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Continuous system diffusion

Solutions for diffusion with and without chemical reaction in continuous systems have been reported elsewhere (G2, G6). In general, all the parameters in this model can be determined or estimated, and the theoretical expressions may assist in the interpretation of mass-transfer data and the prediction of equipment performance. [Pg.359]

This PAGE is a continuous system with respect to pH. Its resolution is lower than that of a disc system. The advantage lies in the use of buffers free of primary amino groups therefore, it is recommended if an electrotransfer is intended onto chemical reactive supports because a buffer change decreases transfer yield and separation performance (broadening of bands by diffusion during buffer change). [Pg.32]

The model (Fig. 23.6) consists of three compartments, (a) the surface mixed water layer (SMWL) or epilimnion, (b) the remaining open water column (OP), and (c) the surface mixed sediment layer (SMSL). SMWL and OP are assumed to be completely mixed their mass balance equations correspond to the expressions derived in Box 23.1, although the different terms are not necessarily linear. The open water column is modeled as a spatially continuous system described by a diffusion/advection/ reaction... [Pg.1085]

Bacterial inactivation is achieved by CO2 absorption in the liquid phase, even though the reason why it happens is still not clear. In this respect, batch- and semi-continuous operating modes are substantially different. In the batch system the residence time, i.e., the time of contact between gas- and liquid phase, must be sufficient to allow the diffusion of CO2 in the liquid, and is therefore a fundamental parameter to assure a desired efficiency. In the semi-continuous system the contact between the phases is localized in the surface of the moving micro-bubbles. In this second case, the efficiency of the process is influenced by temperature, pressure, gas flux, bubble diameter, and other parameters that modify the value of the mass-transfer coefficient. Therefore, it is not correct to use the residence time as a key parameter in the semi-continuous process. In fact, a remarkable microbial inactivation is reached even with an exposure time of 0 min (i.e., pressurizing and immediately depressurizing the system) these two steps are sufficient to allow CO2 to diffuse through the liquid phase. [Pg.633]

A process referred to as vapor-arbitrated pervaporation addresses these issues by manipulating the transmembrane activity gradients of water and ethanol in a pervaporation system. Using a permeate side sweep stream that contains water vapor at a partial pressure corresponding to the activity of water on the feed side, permeation of water is halted while ethanol continues to diffuse through the membrane into the sweep stream and is removed. In this way, the native permselectivity of the membrane system can be altered in a controlled fashion to extract one or more volatile components from a solution. [Pg.378]

This equation shows that the entropy production is a quadratic form in all the forces. In continuous systems, the base of reference for diffusion flow affects the values of transport coefficients and the entropy due to diffusion. Prigogine proved the invariance of entropy for an arbitrary base of reference if the system is in mechanical equilibrium and the divergence of viscous tensors vanishes. [Pg.128]

Transference numbers are quantities which are treated in the thermodynamics of irreversible processes. In a continuous system, the average velocity Vi of a species i related to a reference velocity w, describes the diffusional motion of the species i. The diffusion current density Ji represents in moles/cm sec the flow of species i in unit time perpendicular to a surface of unit area which by itself is moving with velocity... [Pg.133]

Figure 10.9. Continuous system used by Su et al. to implement various anaiyticai methods inciuding a fiow-injection manifoid, a gas-diffusion unit and a buik acoustic impedance sensor. A acceptor, BAWIS buik acoustic wave impedance sensor, C — carrier, GDC — gas diffusion ceii, iV — injection vaive, PP — peristaitic pump, R — reagent, RC — reaction coii, SL — sampie ioop, 1/1/— waste, WB — water bath. (Reproduced with permission of Eisevier, Ref. [98].)... Figure 10.9. Continuous system used by Su et al. to implement various anaiyticai methods inciuding a fiow-injection manifoid, a gas-diffusion unit and a buik acoustic impedance sensor. A acceptor, BAWIS buik acoustic wave impedance sensor, C — carrier, GDC — gas diffusion ceii, iV — injection vaive, PP — peristaitic pump, R — reagent, RC — reaction coii, SL — sampie ioop, 1/1/— waste, WB — water bath. (Reproduced with permission of Eisevier, Ref. [98].)...
After these first experiments it took 11 years until this problem was studied again exploiting the unique possibilities of NSE with respect to contrast variation and energy resolution [29]. The studied microemulsion was an o/w-droplet microemulsion in the system H2O/ -octane/C10E5. It turned out that the NSE data can be analysed using a double exponential fit according to Eq. (2.8), when the translational diffusion coefficient is already measured in advance using PCS. The same approach was also successfully applied to study another water-continuous microemulsion in the system H2 0/n-dodecane/Cio E-[49]. Since the approach works as well for oil-continuous systems an extended example for the approach will be discussed in the next subsection. [Pg.56]

