Quantum-Mechanical of the Energetics of Silver Decahedron Nanoparticles

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Quantum-Mechanical of the Energetics of Silver Decahedron Nanoparticles ( quantum-mechanical-energetics-silver-decahedron-nanoparticle )

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Nanomaterials 2020, 10, 767 5 of 15 Our phenomenological approach of calculating thermodynamic properties of silver nanoclusters/nanoparticles consisting of N atoms at temperature T = 0 K is based on the following procedure. First, the Gibbs energy of the studied nanoparticle has the two contributions mentioned in Equation (6), i.e., gtot = gref + gsur. Importantly, when evaluating the reference energy gref = N · gφ Ag of the Ag nanoparticles we put the gφ equal to the reference Gibbs energy of the bulk Ebulk (per atom), Ag here fcc Ag, which we get from ab initio calculations. All the changes, which are related to the fact, that we assess nanoparticles (and not the bulk), are included in the molar volume of the studied nanoparticles Vm and the surface stress Psur, i.e., in the surface energy term Gsur: Gsur=Psur·Vm where Psur=Gsur =3·C·σsur. (8) Vm r Two further approximations are made. First, the surface stress Psur is evaluated for each relevant surface orientation, i.e., those existing on the facets of the studied nanoparticles, from the DFT calculations of infinite planar surfaces of the bulk system—see its schematic visualization in Figure 3. It means that we use a bulk-related property, the surface stress, instead of the surface stress (or surface energy) which would be related to any actual nanoparticles (there the surfaces contain edges and vertices where individual facets meet). In our particular case of decahedral nanoparticles, which have only {111} facets, our DFT calculations were performed for the (111) surface of fcc Ag. Figure 3. A schematic visualization of a computational cell, so-called slab, used for calculations of surface energy and surface stress in fcc-structure Ag (the visualization shows a 5 × 5 multiple of the studied primitive cell within the surface plane, a side view on the left, and a top view on the right). The surface is formed by the (111) crystallographic plane (see it in the middle also visualized inside a bulk fcc structure elementary cell). The second important approximative step is related to the evaluation of the molar volume of the studied nanocluster/nanoparticle. In order to assign it to a particular decahedral nanoparticle, we put the surface stress Psur equal to a fictitious hydrostatic pressure p which would be acting on every atom of the studied nanoclusters/nanoparticles. We thus do not take into account any elastic strains and stresses which are inside of decahedral nanoparticles due to the unfilled gap of 7.35◦. Instead, we apply the surface stress to all particles as if it were a hydrostatic pressure p acting upon all atoms in the nanoparticle. For calculations of the molar volume of the particle (from the known molar volume of a bulk system) we apply the following three methods.

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