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Hard particles

Due to the application of the described image processing steps on image sequences up to 1000 images per second, it is possible to determine and to analyse the transport process of several hard particles concerning their location, velocity and acceleration inside the molten bath. [Pg.546]

The previous investigations of hard particle transport processes during laser beam dispersing have shown, that the high speed microfocus radioscopy system is a usable arrangement to observe and analyse the movements, velocities and accelerations of particles inside the molten bath. That possibility was, until now, not given by conventional techniques of process... [Pg.546]

Due to the absorbed photon energy in the moment of the beam admission the particles and the substrate surface warm up very fast. As a consquence of the thermal induced stresses between the relative brittle hard particles, some particles brake apart and, because of the released impulse energy, they are ejected out of the effective beam zone, transmission... [Pg.547]

The squares visible in figure 5 represent the position of hard particles at the moment of recording. Therefore the time distance between two video records is about 1,3 ms at a record rate of 750 Hz. With these data it is possible to calculate particle velocity. Figure 8 shows the particle movement in the molten bath caused by flow processes. The particles are captured at the contour of the molten bath and transported into the liquid phase. [Pg.548]

The investigations show that the microfocus high speed radioscopy system is suitable for monitoring the hard particle transport during laser beam dispersing. It is possible to observe and analyse the processes inside the molten bath with the presented test equipment. As a consequence a basis for correlation with the results of a simulation is available. [Pg.549]

It has not proved possible to develop general analytical hard-core models for liquid crystals, just as for nonnal liquids. Instead, computer simulations have played an important role in extending our understanding of the phase behaviour of hard particles. Frenkel and Mulder found that a system of hard ellipsoids can fonn a nematic phase for ratios L/D >2.5 (rods) or L/D <0.4 (discs) [73] however, such a system cannot fonn a smectic phase, as can be shown by a scaling... [Pg.2557]

Case Hardening by Surface Deformation. When a metaUic material is plastically deformed at sufficiently low temperature, eg, room temperature for most metals and alloys, it becomes harder. Thus one method to produce a hard case on a metallic component is to plastically deform the surface region. This can be accomplished by a number of methods, such as by forcing a hardened rounded point onto the surface as it is moved. A common method is to impinge upon the surface fine hard particles such as hardened steel spheres (shot) at high velocity. This process is called shot... [Pg.215]

Tin babbitts are based on the tin—antimony—copper system and commonly contain about 3—8% copper and 5—8% antimony. Within a soft, sohd-solution matrix of antimony in tin are dispersed small hard particles of the intermetaUic copper—tin, Cu Sn [12019-69-1] (13). [Pg.3]

Wear. Ceramics generally exhibit excellent wear properties. Wear is deterrnined by a ceramic s friction and adhesion behavior, and occurs by two mechanisms adhesive wear and abrasive wear (43). Adhesive wear occurs when interfacial adhesion produces a localized Kj when the body on one side of the interface is moved relative to the other. If the strength of either of the materials is lower than the interfacial shear strength, fracture occurs. Lubricants (see Lubricants and lubrication) minimize adhesion between adj acent surfaces by providing an interlayer that shears easily. Abrasive wear occurs when one material is softer than the other. Particles originating in the harder material are introduced into the interface between the two materials and plow into and remove material from the softer material (52). Hard particles from extrinsic sources can also cause abrasive wear, and wear may occur in both of the materials depending on the hardness of the particle. [Pg.326]

Abrasive wear is encountered when hard particles, or hard projections on a counter-face, are forced against and moved relative to a surface. In aUoys such as the cobalt-base wear aUoys which contain a hard phase, the abrasion resistance generaUy increases as the volume fraction of the hard phase increases. Abrasion resistance is, however, strongly influenced by the size and shape of the hard-phase precipitates within the microstmcture, and the size and shape of the abrading species (see Abrasives). [Pg.373]

Composites. Another type of electro deposit in commercial use is the composite form, in which insoluble materials are codeposited along with the electro-deposited metal or alloy to produce particular desirable properties. Polytetrafluoroethylene (PTFE) particles are codeposited with nickel to improve lubricity (see Lubrication and lubricants). SiHcon carbide and other hard particles including diamond are co-deposited with nickel to improve wear properties or to make cutting and grinding tools (see Carbides Tool materials). [Pg.143]

Particle surface characteristics Type of solid (in terms of internal liquid content) gel, flocculated, hard particle Strength of particle (resistance to deformation under pressure) compressibility over time expressed cake... [Pg.1748]

