1971
DOI: 10.1021/i260037a018
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Design Theory and Separations in Preparative-Scale Continous-Flow Annular-Bed Electropheresis

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Cited by 21 publications
(14 citation statements)
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“…Electrochromatography (EC) is a form of gradient liquid chromatography in which an electric potential is applied to columns packed with gel-filtration media (Hybarger et al, 1963;Vermeulen et al, 1971;Salak and Roch, 1972;Luzzio, 1975;O'Farrell, 1985;Scott, 1986;Tsuda, 1987;Rudge et al, 1993). The method of Rudge et al (1993) and Ivory (1988) combines gel electrophoresis and liquid chromatography to resolve biomacromolecules on the basis of molecular weights and electrophoretic mobilities.…”
Section: Introductionmentioning
confidence: 99%
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“…Electrochromatography (EC) is a form of gradient liquid chromatography in which an electric potential is applied to columns packed with gel-filtration media (Hybarger et al, 1963;Vermeulen et al, 1971;Salak and Roch, 1972;Luzzio, 1975;O'Farrell, 1985;Scott, 1986;Tsuda, 1987;Rudge et al, 1993). The method of Rudge et al (1993) and Ivory (1988) combines gel electrophoresis and liquid chromatography to resolve biomacromolecules on the basis of molecular weights and electrophoretic mobilities.…”
Section: Introductionmentioning
confidence: 99%
“…Mathematical models for electrokinetic systems in literature describe heat-transfer effects (Vermeulen et al, 1971;Lynch and Saville, 1981;Datta et al, 1986;Yoshisato et al, 1986;Ivory and Gobie, 1990;Raj and Hunter, 1991). This article presents a modified electrochromatography system that minimizes Joule heating at electric field strengths up to 125 V/cm by heat dissipation through a cooling jacket (6°C) and use of a cooled, low ionic strength eluting buffer.…”
Section: Introductionmentioning
confidence: 99%
“…The relationship between~-potential and electrophoretic mobility is long established: in the case of small Ka (but >0.1), the use of the Debye-Huckel approximation yields the following expression for spheres However, many systems of interest in particle-collector interactions do not correspond exactly to either of these two limiting cases, and it is necessary to assume that the external field (that is deformed by the presence of the colloidal particle) and the field of the double layer are additive. Consequently, Henry [65] derived the following expression for the mobility E( iatJ1 i atJ1 ) U E = -~+ 5a 5 -dr -20 3 -dr 11 00 ,0 00 r 4 (2)(3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17) where r is the radial distance from the centre of the particle. Combining the Debye-Huckel approximation with Eq.…”
Section: Zeta-potential (~)mentioning
confidence: 99%
“…Combining the Debye-Huckel approximation with Eq. (2)(3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17), and integrating yields the so-called Henry equation…”
Section: Zeta-potential (~)mentioning
confidence: 99%
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