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Plate measurement

FIG. 14-31 Pressure drop for a valve plate, measured versus model prediction ofBoUes [Chem. Eng. Progr. 72(9), 43 (1976)]. Reproduced with permission of the American Institute of Chemical Engineers. Copyright 1976 AlChE. All rights reserved. [Pg.1378]

The area that is theoretically available for separation is equal to the sum of the projected areas or all channels on the horizontal plane. Figure 18-88 shows the horizontally projected area A, of a single channel in a clarifier of unit width. If X is the uniform distance between plates (measured perpendicularly to the plate surface), the clarifier will contain sin Ci/X channels per unit length and an effective collection area per unit clarifier length of A, sin O/X, where Ot is the angle of inclination of the plates to the horizontal. It follows that the total horizontally projected plate area per unit volume of sludge in the clarifier Aj is... [Pg.1684]

Explain how you would use a van Deemter plot, as shown in Fig. 14.2 to determine the optimum flow rate for a separation. What are the key variables When using theoretical plate measures for comparing columns, what experimental conditions must be controlled ... [Pg.488]

The cylinder fits into an insert in the baseplate. This plate measures 110 mm x 110 mm and is 6 mm in thickness. Three 6.3 mm rods, 115 mm in height extend from the base plate to the retainer for the ram. The ram itself is 10 mm thick and has a diameter of 39.75 cm, just slightly less than the inside diameter of the coking cylinder so that it can easily coDipact and retain the coal within the cylinder. It is fitted with 76.5 cm long "T-shaped" handle, threaded through the retainer. Thus the ram can be raised or lowered to provide any desired degree of compaction in the coal. [Pg.314]

Fig. 1.4. Evidence for the validity of the stress-optical law [Philippoff (8, 9)]. 15 per cent solution of poiyisobutylene B-100 in decalin. (A) extinction angle % and flow birefringence An vs. shear stress pa at 30° C. (o) and An at 50° C. ( ) calculated % according to eq. 1.3 from cone-and-plate measurements at 30° C. ( , An sin2 at 30 and 50° C, respectively... Fig. 1.4. Evidence for the validity of the stress-optical law [Philippoff (8, 9)]. 15 per cent solution of poiyisobutylene B-100 in decalin. (A) extinction angle % and flow birefringence An vs. shear stress pa at 30° C. (o) and An at 50° C. ( ) calculated % according to eq. 1.3 from cone-and-plate measurements at 30° C. ( , An sin2 at 30 and 50° C, respectively...
Black Microtiter Plate Measured Using a Prototype Luminometer... [Pg.200]

Improved separation of natural oil TGs using short columns packed with 3-//m alkyl bonded-phase particles was reported by Dong and DiCesare (88). The HPLC columns used were HS-3 high-speed columns packed with 3-/um C18 bonded-phase particle (100 X 4.6-mm ID) with a column void volume of ca. 0.8 ml and efficiencies in the range of 13,000-15,000 theoretical plates (measured under optimized conditions) and HS5 C,8 columns (125 X 4.6-mm ID packed with 5-yttm particles). Two detectors were used a modified refractive index detector having an 8-/rl flow cell and 0.007-in. ID inlet tubing and a variable-wavelength UV/visible detector. [Pg.212]

This method has been used to obtain force-separation curves for block copolymers adsorbed on planar substrates and subjected to uniaxial compression. Block copolymers are adsorbed from solution onto atomically flat substrates (e.g. mica, quartz) and the force between the plates measured for separations ranging from —0.1 to contact. Further details of the experiments are given in Section 3.8.2. [Pg.19]

Figure 7. Wilhelmy plate measurements of surface tension for SLS solutions (A) no MM A (B) saturated with MM A... Figure 7. Wilhelmy plate measurements of surface tension for SLS solutions (A) no MM A (B) saturated with MM A...
Fig. 4. Measurement sequence of third-harmonic generation in solution. A THG experiment of fused silica in vacuum yields the calibration of the whole setup. The same fused silica plate measured in air leads to the air contribution, which is afterwards taken into account in the THG measurements of the various sample concentrations... Fig. 4. Measurement sequence of third-harmonic generation in solution. A THG experiment of fused silica in vacuum yields the calibration of the whole setup. The same fused silica plate measured in air leads to the air contribution, which is afterwards taken into account in the THG measurements of the various sample concentrations...
Asbestos, quartz or other minerals can be analyzed by consideration of mineralogical principles and crystal systems. Polarized light, compensation plates, measurement of angles of extinction and dispersion staining are useful techniques. Optical behavior of a mineral is related to the internal crystal structure of the mineral. Tables of optical constants are useful for mineral identification. The microscope is a powerful tool for analysis that should not be overlooked by the industrial hygiene chemist. [Pg.37]

If the sample spot showed some diffusion during development, use the center of the spot in determining the Rf value. Also, if the solvent front migrated unevenly across the plate, measure the distance traveled by the sample (cm) relative to the distance traveled by the solvent front (cm) in each lane. [Pg.117]

