Page 164 - Instant notes
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E8
                     THE MOTION OF LARGER IONS



        Key Notes
                                Large ions are often multiply charged and are surrounded by an
                                electrical double-layer, consisting of a Stern layer of tightly
                                bound counterions and a diffuse double-layer which is an ionic
                                atmosphere containing a majority of counterions. As with smaller
                                ions, this ionic atmosphere is crucial for determining ionic
                                interactions. The residual charge at the outside edge of the Stern
                                layer is the effective charge on the ion, which can vary with
                                electrolyte concentration and type.
                                Electrophoresis is the separation of large ions by applying a field
                                between two plates to induce concentration polarization. Under
                                the influence of the field, ions that have small hydrodynamic radii
                                and large effective charges move further and separate from
                                larger, less charged ions.
                                Electro-osmosis is a method for inducing osmosis by an electric
                                field. It is the counterpart to electrophoresis and involves
                                applying a field across a solution with fixed larger ions. Motion
                                of the counterions is induced, which also produces water flow
                                (osmosis). As with electrophoresis, the rate of water flow is
                                controlled by the effective charge on the ion.
         Related topics         Ions in aqueous solution   Macroscopic aspects of ionic motion
                                (E1)                (E6)



                                 The electrical double-layer

        Larger ions, such as biological polymers or macromolecules, which can contain many
        thousands of atoms and many ionizable groups, are often multiply charged. The resulting
        electrostatic forces between these ions and their small counterions are often sufficiently
        strong that an electrical double-layer is formed (Fig. 1).
           Near the large ion, a layer of counterions (often partially desolvated) is held tightly to
        the  surface  by the very strong attractive electrostatic forces. This is termed the  Stern
        layer,  and  these  strongly  adsorbed  counterions reduce the effective charge of the ion.
        Outside the Stern layer, the remaining charge imbalance is sufficiently small that an ionic
        atmosphere  (see Topic E1) is formed around the ion called a  diffuse double-layer,
        which contains an overall excess of counterions sufficient to balance the residual charge,
        loosely bound to the ion by the electrostatic forces of attraction. As with smaller ions, the
        interaction between the ion and its ionic atmosphere of diffuse double-layer is crucial in
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