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Nanoparticle Transport, Aggregation, and Deposition  271

          Greater surface roughness has been observed to increase deposition rate
        coefficients observed for some nanoparticles [65]. Similar observations
        have also been made for colloid deposition onto membrane surfaces [78,
        79]. Enhanced particle deposition rates on rough surfaces are attributed
        to a combination of a reduced energy barrier on approach and physical
        trapping of the nanoparticles by surface features. For ideally smooth sur-
        faces, interactions occur normal to the interacting surfaces; however, for
        a particle approaching a rough surface, it experiences both normal and
        tangential forces that can capture it in surface depressions. Furthermore,
        the variable height of the surface topography means that the approach-
        ing particle is experiencing a range of interactions as some are more
        prominent than others at different separation distances. For this reason
        it is difficult to fully describe a true surface interaction between hetero-
        geneous surfaces in terms of a single energy curve. Surface roughness can
        also alter the magnitude and type (repulsive or attractive) of interaction
        between two surfaces [78]. This results from a reduction in the relative
        interaction area between the particle and the collector surface. One
        approach is to model surface asperities as a series of small hemispheres
        instead of a flat surface. The resulting calculations yield smaller inter-
        action energies as the interaction energy is determined by the radii of
        curvature of the protrusions rather than that of the interacting bodies.
        Consequently, roughness reduces the height of the energy barrier between
        two surfaces in aqueous media, thus making particle deposition more
        favorable [74, 75]. For instance, Suresh and Walz [74] found that the van
        der Waals interaction energy significantly increased when the separation
        distance between two surfaces approached the height of the surface asper-
        ities. The number of asperities per unit area on the surface had a smaller
        influence on the magnitude of the interaction energy than did asperity
        size. Asimilar conclusion was reached by these authors regarding the elec-
        trostatic interactions—electrostatic repulsion occurs at a larger separa-
        tion distance than would be expected for a smooth surface. At small
        separation distances, surface roughness has a more profound impact on
        van der Waals interactions (i.e., makes the attraction stronger). Hence,
        at shorter separations the height of the energy barrier is substantially
        reduced. In summary, surface roughness tends to reduce the depth of a
        secondary minimum and shifts it to longer separation distances while the
        repulsive energy barrier is decreased and the primary minimum is moved
        to larger separation distances.
          Roughness features may also physically trap nanoparticles on the sur-
        face once contact has been made. This occurs through a combination of
        enhanced surface adhesion and modification of the surface fluid velocity
        pattern. Upon deposition, particles are principally subject to shearing
        forces that would cause them to “roll” across a surface. This rolling motion
        is resisted by the adhesion force acting between the surfaces, as discussed
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