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Twinning, small particles

Figures 2 (b) and (c) show a diffraction pattern obtained from a particle of diameter 1.5 nm and a diffraction pattern calculated for a multiply twinned, decahedral particle. The conclusion drawn from the study of many such observed and calculated patterns obtained from gold particles in the size range of 1.5 to 2 nm contained in a plastic film is that very few particles are multiply twinned, many have one or two twin planes but more than half are untwinned (16). This suggests that, at least for this type of specimen, there is no confirmation of the theoretical prediction that the multiply twinned form is the equilibrium state for very small particles. Figures 2 (b) and (c) show a diffraction pattern obtained from a particle of diameter 1.5 nm and a diffraction pattern calculated for a multiply twinned, decahedral particle. The conclusion drawn from the study of many such observed and calculated patterns obtained from gold particles in the size range of 1.5 to 2 nm contained in a plastic film is that very few particles are multiply twinned, many have one or two twin planes but more than half are untwinned (16). This suggests that, at least for this type of specimen, there is no confirmation of the theoretical prediction that the multiply twinned form is the equilibrium state for very small particles.
Volume 18 of Advances in Chemical Engineering returns to the dominant twin themes of modern chemical engineering the microscale of molecules and small particles, and the macroscale of entire engineering systems, of analysis and synthesis. [Pg.274]

There has been considerable work in the literature on the structure of very small particles and clusters. Interest in this field has been primarily due to Ino s (1966) early experimental studies of normally fee metals prepared by vapour condensation which showed that a sizable portion of the particles exhibited non-crystallographic structures. These non-crystallographic atomic clusters or polycrystalline nuclei have been observed to consist of pentagonal bi-pyramid or icosahedra form of twinned structures and are known as multiply twinned particles (MTPs). EM studies of supported transition metal catalyst systems have indicated that MTPs sinter faster in catalytic reactions leading to the loss of surface area and are not beneficial to catalysis (Gai 1992). We describe the structure and the role of MTPs in catalysis in the following sections. [Pg.171]

Fig. 2 A small particle (about 3 nm in, size) and a big one (about 9 nm in size), both showing multiply twinned structure. The twin boundaries in the images are indicated... Fig. 2 A small particle (about 3 nm in, size) and a big one (about 9 nm in size), both showing multiply twinned structure. The twin boundaries in the images are indicated...
It was also possible, by HRTEM measurements, to observe defects in the crystalline lattice of the Pt(0) NPs prepared in BMI.BF4 (Fig. 6.7). Note that twin defects are typical for small particles. [Pg.206]

The DV process for thermoplastic elastomers can be described as follows After sufficient melt-mixing of plastic and rubber, vulcanizing agents are added. Vulcanization of the rubber phase occurs as mixing continues. After removal from the mixer, the cooled blend can be chopped, extruded, pelletized, injection molded, and so on. Such a composition is described as a dispersion of very small particles of vulcanized rubber in a thermoplastic resin matrix. Such compositions are prepared commercially by a continuous process by using a twin-screw extruder. [Pg.377]

Fillers are mainly used for reasons of economy, but in many cases they also improve some properties of the polymer. The most important fillers for polymers are minerals such as talc, chalk and china clay. Filler content generally used with plastics is up to 60 wt%. The most common practice is to feed the filler downstream into the melt by means of a twin-screw side feeder (Figure 6.3). It is well-known that thermoplastic melts with high loadings of small particles such as calcium carbonate, carbon black and titanium dioxide give both yield values in shear flow [58, 59], and uniaxial extension [60, 61]. [Pg.68]

Leet and others have shown that the temperature must be below 300° C. and the velocity reduced to about 200 ft. per minute before the very small particles will fall out. In the downcomers and in some other parts of the plant the velocity may be as high as 1500 ft. per minute, hence it is obvious that enormous spaces must be erected for settling chambers. Fig. 34 is a diagram of the flues at Washoe sm el try, Anaconda, where some of the fumes travel four-fifths of a mile before they are allowed to pass into the final stack. Fig. 35 is a transverse section of the twin settling chamber. Over 80 tons of fume are collected every 24 hours by this plant. Particles that pass Fiq. 34. into the open from the plant are... [Pg.245]

A microscopist should recognize a paper as rag, mechanical coniferous, chemical nonconiferous, or as combinations of these by studying the paper surface. He/she should recognize such surface features on small particles as scales on wool, crossover marks on silk, striations on viscose rayon, twin bands or calcite, melt and crystal patterns on micrometeorites, lamellar steps on mica, the fibrous structure of incinerated wood sawdust, etc., which help identify that substance. [Pg.145]

It Is not necessarily to be concluded that. In general, the proportion of small metal particles having the multiplicity twinned form decreases as the size Is decreased. The evidence concerning particles formed in other ways shows a great deal of variability. [Pg.336]

From a structural point-of-view the bulk metallic state, that is, fee lattice (with varying densities of defects such as twins and stacking faults) is generally established in gold nanoparticles of about 10 nm diameter and upwards. However, such particles still display many unusual physical properties, primarily as the result of their small size. Shrinking the size of gold particles has an important effect it increases both the relative proportion of surface atoms and of atoms of even lower coordination number, such as edge atoms [49] and these atoms in turn are relatively mobile and reactive. [Pg.325]

Figure 2. Nanodiffraction patterns from small gold particles for an incident beam diameter of 1-2 nm (a) Observed for a particle of 2-3 nm diameter showing twinning on two planes (b) Observed for a multiply twinned particle of 1.5 nm diameter. (c) Calculated for a model multiply twinned particle. The black spots in (a) and (b) are the small mirrors in the optical analyser system used as detectors for imaging. Figure 2. Nanodiffraction patterns from small gold particles for an incident beam diameter of 1-2 nm (a) Observed for a particle of 2-3 nm diameter showing twinning on two planes (b) Observed for a multiply twinned particle of 1.5 nm diameter. (c) Calculated for a model multiply twinned particle. The black spots in (a) and (b) are the small mirrors in the optical analyser system used as detectors for imaging.
Figure 7.8 shows Aref s computation of the twin vortex flow of given amplitude and various time periods. Initially nine marker points were placed along the y axis and six along the x axis. Clearly, for very small periods (the switching between the two vortexes is very fast), we essentially get steady state flow and the marker particles fall along the... [Pg.335]


See other pages where Twinning, small particles is mentioned: [Pg.336]    [Pg.179]    [Pg.339]    [Pg.171]    [Pg.187]    [Pg.418]    [Pg.150]    [Pg.159]    [Pg.47]    [Pg.279]    [Pg.19]    [Pg.269]    [Pg.557]    [Pg.254]    [Pg.63]    [Pg.371]    [Pg.274]    [Pg.302]    [Pg.503]    [Pg.407]    [Pg.188]    [Pg.187]    [Pg.233]    [Pg.890]    [Pg.895]    [Pg.323]    [Pg.347]    [Pg.238]    [Pg.512]    [Pg.81]    [Pg.351]    [Pg.49]    [Pg.658]    [Pg.291]    [Pg.269]    [Pg.182]    [Pg.643]   
See also in sourсe #XX -- [ Pg.336 ]




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