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48   I / CHROMATOGRAPHY/ Derivatization































           Figure 10 van Deemter plot of the column plate height as a function of the mobile-phase velocity. The solid line represents the
           experimental results and the broken lines the theoretical contribution from flow anisotropy (A), axial diffusion (B/u) and resistance to
           mass transfer (Cu).



           resultant peak observed at the column exit is   minimum in the plate height occurs at a high opti-
           broadened about its zone centre, which is located  mum mobile-phase velocity, resulting in efRcient
           where it would have been for instantaneous equilib-  and fast separations. At these high mobile-phase vel-
           rium, provided that the degree of nonequilibrium is  ocities the contribution from axial diffusion to
           small. Contributions from resistance to mass transfer  the column plate height is minimized. For thin-Rlm
           are rather complicated but depend on the column  columns, resistance to mass transfer in the mobile
           residence time, mobile-phase velocity, stationary-  phase is the main cause of zone broadening, while for
           phase Rlm thickness, the particle size for packed  thick-Rlm columns resistance to mass transfer in the
           columns,  the  solute  diffusion  coefRcients  in  stationary phase is equally important. Since dif-
           the mobile and stationary phases, and the column  fusion in gases is relatively favourable, the column
           internal diameter.                              internal diameters required to maintain an acceptable
             The relationship between zone broadening (col-  contribution from resistance to mass transfer in the
           umn plate height) and the mobile-phase velocity is  mobile phase offer little difRculty in practice.
           given by the hyperbolic plot known as a van Deemter  For supercritical Suids, solute diffusivity is not as
           curve (Figure 10). The solid line represents the ex-  favourable as for gases and in the case of liquids must
           perimentally observed results and the dotted lines the  be considered unfavourable. The unfavourable slow
           contributions from Sow anisotropy (A term), axial  optimum mobile-phase velocity in SFC (in practice
           diffusion (B/u) and resistance to mass transfer  open-tubular columns are operated at 10 or more
           (Cu). In this generic plot we see that there is an  times the optimum velocity to obtain an acceptable
           optimum velocity at which a particular chromato-  separation time) requires signiRcantly smaller inter-
           graphic system provides maximum efRciency (a    nal diameter capillary columns than those needed for
           minimum column plate height). The position of this  GC to minimize resistance to mass transfer in the
           optimum velocity and the general curvature of the  mobile phase. At mobile-phase velocities used in prac-
           plot strongly depend on the characteristics of the  tice the contribution of axial diffusion to the col-
           chromatographic system, as shown by the values  umn plate height is negligible compared with the
           given in Table 1.                               contribution of resistance to mass transfer in the mo-
                                                           bile and stationary phases. For fast, high efRciency
           Gas Chromatography                              separations, column internal diameters (100  mare
           Gases of low viscosity with favourable solute dif-  required and much smaller diameters are preferred.
           fusivity, such as hydrogen and helium, are commonly  As densities and solute diffusivity become more
           used as mobile phases in GC. For these gases the  liquid-like,  column  dimensions  for  reasonable
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