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Growth Ostwald ripening

In Nature, however, we always have a contiiinous distribution of particles. This means that we have all sizes, even those of fractional parentage, i.e.-18.56n, 18.57p, 18.58 p, etc. (supposing that we can measure 0.01 p differences). The reason for this is that the mecheuiisms for particle formation, i.e.- precipitation, embryo and nucleation growth, Ostwald ripening, and sintering, are random processes. Thus, while we may speak of the "statistical variation of diameters", and while we use whole numbers for the particle diameters, the actuality is that the diameters are fractional in nature. Very few particle-size" specialists seem to recognize this fact. Since the processes are random in nature, we can use statistics to describe the... [Pg.208]

Fig. 5.39 Conceptual outline of the changes associated with solution-reprecipitation densification where both grain growth (Ostwald ripening) and grain-shape accommodation act to release liquid to fill residual pores. Reproduced with permission from [73]. Copyright 2009, Springer... Fig. 5.39 Conceptual outline of the changes associated with solution-reprecipitation densification where both grain growth (Ostwald ripening) and grain-shape accommodation act to release liquid to fill residual pores. Reproduced with permission from [73]. Copyright 2009, Springer...
At equilibrium, crystal growth and dissolving rates become equal, and the process of Ostwald ripening may now appear, in which the larger crystals grow at the expense of the smaller ones. The kinetics of the process has been studied (see Ref. 103). [Pg.341]

A3.3.4 LATE-STAGE GROWTH KINETICS AND OSTWALD RIPENING... [Pg.745]

The elimination of pores comes about by tire combined effects of grain growth and Ostwald ripening in the hnal stages of sintering. [Pg.215]

Ostwald ripening differs from nuclei growth in that the relative size and numbers of pcU ticles change, whereas in nuclei growth, the numbers of particles growing from nuclei do not change. Sintering, on the other hand, is an entirely different process, and usually occurs when external heat is applied to the particles. [Pg.193]

A log normal distribution will give a straight line when plotted on this ti pe of paper. This means that the PSD is not limited, i.e.- aU sizes of particles are present from - to +°°. However, if the PSD is growth-limited, it will readily apparent from the graph. Ostwald ripening, a mechanism where large... [Pg.221]

If a precipitate is allowed to undergo Ostwald ripening, or is sintered, or is caused to enter into a solid state reaction of some kind, it will often develop into a distribution which has a size limit to its growth. That is, there is a maximum, or minimum limit (and sometimes both) which the particle distribution approaches. The distribution remains continuous as it approaches that limit. The log-probability plot then has the form shown in 5.8.2. on the next page. [Pg.223]

TBP and injected into a hot ( 350 °C) solution of TOPO (12 g). The injection of CdSe precursors into the hot solution ofTOPO resulted in spontaneous nucleation of CdSe nanocrystals and a decrease in temperature. Once the temperature was stabilized, an additional amount (0.4 mL) of the precursor solution was added for the growth of the nucleated nanocrystals. Here, Ostwald ripening was avoided by separating the nucleation and growth processes. All the reagents and the reaction were kept under an Ar atmosphere to avoid fire hazard and surface oxidation of the nanocrystals. [Pg.295]


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See also in sourсe #XX -- [ Pg.61 ]




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