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Separators parameters for

The concentration of the chiral selector, for instance, has considerable influence on the mobility and separation of the enantiomers. Optical resolution varies with the chiral selector concentration and reaches a maximum value at a given optimum concentration. Wren and Rowe proposed a model that describes the influence of the selector concentration on selectivity, and which was extended by Vigh s group ° by including the pH as a separation parameter for weak acidic enantiomers. The latter model shows that the chiral selectivity is determined by the complex s relative mobility, the CD concentration, the degree of dissociation... [Pg.461]

Separation parameters for pAP and AsA using Topas microchip with different end-channel detectors... [Pg.857]

This peak occurs because the solvent composition used to dissolve the sample often differs somewhat from the mobile phase. When this sample solvent volume reaches the detector (at Vo), a refractive index difference upset of the baseline occurs. This Vo peak is very important because it allows us to normalize the separation parameters for variations in column lengths. It also gives us some assurance that the sample was actually loaded into the injector and onto the column. [Pg.47]

Eqn. (3.72) describes retention in LSC in terms of separate parameters for the adsorbent ( a a) solute (S9, At) and the solvent ( °). As such, it has proved invaluable for the interpretation of retention and selectivity phenomena in LSC. For example, the effect of a change in the solvent using the same stationary phase and the same solute can easily be understood in terms of a variation in °. [Pg.77]

Fig. 1 Separation of rabbit liver metallothionein using CE-ICP-MS. The protein sample (1 mg/mL dissolved in deionized water) was first subjeeted to CZE with UV detection to optimize CE separation parameters for the major metallothionein isoforms (MT-1 and MT-2) shown in the upper panel. The CE instrument was then coupled to an ICP-MS instrument using a specially modified direct injection nebulizer (CETAC Technologies Inc., Omaha, NB) which enabled the entire capillary effluent from the CE to be directly injected into the ICP plasma torch, thus avoiding postcolumn dilution and band-broadening effects of conventional spray chamber nebulizers. Specific isotopes of cadmium ( Cd) and zinc ( Zn) associated with each isoform peak were monitored as shown by the figures in the lower panel. Fig. 1 Separation of rabbit liver metallothionein using CE-ICP-MS. The protein sample (1 mg/mL dissolved in deionized water) was first subjeeted to CZE with UV detection to optimize CE separation parameters for the major metallothionein isoforms (MT-1 and MT-2) shown in the upper panel. The CE instrument was then coupled to an ICP-MS instrument using a specially modified direct injection nebulizer (CETAC Technologies Inc., Omaha, NB) which enabled the entire capillary effluent from the CE to be directly injected into the ICP plasma torch, thus avoiding postcolumn dilution and band-broadening effects of conventional spray chamber nebulizers. Specific isotopes of cadmium ( Cd) and zinc ( Zn) associated with each isoform peak were monitored as shown by the figures in the lower panel.
If the feed is placed on the fourth tray from the top, there would be only four rectifying trays and, therefore, a higher reflux ratio, calculated at 2.0, would be required to obtain the same rectification. The stripping section becomes over-trayed, with several trays showing little change in the separation parameter. If the feed tray is too low, the rectifying section becomes over-trayed. Figure 7.11 is a schematic plot (not to scale) of the separation parameters for the different feed tray locations. [Pg.263]

Vo is also known as the void or dead volume it is the volume of mobile phase which will elute a totally excluded molecule (A). The volume required to elute a particular molecule is the elution volume (or retention volume), Fe- The use of these volumes is not very satisfactory in describing the behaviour of particular solutes, because although they are characteristic of the gel and the solutes they also depend on the volume and packing density of the column. Separation parameters for gel columns are shown in Figure 4.8. [Pg.143]

Beyond its influence on IMS separation parameters for a fixed geometry, the gas temperature affects ion geometries. As ion-molecule collisions must be sufficientiy frequent for a steady drift, ions are thermalized their internal, rotational, and translational modes are equilibrated at a single temperature. At low E/N where the ion drift is much slower than the Brownian motion of gas molecules, relative ion-molecule velocities conform to the Maxwell-Boltzmann distribution and ion temperature equals T of the gas. [Pg.29]

FIGURE 3.49 Normalized mean FAIMS separation parameters for ubiquitin ions (z = 6, 7) in N2 gas over 7=35-80 °C, measured at u=15 (A), 20 ( ), and 25 ( ) kV/cm. For each D. we show the first-order regressions through all data (solid lines) and those for T — 50-80 °C (dashed lines). (From Robinson, E.W., Shvartsburg, A.A., Tang, K., Smith, R.D., Anal. Chem. 80, 7508, 2008.) The vertical displacements of datasets for adjacent d values that provide the best coincidence of regressions are labeled (in °C). [Pg.197]

Table 13 Compositions and microphase separation parameters for PU-PBMA semi-IPNs [285]... Table 13 Compositions and microphase separation parameters for PU-PBMA semi-IPNs [285]...

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See also in sourсe #XX -- [ Pg.451 , Pg.452 ]




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