Big Chemical Encyclopedia

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

Articles Figures Tables About

Shapes of nuclei

Figure 13.1. Macroscopic and microscopic appearance of solid tumours, a A metastasis of an intestinal tumour in the liver. The tumour is the bright blob ins the center, showing irregular tissue organization, and yellowish fat deposits and cavities resulting from cell degeneration. The tumour grows invasively into the surroimding liver tissue, b Microscopic picture of a malignant epithelial (squamous cell) tumour. Note the very irregular size and shape of nuclei and of cells. Figure 13.1. Macroscopic and microscopic appearance of solid tumours, a A metastasis of an intestinal tumour in the liver. The tumour is the bright blob ins the center, showing irregular tissue organization, and yellowish fat deposits and cavities resulting from cell degeneration. The tumour grows invasively into the surroimding liver tissue, b Microscopic picture of a malignant epithelial (squamous cell) tumour. Note the very irregular size and shape of nuclei and of cells.
The dehydrations of alums have been of particular interest in kinetic studies because large, relatively perfect crystals can be prepared, and the cubic lattice, common to different alums, should simplify the interpretation of kinetic data. (Some lattice modification does, however, accompany cation variation [102]). Despite these structural similarities, the extents of water loss, the kinetic parameters and the shapes of nuclei developed all show significant differences with changes in cation composition of the alum. [Pg.236]

Arrhenius parameters for the dehydrations of ammonium and potassium aliuninium alums [38] were in agreement with the Polanyi-Wigner equation. Comparisons of the shapes of nuclei on different crystal surfaces indicated that reaction proceeds along (100) planes. The observed decrease of the rate in water vapour is attributed to the blocking of pores by adsorbed molecules. No intranuclear cracking was apparent and the product-reactant boimdaries became irregular because of the influence of water on reorganization of the product phase. The appearance of these nuclei contrasted markedly with those in mixed potassium chromium/aluminium alums, where there is an approximately concentric structure. [Pg.237]

NOTES (i) There is a different pattern of change of intranuclear surface by the two salts, but subsequent textural development is enhanced by exposme to water vapour after previous evacuation, (ii) A specialized reaction zone is required to initiate nucleation in both salts. The shapes of nuclei developed are shghtly different but both grow in three dimensions, (iii) Water is rapidly and easily reaccommodated in the Al " ion coordination shell but reaction of H2O with after dehydration proceeds much more... [Pg.239]

Fig. IV-6. The shape of nuclei when there is condition of a complete non-wetting (a), poor wetting (b), and good wetting of the new phase substrate (c)... Fig. IV-6. The shape of nuclei when there is condition of a complete non-wetting (a), poor wetting (b), and good wetting of the new phase substrate (c)...
We shall again consider only the growth of hemispherical centres although similar equations can be derived for any shape of nuclei. Growth may be controlled either by kinetics or by mass transport. In the former case, the current at a fixed overpotential will depend only on the surface area iS of a nucleus... [Pg.44]

Electronic spectra are almost always treated within the framework of the Bom-Oppenlieimer approxunation [8] which states that the total wavefiinction of a molecule can be expressed as a product of electronic, vibrational, and rotational wavefiinctions (plus, of course, the translation of the centre of mass which can always be treated separately from the internal coordinates). The physical reason for the separation is that the nuclei are much heavier than the electrons and move much more slowly, so the electron cloud nonnally follows the instantaneous position of the nuclei quite well. The integral of equation (BE 1.1) is over all internal coordinates, both electronic and nuclear. Integration over the rotational wavefiinctions gives rotational selection rules which detemiine the fine structure and band shapes of electronic transitions in gaseous molecules. Rotational selection rules will be discussed below. For molecules in condensed phases the rotational motion is suppressed and replaced by oscillatory and diflfiisional motions. [Pg.1127]

Electron Density Surfaces. An alternative technique for portraying molecular size and shape relies on the molecule s own electron cloud. Atoms and molecules are made up of positively-charged nuclei surrounded by a negatively-charged electron cloud, and it is the size and shape of the electron cloud that defines the size and shape of an atom or molecule. Quantum mechanics provides the mathematical recipe for determining the size and shape of the electron cloud, and computer programs can carry out the necessary calculations. [Pg.24]

X= 2) or (P = 0, X = 3) and the distinction between these possibilities is most satisfactorily based upon independent evidence, such as microscopic observations. The growth of compact nuclei inevitably results in the consumption of surfaces and when these outer faces, the sites of nucleation, have been eliminated, j3 necessarily is zero this may result in a diminution of n. The continued inward advance of the reaction interface at high a results in a situation comparable with the contracting volume reaction (discussed below) reference to this similarity was also made in consideration of the Mampel approach discussed above. Shapes of the deceleratory region of a time curves for nucleation and growth reactions and the contracting volume rate process are closely similar [409]. [Pg.58]

SANS is a valuable research technique, since it provides information about the size and shape of the molecular scale structures in the size range 1-10 nm found in polymer or dendrimer systems. Neutrons interact with atomic nuclei, hence are sensitive not only to the details of the way such nuclei are arranged but also to the presence of different isotopes. [Pg.141]


See other pages where Shapes of nuclei is mentioned: [Pg.123]    [Pg.130]    [Pg.52]    [Pg.370]    [Pg.25]    [Pg.228]    [Pg.235]    [Pg.546]    [Pg.415]    [Pg.105]    [Pg.720]    [Pg.257]    [Pg.87]    [Pg.225]    [Pg.222]    [Pg.123]    [Pg.130]    [Pg.52]    [Pg.370]    [Pg.25]    [Pg.228]    [Pg.235]    [Pg.546]    [Pg.415]    [Pg.105]    [Pg.720]    [Pg.257]    [Pg.87]    [Pg.225]    [Pg.222]    [Pg.400]    [Pg.36]    [Pg.462]    [Pg.21]    [Pg.7]    [Pg.13]    [Pg.24]    [Pg.42]    [Pg.44]    [Pg.48]    [Pg.51]    [Pg.62]    [Pg.84]    [Pg.122]    [Pg.122]    [Pg.129]    [Pg.212]    [Pg.225]    [Pg.247]    [Pg.285]    [Pg.483]    [Pg.16]    [Pg.700]    [Pg.814]    [Pg.816]   


SEARCH



Nucleus shape

© 2024 chempedia.info