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General Chemistry Principles, Patterns, and Applications, 2011

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energy levels, as shown on the right in , each of which corresponds to a particular molecular orbital<br />

extending throughout the linear array of metal atoms. The levels that are lowest in energy correspond to<br />

mostly bonding combinations of atomic orbitals, those highest in energy correspond to mostly<br />

antibonding combinations, <strong>and</strong> those in the middle correspond to essentially nonbonding combinations.<br />

The continuous set of allowed energy levels shown on the right in is called anenergy b<strong>and</strong>. The difference<br />

in energy between the highest <strong>and</strong> lowest energy levels is the b<strong>and</strong>width <strong>and</strong> is proportional to the<br />

strength of the interaction between orbitals on adjacent atoms: the stronger the interaction, the larger the<br />

b<strong>and</strong>width. Because the b<strong>and</strong> contains as many energy levels as molecular orbitals, <strong>and</strong> the number of<br />

molecular orbitals is the same as the number of interacting atomic orbitals, the b<strong>and</strong> incontains n energy<br />

levels corresponding to the combining of s orbitals from n metal atoms. Each of the original s orbitals<br />

could contain a maximum of two electrons, so the b<strong>and</strong> can accommodate a total of 2n electrons. Recall,<br />

however, that each of the metal atoms we started with contained only a single electron in each s orbital, so<br />

there are only n electrons to place in the b<strong>and</strong>. Just as with atomic orbitals or molecular orbitals, the<br />

electrons occupy the lowest energy levels available. Consequently, only the lower half of the b<strong>and</strong> is filled.<br />

This corresponds to filling all of the bonding molecular orbitals in the linear array of metal atoms <strong>and</strong><br />

results in the strongest possible bonding.<br />

Multidimensional Systems<br />

The previous example was a one-dimensional array of atoms that had only s orbitals. To extrapolate to<br />

two- or three-dimensional systems <strong>and</strong> atoms with electrons in p <strong>and</strong>d orbitals is straightforward in<br />

principle, even though in practice the mathematics becomes more complex, <strong>and</strong> the resulting molecular<br />

orbitals are more difficult to visualize. The resulting energy-level diagrams are essentially the same as the<br />

diagram of the one-dimensional example in , with the following exception: they contain as many b<strong>and</strong>s as<br />

there are different types of interacting orbitals. Because different atomic orbitals interact differently, each<br />

b<strong>and</strong> will have a different b<strong>and</strong>width <strong>and</strong> will be centered at a different energy, corresponding to the<br />

energy of the parent atomic orbital of an isolated atom.<br />

B<strong>and</strong> Gap<br />

Because the 1s, 2s, <strong>and</strong> 2p orbitals of a period 3 atom are filled core levels, they do not interact strongly<br />

with the corresponding orbitals on adjacent atoms. Hence they form rather narrow b<strong>and</strong>s that are well<br />

separated in energy (). These b<strong>and</strong>s are completely filled (both the bonding <strong>and</strong> antibonding levels are<br />

Saylor URL: http://www.saylor.org/books<br />

Saylor.org<br />

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