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Bubble-free lining

A more complex part, such as a pipefitting, was molded from the same PFA powder mixture. A different cycle was required consisting of heating at 385°C for 45 min followed by 45 min at 357°C. A smooth bubble-free lining on the fitting was obtained. [Pg.233]

The introduction of membrane contactors in industrial cycles might represent an interesting way to realize the rationalization of chemical productions in the logic of the process intensification. Membrane contactors are, in fact, highly efficient systems for carrying out the mass transfer between phases and achieving high removals. They also present lower size than conventional apparatus. Commercial applications are already present (e.g., the electronics industry or bubble-free carbonation lines), however, some critical points must be still overcome and several are the research efforts needed for their further implementation at industrial level, as summarized below ... [Pg.460]

A number of commercial applications of MCs have been already successfully realized. A bubble-free membrane-based carbonation line, using Liqui-Cel equipment, is in operation by Pepsi in West Virginia since 1993. MCs are also used in beer production the CO2 removal stage is followed by nondispersive nitrogenation to obtain a dense foam head. Another important field of application of MC is the production of ultrapure water for semiconductor manufacturing. [Pg.1143]

In an homogeneous (bubble free) fluidised bed the velocity with which the particles are just carried at point b is equal to the fluid velocity. Points on the rising branch of the line for flow around a single sphere to the right of point b are attributed to a fluid velocity greater than the particle velocity. They lie in the region of pneumatic transport. [Pg.363]

A simple cylindrical shape required a temperature of 371°C for 75 min. Alternatively, a temperature of 357°C for 90 min would produce an equally satisfactory lining. The air and/or water media cooled the mold and the part was removed and inspected. A bubble- and porosity-free lining with a uniform wall thickness was obtained. [Pg.233]

Miyauchi and Furusaki, 1974). A bubble-free emulsion then flows down the bed peripherally. This situation clearly leads to some reaction in the dilute phase. An elegant model that accounts for reaction in both the bubbling and dilute regions of the bed has been proposed by Miyauchi (1974), and another by Kunii and Levenspiel (1991) (more in line with their fine particle model). [Pg.298]

The horizontal distribution of bubble frequency in a bubbling free jet which is free from any walls is known to be similar. In other words, the distributions follow a normal (Gaussian) distribution [24,27,28]. The horizontal distribution of bubble frequency near a vertical flat plate is also expected to follow another type of similarity distribution. In order to ascertain this anticipation, each /b value was normalized by the maximum value /B,max and then plotted against a dimensionless horizontal distance from the plate, > /b(= y/y/B,max/2), in Fig- 4.22. The solid line denotes... [Pg.112]

Do not confuse NPSH vdth suction head, as suction head refers to pressure above atmospheric [17]. If this consideration of NPSH is ignored the pump may well be inoperative in the system, or it may be on the border-line and become troublesome or cavitating. The significance of NPSH is to ensure sufficient head of liquid at the entrance of the pump impeller to overcome the internal flow losses of the pump. This allows the pump impeller to operate wfith a full bite of liquid essentially free of flashing bubbles of vapor due to boiling action of the fluid. [Pg.188]

Detector sensitivity is one of the most important properties of the detector. The problem is to distinguish between the actual component and artifact caused by the pressure fluctuation, bubble, compositional fluctuation, etc. If the peaks are fairly large, one has no problem in distinguishing them however, the smaller the peaks, the more important that the baseline be smooth, free of noise and drift. Baseline noise is the short time variation of the baseline from a straight line. Noise is normally measured "peak-to-peak" i.e., the distance from the top of one such small peak to the bottom of the next. Noise is the factor which limits detector sensitivity. In trace analysis, the operator must be able to distinguish between noise spikes and component peaks. For qualitative purposes, signal/noise ratio is limited by 3. For quantitative purposes, signal/noise ratio should be at least 10. This ensures correct quantification of the trace amounts with less than 2% variance. The baseline should deviate as little as possible from a horizontal line. It is usually measured for a specified time, e.g., 1/2 hour or one hour and called drift. Drift usually associated to the detector heat-up in the first hour after power-on. [Pg.11]

The cup shall be filled with the sample to be tested in such a manner that the top of the meniscus is exactly at the filling line at room temperature. The surface of the sample shall be free from bubbles. There shall be none of die sample above the filling line or on the outside of the apparatus... [Pg.463]

The design shown in Figs. I and 2 is an adaptation of the API separator. The gas boot serves as a preseparator flume, slow ing flow to 0.5 ft see (0.15 ire s), downward. This allows entrained free gas [bubbles of 400 microns 400 ft.m) or more) to nse out of the tlowstrcam. The line from the boot to the central riser and the central riser itself arc designed for fluid velocities of 2 to 4 ft/sec (0 6 to 1.2 ire s). These components act together as a forebay. evenly distributing flow to the upper slots. [Pg.200]

Fig. 7.16. The pick-off annihilation rate (q)p, see equation (7.11), for ortho-positronium in 4 He gas at various temperatures, observed by Hautojarvi and Rytsola (1979). At the lowest temperature (q)p is almost independent of density, indicating stable bubble formation. The behaviour gradually changes to that of free ortho-positronium, indicated by the straight line whose slope corresponds to (iZeff) = 0.125 (see table 7.2). The data at 77 K are due to Fox et al. (1977). Fig. 7.16. The pick-off annihilation rate (q)p, see equation (7.11), for ortho-positronium in 4 He gas at various temperatures, observed by Hautojarvi and Rytsola (1979). At the lowest temperature (q)p is almost independent of density, indicating stable bubble formation. The behaviour gradually changes to that of free ortho-positronium, indicated by the straight line whose slope corresponds to (iZeff) = 0.125 (see table 7.2). The data at 77 K are due to Fox et al. (1977).

See other pages where Bubble-free lining is mentioned: [Pg.241]    [Pg.102]    [Pg.385]    [Pg.93]    [Pg.376]    [Pg.679]    [Pg.121]    [Pg.213]    [Pg.813]    [Pg.67]    [Pg.717]    [Pg.38]    [Pg.20]    [Pg.4]    [Pg.444]    [Pg.226]    [Pg.110]    [Pg.225]    [Pg.714]    [Pg.73]    [Pg.122]    [Pg.54]    [Pg.54]    [Pg.54]    [Pg.173]    [Pg.164]    [Pg.211]    [Pg.122]    [Pg.491]    [Pg.850]    [Pg.385]    [Pg.53]   
See also in sourсe #XX -- [ Pg.233 ]




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