Unveiling the Mystery of Unequal Bond Lengths
When we dive into the microscopic world of molecules, we often expect perfect symmetry. However, the reality is that molecules are dynamic, and their shapes are dictated by the invisible forces of electron repulsion. In this problem, we are tasked with finding which of the given molecules—XeF4, SiF4, SF4, or BF4−—breaks the rules of perfect symmetry and exhibits unequal bond lengths. To solve this, we must rely on the Valence Shell Electron Pair Repulsion (VSEPR) theory.
The Perfect Symmetries
Let's first examine the molecules that maintain their symmetry.
Take Xenon tetrafluoride (XeF4). Xenon, a noble gas, has 8 valence electrons. When it bonds with 4 fluorine atoms, the steric number becomes 21(8+4)=6, which corresponds to sp3d2 hybridization. This geometry is octahedral. However, because there are only 4 bond pairs, the remaining 2 electron pairs are lone pairs. To minimize repulsion, these lone pairs position themselves exactly opposite to each other (axially), leaving the 4 fluorine atoms in a perfectly symmetrical square planar arrangement. Because of this symmetry, all four Xe-F bonds are perfectly equal.
Similarly, Silicon tetrafluoride (SiF4) and the Tetrafluoroborate ion (BF4−) both have a steric number of 4, leading to sp3 hybridization. With zero lone pairs, they both adopt a perfect tetrahedral geometry. In a perfect tetrahedron, every bond angle is exactly 109.5∘, and every bond length is identical.
The See-Saw Anomaly
Now, let's look at the rebel of the group: Sulfur tetrafluoride (SF4).
Sulfur has 6 valence electrons. Bonding with 4 fluorine atoms gives a steric number of 21(6+4)=5, which means it has sp3d hybridization. The base geometry for sp3d is trigonal bipyramidal.
Here is where the catch lies: SF4 has 4 bond pairs and 1 lone pair. In a trigonal bipyramidal structure, the equatorial positions offer more space (120∘ apart) compared to the axial positions (90∘ from the equatorial plane). To minimize the intense lone pair-bond pair repulsion, the lone pair smartly occupies an equatorial position.
This creates a see-saw shape. The lone pair pushes strongly against the two axial S-F bonds, forcing them to bend slightly and, more importantly, elongating them. As a result, the axial bonds are significantly longer than the equatorial bonds.
Final Conclusion
By systematically applying VSEPR theory, we can confidently conclude that the presence of an equatorial lone pair in sp3d hybridized SF4 breaks the symmetry, making it the only species among the choices with unequal bond lengths.