Abstract:Variable-temperature scanning tunneling microscopy has been used to observe molecular dynamics in the vicinity of order-disorder transitions in alkane monolayers at the interface between graphite and organic fluids. In crystalline lamellae adsorbed from solution a reversible increase in longitudinal molecular motion with increasing temperature is observed, until the amplitude becomes comparable to the lamella width and the order disappears. A two-dimensional smectic and a columnar phase are observed at the int… Show more
“…A set of n-alkanes (C N H 2Nϩ2 , Nϭ5, 6,7,8,10,12,14,16,18,20,22,24,26,44, 60͒ were purchased having purities of Ͼ98% from Aldrich Chemicals. Acros Chemicals supplied n-alkanes (Nϭ28, 32, 36, 40͒ in purities of Ͼ97%.…”
Section: Methodsmentioning
confidence: 99%
“…These phenomena are similar to those observed by Askadskaya and Rabe in their studies. 26 All the variable temperature STM images of long chain n-alkanes adsorbed on graphite suggest that heating causes displacement of methylene groups from the surface and might thereby decrease ⌬E des ‡ relative to that expected for n-alkanes in an all-trans conformation.…”
Section: Introductionmentioning
confidence: 99%
“…Such disorder has been observed in variable temperature STM images of long chain n-alkanes adsorbed on graphite which indicate that a multitude of conformations may be adopted at elevated surface temperatures. Askadskaya and Rabe 26 used a variable temperature STM to image monolayer coverages of C 24 H 50 and C 32 H 66 on graphite in air. High-resolution images of each monolayer were obtained at 297, 303, 313, and 318 K. At 297 K, highly ordered lamellae of the n-alkanes were observed with their carbon atoms in an all-trans conformation and their molecular backbone parallel to the surface.…”
The dynamics of oligomer desorption from surfaces have been studied by measuring the desorption kinetics of a set of n-alkanes from the surface of single crystalline graphite. Desorption rates were measured using a set of 21 monodispersed n-alkanes (C N H 2Nϩ2 ,5рNр60) each adsorbed at coverages in the range Ͻ0.1 to Ͼ1 monolayers. Desorption is observed to be a first-order process with a desorption barrier (⌬E des ‡ ) that is independent of coverage. The pre-exponential of the desorption rate constant is independent of the oligomer chain length and has a value of ϭ10 19.6Ϯ0.5 s Ϫ1 . We also find that ⌬E des ‡ has a nonlinear dependence on chain length and takes the empirical form ⌬E des ‡ ϭaϩbN ␥ , with the exponent having a value of ␥ϭ0.50Ϯ0.01. More interestingly, we have proposed a mechanism for the desorption process and a model for the energetics and the entropy of the oligomers on the surface that provide an extremely good quantitative fit to the observed chain length dependence of ⌬E des ‡ . ⌬E des ‡ is given by the difference in energy between the gas phase n-alkane and the conformation of the adsorbed n-alkane with the minimum free energy at the desorption temperature. These results reveal that conformational isomerism plays a significant role in determining the desorption kinetics of oligomers from surfaces.
“…A set of n-alkanes (C N H 2Nϩ2 , Nϭ5, 6,7,8,10,12,14,16,18,20,22,24,26,44, 60͒ were purchased having purities of Ͼ98% from Aldrich Chemicals. Acros Chemicals supplied n-alkanes (Nϭ28, 32, 36, 40͒ in purities of Ͼ97%.…”
Section: Methodsmentioning
confidence: 99%
“…These phenomena are similar to those observed by Askadskaya and Rabe in their studies. 26 All the variable temperature STM images of long chain n-alkanes adsorbed on graphite suggest that heating causes displacement of methylene groups from the surface and might thereby decrease ⌬E des ‡ relative to that expected for n-alkanes in an all-trans conformation.…”
Section: Introductionmentioning
confidence: 99%
“…Such disorder has been observed in variable temperature STM images of long chain n-alkanes adsorbed on graphite which indicate that a multitude of conformations may be adopted at elevated surface temperatures. Askadskaya and Rabe 26 used a variable temperature STM to image monolayer coverages of C 24 H 50 and C 32 H 66 on graphite in air. High-resolution images of each monolayer were obtained at 297, 303, 313, and 318 K. At 297 K, highly ordered lamellae of the n-alkanes were observed with their carbon atoms in an all-trans conformation and their molecular backbone parallel to the surface.…”
The dynamics of oligomer desorption from surfaces have been studied by measuring the desorption kinetics of a set of n-alkanes from the surface of single crystalline graphite. Desorption rates were measured using a set of 21 monodispersed n-alkanes (C N H 2Nϩ2 ,5рNр60) each adsorbed at coverages in the range Ͻ0.1 to Ͼ1 monolayers. Desorption is observed to be a first-order process with a desorption barrier (⌬E des ‡ ) that is independent of coverage. The pre-exponential of the desorption rate constant is independent of the oligomer chain length and has a value of ϭ10 19.6Ϯ0.5 s Ϫ1 . We also find that ⌬E des ‡ has a nonlinear dependence on chain length and takes the empirical form ⌬E des ‡ ϭaϩbN ␥ , with the exponent having a value of ␥ϭ0.50Ϯ0.01. More interestingly, we have proposed a mechanism for the desorption process and a model for the energetics and the entropy of the oligomers on the surface that provide an extremely good quantitative fit to the observed chain length dependence of ⌬E des ‡ . ⌬E des ‡ is given by the difference in energy between the gas phase n-alkane and the conformation of the adsorbed n-alkane with the minimum free energy at the desorption temperature. These results reveal that conformational isomerism plays a significant role in determining the desorption kinetics of oligomers from surfaces.
