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Frans_M_Everaerts_Isotachophoresis_378342.pdf

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MOVINGBOUNDARY ELECTROPHORESIS<br />

0<br />

iuf ter<br />

n<br />

0<br />

buffer<br />

A<br />

A+B<br />

A+B+C<br />

r<br />

0<br />

butter<br />

a b<br />

0<br />

buffer<br />

-C<br />

- B+C<br />

Fig.2.3. Separation according to the Tiselius moving-boundary principle. In (a), the lower tube is<br />

filled with a mixture of the anions A, B and C. Specific buffers need to be applied for optimal<br />

separation. In (b), it is shown that zones exist on both the front and rear sides, vii., A, A+B and<br />

A+B+C, and A+BtC, BtC and C, respectively.<br />

A+B+C<br />

B and C. Substance B, mixed with A, forms the second sample zone after the pure A<br />

zone. The third zone contains the mixture At B+C.<br />

This method can be compared with frontal analysis in chromatography. In moving-<br />

boundary electrophoresis, the zones generally contain more ionic species of the sample.<br />

The composition of the sample plays an important role in the determination of the<br />

concentrations, pH values and conductivities of the different zones. This situation<br />

contrasts with that in isotachophoresis, where all of these quantities are independent of<br />

the quantitative composition of the sample. A quantitative description of this method<br />

is given in Section 4.2. As will be clear after the description of isotachophoresis, the first<br />

zone in moving-boundary electrophoresis has a self-correcting effect, so that the first<br />

boundary will be sharp. All other zones are not sharp, although this influence is generally<br />

smaller than in zone electrophoresis. In Appendix A, a method is given with which<br />

effective mobilities can be measured by using moving-boundary electrophoresis. Fig.2.4<br />

shows the temperature, voltage gradients and electrical resistances for the different zones.<br />

All of these quantities show similar relationships.<br />

11

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