We have seen that delayed feedback can be an efficient method for manipulation of essential characteristics of chaotic or noise-induced spatiotem-poral dynamics in a spatially discrete front system and in a continuous reaction-diffusion system. By variation of the time delay one can stabilize particular unstable periodic orbits associated with space-time patterns, or deliberately change the timescale of oscillatory patterns, and thus adjust and stabilize the frequency of the electronic device. Moreover, with a proper choice of feedback parameters one can also effectively control the coherence of spatio-temporal dynamics, e. g. enhance or destroy it. Increase of coherence is possible up to a reasonably large intensity of noise. However, as the level of noise grows, the efficiency of the control upon the temporal coherence decreases. [Pg.177]

As we saw in Sect. 10.1, the stability properties of the uniform steady state of spatially continuous reaction-diffusion systems can be analyzed in terms of normal modes corresponding to the eigenfunctions of the Laplace operator. Othmer and... [Pg.368]

The roots of (13.39) have to be positive, since both k > 0 and r > 0. As for the Turing instability in spatially continuous reaction-diffusion system, see Sect. 10.1.2,... [Pg.374]

In the earlier chapters, transport phenomena involving a barrier have been discussed from the angle of (i) basic understanding of the physico-chemical phenomena and (ii) test of the linear thermodynamics of irreversible processes. Similar phenomena in continuous systems such as thermal diffusion (Soret effect)/Dufour effect are of equal... [Pg.81]

Systems involving thermal diffusion and Dufour effect are continuous systems without a barrier. For investigating continuous systems, the local variation of properties has to be considered. We shall first consider a general case where mass flux, heat flux and chemical reactions are occurring [4, 5]. [Pg.82]

In continuous systems, the situation is not so clear. On account of experimental difficulties, exhaustive tests as in the above case have not been performed. Nevertheless, experimental results on thermal diffusion and Dofour effect/Soret do support the theoretical predictions although in a much limited range, again on account of limited range of validity of Gibbs equation. [Pg.98]

Many liquid and semi-liquid pharmaceutical preparations are disperse systems. Disperse systems are defined as systems in which a substance is distributed as particles (discontinuous) into a dispersion medium (continuous). Three types of disperse systems will be discussed which are pharmaceutically relevant colloidal systems, suspensions and emulsions. In both colloidal systems and suspensions, solid particles are dispersed in a liquid. The difference is that in colloidal systems the particles do not settle, while they do in suspensions. This difference is caused by the size of the particles. In colloidal systems, the particles are so small (1 mn - 1 pm) that the Brownian motion (diffusion caused by thermal energy) is stronger than the force of gravity so that they remain suspended in the liquid and do not settle. In suspensions, the particles are larger (>1 pm) and as a consequence the force of gravity is stronger than the Brownian motion which makes them settle (if the density of the particles is larger than that of the dispersion medium). Emulsions consist of non-miscible liquids. Two types of emulsions will be discussed oil drops dispersed in water (oil-in-water emulsion or o/w emulsion) and water drops dispersed in oil (water-in-oil emulsion or w/o emulsion). There are also more complex structures such as w/o/w emulsions and bi-continuous systems. However, these systems will not be discussed. [Pg.369]

At higher water contents of the support the water layer becomes too thick and the substrate has to diffuse into the water layer, or the catalyst has to diffuse to the interface. The result is a decrease in catalyst-product contact time leading to lower activities. This sensitivity towards water is a drawback of this otherwise attractive concept. Horvath performed experiments using substrates with different solubilities in water and showed that, under optimal conditions, this solubility did not influence the activity [18]. Furthermore, he performed a hydroformylation reaction in a continuous system and even under reaction conditions no leaching of rhodium complex was detected. The water obviously leaches if the SAPC is used in a continuous flow system, which in a practical application should be compensated for by using water-saturated organic solvents. [Pg.261]


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