronene result of 18.3 kJ/mol should, therefore, probably be corrected to 19.6 kJ/mol for a single methanol molecule adsorption on graphene. For our largest unit cell, we find 20.6 kJ/mol and less than a 0.1 kJ/mol correction for the periodicity. Thus, our calculated energy for single methanol molecule adsorption deviates less than 1 kJ/mol (or 5%) from the estimate of the size-modified SCS-MP2 results. The distance of methanol O from graphene, , turns out identical in the two calculations.
Interestingly, in the DFT-D calculations Pankewitz and Klopper find a second, much weaker, local minimum with the methanol O atom pointing away from coronene, much like our “O-up” configuration. For this configuration, the energies and substrate-to-O distances are very similar, with 15.1 kJ/mol at 4.83 Å in the vdW-DF calculations and approximately 11 kJ/mol at 4.8 Å in the DFT-D calculations. In the binding energy curve of Figure 3, we do see a change in methanol angle with graphene as the distance is varied, but at the 4.5–5 Å center-of-mass distance from graphene the interactions are probably too weak for the computational relaxation procedure to rotate the initially almost-parallel molecule to obtain the O-up structure.
Although we did no effort in fitting a full monolayer of methanol on to graphene, it is still of interest to compare our high-coverage results with other calculations of closely packed methanol molecules. S. L. Boyd and R. J. Boyd  used DFT with B3LYP at various basis set levels to calculate the binding energies and structures of (free-floating) methanol clusters of up to 14 molecules. They expect the intermolecular interaction to be dominated by the hydrogen bonds, for which B3LYP behaves reasonably. They find that the binding energy in the optimal clusters to be 27 kJ/mol, which is larger than our largest molecule-molecule energy 17.5 kJ/mol (for the 5-molecule cluster), but then, in our calculations, there is still room for more molecules, and the molecules are constrained by the adsorption to graphene to form interactions only in two dimensions. Our smallest O-O distance of 2.9 Å (in the five-molecule cluster) compares well with the optimal O-O distance 2.77 Å in the trimer calculations of .
A number of experiments of methanol desorption from HOPG or SWCNTs have previously been carried out [3, 9, 10]. Although the desorption energies vary between the experiments, the energies for 1 ML coverage or less all fall in the range 28–51 kJ/mol (kJ/mol at 1 ML , 33–48 kJ/mol at <1 ML , 28 kJ/mol at <1 ML ), with a tendency to increase with increasing coverage. The desorption energy range is in reasonable agreement with our results, that are in the range 20–35 kJ/mol (absent the less favorable methanol orientations), with increasing adsorption energy for increasing coverage (Table 1). None of the mentioned experiments measure the distance of methanol from the substrate nor the orientation of methanol. Further comparison to experiments that are presently in progress will appear in a forthcoming publication .
By use of the first-principles vdW-DF method, we calculate adsorption energies and determine adsorption geometries of methanol on graphene. Our results are in reasonable agreement with other available calculations and experiments. This suggests that the data obtained here may be used as input parameters or tests of results from calculations and models that (unlike DFT) rely on external information, either from experiment or from (preferentially) first-principles calculations. This could, for example, be models that are on larger length scales or with time dependency, such as molecular dynamics calculations.
The author thanks Nikola Markovic, Chalmers, and Jan B. C. Pettersson, Göteborg University, for introduction to this problem and for discussions. The work was partially funded by the Swedish Research Council (VR) and the Chalmers Areas of Advances Nano and Materials. The computations were performed on resources provided by the Swedish National Infrastructure for Computing (SNIC) at C3SE.
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