Frans_M_Everaerts_Isotachophoresis_378342.pdf

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ISOTACHOPHORESIS 13 2.4. PRINCIPLE OF iSOTACHOPHORESIS 2.4.1. Introduction We shall consider here the separation of anionic species in narrow-bore tubes. For the separation of anionic species, the narrow-bore tube and anode compartment are filled with the so-called leading electrolyte, the anions of which must have a mobility that is higher than that of any of the sample anionic species. The cations of the leading electrolyte must have a buffering capacity at the pH at which the analyses will be performed. The cathode compartment is filled with the terminating electrolyte, the anions of whch must have a mobility that is lower than that of any of the sample anionic species. The sample is introduced between the leading and terminating electrolyte, e.g., by means of a sample tap or a micro-syringe. #en an electric current is passed through such a system (see Fig.2.5a), a uniform electric field strength over the sample zone occurs and hence each sample anionic species will have a different migration velocity according to eqn. 2.1. The sample anionic species with the highest effective mobility will run forwards and those with lower mobilities will remain behind. Hence, both in front of and behind the original sample zone, the movingboundary procedure results in two series of mixed zones (comparable with the Tiselius method). In the series of mixed zones, the sample anionic species are arranged in order of their decreasing effective mobilities (see Fig.2.5b), The anionic species of the leading electrolyte can never be passed by sample anions, because its effective mobility is chosen so as to be higher. Similarly, the terminating anions can never pass the anionic species of the sample. In this way, the sample zones are sandwiched between the leading and terminating electrolyte. In the mixed zones of the sample (see Fig.2.5b), the separation continues and, after some time, when the separation is complete, a series of zones is obtained in which each zone contains only one anionic species of the sample if no anionic species with identical effective mobilities are present in the sample. Of course, this series of zones is still sandwiched between leading and terminating electrolyte (see Fig.2.5~). The first sample zone contains the anionic species of the sample with the highest effective mobility, the last zone that with the lowest effective mobility. After this stage, no further changes to the system occur and a steady state has been reached. In such a case, we can speak of an isotachophoretic separated system. (Of course, one or more unmixable ‘mixed zones’, i.e., zones that contain one or more anionic species with identical effective mobilities, may still be present.) In this state, all of the zones must run connected together, in contrast to zone electrophoresis, where all zones release. Here the zones cannot release as there is no background electrolyte that can support the electric current (a requirement for the solvent is that its self-conductance must be negligible; see section 5.2 .)* . *If it is assumed that the zones release, then the concentration of the ionic species at that position will decrease, the electric field strength will increase (working at a constant current density) and hence the migration velocity of the ionic species involved will be higher. Therefore, finally these ionic species will reach the preceding zone.
14 PRINCIPLES OF ELECTROPHORETIC TECHNIQUES b 0 L C , conatant ,,, Fig.2.5. Separation of a mixture of anions according to the isotachophoretic principle. The sample A+B+C is introduced between the leading anionic species L and the terminating anionic species T. A suitable cationic species is chosen as the buffering counter ion. The original conditions are shown in (a). After some time (b), some mixed zones are obtained according to the moving boundary principle. Finally (c), all anionic species of the sample are separated and all zones contain only one anionic species of the sample (‘ideal case’). For this steady state, all zones must have identical migration velocities, determined by the migration velocity of the anionic species of the leading electrolyte. Considering the zones L, A, B, C and T (see Figure 2.5~): v, = VA = V B = vc = VT or m,E, = mAEA = mBEB = m,Ec = mTET (2.4) Eqn. 2.4 will be called the ‘isotachophoretic condition’ and it is characteristic of isotachophoretic separations.
Page 2 and 3: Journal of Chromatogaphy Library -
Page 4 and 5: Journal of Chromatography Library -
Page 6 and 7: Dedicated to Pr0f.Dr.h. A.I.M. Keul
Page 8 and 9: Contents Preface ..................
Page 10 and 11: CONTENTS IX 6.4.2. The d.c. method
Page 12 and 13: CONTENTS XI 12.2.2. Applications ..
