Abstract:The deposition of reactive and unreactive particles on polymer surfaces at hyperthermal incident energies is investigated using classical molecular dynamics simulations. The forces are calculated with the second‐generation reactive empirical bond‐order potential with modified parameters for C,H,O interactions. Three prototypical polymers, polyethylene (PE), polypropylene (PP) and polystyrene (PS), are modified by atomic oxygen and argon that are deposited with kinetic energies of 25, 50 and 100 eV. The non‐rea… Show more
“…2) are considerably bigger than the bond energies for C-C and C-O bonds in cellulose ($3 À 4 eV for REBO potential 14 ). Similar effect can be seen in other materials, such as Si: E bond ¼ 2.3 eV and E thresh ¼ 13 eV, 16 and Fe: E bond ¼ 1.1 eV and E thresh ¼ 16 À 20 eV.…”
Using molecular dynamics simulations, we determined the threshold energy for creating defects as a function of the incident angle for all carbon and oxygen atoms in the cellulose monomer. Our analysis shows that the damage threshold energy is strongly dependent on the initial recoil direction and on average slightly higher for oxygen atoms than for carbon atoms in cellulose chain. We also performed cumulative bombardment simulations mimicking low-energy electron irradiation (such as TEM imaging) on cellulose. Analyzing the results, we found that formation of free molecules and broken glucose rings were the most common forms of damage, whereas cross-linking and chain scission were less common. Pre-existing damage was found to increase the probability of cross-linking.
“…2) are considerably bigger than the bond energies for C-C and C-O bonds in cellulose ($3 À 4 eV for REBO potential 14 ). Similar effect can be seen in other materials, such as Si: E bond ¼ 2.3 eV and E thresh ¼ 13 eV, 16 and Fe: E bond ¼ 1.1 eV and E thresh ¼ 16 À 20 eV.…”
Using molecular dynamics simulations, we determined the threshold energy for creating defects as a function of the incident angle for all carbon and oxygen atoms in the cellulose monomer. Our analysis shows that the damage threshold energy is strongly dependent on the initial recoil direction and on average slightly higher for oxygen atoms than for carbon atoms in cellulose chain. We also performed cumulative bombardment simulations mimicking low-energy electron irradiation (such as TEM imaging) on cellulose. Analyzing the results, we found that formation of free molecules and broken glucose rings were the most common forms of damage, whereas cross-linking and chain scission were less common. Pre-existing damage was found to increase the probability of cross-linking.
“…For cellulose simulations involving oxygen, we used the REBO potential for C, H, and O interactions by Ni et al 23 that was recently improved and updated by Kemper and Sinnott. 24 These simulations were carried out using a MD code written by Travis Kemper, the same code that was used in ref 24. Often irradiation of materials is simulated as a bombardment by a high-energy particle, like argon or deuteron, into the surface of the specimen. For example in the work of Beardmore et al 14 HDPE was bombarded by argon atoms with an energy of 1 keV.…”
Section: ■ Methodsmentioning
confidence: 99%
“…For cellulose simulations involving oxygen, we used the REBO potential for C, H, and O interactions by Ni et al that was recently improved and updated by Kemper and Sinnott . These simulations were carried out using a MD code written by Travis Kemper, the same code that was used in ref .…”
Irradiation effects in polyethylene and cellulose were examined using molecular dynamics simulations. The governing reactions in both materials were chain scissioning and generation of small hydrocarbon and peroxy radicals. Recombination of chain fragments and cross-linking between polymer chains were found to occur less frequently. Crystalline cellulose was found to be more resistant to radiation damage than crystalline polyethylene. Statistics on radical formation are presented and the dynamics of the formation of radiation damage discussed.
“…The reactive term in the name indicates that this potential has the capacity to model bond breaking and bond formation. The second-generation REBO potential (REBO2) 15 provided even more accurate descriptions of short-range bonding in solid state carbon materials and hydrocarbon systems, and was subsequently further extended to C-H-O, [16][17][18] C-H-F, 19 and C-H-S 20 systems. Most recently, Liang et al 21 parameterized REBO2 to model the metallic, ionic and covalent bonding present in Mo-S systems.…”
The last two decades have witnessed a dramatic rise in computational resources that has facilitated tremendous progress in computational science. In particular, this progress has enabled the application of quantum-based methods such as Hartree-Fock (HF) theory and density functional theory (DFT) to compute the potential energy surfaces of numerous complex reactions that are critical to understanding catalytic reactions. These approaches provide high fidelity because of their explicit treatment of electronic structure; however, their computational cost increases rapidly with system size. Therefore, they are limited to a relatively small number of atoms (o500). To overcome this limitation, classical empirical methods (also known as interatomic potentials) that model molecules and materials at the atomic scale without explicitly treating electrons have been developed and have been employed in molecular dynamics (MD) and Monte Carlo (MC) simulations. Such simulations have been employed to examine catalysis at length and time scales beyond the reach of quantum-based approaches.The main strength of classical empirical potentials is their low computational cost relative to electronic-structure calculations. Recently, systems with billions of atoms have been modeled in MD simulations.
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