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48    INTRODUCING INTERACTIONS AND BONDS







                                   −                +              −                +
                                  d                d              d                d
                                  Electrons  Atomic
                                             nucleus



                      Figure 2.6 Schematic diagram to show how an induced dipole forms when polarizable electrons
                      move within their orbitals and cause a localized imbalance of charge (an ‘induced dipole’ in which
                      the negative electrons on one atom attract the positive nucleus on another). The dotted line represents
                      the electrostatic dipole interaction


                                                        Aside

                         The existence of an attractive force between non-polar molecules was first recognized
                         by van der Waals, who published his classic work in 1873. The origin of these forces
                         was not understood until 1930 when Fritz London (1900–1954) published his quantum-
                         mechanical discussion of the interaction between fluctuating dipoles. He showed how
                         these temporary dipoles arose from the motions of the outer electrons on the two
                         molecules.
                           We often use the term ‘dispersion force’ to describe these attractions. Some texts
                         prefer the term ‘London–van der Waals’ forces.



                                       Polarizability

                                      The electrons in a molecule’s outer orbitals are relatively free to
              The ease with which     move. If we could compare ‘snapshots’ of the molecule at two
              the electron distribu-  different instants in time then we would see slight differences in
              tion around an atom
                                      the charge distributions, reflecting the changing positions of the
              or molecule can be
              distorted is called its  electrons in their orbitals. The ease with which the electrons can
                                      move with time depends on the molecule’s polarizability, which
              ‘polarizability’.
                                      itself measures how easily the electrons can move within their
                                      orbitals.
                                        In general, polarizability increases as the orbital increases in size:
              The weakest of all the
                                      negative electrons orbit the positive nucleus at a greater distance
              intermolecular forces in  in such atoms, and consequently experience a weaker electrostatic
              nature are always Lon-
              don dispersion forces.  interaction. For this reason, London dispersion forces tend to be
                                      stronger between molecules that are easily polarized, and weaker
                                      between molecules that are not easily polarized.
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