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Total energy density

A typical molecular dynamics simulation comprises an equflibration and a production phase. The former is necessary, as the name imphes, to ensure that the system is in equilibrium before data acquisition starts. It is useful to check the time evolution of several simulation parameters such as temperature (which is directly connected to the kinetic energy), potential energy, total energy, density (when periodic boundary conditions with constant pressure are apphed), and their root-mean-square deviations. Having these and other variables constant at the end of the equilibration phase is the prerequisite for the statistically meaningful sampling of data in the following production phase. [Pg.369]

In order to interpret the above results, consider the expectation value of the total energy density in the vacuum state, i.e., of the hamiltonian density, Eq. (10-12). There is a contribution J u(x)Al(x) from the external field and a contribution m<0 j (a ) 0)ln 4 (a ) from the induced current, hence to lowest order... [Pg.597]

Wang and Rikvold [60] have applied ab initio total-energy density-functional methods in combination with supercell models to calculate the c(2 x 2) structure of bromide adsorbed on Au(lOO) and Ag(lOO) surfaces. The preferred bonding sites have been determined. The calculations have shown that bromide favorably binds the bridge site on the Au(lOO) surfaces. These results explain experimental observations that adsorption of bromide on the Au(lOO) and Ag( 100) surfaces proceeds via different bonding configurations. [Pg.848]

The total energy density of the particle is the sum of the anisotropy energy density and the Zeeman energy density in the external field ... [Pg.95]

And then the most probable distribution, Eq. (5.6.3), is obtained the total energy density U/V becomes finally... [Pg.308]

Figure 9 Variation of orbital energies in HAH molecule on going from 90° bent molecule to linear molecule. The classification of states, built from s and p atomic orbitals, is discussed in the main text. The steep rise in the curve joining ai and favours the bent molecular form for H2O, whereas with four valence electrons, as in BeH2 or HgH2, the linear configuration is favoured. This argument is based on an intimate relation, which Walsh assumed, between the sum of orbital energies and total energy. Density theory in its simplest form supplies such a relation, namely equation (84). The figure is a schematic version of that of Walsh,46 who noted that the line 180° must be either a maximum or a minimum... Figure 9 Variation of orbital energies in HAH molecule on going from 90° bent molecule to linear molecule. The classification of states, built from s and p atomic orbitals, is discussed in the main text. The steep rise in the curve joining ai and favours the bent molecular form for H2O, whereas with four valence electrons, as in BeH2 or HgH2, the linear configuration is favoured. This argument is based on an intimate relation, which Walsh assumed, between the sum of orbital energies and total energy. Density theory in its simplest form supplies such a relation, namely equation (84). The figure is a schematic version of that of Walsh,46 who noted that the line 180° must be either a maximum or a minimum...
The main obstacle in the many-body problem is to obtain accurate and satisfactory forms of the energy functional in terms of the electron density. Exchange-correlation energies and total energy density functionals have been related by simple and surprisingly accurate formulas by Parr and Ghosh [68]. [Pg.195]

R. G. Parr and S. K. Ghosh, Toward understanding the exchange-correlation energy and total-energy density functionals, Phys. Rev. A 51, 3564-3570 1995. [Pg.222]

The total energy density of a system involves contributions from the internal energy density e, the kinetic energy density JC, and the potential energy density V. [Pg.350]

In general for a /-component fluid mixture one has a (z/ + 3 l 1)-component set p yd of dynamic variables, containing //-component of the number densities / k,a, the three components of the total current density Jk, and the total energy density E. However, as follows from the symmetric properties, the number ttk.a and energy densities are coupled only with the longitudinal component of Jk, directed along k. This is due to the space isotropy of the system. As a result, one may split the set of the hydrodynamic variables into two separate subsets ... [Pg.112]

Such a tunnel switching of the magnetization can be described by the so-called one-domain approximation, when the total magnetization vector M is taken as a main dynamic variable with fixed absolute value M. Then the total energy density, or the anisotropy energy E, is obtained from the spin-Hamiltonian H using a spin coherent state n) chosen along the direction n [332,333] ... [Pg.475]

However, for the Hellman-Feynman theorem, (11), to be valid, the electronic density should be the one minimizing the total energy density functional... [Pg.249]

For matter (non-relativistic matter often called dust ), p p, so that p/po = (ao/a)3. In contrast, for radiation (relativistic particles) p = pi3, so that p/po = (ao/a)4. Another interesting case is that of the energy density and pressure associated with the vacuum (the quantum mechanical vacuum is not empty ). In this case p = —p, so that p = po- This provides a term in the Friedmann equation entirely equivalent to Einstein s cosmological constant A. More generally, for p = wp, p/po = (ao/a)3(1+w Allowing for these three contributions to the total energy density, eq. 2.9 may be rewritten in a convenient dimensionless form... [Pg.4]

The local value of the total energy density at a point r, H(r), is another useful topological descriptor that provides supplementary information about the nature of the interaction at r. The total energy density H(r) is the sum of the kinetic energy density G(r), a positive quantity, and the potential energy density F(r), a negative quantity, both densities related with the Laplacian of p(r) through the local expression for the virial theorem [45, 46] ... [Pg.124]

E. Espinosa, I. Alkorta, I. Rozas, J. Elguero and E. Mollins, About the evaluation of local kinetic, potential and total energy densities is closed-shell interactions, Chem. Phys. Lett. 336, 457 61 (2001). [Pg.470]

Analogous relationships liold for thci two otlu. r components. According to the laws of olectro(lynainie.s, the total energy-density of the radiation field is then given by... [Pg.333]

Early work suggested the existence of two crystal structures of Mg(B 114)2, a tetragonal low-temperature phase and a cubic high-temperature phase." However, no structural data have been reported experimentally, though total-energy density functional theory (DFT) calculations were performed. ... [Pg.429]

Figure 19.22 Total energy density versus applied true strain for cyclic tension. (From Reference 10 with permission from Elsevier Inc.)... Figure 19.22 Total energy density versus applied true strain for cyclic tension. (From Reference 10 with permission from Elsevier Inc.)...

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See also in sourсe #XX -- [ Pg.132 ]




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