Most metals are subject to erosion-corrosion in some specific environment. Soft metals, such as copper and some copper-base alloys, are especially susceptible. Erosion-corrosion is accelerated by, and frequently involves, a dilute dispersion of hard particles or gas bubbles entrained in the fluid. [Pg.240]

Although it is entirely possible for erosion-corrosion to occur in the absence of entrained particulate, it is common to find erosion-corrosion accelerated by a dilute dispersion of fine particulate matter (sand, silt, gas bubbles) entrained in the fluid. The character of the particulate, and even the fluid itself, substantially influences the effect. Eight major characteristics are influential particle shape, particle size, particle density, particle hardness, particle size distribution, angle of impact, impact velocity, and fluid viscosity. [Pg.245]

Slides Split-shell bearings hard particles embedded in soft bearing alloys micrograph of section through layered bearing shell skiers automobile tyres. [Pg.295]

The use of Ni-base superalloys as turbine blades in an actual end-use atmosphere produces deterioration of material properties. This deterioration can result from erosion or corrosion. Erosion results from hard particles impinging on the turbine blade and removing material from the blade surface. The particles may enter through the turbine inlet or can be loosened scale deposits from within the combustor. [Pg.418]

Erebs, m. cancer crayfish grain, hard particle (in clay, etc.) knot (in ore, etc.) wart canker crab crustacean. [Pg.259]

To combat this problem, soft materials such as Babbitt are used when it is known that a bearing will be exposed to abrasive materials. Babbitt metal embeds hard particles, which protects the shaft against abrasion. When harder materials are used in the presence of abrasives, scoring and galling occurs as a result of abrasives caught between the journal and bearing. [Pg.1023]

Nielsen [216] believes an agglomerate to be a plurality of contacting primary particles. Assuming that agglomerates behave like hard particles below a certain stress threshold, the author expects that high stresses should cause the particles constituting an agglomerate to move relative to each other. [Pg.30]

Talbot J. A statistical model for the dynamical properties of hard particle fluids, Mol. Phys. 75, 43-58 (1992). [Pg.282]

Now, we show the relation between the ratio of 8 to Tq, 8/ro and the volume fraction of carbon black (p in Table 18.1, when the diameter of the hard particle (including carbon black, the GH layer and a little more contribution from the cross-links at the surface of particle) is tq and the distance between the hard particles is 8. In the carbon black-filled rubber (ip g 0.23-0.25), the fact that the stress of the filled system is 10-15 times larger than that of the unfilled rubber as shown in Figure 18.1 indicates that more than 90% of the stress of the system is supported by the supernetwork and the remainder of the stress results from the matrix rubber. In the present calculation, however, we can ignore the contribution from the matrix mbber. [Pg.533]

Metal cups are sometimes inserted in detonators to provide extra confinement for the composition. It is often claimed that such cups, by increasing the mechanical strength, also increase the safety of handling of the detonator. In the case of plain detonators this is true to a limited extent, but the difference is not of practical importance. Of much greater importance is the ensurance of the absence of grit or hard particles, the presence of which can cause dangerous sensitiveness in the detonator. [Pg.100]


See other pages where Hard particles is mentioned: [Pg.542]    [Pg.543]    [Pg.546]    [Pg.546]    [Pg.546]    [Pg.548]    [Pg.548]    [Pg.548]    [Pg.298]    [Pg.62]    [Pg.209]    [Pg.374]    [Pg.162]    [Pg.1774]    [Pg.106]    [Pg.251]    [Pg.279]    [Pg.279]    [Pg.171]    [Pg.153]    [Pg.220]    [Pg.8]    [Pg.534]    [Pg.25]    [Pg.50]    [Pg.428]    [Pg.67]    [Pg.563]    [Pg.639]   
See also in sourсe #XX -- [ Pg.331 ]




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Brownian hard particles

Computer simulation hard particle models

Dipolar hard-sphere particles

Dispersed phase particles, hard

Hard Spheres and Lennard-Jones Particles

Hard particle simulations

Hard particle simulations spherocylinders

Hard particle theories

Hard particles theory, elastic properties

Hard shell particles

Hard sphere solvents, scaled particle theory

Hard-particle fluid compressibility

Hard-particle methods

Hard-particle methods characteristics

Hard-particle methods lubricants

Hard-particle methods preparation

Hard-particle methods surfactants

Hardness of particles

Hardness, Abrasive Particle

Particle concentrationeffectstability of hard spherical dispersions

Potential and Charge of a Hard Particle

Results of Hard Particle Simulations

Stoner-Wohlfarth Theory for Hard-Magnetic Particle Arrays

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