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Covalent bonds continued

In general, the FEUDAL model appears to answer many of the fundamental questions regarding the bonding within f-electron systems however, certain discrepancies exist within the physical data of the actinide systems and the theoretical understanding of the radial distribution functions of the actinides. Evidence that the f orbitals are accessible for covalent bonding continues to be found. [Pg.11]

Copper (continued) properties, 400. 408 Core, of earth, 440 Corrosion, 405 Coulomb, 241 Coulombic forces, 416 Coulson, C A., 252 Covalent bonds, 274, 277, 288 elements that form solids using, 302... [Pg.458]

The positions of the covalent bonds and the hydrogen bonds are continually changing, so that Figure 4.9 represents only an instantaneous picture of the atomic arrangement. [Pg.173]

In addition to the ratio of concentrations olefine/HA, the donor ability, or the nucleophilicity of the anion A- is a deciding factor for the manner in which the reaction continues. This anion is formed simultaneously with the carbenium ion. When the nucleophilicity of the anion is sufficiently high, as in the case of CP, Br-, I-, for instance, the reaction proceeds as an addition by the formation of a covalent bond between A- and the carbenium ion72). [Pg.207]

When the difference in electronegativities is great, the orbital may be so far over to one side that it barely covers the other nucleus. This is an ionic bond, which is seen to arise naturally out of the previous discussion, leaving us with basically only one type of bond in organic molecules. Most bonds can be considered intermediate between ionic and covalent. We speak of percent ionic character of a bond, which indicates the extent of electron-cloud distortion. There is a continuous gradation from ionic to covalent bonds. [Pg.15]

An actual molecule is d Tiamic, not static. Electrons move continuously and can be thought of as being spread over the entire molecule. In a covalent bond, nevertheless, the distribution of electrons has the general characteristics shown by the static view in the figure. The most probable electron locations are between the nuclei, where they are best viewed as being shared between the bonded atoms. [Pg.573]

If the covalent bonds connect elements of the structure along one dimension only, as in silicon disulfide, it may be desirable to consider the substance as a polymer. This will certainly be appropriate if the valence structure supersedes whatever crystalline arrangement prevails, i.e., if the substance can be melted without seriously disrupting the continuity of the interunit connections. [Pg.65]

A suitable approach to the equilibration of an amorphous polymer system at bulk density becomes much more likely when the fully atomistic model in continuous space is replaced by an equivalent coarse-grained model on a lattice with sufficient conformational flexibility. Different strategies, which seek results at different levels of detail, can be employed to create an appropriate coarse-grained model. Section 4 (Doruker, Mattice) describes an approach which attempts to retain a connection with the covalent bonds in the polymer. The rotational isomeric state (RIS) [35,36] model for the chain is mapped into... [Pg.50]

The first intravascular sensor for simultaneous and continuous monitoring of the pH, pC>2, and pCC>2 was developed by CDI-3M Health Care (Tustin CA)14 based on a system designed and tested by Gehrich et al.15. Three optical fibres (core diameter = 125 pm) are encapsulated in a polymer enclosure, along with a thermocouple embedded for temperature monitoring (Figure 3). pH measurement is carried out by means of a fluorophore, hydroxypyrene trisulfonic acid (HTPS), covalently bonded to a matrix of cellulose, attached to the fibre tip. Both the acidic ( eXc=410 nm) and alkaline ( exc=460 nm) excitation bands of the fluorophore are used, since their emission bands are centred on the same wavelength (/-cm 520 nm). The ratio of the fluorescence intensity for the two excitations is measured, to render the sensor relatively insensitive to fluctuations of optical intensity. [Pg.420]

Turning to macromolecular inorganic compounds, say ZnS, the two hypothetical ionic extremes are Zn2+S2- and Zn6-S6+ (an inverted, unusual formulation). We can imagine a continuous array of possible electron distributions between these extreme limits, one of which is the electron-pair covalent bonding state. The association of covalency with = Ay in Eqn. III.3 warrants non-polar formal MOs. However, a different situation arises when electrons are permitted to enter the empty MO skeleton. The electron-pair "covalent state corresponds to... [Pg.75]

Chain stretching is governed by the covalent bonds in the chain and is therefore considered a purely elastic deformation, whereas the intermolecular secondary bonds govern the shear deformation. Hence, the time or frequency dependency of the tensile properties of a polymer fibre can be represented by introducing the time- or frequency-dependent internal shear modulus g(t) or g(v). According to the continuous chain model the fibre modulus is given by the formula... [Pg.20]

Thus, by virtue of the continuity of the bond-order-bond-length relationship across the entire proton-transfer region, the interpretation of the H-bonded complexes in terms of partial proton transfer (with associated charge and covalent-bond transfer) can hardly be avoided. (Additional discussion of the properties of transition-state species in relation to the associated reactant and product species will be presented in Section 5.4.)... [Pg.656]


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Bonding continued)

Bonds - continued

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