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Molecular orbitals hybrid

A conglomerate of three hexagons contains one central atom and 12 atoms around it. A conglomerate of seven hexahedrons comprises 12 external and 12 internal (common) atoms. In these two cases geometric centers of hybridized molecular orbitals of each hexahedron are equidistant from such nearest centers of a conglomerate. This, apparently, explains the experimental fact that polyhedrons of carbon clusters represent an icosahedron - 12-apex crystalline structure each apex of which is connected with five other apexes. [Pg.213]

The other electron-pair geometries that are listed in Table 9-2 are also related to specific hybrid molecular orbitals, but they are more complicated because they involve midp. In every case, the ami/ orbitals are of the same priflfap l( BMlSqis%mfeehySflffMftrofif feg... [Pg.136]

I believe essentially all of the material in the first five chapters is accessible to the advanced general chemistry students at most universities. The final three chapters are written at a somewhat higher level on the whole. Chapter 6 introduces Schrodinger s equation and rationalizes more advanced concepts, such as hybridization, molecular orbitals, and multielectron atoms. It does the one-dimensional particle-in-a-box very thoroughly (including, for example, calculating momentum and discussing nonstation-ary states) in order to develop qualitative principles for more complex problems. [Pg.225]

T. Vreven, B. Mennucci, C. O. da Silva, K. Morokuma and J. Tomasi, The ONIOM-PCM method Combining the hybrid molecular orbital method and the polarizable continuum model for solvation. Application to the geometry and properties of a merocyanine in solution, J. Chem. Phys., 115 (2001) 62-72. [Pg.537]

Fig. 1.5. Illustration of the bonding configuration of (a) silicon and (b) selenium atoms constructed from hybridized molecular orbitals. The position of the Fermi energy, E, is indicated. Fig. 1.5. Illustration of the bonding configuration of (a) silicon and (b) selenium atoms constructed from hybridized molecular orbitals. The position of the Fermi energy, E, is indicated.
VSEPR concept, valence bond description and hybridization, molecular orbital description, bond energies, covalent and van der Waals radii of the elements, intermolecular forces... [Pg.5]

The hydration of metal ions is a process that belongs to what we call the acid-base reaction in chemistry. The acid-base reaction involves no electron transfer between separate partners but a localized electron rearrangement to make up or break down a hybrid molecular orbital between an acid particle and a base particle, that is, the formation or the dissolution of a bonding molecular orbital due to the interaction between the frontier donor orbital of a particle Lewis base) and the frontier acceptor orbital of another particle Lewis acid). In order for an acid-base reaction to occur between a base particle and an acid particle, the electronic energy levels of the frontier orbitals for both acid and base particles are required to be close enough to each other for the orbital hybridization to prevail [3]. [Pg.534]

Open problems in writing the basic organic chonistry textbook include the selection of concepts for the representation of the material, but also the level of the explanation of the complex phenomena such as reaction mechanisms or the electron structure. Here I propose the compromises. First compromise is related to the mode of the systematization of the contents, which can traditionally be based either on the classes of compounds, or on the classes of reactions. Here, the main chapter titles contain the reaction types, but the subtitles involve the compound classes. The electronic effects as well as the nature of the chemical bond is described by using the quasi-classical approach starting with the wave nature of the electron, and building the molecular orbitals from the linear combination of the atomic orbitals on the principle of the qualitative MO model. Hybridization is avoided because all the phenomena on this level can be simply explained by non-hybridized molecular orbitals. [Pg.187]

Figure 3.61. Ideal hybridization molecular orbital interaction scheme in BeH2. Figure 3.61. Ideal hybridization molecular orbital interaction scheme in BeH2.
Mixing atomic orbitals forms hybrid molecular orbitals, and the number of s- and p-orbitals used to form the hybrid determines the hybridization (sp , for example). [Pg.46]

Mixing the atomic s-orbitals of two hydrogen atoms to form hybrid molecular orbitals seems to predict the bonding in diatomic hydrogen. There are limitations, however, and if the two atoms to be mixed have both s- and p-orbitals, problems... [Pg.60]

In Figure 3.7, a 2s-orbital and the three degenerate 2p-orbitals of carbon are mixed together and transformed into four identical hybrid molecidar orbitals. Mixing one s- and three 2p-orbitals results in a hybrid called an sp hybrid molecular orbital, 3. The alternative view shows the filled 2s-orbital and the two electrons in the 2p-orbitals. Promoting a 2s-electron and making all four new orbitals of the same energy leads to the four sp hybrids. The hybridization... [Pg.62]

