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Silicon atomic radius

Arrange the elements in each of the following sets in order of decreasing atomic radius (a) sulfur, chlorine, silicon ... [Pg.178]

Boron forms perhaps the most extraordinary structures of all the elements. It has a high ionization energy and is a metalloid that forms covalent bonds, like its diagonal neighbor silicon. However, because it has only three electrons in its valence shell and has a small atomic radius, it tends to form compounds that have incomplete octets (Section 2.11) or are electron deficient (Section 3.8). These unusual bonding characteristics lead to the remarkable properties that have made boron an essential element of modern technology and, in particular, nan otechn ol ogy. [Pg.718]

Because carbon stands at the head of its group, we expect it to differ from the other members of the group. In fact, the differences between the element at the head of the group and the other elements are more pronounced in Group 14/IV than anywhere else in the periodic table. Some of the differences between carbon and silicon stem from the smaller atomic radius of carbon, which explains the wide occurrence of C=C and G=Q double bonds relative to the rarity of Si=Si and Si=0 double bonds. Silicon atoms are too large for the side-by-side overlap of p-orbitals necessary for -it-bonds to form between them. Carbon dioxide, which consists of discrete 0=C=0 molecules, is a gas that we exhale. Silicon dioxide (silica), which consists of networks of —O—Si- O - groups, is a mineral that we stand on. [Pg.724]

Figure 5.9 Structure of silicon viewed down [110]. The atoms are drawn smaller than the atomic radius suggests for clarity. Channels parallel to <110> facilitate interstitial diffusion in this material. Figure 5.9 Structure of silicon viewed down [110]. The atoms are drawn smaller than the atomic radius suggests for clarity. Channels parallel to <110> facilitate interstitial diffusion in this material.
The feldspars are widely distributed and comprise almost two-thirds of all igneous rocks. Orthoclase and albite (NaAlSisOg) are feldspars in which one-fourth of the silicon atoms are replaced by aluminum and anorthite (CaAl2Si20g) and has one-half of the silicon atoms replaced by aluminum. Because the ionic radius of Na+ (0.095 nm) and Ca" " (0.1 nm) are the same, solid solutions are often formed between albite and anorthite. Good stones of albite and orthoclase are known as moonstones. [Pg.389]

Which has a larger atomic radius, silicon barium ... [Pg.48]

Barium s atomic radius is larger. Atomic size tends to increase from top to bottom and from right to left. Barium (Ba) is farther down and to the left on the periodic table than silicon (Si). Barium has more energy levels and is therefore larger. [Pg.55]

Hightened reactivity of functional groups (e.g. Cl, Br, OH, OR, OCOR, NH2, SH) at the atoms of silicon, aluminum, titanium, phoshorus and other elements in comparison with their reactivity binded with oxygen. This is due to the fact that the silicon atom is one and a half times bigger than the carbon atom it has a covalent radius of 0.117 nm, whereas the radius of the carbon atom is only 0.077 nm. It follows that functional groups of the Si atom are much more distanced from each other than... [Pg.5]

This is explained by the fact that a silicon atom is much larger (the covalence radius of a Si atom is 0.117 nm) than a carbon atom (the covalence radius of a C atom is 0.077 nm) therefore, the distances between the hydroxyl groups at the silicon atom are rather large and impair intramolecular condensation (such a reaction requires a considerable deformation of valence angles). [Pg.149]

The covalent radius of the silicon atom is one and one half that of the carbon atom thus rendering the silicon atom more sterically accessible. [Pg.104]

FIGURE 7.6 Critical nudeus radius of silicon calculated by homogeneous nucleation theory for 0.2 atm and 0.7 atm. Atomic radius of silicon is 0.146 run. From Sawano [18]. [Pg.273]

Going from sila- to stannaethenes the polarity of the double bond remains nearly constant. But the formation of an asymmetrical transition state with stannaethenes is disadvantaged for two reasons the tin atomic radius is much greater than the silicon or germanium radius and Sn-C single bonds (which have to be newly formed) are much weaker than Si-C and Ge-C bonds, respectively. Therefore, stannaethenes are poorer enophiles and [2+2] cycloadduct partners in comparison to sila- or germaethenes. [Pg.119]

Silicon is a semiconductor with an intrinsic conductivity of 4.3 x 10" Q" cm and a band gap of I.I2eV at 300K. It has a diamond crystal structure characteristic of the elements with four covalently bonded atoms. As shown in Fig. 2.1, the lattice constant, a, is 5.43 A for the diamond lattice of silicon crystal structure. The distance between the nearest two neighbors is V3a/4, that is, 2.35 A, and the radius of the silicon atom is 1.18 A if a hard sphere model is used. Some physical parameters of silicon are listed in Table 2.1. [Pg.45]


See other pages where Silicon atomic radius is mentioned: [Pg.289]    [Pg.289]    [Pg.155]    [Pg.34]    [Pg.395]    [Pg.235]    [Pg.4]    [Pg.469]    [Pg.45]    [Pg.190]    [Pg.189]    [Pg.192]    [Pg.236]    [Pg.1475]    [Pg.497]    [Pg.817]    [Pg.817]    [Pg.11]    [Pg.286]    [Pg.127]    [Pg.155]    [Pg.349]    [Pg.139]    [Pg.4]    [Pg.272]    [Pg.275]    [Pg.1119]    [Pg.697]    [Pg.443]    [Pg.71]    [Pg.20]    [Pg.397]    [Pg.46]    [Pg.340]    [Pg.151]    [Pg.35]    [Pg.199]   
See also in sourсe #XX -- [ Pg.195 ]




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