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The total binding energy

Similar calculations can be made for other nuclei. A significant comparison between nuclear binding energies can be made if we divide the total binding energy of each nucleus by the... [Pg.418]

C22-0006. Fluorine has only one stable Isotope, F. Compute the total binding energy and the binding energy per nucleon for this nuclide. [Pg.1563]

In Fig. 1 there is presented the first-order shell correction of the total binding energy of atoms, cations, and anions from beryllium to calcium. As expected, the oscillating part of the energy displays minima for the atoms... [Pg.170]

Figure 1. The first-order shell correction SiE of the total binding energy of atoms (squares), cations (circles) and airions (triangles) from beryllium to calcium, as a function of the atomic number Z. Figure 1. The first-order shell correction SiE of the total binding energy of atoms (squares), cations (circles) and airions (triangles) from beryllium to calcium, as a function of the atomic number Z.
The binding energy curves for the four-atom molecules shown in Fig. 4.1 will be sensitive to the degree of normalized hardness, och. Summing over all the bonds in eqn (4.1), the total binding energies of the tetrahedron (t), rhombus (r), square (s), and linear chain (1) are given by... [Pg.79]

The energy difference between two competing structure types is usually very small compared to the total binding energy. Moreover, the simplest assumption that the first nearest-neighbour bond length is structure-independent can lead to incorrect predictions. For example, for the degree... [Pg.81]

We can understand the behaviour of the binding energy curves of monovalent sodium and other polyvalent metals by considering the metallic bond as arising from the immersion of an ionic lattice of empty core pseudopotentials into a free-electron gas as illustrated schematically in Fig. 5.15. We have seen that the pseudopotentials will only perturb the free-electron gas weakly so that, as a first approximation, we may assume that the free-electron gas remains uniformly distributed throughout the metal. Thus, the total binding energy per atom may be written as... [Pg.127]

The total binding energy of a NFE metal can be evaluated within second-order perturbation theory. In the presence of a perturbation fi to the Hamiltonian operator of a system, the energy of state is given by... [Pg.145]

The so-called band-structure contribution to the total binding energy per atom is given by subtracting this double-counting term, eqn (6.55), from Using eqn (6.26) we have... [Pg.147]

The total binding energy per atom of the NFE metal can then be written as the sum of the three terms ... [Pg.148]

The total binding energy can be rewritten as a sum over real space rather than q-space vectors by changing the order of their summation in . From eqn (6.57) the band-structure energy is given by... [Pg.150]

Thus, the total binding energy per atom of a NFE metal can be expressed in a physically transparent form, as the sum of a volume-dependent contribution and a pair-potential contribution in a manner that is reminiscent of the semi-empirical embedded atom potential of eqn (5.68). It follows from eqs (6.59M6.72) that... [Pg.151]

The beauty of the real-space representation is that it separates out the very small structure-dependent contribution to the total binding energy as a single sum over pair potentials. As illustrated in Fig. 6.7, these metallic pair... [Pg.156]

We have seen in the previous chapter that the total binding energy per atom of an elemental sp-valent system may be written within the approximation as the sum of three terms, namely... [Pg.214]


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