“…3,24,25 Of these systems, probably the best characterized are monolayers of C32 and C24 on high-quality graphite basal-plane surfaces that have been investigated by scanning tunneling microscopy ͑STM͒, [10][11][12][13][14] x-ray diffraction, 15 and neutron scattering. [16][17][18][19][20][21] Graphite substrates also have the advantage that relatively reliable empirical atom-atom potentials are available for representing the molecule/graphite basal-plane interaction.…”
Section: Introductionmentioning
confidence: 99%
“…Previous experimental studies of the monolayer structure of intermediate-length alkanes have focused on high-quality solid surfaces of graphite, [7][8][9][10][11][12][13][14][15][16][17][18][19][20][21] Ag͑111͒, 22,23 and SiO 2 . 3,24,25 Of these systems, probably the best characterized are monolayers of C32 and C24 on high-quality graphite basal-plane surfaces that have been investigated by scanning tunneling microscopy ͑STM͒, [10][11][12][13][14] x-ray diffraction, 15 and neutron scattering.…”
We present evidence from neutron diffraction measurements and molecular dynamics ͑MD͒ simulations of three different monolayer phases of the intermediate-length alkanes tetracosane ͑n-C 24 H 50 denoted as C24͒ and dotriacontane ͑n-C 32 H 66 denoted as C32͒ adsorbed on a graphite basal-plane surface. Our measurements indicate that the two monolayer films differ principally in the transition temperatures between phases. At the lowest temperatures, both C24 and C32 form a crystalline monolayer phase with a rectangular-centered ͑RC͒ structure. The two sublattices of the RC structure each consists of parallel rows of molecules in their all-trans conformation aligned with their long axis parallel to the surface and forming so-called lamellas of width approximately equal to the all-trans length of the molecule. The RC structure is uniaxially commensurate with the graphite surface in its ͓110͔ direction such that the distance between molecular rows in a lamella is 4.26 Å = ͱ 3a g , where a g = 2.46 Å is the lattice constant of the graphite basal plane. Molecules in adjacent rows of a lamella alternate in orientation between the carbon skeletal plane being parallel and perpendicular to the graphite surface. Upon heating, the crystalline monolayers transform to a "smectic" phase in which the inter-row spacing within a lamella expands by ϳ10% and the molecules are predominantly oriented with the carbon skeletal plane parallel to the graphite surface. In the smectic phase, the MD simulations show evidence of broadening of the lamella boundaries as a result of molecules diffusing parallel to their long axis. At still higher temperatures, they indicate that the introduction of gauche defects into the alkane chains drives a melting transition to a monolayer fluid phase as reported previously.
Monolayers of isophthalic acid derivatives at the liquid/solid interface have been studied with scanning tunneling microscopy (STM). We have investigated the dynamics related to the phenomenon of solvent co-deposition, which was previously observed by our research group when using octan-1-ol or undecan-1-ol as solvents for 5-alkoxy-isophthalic acid derivatives. This solvent co-deposition has now been visualized in real-time (two frames per second) for the first time. Dynamics of individual molecules were investigated in mixtures of semi-fluorinated molecules with video-STM. The specific contrast arising from fluorine atoms in STM images allows us to use this functionality as a probe to analyze the data obtained for the mixtures under investigation. Upon imaging the same region of a monolayer for a period of time we observed that non-fluorinated molecules progressively substitute the fluorinated molecules. These findings illustrate the metastable equilibrium that exists at the liquid/solid interface, between the physisorbed molecules and the supernatant solution.
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