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Volume dispersion from

Until recently most industrial scale, and even bench scale, bioreactors of this type were agitated by a set of Rushton turbines having about one-thind the diameter of the bioreactor (43) (Fig. 3). In this system, the air enters into the lower agitator and is dispersed from the back of the impeller blades by gas-fiUed or ventilated cavities (44). The presence of these cavities causes the power drawn by the agitator, ie, the power requited to drive it through the broth, to fall and this has important consequences for the performance of the bioreactor with respect to aeration (35). k a has been related to the power per unit volume, P/ U, in W/m and to the superficial air velocity, in m/s (20), where is the air flow rate per cross-sectional area of bioreactor. This relationship in water is... [Pg.334]

Having established that a finite volume of sample causes peak dispersion and that it is highly desirable to limit that dispersion to a level that does not impair the performance of the column, the maximum sample volume that can be tolerated can be evaluated by employing the principle of the summation of variances. Let a volume (Vi) be injected onto a column. This sample volume (Vi) will be dispersed on the front of the column in the form of a rectangular distribution. The eluted peak will have an overall variance that consists of that produced by the column and other parts of the mobile phase conduit system plus that due to the dispersion from the finite sample volume. For convenience, the dispersion contributed by parts of the mobile phase system, other than the column (except for that from the finite sample volume), will be considered negligible. In most well-designed chromatographic systems, this will be true, particularly for well-packed GC and LC columns. However, for open tubular columns in GC, and possibly microbore columns in LC, where peak volumes can be extremely small, this may not necessarily be true, and other extra-column dispersion sources may need to be taken into account. It is now possible to apply the principle of the summation of variances to the effect of sample volume. [Pg.194]

Dispersion in the sensor volume resulting from Newtonian flow... [Pg.287]

It is seen that columns having diameters less than 2 mm will only tolerate a maximum sample volume of a fraction of a microliter. Although larger volume valves can be used to inject sample volumes of this size, the dispersion from the valve is still likely... [Pg.291]

Most sensor volumes, whether in LC (e.g., a UV absorption cell) or in GC (e.g., a katharometer cell), are cylindrical in shape, are relatively short in length and have a small length-to-diameter ratio. The small length-to-diameter ratio is in conflict with the premises adopted in the development of the Golay equation for dispersion in an open tube and, consequently, its conclusions are not pertinent to detector sensors. Atwood and Golay [12] extended the theory of dispersion in open tubes to tubes of small length-to-diameter ratio. The theory developed is not pertinent here as it will be seen that, with correctly designed cells, that dispersion from viscous sources can be... [Pg.305]

Apparent Dispersion from Detector Sensor Volume... [Pg.306]

To minimize the effect of sample volume on dispersion, and ensure that there was minimum dispersion from the valve and valve connections, a 0.2 pi Valeo internal... [Pg.317]

To determine the band dispersion that results from a significant, but moderate, sample volume overload the summation of variances can be used. However, when the sample volume becomes excessive, the band dispersion that results becomes equivalent to the sample volume itself. In figure 10, two solutes are depicted that are eluted from a column under conditions of no overload. If the dispersion from the excessive sample volume just allows the peaks to touch at the base, the peak separation in milliliters of mobile phase passed through the column will be equivalent to the sample volume (Vi) plus half the base width of both peaks. It is assumed in figure 10 that the efficiency of each peak is the same and in most cases this will be true. If there is some significant difference, an average value of the efficiencies of the two peaks can be taken. [Pg.119]

T. E. Allen. New concepts in spraying dispersants from boats. In Proceedings Volume, pages 3-6. 9th Bien API et al Oil Spill (Prev, Behav, Contr, Cleanup) Conf (Los Angeles, CA, 2/25-2/28), 1985. [Pg.348]

The colloidal stability of silica Suspensions in the present work was assessed by sediment volumes and from the optical coagulation rate constant. In the first method, 50 mg of silica was dispersed in 5 cm3 polymer solution (concentration 10-2 g cm 3) in a narrow tube and the sediment height found at equilibrium. Coagulation rates of the same systems were found by plotting reciprocal optical densities (500nm, 1cm cell) against time. When unstable dispersions were handled, the coagulation was followed in... [Pg.298]

A comparison of the Pt dispersion from SEA vs. DI has also been performed with CPA/alumina [60], In this study, a A-alumina with surface area of 277 m2/g and pore volume of 1.0 mL/g was... [Pg.185]

Figure 5.5 The dynamic viscosity for a quasi-hard sphere dispersion from the data of Mellema et al.13 The frequency has been normalised to the diffusion time for two different particle radii. The volume fraction is

Figure 5.5 The dynamic viscosity for a quasi-hard sphere dispersion from the data of Mellema et al.13 The frequency has been normalised to the diffusion time for two different particle radii. The volume fraction is <p = 0.46...
Eigure 4.2. The E dependence of the storage G (solid symbols) and loss G" (open symbols) moduli of a mono-disperse silicon oil-in-water emulsion stabilized with SDS, with radius a = 0.53 jam, for three volume fractions from top to bottom (j> = 77%, 60%, and 57%. The frequency is 1 rad/s the lines are visual guides. (Adapted from [10].)... [Pg.130]

Flow models show potential or velocity fields resulting from the groundwater flow, unsaturated flow, or in the soil. These potential fields adequately describe the flow process together with further boundary conditions, such as pore volume, dispersivity, etc., in order to calculate the transport behavior (Table 16). [Pg.57]

Equal mass transfer capability per unit of batch volume for gas dispersion from the vessel headspace. [Pg.322]


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Apparent Dispersion from Detector Sensor Volume

Dispersion from sample volume

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