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Suspension of particles

Note Powder is a generic term for subdivided solid material, comprising pellets, granules and dust. Pellets have a diameter greater than 2 mm (U.S. No. 10 Standard Sieve) and typically above 3 mm. Granules have a diameter between 0.42 and 2 mm, although granular powders typically contain dust. Dusts have a diameter less than 0.42 mm and as low as I pm. Suspensions of particles smaller than I pm are known as fumes. [Pg.167]

Hence, the application of these formulas only applies to very dilute systems. At high particle concentrations, mutual interference in the motion of particles exists, and the rate of settling is considerably less than that computed by the given expressions. In the latter case, the particle is settling through a suspension of particles in a fluid, rather than through a simple fluid medium. [Pg.275]

Equal suspension of particles referenced to visual appearances and physical sample testing. Empirical correlations generalized to apply to most problems. [Pg.317]

The representation of the dispersion viscosity given above related to suspensions of particles of spherical form. Upon a transition to anisodiametrical particles a number of new effects arises. The effect of nonsphericity is often discussed on the example of model dispersions of particles of ellipsoidal form. An exact form of particles to a first approximation is not very significant, the degree of anisodiametricity is only important, or for ellipsoidal-particles, their eccentricity. [Pg.88]

Whereas smokes are often characterized by the mode of their formation, any coned suspension of particles ranging from 0.01 to about 5.0 pm can be considered a smoke. These particles, when suspended in air, reflect, scatter and absorb radiation in a complex manner. A comprehensive model of these interactions in terms of visibility under various conditions was described recently (Ref 62)... [Pg.984]

Colloids are suspensions of particles too small to be seen with a microscope but... [Pg.464]

The effective viscosity of a suspension of particles in a fluid medium is greater than that of the pure fluid, owing to the energy dissipation within the electrical double layers. [Pg.103]

Prager [302] examined diffusion in concentrated suspensions using the variational approach. (A discussion of the basic principles in variational theory is given in Ref. 6.) Prager s result is applicable to a very general class of isotropic porous media. Prager s solution for a limiting case of a dilute suspension of particles was... [Pg.574]

A colloid is a suspension of particles with diameters between 1 nm and 100 nm. The particles are charged and can be subjected to cataphoresis (electrophoresis). They are subject to Brownian movement and have a large amount of surface activity. Their properties lie between those of true solutions and coarse suspensions. [Pg.18]

For suspensions of particles larger than the pores in the membrane, the formation of a filter cake leads to progressively increasing resistance and a declining filtration rate. The higher the suspension concentration, the more rapidly does the rate decline. [Pg.448]

Consider a highly resolved simulation of a set of microscopic TFM equations for a fluidized suspension of particles in a large periodic domain. The filtering operation does not require a periodic domain however, as each location in a periodic domain is statistically equivalent to any other location, statistical averages can be gathered much faster when simulations are done in periodic domains. After an initial transient period that depends on the initial conditions,... [Pg.136]

But the microscopic fat particles suspended in milk have an average diameter in the range 10-7 to 10-5 m, i.e. much larger than k of visible light. A beam of incident light is scattered rather than transmitted by a suspension of particles - a phenomenon known as the Tyndall effect. [Pg.505]

Figure 10. Optical setup for LDA consisting of a laser beam being split and focused by a lens through a suspension of particles in a sample cell. Scattered light is focused through a pinhole and detected by a photomultiplier tube. Figure 10. Optical setup for LDA consisting of a laser beam being split and focused by a lens through a suspension of particles in a sample cell. Scattered light is focused through a pinhole and detected by a photomultiplier tube.
Integrating this equation to any volume fraction, q>, with the boundary conditions that the elasticity is equal to the network value when there are no particles present, and that when the volume fraction reaches packed filler bed), then gives us Equation (2.64). There is an analogous equation describing the viscosity of suspensions of particles and this will be introduced in Chapter 3. When a value of 0.64 is used for the maximum filler concentration, Equation (2.64) becomes... [Pg.46]

