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Sedimentation Equilibrium of Mixtures of Charged Colloids

Sedimentation Equilibrium of Mixtures of Charged Colloids

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numbers for the parameters Z i , L i , σ i , ρ s , λ B and a mean density ¯ρ i to fix a i .By using an iteration method, shown and discussed in chapter 6, a common,four-year-old computer can calculate the solution for a polydisperse system<strong>of</strong> n = 20 components and H = 20cm in a minute. We will now explore somenumerical results, before we continue the analytical path for which we needassumptions.4.3 Binary systemsWe will start with a binary system, i.e. a system with n = 2 colloidalcomponents. The reason for this choice is that, considering these systems,the complexity is still reduced, while several multi-component phenomenacan already be examined. The next examples will show if the componentswill form layers, if they will order, and how their pr<strong>of</strong>iles are influenced whenthey are put together.After careful study three binary systems were selected for comparison. Thegravitational length are fixed at L 1 = 1mm, L 2 = 2mm and Z 1 = 250. Thecharge number Z 2 , however, will be varied, in case (a) Z 2 = 125, in case (b)Z = 500, in case (c) Z = 1000. The calculated density pr<strong>of</strong>iles are shownbelow in figure 4.1, in terms <strong>of</strong> the so-called packing fraction, a dimensionlessdensity that expresses the ratio <strong>of</strong> the volume that is occupied by the colloids,η i (x) = πσ3 i6 ρ i(x). (4.6)The particles <strong>of</strong> component 2 are twice as heavy as the particles <strong>of</strong> component1, and on the basis <strong>of</strong> their gravitational length, component 2 is expected tobe on the bottom. However, due to their charge ratio, other situations mayoccur as well, as is shown. Figure 4.1a shows a strong segregation <strong>of</strong> thecomponents, not a mixture <strong>of</strong> barometric distributions like our atmosphere.Although the heavier component 2 is below component 1, the situation isreversed in figure 4.1c. Apparently independent <strong>of</strong> mass, the colloidal componentscan live together as well in figure 4.1b.How can this be?We cannot see this directly from theory, the ’Donnan-method 2 ’ needed toomany assumptions and the ’PB-method 3 ’ could not be solved analytically.An explanation can still be found after an examination <strong>of</strong> φ(x), or equivalently,the salt pr<strong>of</strong>iles, and related, the electric field (see figure 4.2)2 see section 3.23 see section 3.318

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