Page 30 - Subyek Encyclopedia - Encyclopedia of Separation Science
P. 30

Sepsci*11*TSK*Venkatachala=BG
                                                                                  I / CENTRIFUGATION  25


           centrifugal speeds. This is achieved by routing the    be stable in solution;
           solutions to the rotor wall through veins in the central    be inert towards the fractionated materials, includ-
           core. When such self-generating gradients are used, it  ing biological activity;
           is not necessary that the sample be layered on top of    exert  the  minimum  osmotic  effect,  ionic
           the solution but instead it may be mixed with the  strength and pH;
           medium prior to loading (Figure 5). While self-    be removable from the product;
           generating gradients offer greater simplicity, they    be readily available and either inexpensive or easily
           often require a signiRcant increase in run time. For  recyclable;
           instance, though the advent of vertical tubes, faster    be sterilizable.
           centrifugal speeds, and overspeeding techniques have
           reduced run times to about one-third of those re-  It should not:
           quired only a few years ago, runs of 3 to 12 h are still    generate a prohibitively high viscosity;
           typical for DNA banding experiments.              interfere with the assay technique (e.g. absorb UV
             Isopycnic separation is a more powerful separation  or visible light);
           tool than rate-zonal separation in the sense that a gen-    be corrosive; or
           erally greater number of particle types can be re-    generate Sammable or toxic aerosols.
           solved. However, rate runs may still be preferred for
           separating large and/or fragile particles, since shorter  From this list of properties, it is apparent that no
           run times and lower centrifugal forces are used. Run  single ideal gradient material exists, as each separ-
           duration is crucial for a rate separation, whereas  ation problem imposes its own set of requirements.
           isopycnic runs simply require a minimum time for the  Rather, selection can only be made after a careful
           particles to reach a stationary state. It is sometimes  evaluation of the gradient properties with respect to
           useful to conduct a two-dimensional separation in  the requirements imposed by the separation to be
           which, for instance, a rate-zonal run generates frac-  conducted. The list of materials that have been used
           tions of particles with similar S values that are further  for gradient formation is extensive with examples
           fractionated according to density in an isopycnic sep-  of the more commonly used materials along with
           aration. The reverse process can also be performed to  selected properties listed in Table 1.
           yield particles of similar density but different  With respect to biological inertness and low viscos-
           particle size distributions.                    ity, the ideal aqueous gradient material is deuterium
                                                           oxide (D 2 O). However, D 2 O is expensive and has
           Gradient materials The selection of an appropriate  a relatively low maximum density (1.11 g cm  ).
                                                                                                    3
           gradient material is an important consideration as the  Sucrose was used in the pioneering density-gradient
           gradient properties must be compatible with the sep-  work of Brakke and, due to its low cost, transpar-
           aration objectives. The desired properties of an ideal  ency, ready availability and nontoxic nature, is still
           gradient material, as set forth by GrifRth and by  the most widely used. Densities to 1.33 g cm  can be
                                                                                                  3
           Ridge, are summarized below.                    achieved, which is sufRcient for separating most
             The ideal gradient material should:           cells and intracellular organelles. However, sucrose
             span a density range sufRcient to permit separ-  solutions are not completely physiologically in-
             ation of the particles of interest without overstress-  active and often contain UV-absorbing components.
             ing the rotor;                                Mannitol and sorbitol can be used as substitutes to



           Table 1 Physical properties of gradient materials in aqueous solutions at 203C (from Sheeler, 1981)
           Gradient material  Tradename  Maximum solution concentration         20% w/w solution

                                        Concentration  Density  Viscocity (cP)  Density     Viscosity (cP)
                                        (% w/w)     (gcm  )                     (gcm  )
                                                         3
                                                                                     3
           Sucrose                      65          1.33        182             1.08         2
           Sucrose polymer   Ficoll     43          1.17        600             1.07        27
           Colloidal silica  Ludox-SM   }           1.40         }              1.13         2
           Colloidal silica  Percoll    23          1.13         10             1.11         8
           Metrizamide                  56          1.44         58             1.12         2
           CsCl                         65          1.91         1.3            1.17         0.9
           Polytungstate salt  LST      85          2.89         14             1.20         }
           Polytungstate salt  SPT      85          2.89         26             1.20         2
   25   26   27   28   29   30   31   32   33   34   35