Page 440 - Book Hosokawa Nanoparticle Technology Handbook
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FUNDAMENTALS                                 CH. 7 ENVIRONMENTAL AND SAFETY ISSUES WITH NANOPARTICLES
                  the permeate, and v the fictitious filtrate volume per  destabilized by such consideration as depression of the
                                 m
                  unit membrane area, equivalent to the flow resistance  electrical double layer. Thus, the BSA molecules have
                  of the membrane [4].                           water bound to them even around the isoelectric point.
                    For fine particle suspensions, colloidal forces which  The hydrophilic BSA molecules maintain a dispersed
                  arise from interaction between the suspended particles  state in the solution due to hydration of the surface
                  control the nature of the filter cake. The average spe-  layers of the protein even around the isoelectric point.
                  cific filtration resistance   and the average porosity  When a BSA molecule acquires a charge, the filter
                                       av
                    of the filter cake are strongly affected by the solu-  cake becomes loose and wet due to electrostatic repul-
                   av
                  tion properties, including pH and electrolyte strength.  sion between the charged BSA molecules. This con-
                  For instance, in MF of suspensions of the titanium  trasts to the compact filter cake around the isoelectric
                  dioxide (pI 8.1, the original mean specific surface area  point. The average specific filtration resistance   has
                                                                                                       av
                  size 470 nm),   goes through a minimum, and   is  a definite maximum around the isoelectric point since
                                                          av
                              av
                  much larger near the isoelectric point [5], as shown in  a compact filter cake provides a large hydraulic flow
                  Fig. 7.4.7. The titanium dioxide particles are destabi-  resistance.
                  lized around the isoelectric point where the van der  Most membrane filtration processes are operated in
                  Waals attraction is more dominant. Consequently, the  the cross-flow mode, in which the feed is moved tan-
                  particle tends to come together, that is, to flocculate,  gentially to the membrane surface so that the filter
                  and the very porous flocs are then formed. Thus, it is  cake is continuously sheared off. During membrane fil-
                  speculated that the filter cake formed from such  tration, particles in the feed are brought to the upstream
                  porous flocs has often loose and wet structures. On the  surface of the membrane by convective transport, and
                  other hand, the filter cake becomes compact and dry  this results in a higher local concentration of the
                  when the particle carries the charge. Since the most  rejected particles at the membrane surface as com-
                  loose filter cake forms around the isoelectric pH, the  pared to the bulk solution which is referred to as con-
                  filter cake is most permeable.                 centration polarization [7].
                    It is interesting to note that the results in protein UF  The particle concentration in the solution adjacent
                  had a distinctly different behavior. In protein UF of  to the membrane varies from the value at the mem-
                  BSA solution, the filter cake is in its most compact  brane surface, C , to that in the bulk feed solution, C ,
                                                                                                          b
                                                                             m
                  state around the isoelectric point [6], as shown in  over a distance equal to the concentration boundary
                  Fig. 7.4.8. Since the BSA molecules are hydrophilic  layer thickness  . The resulting concentration gradient
                  colloids, their stability in the solution would appear to  causes the particles to be transported back into the
                  be influenced not only by the presence of a surface  bulk solution due to diffusional effects.  At steady
                  charge on the protein but also by hydration of the sur-  state, the rate of convective transport of particle
                  face layers of the protein.  The BSA molecules,  toward the membrane is balanced by the rate of parti-
                  because of hydrated layers surrounding them, are not  cle transport through the membrane plus the rate of

                        ×  10 12                                       × 10 15
                     12                               0.75           8                               1.00
                              TiO 2
                     10       s =0 .02                0.70
                              p = 196 kPa
                                                                     6
                      8                               0.65
                    (m/kg)  6                         0.60  (−)    α av  (m/kg)  4       BSA         0.95  (−)

                        av                                       av                      s =6 ×10 -3      ε av
                      4                               0.55                               p =98 kPa
                                                                     2
                                                                                                     0.90
                      2                               0.50
                      0                               0.45           0
                       2     4     6     8     10   12                   2    4     6    8    10    12
                                      pH                                             pH
                  Figure 7.4.7                                   Figure 7.4.8
                  Effect of pH on average specific filtration resistance and  Effect of pH on average specific filtration resistance and
                  average porosity of filter cake formed in microfiltration of  average porosity of filter cake formed in ultrafiltration of
                  titanium dioxide suspensions.                  BSA solutions.

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