Page 14 and 15: It is very well known that charged
Page 16 and 17: Chapter 1 Historical review SUMMARY
Page 18 and 19: HISTORICAL REVIEW 3 Independently i
Page 20 and 21: THEORY
Page 22 and 23: Chapter 2 Principles of electrophor
Page 24 and 25: MOVINGBOUNDARY ELECTROPHORESIS a S
Page 26 and 27: MOVINGBOUNDARY ELECTROPHORESIS 0 iu
Page 30 and 31: ISOTACHOPHORESIS 15 As the anionic
Page 32 and 33: ISOTACHOPHORESIS velocities, so tha
Page 34 and 35: ISOTACHOPHORESIS 19 d.t ’.t I Fig
Page 36 and 37: ISOTACHOPHORESIS 21 t Fig.2.8. Isot
Page 38 and 39: ISOELECTRIC FOCUSING 23 The four is
Page 40 and 41: DISCUSSION 25 Fig.2.11. Survey of t
Page 42 and 43: Chapter 3 Concept of mobility SUMMA
Page 44 and 45: IONIC MOBILITY AND IONIC EQUIVALENT
Page 46 and 47: EFFECTIVE IONIC MOBILITY 31 obtain
Page 48 and 49: EFFECTIVE IONIC MOBILITY 33 compari
Page 50 and 51: EFFECTIVE IONIC MOBILITY Fig.3.4. R
Page 52 and 53: DETERMINATION OF IONIC MOBILITIES 3
Page 54 and 55: DETERMINATION OF IONIC MOBILITIES 3
Page 56 and 57: Chapter 4 Mathematical model for is
Page 58 and 59: GENERAL EQUATIONS 43 anionic specie
Page 60 and 61: GENERAL EQUATIONS 4.2.1. Equilibriu
Page 62 and 63: GENERAL EQUATIONS 41 i Similar equa
Page 64 and 65: GENERAL EQUATIONS 49 Uthzone (U-llt
Page 66 and 67: GENERAL EQUATIONS 4.2.4. Modified O
Page 68 and 69: GENERAL EQUATIONS TABLE 4.2 REDUCED
Page 70 and 71: MATHEMATICAL MODEL FOR THE STEADY S
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MATHEMATICAL MODEL FOR THE STEADY S
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VALIDITY OF THE ISOTACHOPHORETIC MO
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CHECK OF THE ISOTACHOPHORETIC MODEL
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CHECK OF THE ISOTACHOPHORETIC MODEL
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REFERENCES 81 Fig.4.17. Relationshi
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Chapter 5 Choice of electrolyte sys
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CHOICE OF THE SOLVENT 85 In general
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CHOICE OF THE SOLVENT TABLE 5.2 THE
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CHOICE OF THE SOLVENT pH and pKvalu
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CHOICE OF THE SOLVENT 91 TABLE 5.4
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CHOICE OF THE pH OF THE LEADING ELE
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CHOICE OF THE pH OF THE LEADING ELE
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CHOICE OF THE TERMINATING AND LEADI
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ADDITIONS TO THE ELECTROLYTE SOLUTI
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EXAMPLES Choice of solvent. Can wat
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EXAMPLES 103 solvent, hoping that a
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EXAMPLES TABLE 5.11 STEP HEIGHTS OF
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EXAMPLES TABLE 5.12 STEP HEIGHTS OF
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Fig.5.9. Isotachopherograms of the
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EXAMPLES II 4 3 Fig.5.11. Isotachop
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REFERENCES 113 Example I. As exampl
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INSTRUMENTATION
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Chapter 6 Detection systems SUMMARY
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THERMOMETRIC RECORDING 6.1.3. Combi
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THERMOMETRIC RECORDING Potential gr
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THERMOMETRIC RECORDING /2 Fig.6.1.
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THERMOMETRIC RECORDING T t l Fig.6.
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THERMOMETRIC RECORDING 7 127 It-- I
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THERMOMETRIC RECORDING a concentrat
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HIGH-FREQUENCY CONDUCTIVITY DETECTI
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CONDUCTIVITY DETECTION 133 Fig.6.9.
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CONDUCTIVITY DETECTION 135 The d.c.
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CONDUCTIVITY DETECTION 137 Hi V 1kR
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CONDUCTIVITY DETECTION Fig.6.12. Co
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CONDUCTIVITY DETECTION Fig.6.14. Th
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CONDUCTIVITY DETECTION 143 6.4.4. T
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CONDUCTIVITY DETECTION 145 contact
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CONDUCTIVITY DETECTION 147 We can n
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CONDUCTIVITY DETECTION 149 N.Y., U.
