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Particles of materials

The P-t histories illustrated by Fig. 2.9 are not histories of a particle of material moving with the flow, because the coordinate that is fixed is x, and material is flowing past it. A more useful P-t history would use a coordinate system which is attached to the material itself, as a stress or particle velocity gauge would be. Such a coordinate system is defined in the next section. [Pg.24]

Artifacts may be introduced from the environment or through preparative techniques. When assessing individual tiny particles of material, the risk of loss or contamination is high, so that samples of this nature are handled and prepared for examination in a clean bench or a cleanroom (class 100 or better). [Pg.67]

Fig. 1. (a) Adhesive vs. cohesive failure, (b) Close-up view of adhesive failure in the pre.sence of an interphase. The locus of failure may be adjacent to or within the interphase (as shown), and particles of material may be ejected during the debonding process. [Pg.2]

Electrodes of this type can, for instance, be used to extract traces of certain metals from seawater or to perform reactions with gases having very low solubility in a given medium. They can also be used to reduce electrochemically or to oxidize particles of materials having very low conductivity. Their efficiency depends on many factors, including the time of contact of the particles with the feeder electrode and the quality of this contact (low resistance to charge transfer during the encounters). [Pg.342]

Particles of materials 1 and 2 whose diameters conform to the above equation are called equal-settling particles ... [Pg.157]

Figure 1. Approach, contact, and separation of two dissimilar solid materials leads to triboelectric charge separation. Here, the particle of material A is assumed to have lower work function and much higher electrical resistivity than the material B. Figure 1. Approach, contact, and separation of two dissimilar solid materials leads to triboelectric charge separation. Here, the particle of material A is assumed to have lower work function and much higher electrical resistivity than the material B.
An interesting point arises from this method. The particles of material are exposed to water vapour at a set humidity and hence the results equate to that humidity. The measured equilibrium absorption is substantially the same as the equilibrium absorption that would be obtained by immersion in an aqueous solution which would maintain the test humidity. As this implies, the equilibrium water absorption is reduced if the water is not pure. Hence, exposure to aqueous solutions should be made at the concentration of interest. As the humidity approaches 100% even small amounts of a salt have a significant effect on equilibrium absorption. [Pg.69]

The microniser, probably the best known of this type of pulveriser, effects comminution by bombarding the particles of material against each other. Pre-ground material, of about 500 im in size, is fed into a shallow circular grinding chamber which may be horizontal or vertical, the periphery of which is fitted with a number of jets, equally spaced, and arranged tangentially to a common circle. [Pg.135]

It is believed that in the presence of dampproofing admixtures, the surfaces of the concrete, and the internal surfaces of the pores become coated with either a layer of molecules in the case of stearic acid and other fatty acids (Fig. 4.5b) or a layer of coalesced or separate particles of material in the case of waxes and bitumens, etc. (Fig. 4.5c). The end result in both cases is the production of hydrophobic surfaces exhibiting high contact angles to water, as shown in Fig. 4.6. [Pg.235]

Under the term spots may be understood small, hard particles of material, such as sand, powdered glass, carborundum, etc, incorporated in an explosive either on purpose or present as impurities. Such particles are known as grit. The term spots may also be applied to small bubbles of air or other gases entrapped in cast explosives or incorporated on purpose in other expls, such as by rolling cartridges of gelatinous Dynamites. The reason why these spots are called hot spots is explained below... [Pg.563]

Dust around the carbon star shows an excess emission feature between about 10.2 and 11.6 jam, clearly distinguishable in both shape and position from the 9.7-jum feature of the oxygen star, which has been attributed to small SiC particles. These particles cannot be spherical, however. According to the discussion in Section 12.2, shape effects spread an absorption band in small particles of materials like SiC between the transverse (to,) and longitudinal (to,) optical mode frequencies these frequencies for SiC are indicated on the figure. This point was made by Treffers and Cohen (1974) using Gilra s unpublished calculations. To illustrate this further, calculations for a random distribution of... [Pg.462]