The principles of absorptiometry have been applied to the measurement of turbidity. Suspensions of particles scatter incident radiation and, while there is no absorption of radiation by the analyte, the reduction in the transmitted radiation can be used as a measure of the degree of turbidity. Because absorption is not involved, there is no requirement for monochrornation but the fact that the extent of light scattering increases as the wavelength of the incident radiation decreases explains the fact that some instruments do incorporate a simple monochrornation system. [Pg.72]

Turbidimetry Is the measurement of the apparent absorbance when light Is scattered by a suspension of particles. [Pg.238]

A suspension of particles in an electrolyte is drawn through a small orifice on either side of which is positioned an electrode. A constant electrical current supply is connected to the electrodes and the electrolyte within the orifice constitutes the main resistive component of the circuit. As particles enter the orifice they displace an equivalent volume of electrolyte, thereby producing a change in the electrical resistance of the circuit, the magnitude of which is related to the displaced volume. The consequent voltage pulse across the electrodes is fed to a multi-channel analyser. The distribution of pulses arising from the passage of many thousands of particles is then processed to provide a particle (volume) size distribution. [Pg.7]

By using orifices of various diameters, different particle size ranges may be examined and the resulting data may then be combined to provide size distributions extending over a large proportion of the sub-millimetre size range. The prior removal from the suspension of particles of sizes upwards of about 60 per cent of the orifice diameter helps to prevent problems associated with blocking of the orifice. The Coulter Counter and the Elzone Analyser work on this principle. [Pg.8]

For relatively coarse particles, the rates of fall of the interface between (a) and (b) and between (b) and (c) can be calculated approximately if the relation between sedimentation velocity and voidage, or concentration, is given by equation 5.76. Richardson and Shabi 65) have shown that, in a suspension of particles of mixed sizes, it is the total concentration which controls the sedimentation rate of each species. [Pg.282]

Fluorescence excitation spectroscopy is thus a powerful technique for obtaining molecular information about systems of cellular size. At present, the technique is restricted to single small objects because of the requirement of angular integration of the emitted fluorescence. As work progresses, similiar information will be obtainable from spectra taken at a particular angle with respect to the exciting beam. This will allow extension of the photoselection concept to suspensions of particles and perhaps to individual cells. [Pg.365]

In suspensions of particles with an aspect ratio (length to diameter) greater than 1, particle rotation during flow results in a large effective hydrodynamic volume, and Kh > 2.5 (see Figure 4.7). At particle volume fractions above about 5-10%, interaction between particles during flow causes the viscosity relationship to deviate from the Einstein equation. In such instances, the reduced viscosity is better described by the following relationship ... [Pg.299]

Other biological fluids can be modeled as suspensions of particles in a solvent, such as was used for the description of suspensions and slurries in Section 4.1.2.2, namely, that the relative viscosity of the suspension is related to the hydrodynamic shape factor. [Pg.312]

A sol is a colloidal suspension of particles in a liquid for the materials being discussed here, these particles will typically be 1 to 100 nm in diameter. A gel is a semi-rigid solid in which the solvent is contained in a framework of material which is either colloidal (essentially a concentrated sol) or polymeric. [Pg.155]


See other pages where Suspension of particles is mentioned: [Pg.250]    [Pg.69]    [Pg.548]    [Pg.289]    [Pg.118]    [Pg.1630]    [Pg.537]    [Pg.531]    [Pg.201]    [Pg.197]    [Pg.405]    [Pg.177]    [Pg.154]    [Pg.68]    [Pg.9]    [Pg.288]    [Pg.1158]    [Pg.156]    [Pg.2]    [Pg.634]    [Pg.221]    [Pg.311]    [Pg.753]    [Pg.6]    [Pg.392]   
See also in sourсe #XX -- [ Pg.295 , Pg.296 ]

See also in sourсe #XX -- [ Pg.289 , Pg.293 , Pg.294 ]

See also in sourсe #XX -- [ Pg.295 , Pg.296 ]

See also in sourсe #XX -- [ Pg.295 , Pg.296 ]

See also in sourсe #XX -- [ Pg.295 , Pg.296 ]




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