The sp d hybrid orbital configuration continues to be invoked to explain some binding geometries with significant covalent character. Write any two normalized and mutually orthogonal sp d hybrid molecular orbitals in terms of the atomic orbitals 4s, 4p Apy, and... [Pg.256]

On the coordinate system provided, draw a simple sketch to show the direction and phase of greatest electron density for the sp d hybrid molecular orbital represented by... [Pg.256]

In hybridization, molecular orbital, and valence bond theory, not only is energy conserved, but also the number of orbitals is conserved. For example, for an sp hybridized atom, there is still one p orbital left over and for an sp hybridized atom, there are two unhybridized p orbitals left over. Carbon readily uses the leftover p orbitals to form TT bonds (see page 482). In contrast, silicon, the element one below carbon, does not use the p orbitals as readily to form tt bonds. As we will see in Section 11-4, the formation of a 77 bond involves the side-to-side overlap of unhybridized p orbitals. An unhybridized 3p orbital of silicon does not project out far enough to form 77 bonds. [Pg.476]

The energy difference between the bonding or antibonding states and the hybrid molecular orbital energy is referred to as the homopolar energy, V2 and the bondingantibonding orbital energy difference is 2V2. V2 can be shown [see Harrison, Ref. 1 for example] to depend approximately upon the inverse square of the interatomic distance, d, as ... [Pg.200]

Figure 5.4 A schematic diagram of the evolution of bonding of Si atoms. The filled 3s and partially filled 3p atomic orbitals of two atoms combine to form half-filled sp hybrid molecular orbitals. These combine to form bonding and antibonding orbtials. As more atoms collect atoms collect to create a bulk solid, bands form. Figure 5.4 A schematic diagram of the evolution of bonding of Si atoms. The filled 3s and partially filled 3p atomic orbitals of two atoms combine to form half-filled sp hybrid molecular orbitals. These combine to form bonding and antibonding orbtials. As more atoms collect atoms collect to create a bulk solid, bands form.
Heteropolar semiconductors can be thought to form sp hybrid molecular orbitals exactly as do homopolar semiconductors. When we considered two atoms together in a homopolar semiconductor, bonding and antibonding states resulted from symmetric and antisymmetric mixtures of identical hybrid orbitals. The same combinations occur in a heteropolar semiconductor, but now the cation and anion hybrid orbitals sp c snd sp A are more distinguishable and have different electron densities. Furthermore, the symmetric and antisymmetric states now have different contributions from the cation and anion molecular orbitals. [Pg.203]

Here the crystallographic indices in the subscripts refer to the hybrid molecular orbital directions. Because the Schrbdinger Equation governing electron motion is linear, any combination of wave functions that solve it will also be a solution. In other words, choosing the hybrid orbitals or the atomic orbitals as a starting point for the calculation must yield identical results. The most flexible and general approaeh is not to be restricted to specific hybrid orbitals but rather to consider all possible orbital-by-orbital interactions of the fundamental atomic states. These states apply to a given atom in any environment. Thus, their use is valid for any material in which the atom occurs. As an example of a specific interaction, one can ask how does the Px orbital on one atom interact with the orbital on another atom. [Pg.207]

Figure 9.2 A schematic of the hybridization and bonding in poly-ene structures, (a) shows the valence atomic orbitals of C, (b) the hybrid molecular orbitals in poly-enes, (c) the resonant backbone structure of a poly-ene, and (d) the structure resulting from the choice of one of the two possible double bonding structures. Figure 9.2 A schematic of the hybridization and bonding in poly-ene structures, (a) shows the valence atomic orbitals of C, (b) the hybrid molecular orbitals in poly-enes, (c) the resonant backbone structure of a poly-ene, and (d) the structure resulting from the choice of one of the two possible double bonding structures.

See other pages where Molecular orbitals hybrid is mentioned: [Pg.32]    [Pg.8]    [Pg.66]    [Pg.316]    [Pg.77]    [Pg.727]    [Pg.408]    [Pg.83]    [Pg.126]    [Pg.11]    [Pg.63]    [Pg.123]    [Pg.124]    [Pg.225]    [Pg.252]    [Pg.4]    [Pg.799]    [Pg.144]    [Pg.172]    [Pg.206]    [Pg.299]   
See also in sourсe #XX -- [ Pg.122 ]

See also in sourсe #XX -- [ Pg.106 ]

See also in sourсe #XX -- [ Pg.225 ]




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