Instantaneous dipoleinduced dipole interactions between nonpolar molecules can produce intermolecular attractions just as they produce interatomic attractions in monatomic substances like Xe. This effect, illustrated for two H2 molecules in part (b) in Figure \(\PageIndex<3>\), tends to become more pronounced as atomic and molecular masses increase (Table \(\PageIndex<2>\)). For example, Xe boils at ?108.1°C, whereas He boils at ?269°C. The reason for this trend is that the strength of London dispersion forces is related to the ease with which the electron distribution in a given atom can be perturbed. In small atoms such as He, the two 1s electrons are held close to the nucleus in a very small volume, and electronelectron repulsions are strong enough to prevent significant asymmetry in their distribution. In larger atoms such as Xe, however, the outer electrons are much less strongly attracted to the nucleus because of filled intervening shells. The ease of deformation of the electron distribution in an atom or molecule is called its polarizability . Because the electron distribution is more easily perturbed in large, heavy species than in small, light species, we say that heavier substances tend to be much more polarizable than lighter ones.
The polarizability of a substance also determines how it interacts with ions and species that possess permanent dipoles. Thus, London dispersion forces are responsible for the general trend toward higher boiling points with increased molecular mass and greater surface area in a homologous series of compounds, such as the alkanes (part (a) in Figure \(\PageIndex<4>\)). The strengths of London dispersion forces also depend significantly on molecular shape because shape determines how much of one molecule can interact with its neighboring molecules at any given time. For example, part (b) in Figure \(\PageIndex<4>\) shows 2,2-dimethylpropane (neopentane) and n-pentane, both of which have the empirical formula C5Ha dozen. Neopentane is almost spherical, with a small surface area for intermolecular interactions, whereas n-pentane has an extended conformation that enables it to come into close contact with other n-pentane molecules. As a result, the boiling point of neopentane (9.5°C) is more than 25°C lower than the boiling point of n-pentane (36.1°C).
Figure \(\PageIndex<4>\): Mass and Surface Area Affect the Strength of London Dispersion Forces. (a) In this series of four simple alkanes, larger molecules have stronger London forces between them than smaller molecules do, and consequently have higher boiling points. (b) Linear n-pentane molecules have a larger surface area and stronger intermolecular forces than spherical neopentane molecules. As a result, neopentane is a gas at room temperature, whereas n-pentane is a volatile liquid.
Generally speaking, but not, dipoledipole affairs inside the quick polar particles are rather stronger than London dispersion pushes, therefore the former predominate.
The fresh four compounds is actually alkanes and you will nonpolar, very London dispersion pushes certainly are the merely crucial intermolecular forces
Dictate the brand new intermolecular pushes from the substances, then strategy the compounds with respect to the fuel of these pushes. New substance into the weakest forces get a low boiling part.
These forces are generally stronger with increasing molecular mass, so propane should have the lowest boiling point and n-pentane should have the highest, with the two butane isomers falling in between. Of the two butane isomers, 2-methylpropane is hookup spots Chico more compact, and n-butane has the more extended shape. Consequently, we expect intermolecular interactions for n-butane to be stronger due to its larger surface area, resulting in a higher boiling point. The overall order is thus as follows, with actual boiling points in parentheses: propane (?42.1°C) < 2-methylpropane (?11.7°C) < n-butane (?0.5°C) < n-pentane (36.1°C).