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Defects movement

WE WILL FIND THAT ALL DIFFUSION MOTION OCCURS BY DEFECT MOVEMENT IN THE LATTICE. ... [Pg.151]

Until now we have considered the ideal structures of crystals only when each atom or ion is on a regular site in the crystal. Real crystals contain a variety of imperfections or defects. In crystalline ceramics and glasses, the structure and chemistry of the material will be determined by the kinetics of defect movement. For example, the kinetics of the glass-to-crystal transformation are slow if the temperature is low (typically less that 1000°C) because the transformation occurs by atoms moving—in ceranucs, this usually occurs by point defects moving. If point defects move too slowly, the structure with the lowest energy (the equilibrium structure) may never actually be achieved. How fast they move is determined by their structure. [Pg.181]

Fig. 10.2. Schemes of defect structures and defect movements in ice. Small arrows show the actual displacements of protons large arrows show the resulting displacements of the defects. Fig. 10.2. Schemes of defect structures and defect movements in ice. Small arrows show the actual displacements of protons large arrows show the resulting displacements of the defects.
Just as with liquid crystals, electric fields could be used to study defect mobility. For such a study one would want to begin with a well-defined and simple system. For example, two sections with uniformly aligned lamellae could be annealed together with an orthogonal lamellar orientation, thus forming a wall defect. Movement of the wall defect in response to an electric field would reveal the mobility of the wall, because the alignment force can be calculated and the velocity measured. [Pg.1128]

Shown in Fig. 19(a) are the strain-time curves resulting from the compression creep of 95.5Sn-3.9Ag-0.6Cu samples in the as-cast condition these tests were performed at 25 °C, or 77 °F (Ref 65). All of the curves show primary creep leading into steady-state creep. The extent of creep strain is not entirely monotonically dependent upon stress level this variability indicates a non-uniformity in the defect density and/or defect movement between different test specimens that affects the creep response. Similar behaviors were observed in tests performed at -25 and 75 °C (-13 and 167 °F). [Pg.92]

The measure of the inductance variation observed during of the movement of the product in the solenoid generator allows to calculate directly the surface of the straight section of the defect of greater lengtli that the solenoid. More, tlie variation of the resistance allows to determine the height of the defect. [Pg.350]

More recently, studies employing STM have been able to address surface self-diffiision across a terrace [16, 17. 18 and 19], It is possible to image the same area on a surface as a fiinction of time, and watch the movement of individual atoms. These studies are limited only by the speed of the instrument. Note that the performance of STM instruments is constantly improving, and has now surpassed the 1 ps time resolution mark [20]. Not only has self-diflfiision of surface atoms been studied, but the diflfiision of vacancy defects on surfaces has also been observed with STM [18]. [Pg.293]

Theoretical studies of diffusion aim to predict the distribution profile of an exposed substrate given the known process parameters of concentration, temperature, crystal orientation, dopant properties, etc. On an atomic level, diffusion of a dopant in a siUcon crystal is caused by the movement of the introduced element that is allowed by the available vacancies or defects in the crystal. Both host atoms and impurity atoms can enter vacancies. Movement of a host atom from one lattice site to a vacancy is called self-diffusion. The same movement by a dopant is called impurity diffusion. If an atom does not form a covalent bond with siUcon, the atom can occupy in interstitial site and then subsequently displace a lattice-site atom. This latter movement is beheved to be the dominant mechanism for diffusion of the common dopant atoms, P, B, As, and Sb (26). [Pg.349]

Sialin was first identified as the product of the gene defective in sialidosis, a lysosomal storage disorder. The transporter mediates the movement of sialic acid out of lysosomes by coupling to the proton electrochemical gradient across the lysosomal membrane. Unlike the vesicular neurotransmitter transporters which are antiporters, sialin is a sympoiter with sialic acid and protons both moving out of the lysosome. [Pg.1131]

Such defects facilitate movement of C02 within the crystal by transfer from HCOj to OH" and of Ag+ in the cation vacancies. This interpretation is supported [758,759] by the observed increase in reactivity resulting from doping of Ag2C03 with Cd2+, Y3+ or Gd3+, where incorporation of the additive is accompanied by the creation of cation vacancies. [Pg.172]

Global planeness and large scale scratches are usually evaluated by HDI instruments as shown in Fig. 3(a) [8], which is a surface reflectance analyzer to measure flatness, waviness, roughness of a surface, and observe scratches (Fig. 3(h)), pits (Fig. 3(c)), particles (Fig. 3(d)) on a global surface. These surface defects can also be observed by SEM, TEM, and AFM. Shapes of slurry particles can be observed by SEM and TEM, and their movement in liquid by the fluorometry technique as shown in Chapter2. [Pg.237]

Point defects in solids make it possible for ions to move through the structure. Ionic conductivity represents ion transport under the influence of an external electric field. The movement of ions through a lattice can be explained by two possible mechanisms. Figure 25.3 shows their schematic representation. The first, called the vacancy mechanism, represents an ion that hops or jumps from its normal position on the lattice to a neighboring equivalent but vacant site or the movement of a vacancy in the opposite direction. The second one is an interstitial mechanism where an interstitial ion jumps or hops to an adjacent equivalent site. These simple pictures of movement in an ionic lattice, known as the hopping model, ignore more complicated cooperative motions. [Pg.426]

Step movement during chemisorption appears to be a general phenomenon. Real-time images observed (Figure 4.4) for chlorine chemisorption at Cu(110) indicate that nucleation takes place at a defect site, resulting in a single string... [Pg.53]


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