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Transforming materials

Z. Nishiyama, Martensitic Transformation, Materials Science Series, Academic Press, New York (1978). [Pg.331]

Movement of raw and transformed materials can take place within the soil and results in zones of accumulation, depletion, or mixing. Formation, migration, and accumulation of different elements, clays, oxides, and organic matter can occur in different parts of the soil. These different zones or layers in soil that are approximately parallel to the surface are called soil horizons. Depleted or enriched soil horizons result in different depths in the soil having different chemical and physical properties. Translocations are caused by a combination of physical, chemical, and biological processes. [Pg.169]

The continuous availability of trillions of independent microreactors greatly multiplied the initial mixture of extraterrestrial organics and hydrothermal vent-produced chemicals into a rich variety of adsorbed and transformed materials, including lipids, amphiphiles, chiral metal complexes, amino add polymers, and nudeo-tide bases. Production and chiral amplification of polypeptides and other polymeric molecules would be induced by exposure of absorbed amino adds and organics to dehydration/rehydration cydes promoted by heat-flows beneath a sea-level hydro-thermal field or by sporadic subaerial exposure of near-shore vents and surfaces. In this environment the e.e. of chiral amino adds could have provided the ligands required for any metal centers capable of catalyzing enantiomeric dominance. The auto-amplification of a small e.e. of i-amino adds, whether extraterrestrially delivered or fluctuationally induced, thus becomes conceptually reasonable. [Pg.199]

Structures made of transforming materials exhibit a striking capacity to hysteretically recover significant deformation with a controllable amount of energy absorbed m the process. The unusual properties of these materials are due to the fact that large deformations and inelastic behavior are accomplished by coordinated migration of mobile phase or domain boundaries. Intensive research in recent years has led to well-defined static continuum theories for some of the transforming materials (see Pitteri and Zanzotto (1997) for a recent review). Within the context of these theories, the main unresolved issues include history and rate sensitivity in the constitutive structure. [Pg.185]

In this overview we focus on the elastodynamical aspects of the transformation and intentionally exclude phase changes controlled by diffusion of heat or constituent. To emphasize ideas we use a one dimensional model which reduces to a nonlinear wave equation. Following Ericksen (1975) and James (1980), we interpret the behavior of transforming material as associated with the nonconvexity of elastic energy and demonstrate that a simplest initial value problem for the wave equation with a non-monotone stress-strain relation exhibits massive failure of uniqueness associated with the phenomena of nucleation and growth. [Pg.185]

In the wet oxidation process, materials partially or completely dissolve into a homogeneous, condensed-phase mixture of oxygen and water, and chemical reactions between the material and oxygen take place in the bulk water phase. This condensed-phase makes wet oxidation an ideal process to transform materials which would otherwise be non-soluble in water to a harmless mixture of carbon dioxide and water. Since oxidation reactions are also exothermic, the high thermal mass of supercritical water makes this reaction medium better suited for thermal control, reactor stability, and heat dissipation. The purpose of this research was to establish a new method for selectively oxidizing waste hydrocarbons into new and reusable products. [Pg.439]

Such transformations have been extensively studied in quenched steels, but they can also be found in nonferrous alloys, ceramics, minerals, and polymers. They have been studied mainly for technical reasons, since the transformed material often has useful mechanical properties (hard, stiff, high damping (internal friction), shape memory). Martensitic transformations can occur at rather low temperature ( 100 K) where diffusional jumps of atoms are definitely frozen, but also at much higher temperature. Since they occur without transport of matter, they are not of central interest to solid state kinetics. However, in view of the crystallographic as well as the elastic and even plastic implications, diffusionless transformations may inform us about the principles involved in the structural part of heterogeneous solid state reactions, and for this reason we will discuss them. [Pg.296]

The transforming material portion may be adjacent to its prospective phase, which is the case for growth of a new phase or the portion may be isolated, which is the case for nucleation of a new phase. In any case, the spatial variation of... [Pg.417]

The number of nuclei per volume of untransformed material formed in a time increment, dr, is Ardr. In the early stage of transformation impingement of transformed material may be neglected. In that case, the fraction transformed is... [Pg.109]