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CONDUCTIVITY DETECTION 151 achieved
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UV ABSORPTION METER 153 -_-.- +- R
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UV ABSORPTION METER Fig.6.22. Contr
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W ABSORPTION METER r +15V -15V Mod
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W ABSORPTION METER 159 TABLE 6.4 PR
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W ABSORPTION METER 230 240 2% m zm
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to Mod (Fig 6.24) oscillator I sync
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UV ABSORPTION METER 165 dicular to
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Fig.6.31. Isotachopherograms for th
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UV ABSORPTION METER 169 50 Fig.6.33
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ADDITIVES TO THE ELECTROLYTES 171 6
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ADDITIVES TO THE ELECTROLYTES 173 e
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ADDITIVES TO THE ELECTROLYTES 175 a
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ADDITIVES TO THE ELECTROLYTES 177 o
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ADDITIVES TO THE ELECTROLYTES 179 d
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ADDITIVES TO THE ELECTROLYTES 181 T
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ADDITIVES TO THE ELECTROLYTES Fig.6
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ADDITIVES TO THE ELECTROLYTES 185 F
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ADDITIVES TO THE ELECTROLYTES 1 2 3
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ADDITIVES TO THE ELECTROLYTES 189 n
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COATING OF THE MICRO-SENSING ELECTR
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DETECTION LIMITS 193 electric drivi
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DETECTION LIMITS 195 Fig.6.48. Infl
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DETECTION LIMITS 197 TABLE 6.6 SURV
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CONCLUSION 199 average length of a
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REFERENCES 201 seen. Again it is cl
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Chapter 7 Instrumentation SUMMARY T
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INJECTION SYSTEMS I! I n Fig.7.1. P
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INJECTION SYSTEMS Fig.7.3. Exploded
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INJECTION SYSTEMS Fig.7.5. Injectio
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COUNTER ELECTRODE COMPARTMENTS 21 1
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COUNTER ELECTRODE COMPARTMENTS Even
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COUNTER ELECTRODE COMPARTMENTS 21 5
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EQUIPMENT the large bore, a more di
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EQUIPMENT 219 belonging to three cl
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EQUIPMENT 221 signal of the thermoc
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EQUIF'MENT 223 No effect on the res
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EQUIPMENT 225 Fig.7.14. Electrophor
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EQUIPMENT Fig.7.16. Photograph of t
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EQUIPMENT 229 mounted equiplanar, w
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COUNTER FLOW OF ELECTROLYTE 231 ins
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COUNTER FLOW OF ELECTROLYTE p High
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COUNTER FLOW OF ELECTROLYTE Fig.7.2
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COUNTER FLOW OF ELECTROLYTE 231 aro
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COUNTER FLOW OF ELECTROLYTE p high
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COUNTER FLOW OF ELECTROLYTE 24 1 7.
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COUNTER FLOW OF ELECTROLYTE I I 31
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COUNTER FLOW OF ELECTROLYTE max. 15
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APPLICATIONS
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Chapter 8 Introduction SUMMARY In t
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INTRODUCTION 25 1 the various ionic
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Chapter 9 Practical aspects SUMMARY
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DISTURBANCES CAUSED BY H+ AND OH 25
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DISTURBANCES CAUSED BY H+ AND OH- 2
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DISTURBANCES DUE TO CO, 263 Electro
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ENFORCED ISOTACHOPHORESIS 265 t T T
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WATER AS TERMINATOR 267 function of
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PURIFICATION OF THE TERMINATOR 7 4
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REFERENCES 271 AS an example, the c
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Chapter 10 Quantitative aspects SUM
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THERMOMETRIC MEASUREMENTS 215 vj c
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THERMOMETRIC MEASUREMENTS TABLE 10.
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CONDUCTIMETRIC MEASUREMENTS factor
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CONCLUSION 28 1 Tables 10.3-10.5 wa
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Chapter 11 Separation of cationic s
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SEPARATION USING A THERMOCOUPLE AS
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I SEPARATION USING A THERMOCOUPLE A
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SEPARATION USING CONDUCTIVITY AND U
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Chapter I2 Separation of anionic sp
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SEPARATION USING A THERMOMETRIC DET
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SEPARATION USING CONDUCTIVITY AND W
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Chapter 13 Amino acids, peptides an
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AMINO ACIDS TABLE 13.1 OPERATIONAL
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AMINO ACIDS 8- ?- 6- 5- 4- 3- 2- f-
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AMINO ACIDS 317 TABLE 13.5 STEP HEI
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AMINO ACIDS Fig.13.3. Schematic dia
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AMINO ACIDS TABLE 13.6 DETERMINATIO
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SEPARATION OF PROTEINS IN AMPHOLYTE
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SEPARATION OF SMALL PEPTIDES reprod
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Chapter I4 Separation of nucleotide
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Chapter 15 Enzymatic reactions SUMM
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ENZYMATIC CONVERSION OF GLUCOSE (FR
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ENZYMATIC CONVERSION OF PYRUVATE 35
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Chapter 16 Separations in non-aqueo
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SEPARATION OF ANIONIC SPECIES IN ME
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SEPARATION OF CATIONIC SPECIES IN M
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EXPERIMENTS IN AQUEOUS METHANOLIC S
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Chapter I7 Counter flow of electrol
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INTRODUCTION 317 In various operati
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EXPERIMENTAL 0% 10 % a b 60 % a b a
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EXPERIMENTAL 381 caused by the coun
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CONCLUSION 383 c t r ’r; I I"
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APPENDICES
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Appendix A Simplified model of movi
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PROCEDURE OF COMPUTATION A.3. PROCE
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EXPERIMENTAL 39 1 TABLE A1 THEORETI
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DISCUSSION E I I Fig.A2. Graphical
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Appendix B Diameter of the narrow-b
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Appendix C Literature 1897-1966 F.
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LITERATURE 399 B.P. Konstantinov an
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LITERATURE 401 1971 L. Arlinger, Is
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LITERATURE 403 1973 L. Arlinger and
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LITERATURE 405 A. Chrambach and J.S
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LITERATURE 407 M. Coxon and M.J. Bi
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Symbols and abbreviations SYMBOLS A
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SYMBOLS AND ABBREVIATIONS SUPERSCRI
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Subject index A Absorption meter, U
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SUBJECT INDEX 41 5 Detection limit
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SUBJECT INDEX 41 7 --_ , separation
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