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VSEPR theory

physical science Maturity 9-11 Next article →

Valence shell electron pair repulsion (VSEPR) theory is a vital model in chemistry. It allows scientists to predict the specific geometry of individual molecules. This geometry is determined by the number of electron pairs surrounding a central atom. Understanding these shapes is essential because molecular structure influences how substances behave. The theory is also known as the Gillespie-Nyholm theory. It is sometimes called the Sidgwick-Powell theory due to earlier foundational work.

AX2E0-3D-balls
AX2E0-3D-balls

The mechanism of VSEPR is based on the principle of electrostatic repulsion. Electron pairs in the valence shell of an atom tend to repel one another. To achieve stability, these pairs move as far apart as possible. They seek positions that minimize their mutual repulsion by maximizing the distance between them. You can imagine this using inflated balloons tied together at their stems. The balloons push against each other and naturally adopt specific geometric shapes.

AX3E1-3D-balls
AX3E1-3D-balls

To determine a molecule's shape, chemists first identify the central atom. A central atom is bonded to two or more other atoms. The other atoms, bonded to only one atom, are called terminal atoms. Scientists draw a Lewis structure to find the number of electron pairs. They then calculate the steric number for the central atom. The steric number is the sum of bonded atoms and nonbonding lone pairs. A double or triple bond is treated as a single bonding group.

Sulfur-tetrafluoride-2D-dimensions
Sulfur-tetrafluoride-2D-dimensions

Different steric numbers result in distinct electron geometries. If a central atom has two electron pairs, it adopts a linear geometry. Three pairs result in a trigonal planar arrangement. Four pairs create a tetrahedral shape. Five pairs lead to a trigonal bipyramidal geometry. Six pairs result in an octahedral shape. For example, the molecule PCl5 has five bonding pairs and adopts a trigonal bipyramidal shape.

AX5E0-2D
AX5E0-2D

The history of this theory involves several key scientific contributions. In 1939, Ryutaro Tsuchida in Japan proposed a correlation between geometry and electron pairs. In 1940, Nevil Sidgwick and Herbert Powell presented similar ideas at the University of Oxford. Later, in 1957, Ronald Gillespie and Ronald Nyholm of University College London refined these concepts. Their work created a detailed theory capable of choosing between various alternative geometries. This refinement made VSEPR a powerful predictive tool for modern chemistry.

Repulsion is not uniform among all electron pairs. Lone pairs, or nonbonding pairs, exert more repulsion than bonding pairs. This is because lone pairs are held closer to the positively charged nucleus. There is a specific hierarchy of repulsion strengths. Lone pair–lone pair (lp–lp) repulsion is the strongest. This is followed by lone pair–bonding pair (lp–bp) repulsion. Finally, bonding pair–bonding pair (bp–bp) repulsion is the weakest.

Water-dimensions-from-Greenwood&Earnshaw-2D
Water-dimensions-from-Greenwood&Earnshaw-2D

These varying strengths cause deviations from ideal bond angles. In a water molecule, there are two lone pairs and two bonding pairs. The four pairs point toward the corners of a tetrahedron. However, the lone pairs push the hydrogen atoms closer together. This changes the bond angle from the ideal 109.5 degrees to 104.5 degrees. Similarly, in the molecule SF4, the steric number is five. It has four ligands and one lone pair, creating a seesaw shape.

AX4E1-2D
AX4E1-2D

Chemists often use the AXE method to organize these observations. In this formula, A is the central atom. X represents the number of bonded ligands. E represents the number of lone pairs on the central atom. For example, a molecule labeled AX2E2 is considered bent. This method helps categorize molecules like XeF4, which is square planar. While VSEPR works well for main-group elements, transition metals often follow the Kepert model. In transition metals, lone pairs are usually stereochemically inactive and do not change the geometry.

AX4E2-2D
AX4E2-2D
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