Page 361 - Environmental Nanotechnology Applications and Impacts of Nanomaterials
P. 361

346   Environmental Applications of Nanomaterials

        Application to dense membranes:
        Reverse osmosis
        Reverse osmosis membranes are permeable to water while rejecting, to
        a large extent, solutes present in the feed. If, in the absence of any
        applied pressure, pure water is placed on one side of such a membrane
        (1) and an aqueous salt solution on the other (2), water will is pass from
        side 1 to side 2 by osmosis resulting in a decrease in the concentration
        of salt in compartment 2. If the compartments separated by the mem-
        brane are open to the atmosphere and allow for the height of water to
        adjust in each compartment (as in Figure 9.2), water will diffuse until
        the driving force of an increasing pressure from a greater height of
        water in compartment 2 comes to equilibrium with the decreasing driv-
        ing force for diffusion from 1 to 2.
          At equilibrium, the total available energy per mole of water, E w , is
        equal on the two sides of the membrane, i.e.,  E 5 0 . In the absence
                                                     w
        of an electrical potential, and further noting that water is uncharged
        (z w   0), according to Eq. 6, this condition is met when:

                              0 5 V  P 1 RT ln a  w
                                    w
                                                  a w,2
                            V sP 2 P d 52RT ln    a w,1               (16)
                              w
                                 2
                                      1
        where the subscripts 1 and 2 refer to the dilute and concentrated solu-
        tions, respectively. Eq. 15 indicates that if the activity of water is greater
        on one side of the membrane, the system can be in equilibrium only if
        the hydrostatic pressure is greater on the other side. If we take the
        activity of the pure water to be unity, and note that the pressure dif-
                               d
        ferential sP 2 Ppure water  is known as the osmotic pressure of the solu-
                   2
        tion, commonly designated as  , we obtain an expression for the osmotic
        pressure:






                      2
                       P = S
                                 P 2
                 P 1
                                             Figure 9.2 Pure water (1) diffuses
               1                             across a salt-rejecting membrane
                                             resulting in a dilution of (2) and dif-
                               2             ference in pressure between the two
                                             compartments.
   356   357   358   359   360   361   362   363   364   365   366