Van der Waals (VdW) interactions are a group of weak, short-range attractive forces that occur between all neutral atoms and molecules. Unlike the strong forces that form chemical bonds, these attractions do not involve the sharing or transfer of electrons to create covalent or ionic bonds. Instead, they represent a collective, non-covalent force that is pervasive in all matter, influencing physical properties like boiling points and molecular structure. To understand their relative weakness, imagine a chemical bond as super glue, which permanently locks atoms together. Van der Waals forces, in contrast, function more like the mild stickiness of a Post-it Note, providing a gentle, temporary attraction that is easily overcome.
The Nature of Van der Waals Attractions
The underlying mechanism for all Van der Waals forces stems from the inherent movement of electrons within a molecule or atom. Although electrons are generally distributed evenly around a nucleus, their constant motion means that at any given instant, the electron cloud can shift, creating a transient, unequal distribution of charge. This fleeting imbalance results in a temporary, instantaneous dipole, where one side of the atom is slightly more negative and the other is slightly more positive.
This temporary dipole can then influence a neighboring atom or molecule, causing it to instantly form a corresponding induced dipole. These forces are extremely short-range, only becoming significant when molecules are in very close proximity, typically within a distance of 0.4 to 0.6 nanometers. If the molecules get much closer than this optimal distance, the repulsion between their electron clouds takes over, pushing them apart.
Individual VdW forces are weak, but their strength becomes substantial because they are additive. A large molecule with an extensive surface area can engage in thousands of simultaneous VdW interactions with a neighboring molecule. This cumulative effect means that larger molecules, which possess more electrons and a greater surface area for contact, exhibit much stronger overall VdW attraction than smaller ones. For example, the boiling point of xenon is significantly higher than that of neon because the larger xenon atom has a more easily distorted electron cloud, leading to stronger, more numerous attractions.
The Three Distinct Types of Interactions
The umbrella term Van der Waals interactions encompasses three distinct types of forces, each arising from a different combination of temporary or permanent charge separation. These different forces are classified based on the nature of the dipoles involved in the attraction.
London Dispersion Forces (LDF)
London Dispersion Forces (LDF) are the most fundamental and occur between all atoms and molecules, regardless of their polarity. This force is solely responsible for the attraction between nonpolar molecules, such as those found in gasoline or noble gases like argon. LDF relies on the instantaneous dipole-induced dipole interaction, where electron fluctuation in one molecule induces a temporary dipole in its neighbor.
The strength of LDF is directly related to the molecule’s polarizability, or how easily its electron cloud can be distorted. This explains why, within the halogen group, the small gas chlorine (\(Cl_2\)) is less polarizable than the large solid iodine (\(I_2\)), resulting in much weaker LDF for chlorine. Dispersion forces are often the largest contributor to the total VdW force, even in molecules that also experience other types of VdW attraction.
Dipole-Dipole Interactions
Dipole-Dipole Interactions, also known as Keesom forces, occur only between molecules that possess a permanent dipole moment. These are polar molecules, like hydrogen chloride (\(HCl\)), where a difference in electronegativity causes a fixed, uneven distribution of charge. The positive end of one polar molecule attracts the negative end of a neighboring polar molecule, causing them to align for maximum attraction.
Dipole-Induced Dipole Interactions
Dipole-Induced Dipole Interactions, or Debye forces, occur when a molecule with a permanent dipole comes near a nonpolar molecule. The permanent dipole uses its fixed electric field to distort the neighbor’s electron cloud. This action induces a temporary dipole in the nonpolar molecule, leading to an attraction between the permanent and the newly induced dipoles. A practical example is the slight solubility of the nonpolar gas oxygen (\(O_2\)) in polar water, where the water molecule induces a dipole in the oxygen.
Essential Functions in Nature and Biology
Despite their individual weakness, the collective power of VdW forces profoundly impacts the physical world, especially by governing the phase changes of matter. The melting and boiling points of nonpolar substances are determined almost entirely by the strength of their VdW forces. For a substance to transition from a liquid to a gas, enough thermal energy must be supplied to overcome the intermolecular attractions. Since stronger VdW forces hold molecules more tightly, a substance like octane (a larger hydrocarbon) boils at a much higher temperature than methane (a smaller hydrocarbon).
These forces are also fundamental to the structures of life. In large molecules like proteins, VdW interactions stabilize the complex three-dimensional shape, or tertiary structure. This is accomplished by allowing non-polar amino acid side chains to cluster together in the protein’s interior, maximizing the number of attractive VdW contacts between them.
VdW forces are also crucial for maintaining the iconic double helix of DNA, where they contribute significantly to the stability of the molecule through base stacking. On a macroscopic scale, VdW forces are the primary mechanism behind the adhesion of geckos to vertical surfaces. The millions of microscopic hairs, called setae, on a gecko’s foot maximize the surface area contact. This generates a huge number of simultaneous, weak VdW interactions that collectively create a strong, yet reversible, grip.

