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Suction at the Permeate Side

The gas is applied as a mixture to the retentate (high pressure) side of the membrane, the components of the mixture diffuse with different rates through the membrane under the action of a total pressure gradient and are removed at the permeate side by a sweep gas or by vacuum suction. Because the only segregative mechanisms in mesopores are Knudsen diffusion and surface diffusion/capillary condensation (see Table 9.1), viscous flow and continuum (bulk gas) diffusion should be absent in the separation layer. Only the transition state between Knudsen diffusion and continuum diffusion is allowed to some extent, but is not preferred because the selectivity is decreased. Nevertheless, continuum diffusion and viscous flow usually occur in the macroscopic pores of the support of the separation layer in asymmetric systems (see Fig. 9.2) and this can affect the separation factor. Furthermore the experimental set-up as shown in Fig. 9.11 can be used vmder isobaric conditions (only partial pressure differences are present) for the measurement of diffusivities in gas mixtures in so-called Wicke-Callenbach types of measurement. [Pg.356]

The permeate is continuously withdrawn through the membrane from the feed sueam. The fluid velocity, pressure and species concentrations on both sides of the membrane and permeate flux are made complex by the reaction and the suction of the permeate stream and all of them depend on the position, design configurations and operating conditions in the membrane reactor. In other words, the Navier-Stokes equations, the convective diffusion equations of species and the reaction kinetics equations are coupled. The transport equations are usually coupled through the concentration-dependent membrane flux and species concentration gradients at the membrane wall. As shown in Chapter 10, for all the available membrane reactor models, the hydrodynamics is assumed to follow prescribed velocity and sometimes pressure drop equations. This makes the species transport and kinetics equations decoupled and renders the solution of... [Pg.487]

In the filtration of fermentation broths, lysed yeast [21,88-91] microfiltration is used to separate the yeast cells and/or cell fragments. For the Ceramesh ceramic/metal composite membrane of 0.2 pm pore size a flux of 60 1/m h is reported [21] for lysed yeast, at a temperature of about 55°C and a solids concentration of up to 16-17%. The same magnitude of flux and solids concentration are obtained with whole yeast suspensions. Using Kubota membranes in the range of 50 nm to 0.8 pm Narukami et al. [88] choose 0.8 pm for their work with fermentation broth. They report a stable flux of 20 1/m h using suction (0.8 bar) on the permeate side as driving force, whereas the flux decreases as a... [Pg.632]

Submerged membranes are operated with the feed in a vessel at atmospheric pressure. To obtain a TMP, the permeate side has to be below atmospheric pressure, and this is achieved by suction provided by permeate pumping. The pressure on the permeate side will be determined by the TMP defined by Eq. (10.3) as well as a presstrre drop due to permeatc-side (lumen) flow, which may be significant for hollow fibers. This situation has been analyzed for vertical submerged hollow fibers closed at the bottom and with suction at the top. The situation is depicted in Figure 10.18a for a clean water feed, and the axial flux distribution can be estimated from (Chang et al., 2000)... [Pg.260]


See other pages where Suction at the Permeate Side is mentioned: [Pg.222]    [Pg.222]    [Pg.222]    [Pg.224]    [Pg.232]    [Pg.222]    [Pg.222]    [Pg.222]    [Pg.224]    [Pg.232]    [Pg.106]    [Pg.168]    [Pg.223]    [Pg.182]    [Pg.153]    [Pg.742]   


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Permeate Side

Suction

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