For two electrons, whenever : both sides of are positive and squaring reduces the inequality to . Since , the trapezium then has a higher total electronic energy than the square. The two-electron model favours the square. For four electrons, , so : the four-electron model favours the distortion toward a trapezium. The lower split middle orbital is occupied while the upper one is empty.
The distinction is especially clear near the square. Write ; then and
In particular the four-electron lowering in this specified one-edge model is quadratic near the square; a first-order lowering of the entire occupied sum should not be asserted merely from the middle-level splitting. This Hückel square-to-trapezium distortion is an electronic comparison under the stated fixed-, fixed-short-edge- assumptions. Nuclear repulsion, other bonding contributions and the structural cost of distortion are omitted, so an actual equilibrium geometry or optimum is not determined by this calculation alone.
Figure 1.
Two- and four-electron total-energy changes for the one-edge Hückel distortion model
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