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3.091 – Introduction to Solid State Chemistry Lecture Notes No. 2 ...

3.091 – Introduction to Solid State Chemistry Lecture Notes No. 2 ...

3.091 – Introduction to Solid State Chemistry Lecture Notes No. 2 ...

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LN–2established between them:experimental BE AB+ BE AAxBE BB) k(x A* x B) 2orD + 96.3 (x A* x B) 2 kJAccording <strong>to</strong> Pauling, the bonding character between two different elements may bedefined as:ionic bonding for: Dx > 1.7 ; covalent bonding for: Dx < 1.7The fractional ionicity of polar covalent bonding as listed in the P/T is obtained by therelationship:*0.25(x A% ionic bonding + 1 * e*x B ) 2 x 100Bonding In Polya<strong>to</strong>mic MoleculesIn the formation of covalent bonds between a<strong>to</strong>ms in polya<strong>to</strong>mic molecules, theconditions that a<strong>to</strong>mic orbitals dis<strong>to</strong>rt so that maximum overlap may be achieved whenbonding occurs produces more extensive changes of orbital geometry than is the casewith dia<strong>to</strong>mic molecules. It will be remembered that the changes which result in a σbond formation in dia<strong>to</strong>mic molecules are a dis<strong>to</strong>rtion of the s orbitals or p lobes so thatstrongest bond formation results from the maximum overlap between the two joinednuclei. For polya<strong>to</strong>mic molecules extensive alterations in the spatial disposition ofa<strong>to</strong>mic orbitals do occur, and very often the unique orbital geometry of the originala<strong>to</strong>mic orbitals is completely lost (fig. 7). It is sometimes convenient <strong>to</strong> view thesealterations as occurring in each a<strong>to</strong>m prior <strong>to</strong> bonding by a process involving themixing, or hybridization, of a<strong>to</strong>mic orbitals.21

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