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234   Principles and Methods

        magnitudes of the attractive (negative energy potential) and repulsive
        (expressed as a positive quantity) phenomena involved. In the first
        case, the interaction between surfaces is attractive at all separation dis-
        tances. In the second case, the interaction is repulsive as the surfaces
        approach one another until a repulsive energy barrier is overcome, at
        which point the interactions become attractive. In the third case
        (depicted in Figure 7.1), interactions are at first attractive, then repul-
        sive, and finally attractive once again (as in the second case) as the
        approach distances became smaller. The features of the potential energy
        curve in this last case are designated as an attractive secondary
        minimum (I), a repulsive barrier (II), and an attractive primary mini-
        mum (III). As separation distance between two surfaces increases, the
        different components of the interaction energies diminish from their
        corresponding values at near-contact following a unique decay pattern,
        which affects the shape of the resulting energy plot [4]. For instance,
        the secondary minimum develops because repulsive electrostatic inter-
        actions decay exponentially with separation distance while attractive
        van der Waals interactions decay somewhat more slowly over a longer
        range. The magnitudes of different interaction energies depend on par-
        ticle size and thus, so does the overall interaction energy curve. For
        example, as particle size decreases, the height of the energy barrier, if
        present, also decreases; similarly, the secondary minimum becomes
        more shallow with decreasing particle size. This is particularly evi-
        dent at separation distances greater than 5 nm. Below this separation
        distance, shorter-range interactions tend to be less impacted by parti-
        cle size. Nevertheless, size effects on interaction energies have conse-
        quences with regards to the stability of particle dispersions and particle
        mobility [6].
          The components of interaction energy that are accounted for in the
        DLVO and other similar theories are discussed in more detail in the
        following sections. These discussions, however, are not meant to be exhaus-
        tive reviews of these subjects; the reader is instead referred to other sources
        [4, 7, 8] for such detailed overviews. The purpose here is to consider the
        effect of diminishing particle size on those interaction energies as they may
        be relevant in determining nanoparticle fate and transport in the
        environment.

        Van der waals interactions.  Van der Waals interactions are in most
        cases attractive and act universally between surfaces in aqueous media.
        These interactions incorporate three different electrodynamic forces:
        dispersion, induction, and orientation [4]. The three electrodynamic
        forces may be summed together to equal the total van der Waals
        interfacial energy term. Lifshitz-van der Waals interaction energies
                             2
        decay according to L , where L represents the distance between two
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