It is convenient to consider the stable. flow in a clearance between two infinitely long cylinders with radii and R2, one of which is rotating with angular velocity Q in a cylindrical system of coordinates. Each particle of material describes a curve along the common axis of cylinders z with angular velocity to(r) and longitudinal velocity U(r). [Pg.49]

The active centers in silica are generated upon mechanical treatment not only due to the cleavage of the particles of material but also to their mutual contacts (so-called friction regime [11-13]). For this reason, the mechanical treatment can be used for generating defects at the surface of high-dispersed silica (aerosol). [Pg.238]

The Hamaker constant for two particles of materials 1 and 2, respectively, interacting across a vacuum is given by [3] ... [Pg.424]

The problems, which arise from the volatilization of lithium and oxygen, are possible to overcome, by employing low-temperature methods. These methods could produce homogeneous monophase fine particles of materials which sinter to near theoretical densities at relatively low... [Pg.123]

Fig. 6. Interaction between two spherical particles of material I in a liquid medium of material 2.o = radius of spherical particle k — distance of surface s aration. Fig. 6. Interaction between two spherical particles of material I in a liquid medium of material 2.o = radius of spherical particle k — distance of surface s aration.
In multiphase complex fluids, it is useful to account for van der Waals forces on a continuum, rather than a molecular, basis. Consider, for example, two spherical particles of material A, each of radius a, approaching each other in a medium of substance B. Let r be the distance separating the centers of the spheres and let D = r —2a he the gap between them. Defining a = Dfla, the van der Waals potential of interaction is found to be (Goodwin et al. 1986)... [Pg.85]

On account of the numerous chain joints subject to the abrasive action of dust and fine particles of material, the depreciation of bucket carriers is much more rapid when in operation than when idle, so, provided the hours of operation per year number 60 per cent or more of the available annual working hours—usually taken as 2,500— depreciation per year is customarily taken as chargeable only during actual working hours. [Pg.104]

TABLE 12.1 Hamaker Constants (A) for Interaction Between Two Particles of Materials 1 and 2, Separated by a Material 3... [Pg.460]

FIGURE 14.5 Homogeneous and heterogeneous nucleation. Embryos (radius r) of phase p formed from phase a (a) in the absence of foreign particles, and (b) at the surface of foreign particles of material k1 or k2 in frames 2-5, the contact angle 0 = 45 degrees. [Pg.581]

Particles immersed in a liquid medium experience a smaller attractive force. The calculation of such forces and their relationship to the nature of the particles and of the dispersion medium has been, and continues to be, a major theoretical problem. Important advances towards its solution have been made in recent years, and they will be mentioned briefly in Chapter 15. For the present purposes it is sufficient to use a relatively simple approximate equation according to which the appropriate Hamaker constant to be employed when two particles of material 1 are separated by a medium 2 is given by... [Pg.36]

Radiofrequency arc (RF arc) has also been used for removzd of particles of material from the sample surface. In this system a modified ICP torch is used, and the sample is in electrical contact with a ground copper base. The base is water-cooled and argon flow is introduced at the base. A stable filament from the plasma forms between the induction region and the sample, when the plasma discharge is initiated. Boron nitride is used as thermal and electrical insulator between the base and the RF arc. [Pg.172]

When the temperature rises above the fusion temperature of the glass material, the glass material links the film to the substrate, and also links the particles of material between them. [Pg.262]


See other pages where Particles of materials is mentioned: [Pg.570]    [Pg.209]    [Pg.24]    [Pg.346]    [Pg.819]    [Pg.209]    [Pg.155]    [Pg.39]    [Pg.156]    [Pg.156]    [Pg.257]    [Pg.958]    [Pg.150]    [Pg.201]    [Pg.230]    [Pg.424]    [Pg.285]    [Pg.300]    [Pg.153]    [Pg.29]    [Pg.595]    [Pg.781]    [Pg.4]    [Pg.36]    [Pg.370]    [Pg.666]    [Pg.177]   
See also in sourсe #XX -- [ Pg.7 ]




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