As a consequence, research in nanotechnology has not produced any remarkable breakthroughs that have transformed materials... [Pg.103]

If a phase (density) transformation occurs during the shock compression process, the concomitant change in V versus P will be detected. If the transition requires a brief time to be completed, a double wave will form, with the faster wave traveling in the compressed but yet untransformed material. Upon pressure release the transformed material may change back into the low-pressure form, and this process, if slightly delayed, will again produce a separate wave. [Pg.327]

If ( i = Cii = I, i. e. if the solution be normal with respect to alkali and ester, and if the transformed materials be continuously replaced, times the quantity originally present would be saponified in a minute. The reaction is therefore a very rapid one. [Pg.195]

At this point, if you have faithfully done the exercises and assignments laid out in previous chapters, you will have learned, among other things, how to write and revise both character description and location description in format how to use offscreen sound to create mood and evoke offscreen events how to begin to develop a character how to gather and transform material for an adaptation and how to do a story outline for a short screenplay to be written using that material. [Pg.65]

What we are seeing is a typical practical situation The temperature rise is 15°C higher than we were expecting However, 55°C is perhaps still acceptable (even from the standpoint of getting safety approvals without special transformer materials). Admittedly, there is room for more optimization. However, the next time we do the process, we must note that the core loss is only a third the total loss, not half, as we had initially assumed. [Pg.176]

From Figure 2 it is clear that the onset temperature of the coil-to-helix transition is independent of the fraction of v-units present in the sample. For all v-contents probed in this study the onset temperature is found to be 86 °C. The helical fraction in fully transformed material decreases monotonously with increasing v-content. The sharpness of the transition broadens with increasing v-content. The latter is comparable with experimental results and theoretical... [Pg.206]

Consolidants have been found in many forms many elastic and transformable materials have useful characteristics. Adhesives, in particular, have effective properties that stem from their ability to reintegrate dissociated tissue. Chapter 14 presents a more thorough explanation of the principles and mechanisms of adhesion and cohesion. [Pg.329]

IL are generally glass-transforming materials whose useful liquid ranges are boxmded by their glass transition temperatures at the lower end and their decomposition temperatures at the higher end. [Pg.453]

Fig. 65. Raman maps of the surface of a lapped Si wafer [275]. (a) Optical micrograph, (b) The ratio of transformed Si (amorphous material and metastable phases) to pristine Si-I. (c) The same, after the wafer surface was chemically etched. Here, all of the transformed phases are removed. Brighter areas in (b) and (c) correspond to higher content of transformed material. Fig. 65. Raman maps of the surface of a lapped Si wafer [275]. (a) Optical micrograph, (b) The ratio of transformed Si (amorphous material and metastable phases) to pristine Si-I. (c) The same, after the wafer surface was chemically etched. Here, all of the transformed phases are removed. Brighter areas in (b) and (c) correspond to higher content of transformed material.
Figure 8.59 Optical micrograph showing the transformation zone around a crack in a partially stabilized zirconia. Nomarski interference is used to provide the contrast which is caused by the surface uplift of the transformed material. (From D. B. Marshall et al., 1990, reproduced courtesy of The American Ceramic Society, Westerville, OH.)... Figure 8.59 Optical micrograph showing the transformation zone around a crack in a partially stabilized zirconia. Nomarski interference is used to provide the contrast which is caused by the surface uplift of the transformed material. (From D. B. Marshall et al., 1990, reproduced courtesy of The American Ceramic Society, Westerville, OH.)...
A soft zone-edge mode is expected to induce a crystalline-to-crystalline transition. Such a transition has been reported recently from a detailed x-rays diffraction study of quartz, just below the amorphization pressure[45, 46], The transformed material appears to involve a microstructure, and the amorphous phase seems to nucleate and grow as the sample is pressur-ized[45]. In view of the small width for the whole acoustic branch at such pressure, these results are not too surprising. [Pg.25]


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See also in sourсe #XX -- [ Pg.185 ]




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