Cubical atom
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The cubical atom was an early atomic model published by Gilbert N. Lewis in 1916 (although, by his account, he had developed it as early as 1902) to account for the phenomenon of valency. It was further developed in 1919 by Irving Langmuir as the cubical octet atom. The figure below shows the structures for the elements of the second row of the periodic table.
Although the cubical model of the atom was soon abandoned in favor of the quantum mechanical model based on the Schrödinger equation, and is therefore only of historical interest, it represented an important step towards the understanding of the chemical bond. The 1916 article by Lewis also introduced the concept of the electron pair in the covalent bond, the octet rule, and the now-called Lewis structure.
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[edit] Bonding in the cubical atom model
Single covalent bonds are formed when two atoms share an edge, as in structure C below. This results in the sharing of two electrons. Ionic bonds are formed by the transfer of an electron from one cube to another, without sharing an edge (A). An intermediate state B where only one corner is shared was also postulated by Lewis.
Double bonds are formed by sharing a face between two cubic atoms. This results in sharing four electrons:
Triple bonds could not be accounted for by the cubical atom model, because there is no way of having two cubes share six corners. Lewis suggested that the electron pairs in atomic bonds have a special attraction, which result in a tetrahedral structure, as in the figure below (the new location of the electrons is represented by the dotted circles in the middle of the thick edges). This allows the formation of a single bond by sharing a corner, a double bond by sharing an edge, and a triple bond by sharing a face. It also accounts for the free rotation around single bonds and for the tetrahedral geometry of methane. Remarkably, it could be said that there was a grain of truth in this idea, because it was later shown that the Pauli exclusion principle results in a "Fermi hole" of decreased repulsion between a pair of electrons with opposite spins in the same orbital.
[edit] See also
[edit] References
- Lewis, G. N. The Atom and the Molecule. J. Am. Chem. Soc. 1916, 38, 762-785. [1]
- Langmuir, I. The Arrangement of Electrons in Atoms and Molecules. J. Am. Chem. Soc. 1919, 41, 868-934.
