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By Nissim Garti, Kiyotaka Sato

Members in pharmaceutical sciences, chemistry, foodstuff technological know-how, and biology evaluate rising options, approaches, and mechanisms in fats crystallization and polymorphism of latest fat, advanced blends of area of expertise fat, fatty acids, non-saponifiable lipids, and mono- and diglycerides. a few issues contain interfacial crystallization in emulsions and microemulsions, lyotropic liquid crystals and different self-assembled constructions, and crystallization in limited volumes. different themes contain polymorphism and part transitions of fatty acids and acylglycerols, fats crystal networks, crystallization houses of cocoa butter, and separation and crystallization of oleaginous ingredients in cosmetics. Garti is professor of chemistry and head of the Casali Institute of utilized Chemistry on the Hebrew college of Jerusalem, Israel. Sato teaches utilized organic technology at Hiroshima collage, Japan.

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Extra resources for Crystallization Processes in Fats and Lipid Systems

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Labeling E 0 the bonding energy per molecule within the regular nucleus and E T that for the twinned one, one may define the fault energy of the twin (per mole- Equilibrium and Crystallization Kinetics 21 Fig. 9 Twins and polytypes. The black and white domains represent two individuals of the same type symmetry related by twinning operation: (a) normal crystal, (b) twin, (c) periodic polysynthetic twin. Two polytypes are represented in (d) and (e): the same basic structure layer repeats either periodically (d) without changing orientation (stacking .

40) is strictly valid only in the case of spherical droplets suspended in a vapor or in another fluid. , that they have already reached their equilibrium morphology according to GibbsWulf [46]. Generally, Ostwald ripening is very fast for crystals of size L ϭ 2r 0 Ͻ 1 µm, fast for crystals of L Ն 1 µm, but negligible as soon as L reaches about 100 µm [48]; the process occurs easily for sparingly soluble materials, owing to the large value of their interfacial energy (several tens of erg/cm 2 ) and resultant wide metastable zone.

2. Recall that the rate of growth of a perfect flat face through 2D nucleation (R 2D F ) should be proportional to J 2D and, hence, its expression contains the exponential term dependent on the Gibbs free energy of formation of critical 2D clusters. Point out that the behavior of R 2D F , as a function of the supersaturation β v ϭ 1 ϩ σ v , is, mutatis mutandis, that shown in Fig. 17. 20 is the growth rate not null and that just beyond this value it becomes more or less catastrophic [as for 3D nucleation (Fig.

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