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Pure covalent bond

We have constructed a number of sets of atomic radii for use in compounds containing covalent bonds. These radii have been obtained from the study of observed interatomic distances. They are not necessarily applicable only to crystals containing pure covalent bonds (it is indeed probable that very few crystals of this type exist) but also to crystals and molecules in which the bonds approach the covalent type more closely than the ionic or metallic type. The crystals considered to belong to this class are tetrahedral crystals, pyrite and marcasite-type crystals, and others which have been found on application of the various criteria discussed in the preceding section to contain covalent bonds or bonds which approach this extreme. [Pg.163]

If two atoms have the same electronegativity, then the bond between them is purely covalent. Hydrogen, for instance, occurs as two joined atoms, H-H. Since both atoms in the molecule have the same electronegativity, they form a pure covalent bond with two electrons shared equally by the atoms. [Pg.85]

Because of the electric interaction, hydrogen-bonded molecules hold on to each other more tightly than those in substances with pure covalent bonds. This cohesiveness is why water is a liquid at room temperature, whereas heavier covalent-bonded molecules such as chlorine, in the form of CI2, are gases. [Pg.87]

It is important to point out that almost all bonds are polar bonds, whether they are approximately described as covalent or ionic. The bonds in the molecules of the various forms of the elements such as the diatomic molecules H2, CI2, and N2, larger molecules such as P4 and Sg, and infinite molecules such as diamond may be described as pure covalent bonds... [Pg.15]

The first represents a hypothetical HC1 molecule with a purely covalent bond in which the two bonding electrons are equally shared between the two atoms, and the second a hypothetical molecule with a purely ionic bond in which both the bonding electrons have been transferred to the chlorine atom. In this case the two resonance structures do not necessarily... [Pg.32]

Polar bonds range from bonds between atoms that have large but slightly less than integral charges and are therefore close to the ionic limit to pure covalent bonds between... [Pg.277]

A hydrogen atom, with only one stable orbital, cannot form more than one pure covalent bond, and the attraction of two atoms observed in hydrogen-bondformation must be due to ionic forces. [Pg.583]

Pauling (1947) has also shown that, in purely covalent bonds, modification of bond distance within a given coordination polyhedron may be associated with the bond number (n number of shared electrons per bond) through arbitrary constant Ki—i.e.. [Pg.906]

Two atoms of the same electronegativity will share electrons equally in a pure covalent bond therefore, any molecule that contains atoms of only one element, like H2 or CI2, has pure covalent bonding. Two atoms of different electronegativities, however, will have either the distorted electron distribution of a polar bond or the complete electron transfer of an ionic bond. Table 5-6 interprets the bonding between two elements as a function of the difference in their electronegativity. [Pg.53]

You can interpolate this value in the first column of Table 5-6 to find that such a bond is about 4% ionic and 96% covalent, which is virtually a pure covalent bond. [Pg.54]

It is easy to see from the examples in the previous section how two identical atoms can share electrons to achieve an octet and form diatomic molecules. Because each of our examples dealt with identical atoms, the electrons can be considered to be shared equally by each atom. The bond formed when the atoms are equally shared can be thought of as a pure covalent bond. But what happens in covalent compounds Remember, a compound contains two different elements. When atoms of two different elements are held together by covalent bonds, there is an unequal sharing of the electrons. The sharing of electrons in a covalent bond may be compared to you and a friend sharing a flashlight while walking down a dark street. If you and your friend both held the... [Pg.76]

Owing to its single composition and pure covalent bonding, diamond is a standard solid material, and takes the role of the most appropriate sample in explaining the effects upon structure-sensitive properties when the structure of solid material deviates from the ideal state. [Pg.170]

The Schomaker-Stevenson relaltonship states that heleropolar bonds are always stronger and shorter than hypothetical, purely covalent bonds between the same atoms. In uit ionic crystal, would you expect some covalency to shorten or lengthen the bond9 Explain. (Shannon. R. D. Vincent. H. Struct. Bunding (Berlin) 1974.19. I.)... [Pg.703]

For transition elements, purely covalent bonds exhibit a resistance in the limit 2.694-2.983 (Fig. 3.1). Compounds of this type have very few repre-... [Pg.188]

We see then a gradation from purely ionic to purely covalent bonding in different molecules, and this is manifest in their chemical and physical properties. Consider, for instance, the hydrides of the elements in the second horizontal row of the periodic table. Their melting and boiling points,7 where known, are given below. [Pg.19]

Pentacoordinate silicon forms two types of bonds with tricoordinate nitrogen atoms, a pure covalent bond and a N - Si dative bond. The first is significantly shorter than the second. The average covalent Si—N bond length in compounds where pentacoordinate silicon atom is bonded to tricoordinate nitrogen atom was calculated from 48 XRD experimental values to be 1.761 A (s.d. 0.06 A, s.m. 0.009 A). An example of the difference in bond length is shown in 127141 where the covalent Si—N bond lengths are 1.766 and 1.770 A and the dative bond is 2.333 A. [Pg.210]

To analyze the surface structures, infrared spectra were studied. It was concluded from the similarities between the spectra and the deprotonated CT2- that CT forms a bidentate structure on TiOz (Martin et al., 1996). The infrared (IR) peak positions also suggest that the CT adsorbate carries a negative charge. For a purely covalent bond, the charge would be zero. This suggests that the bond formed may have a 60% ionic character and a 40% covalent character. The concentration of 4-chlorocatechol apparently determines the type of surface structure formed. At concentrations below 50 pM, 4-chlorocatechol adsorbs as a bidentate structure. At concentrations above 50 uM, 4-chlorocatechol adsorbs nonspecifically in a multilayer environment. [Pg.348]

Carbon, with four valence electrons, mainly forms covalent bonds. It usually forms four such bonds, and these may be with itself or with other atoms such as hydrogen, oxygen, nitrogen, chlorine, and sulfur. In pure covalent bonds, electrons are shared equally, but in polar covalent bonds, the electrons are displaced toward the more electronegative element. Multiple bonds consist of two or three electron pairs shared between atoms. [Pg.1]

The second formula means merely that the HC1 molecule is a resonance hybrid between the ionic molecule H+Cl" and the molecule with the purely covalent bond, the direction of the arrow giving the direction in which the electrons have, on the average, been displaced (66). As, however, such an arrow is used by others (57), for indicating a coordinate link (semipolar double bond) caused by a lone electron pair of the donor atom, which likewise produces a dipole with its positive end on the donor side and its negative one on the acceptor side, the author suggests that the symbol — be used for the normal covalent bond, which, by resonance with an ionic structure, possesses a dipole. The point of this half arrow also indicates the direction of the negative end of the dipole. The full arrow — will then be reserved for the coordinate link. Both links play their roles in chemisorption, and it may be useful for the purposes of this article to introduce relatively simple symbols. According to this principle HC1 should be formulated as H—1-Cl. [Pg.44]

For convenience and to avoid confusion, we will symbolize a purely covalent bond between A and B centers as A — B, while the notation A—B will be employed for a composite bond wave function like the one displayed in Equation 3.4. In other words, A—B refers to the real bond while A — B designates its covalent component. [Pg.41]


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See also in sourсe #XX -- [ Pg.286 , Pg.288 ]

See also in sourсe #XX -- [ Pg.308 , Pg.310 ]




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Pure covalent bonding

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