Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Polyhedral Crystal Shapes

This law was proposed by the Dane Nils Steensen Nicolaus Steno, 1669) for crystals of quartz. Generalized by the Italian Domenico Guglielmini (1688) and by the Swiss Moritz Anton Cappeller (1723), the definitive form was proposed by the Frenchman Rome de lisle (1783)  [Pg.7]

From here we arrive at the Bernhardi principle (1809) The number and dimensions of the faces are not characteristic for a crystal every crystal has its own habit. Only the directions and orientations are important, in other words, the [Pg.7]

We measure the angle between the normals of the faces of a crystal with an optical goniometer (theodolite) by observing the reflection of a ray of light from the faces. The precision is about 5 seconds of arc. [Pg.8]

In practice, we only measure the orientations of the faces, and not those of the edges. We will thus establish our coordinate system with the aid of this information (Fig. 1.5). We first choose three faces which form a trihedron whose intersections define the directions a, b and c. The choice of a fourth face which cuts these three directions establishes the ratio a b c. Thus we choose four faces, all other faces being referred to the coordinate system thus defined. [Pg.8]

Relative to this coordinate system, all the other faces and edges satisfy the law [Pg.9]


Since an actual crystal will be polyhedral in shape and may well expose faces of different surface tension, the question is what value of y and of r should be used. As noted in connection with Fig. VII-2, the Wulff theorem states that 7,/r,- is invariant for all faces of an equilibrium crystal. In Fig. VII-2, rio is the... [Pg.262]

The amount of structural information obtainable by the morphological Study of skeletal crystals is naturally very limited, especially when they are distorted. In order to be able to deduce the shape of the unit cell it is necessary to have well-fotmed polyhedral crystals. The faces of such crystals are, as we have already seen, related in some simple way to the unit cells. We must now define more closely what is meant by the last phrase— related in some simple way to the unit cells —and to do this it is necessary to give some account of the accented nomenclature of crystal planes. [Pg.24]

Crushing has been recommended as a primary method because it is safe and will lead to the determination of the principal refractive indices of any crystalline substance, provided a sufficient number of randomly oriented fragments is observed it is a beginner s method. But the more experienced worker may often dispense with it, when the crystals being examined have a well-defined polyhedral shape. If the relation between crystal shape and optical properties is properly understood, it is possible to determine the principal indices by a limited number of observations on crystals selected because they lie in such positions that they necessarily show their principal indices. [Pg.101]

The solid state displacement reaction method and wet chemical precipitation method were employed for synthesizing the ceria powders, and thus the ceria properties showed different features in several experiments. Figure 15.10 shows the morphology of the ceria particles observed with high-resolution scanning electron microscopy (SEM S900, Hitachi, Japan) and transmission electron microscopy (TEM JEM-2010, JEOL, Japan). In the figure, the ceria particles have a polyhedral shape. Both of the powders have nearly the same size. The primary particle size is approximately 40 mn. However, the difference in crystal shape of the ceria particles was found on TEM analysis. [Pg.187]

Heterogeneous catalysis is a surface phenomenon in which the crystal face plays a major role. NAP-MgO has a polyhedral shape with a three-dimensional structure with reactive ions on the surface. The crystal morphology and crystal shape induce the chirality in the reaction. [Pg.156]

Crystal is a matter constituted by atoms (ions, molecules or atom clusters) ranked periodically in three-dimensional space, otherwise it is called amorphous matter. In fact, there is no strict limit between crystal and amorphous one, because the difference between amorphous and crystal can be considered as the repetitive times of periodicity—from less to more causing quantitative change to quahtative change in the process, but once the formation the crystal with internal structme ranked in rules, it displays a series of different characteristics unlike that of amorphous matters. Solid crystals possess regular polyhedral shape, symmetry of a crystal shape, with the anisotropy for electricity, heat, light, and constant melting point and so on. [Pg.609]

Crystals are often associated with their unique polyhedral shapes. Their smooth, shining facets provide a constant source of fascination to ancient, arid modem beings alike. Advances in microscopy have not, tainted the myth a bit interesting surface stmctures are found down to the atomic level, be it surface reconstmction, surface ripples and dimples, or snow-flakish fractals... [Pg.169]

The simplest solid-liquid reaction is the dissolution of a solid in a liquid. The rate at which a solid dissolves in a liquid depends on the particular crystallographic plane (face) exposed. The effect of crystallographic planes on dissolution is clear from the observation that spherical single crystals acquire polyhedral shapes while dissolving. In... [Pg.490]

Polyhedral niosomes were found to be thermoresponsive Fig. 7 (a). Above 35 °C, there was an increase in the release of CF from these niosomes even though the polyhedral shape was preserved until these vesicles were heated to 50 °C. Solulan C24-free polyhedral niosomes do not exhibit this thermoresponsive behavior [160] due to a decrease in the interaction of the polyoxyethylene compound solulan C24 with water at this temperature (due to decreased hydrogen bonding) as identified by viscometry [161]. This observed thermoresponsive behavior was used to design a reversible thermoresponsive controlled release system Fig. 7 (b). Thermoresponsive liposomal systems which rely on the changing membrane permeability, when the system transfers from the gel state (La) to the liquid crystal state (L 3) [162], are not reversible. This is not unex-... [Pg.74]


See other pages where Polyhedral Crystal Shapes is mentioned: [Pg.2]    [Pg.7]    [Pg.2]    [Pg.7]    [Pg.299]    [Pg.299]    [Pg.406]    [Pg.823]    [Pg.517]    [Pg.70]    [Pg.595]    [Pg.388]    [Pg.252]    [Pg.38]    [Pg.396]    [Pg.397]    [Pg.81]    [Pg.89]    [Pg.90]    [Pg.111]    [Pg.120]    [Pg.60]    [Pg.75]    [Pg.245]    [Pg.248]    [Pg.288]    [Pg.507]    [Pg.204]    [Pg.340]    [Pg.71]    [Pg.381]    [Pg.14]    [Pg.337]    [Pg.80]    [Pg.131]    [Pg.2]    [Pg.33]    [Pg.102]    [Pg.141]    [Pg.652]    [Pg.41]    [Pg.825]    [Pg.826]   


SEARCH



Crystal shape

Crystal shaping

Polyhedral crystal

© 2024 chempedia.info