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102  A. R. HEMSLEY AND P. C. GRIFFITHS



                               obey the ideal gas law, van der Waals introduced a force (which now bears
                               his name) to account for an attractive interaction between molecules.
                               However, it was not until the advent of quantum theory in the 1920s and
                               the ability to elucidate the electronic structure of molecules, that it
                               become clear that all intermolecular interactions are in fact, electrostatic
                               in origin. Today, intermolecular forces can be calculated from a knowledge
                               of the distribution of electron clouds associated with the molecules.
                                  The characteristics of colloidal particles, as described by Shaw, are
                               somewhat different to those of a molecule, yet the same basic forces
                               operate. The generalised interaction between identical spherical colloid
                               particles dispersed in a solvent depends on the nature of the particles and
                               the solvent and varies with the distance between the particles.
                               Interestingly, and independent of the nature of the particles, it turns out
                               that there is always an attractive interaction between such identical parti-
                               cles dispersed in a solution. This attractive interaction tends to induce
                               aggregation and thus, colloidal dispersions are inherently thermodynami-
                               cally unstable. If an organism can synthesise a colloidal dispersion, either
                               through aggregation of dissolved minerals or polymerisation of self-assem-
                               bled molecules, the formation of the colloidal crystals such as those
                               present in some spore walls (Figure 6.1(c)) should come as no surprise! It is
                               this very potential, i.e. to form aggregates rather than dispersions, that
                               organisms have used to great effect.
                                  This simple thermodynamic picture is substantially altered if we
                               introduce dissimilar particles into our dispersion. The various interactions
                               now depend on the nature of the two particles, relative to the solvent, and
                               can either favour dispersal or aggregation. Again, this could be the basis for
                               a natural control mechanism; as the number and composition of the col-
                               loidal building blocks evolve, subtle changes in the interactions could
                               switch a dispersion from stable to unstable.
                                  The overall interaction between colloidal particles in solution some-
                               times includes two further terms, an electrostatic term arising through the
                               presence of charged groups on the surface of the particle or a steric term
                               resulting from the presence of polymers adsorbed onto the surface of the
                               particles. Several mechanisms lead to surface charge – dissociation of ionic
                               groups, adsorption/desorption of potential determining ions and other
                               ionic materials such as surfactants. The presence of surface charges
                               induces a re-distribution of nearby ions; like-charges are repelled and
                               unlike-charges attracted. Combined with their thermal motion, this leads
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