Fig. 2.4 presents a measuring cell with a porous plate made of sintered glass (similar to variant C, Fig. 2.2). Porous plates of various pore radii can be used (usually the smallest radius is about 0.5 p.m) [23]. In this case the meniscus penetrates into the pores and their radius determines the radius of curvature, i.e. the small pore size allows to increase the capillary pressure until the gas phase can enter in them. The radius of the hole in which the film is formed is usually 0.025 - 0.2 cm. To provide a horizontal position of the film the whole plate is made very thin. In the porous plate measuring cell (Fig. 2.4) the capillary pressure can be varied to more than 10s Pa, depending on the pores size and the surface tension of the solution. When the maximum pore radius is 0.5 (tm, the capillary pressure is 3- 10s Pa at a - 70 mN/m. Fig. 2.4 presents a measuring cell with a porous plate made of sintered glass (similar to variant C, Fig. 2.2). Porous plates of various pore radii can be used (usually the smallest radius is about 0.5 p.m) [23]. In this case the meniscus penetrates into the pores and their radius determines the radius of curvature, i.e. the small pore size allows to increase the capillary pressure until the gas phase can enter in them. The radius of the hole in which the film is formed is usually 0.025 - 0.2 cm. To provide a horizontal position of the film the whole plate is made very thin. In the porous plate measuring cell (Fig. 2.4) the capillary pressure can be varied to more than 10s Pa, depending on the pores size and the surface tension of the solution. When the maximum pore radius is 0.5 (tm, the capillary pressure is 3- 10s Pa at a - 70 mN/m.
Fig. 2.4. Scheme of the porous plate measuring cell employed in the Thin Liquid Film - Pressure... [Pg.46]

The porous plate measuring cell can be regarded as an appropriate development of the cell with porous disk, proposed earlier by Maysels and Jones [24,25] (Fig. 2.5). This disk is made of a sintered porcelain glued to a Perspex holder. A channel around the circumference of... [Pg.46]

A block-scheme of the apparatus for the study of foam films under applied pressure is shown in Fig. 2.11. The films are formed in the porous plate of the measuring cell (Fig. 2.4, variant D and E). The hydrodynamic resistance in the porous plate is sufficiently small and the maximum capillary pressure which can be applied to the film is determined by the pore material. The porous plate measuring cell (Fig. 2.4, variants D and E) permits to increase the capillary pressure up to 105 Pa, depending on the pore size and the surface tension of the solution. When the maximum pore size is 0.5 pm, the capillary pressure is 310s Pa (at cr = 70 mN/m). The cell is placed in a thermostating device, mounted on the microscopic table. [Pg.58]

In order to understand the nature of surface forces which characterise the thermodynamic state of black foam films as well as to establish the CBF/NBF transition, their direct experimental determination is of major importance. This has been first accomplished by Exerowa et al. [e.g. 171,172] with the especially developed Thin Liquid Film-Pressure Balance Technique, employing a porous plate measuring cell (see Section 2.1.8). This technique has been applied successfully by other authors for plotting 11(A) isotherms of foam films from various surfactants solutions [e.g. 235,260,261]. As mentioned in Chapter 2, Section 2.1.2, the Pressure Balance Technique employing the porous ring measuring cell has been first developed by Mysels and Jones [262] for foam films and a FI(A) isotherm was... [Pg.170]

In the device presented in Fig. 3.120,a the asymmetric film forms when a water droplet approaches the surface of an organic liquid. The thickness of the film obtained is controlled by either lowering the level of the organic liquid or by rising the water level, with the aid of microscrews. In the cell shown in Fig. 3.120,b the film forms in a capillary contacting a porous material. The principle of action of this device is similar to that employed in the study of foam films formed in the porous plate measuring cell of Exerowa-Scheludko (see Chapter 2, Fig. 2.2C). [Pg.320]

Under Roscoe Dickinson s guidance, Pauling learned how to use the finicky and complicated X-ray instrument, how to grow his own crystals, how to cut and polish them at specific angles, place them carefully in the apparatus, capture the X-ray diffraction patterns on photographic plates, measure the intensity and position of each important point, and analyze the patterns mathematically to see what they said about the atomic structure. [Pg.32]

Other points are of interest in this TICA scan the minima that occur between the Tg s identified above. There is an obvious minimum of all three components at the same temperature indicating an R point where dT /dt = dT/dt as described previously ( 7). This occurs at =265°C. There should be another such minimum in the first part of the scan during the fluid melt phase of the reaction but it cannot be seen on a TICA scan due to its insensitivity at regions of low matrix resin modulus. Parallel plate measurements on the RMS under the same environmental conditions as the TICA scan indicate a minimum occurring at 142°C. [Pg.57]


See other pages where Plate measurement is mentioned: [Pg.188]    [Pg.37]    [Pg.565]    [Pg.236]    [Pg.21]    [Pg.149]    [Pg.188]    [Pg.189]    [Pg.373]    [Pg.44]    [Pg.156]    [Pg.43]    [Pg.52]    [Pg.10]    [Pg.25]    [Pg.123]    [Pg.240]    [Pg.245]    [Pg.146]    [Pg.47]    [Pg.58]    [Pg.58]    [Pg.268]    [Pg.445]    [Pg.226]   
See also in sourсe #XX -- [ Pg.9 ]




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Bending plate measurement

Contact angle measured glass plates covered with

Parallel plate measurements

Parallel plate viscometers, rheological measurements

Plate number measurement

Viscosity measurement oscillating plate method

Wilhelmy plate technique, surface tension measurement

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