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Matrix geometric model

It is reasonable to hope to assemble a complete set of representations to provide a full and non-redundant description of the symmetry species compatible with a point group The problem is that there are far too many representations of any group. On the one hand, matrices in representations derived from expressing symmetry operations in terms of coordinates - as in problem 5-18 - depend on the coordinate system. Thus there are an infinite number of matrix representations of C2v equivalent to example 7, derivable in different coordinate systems. These add no new information, but it is not necessarily easy to recognize that they are related. Even in the cases of representations not derived from geometric models via coordinate systems, an infinite number of other representations are derivable by similarity transformations. [Pg.43]

Neuts, M., Matrix-Geometric Solutions in Stochastic Models An Algorithmic Approach, Johns Hopkins University Press, Baltimore, 1981. [Pg.411]

Simplifications can be brought about whenever the surface structure has symmetries. Point-group symmetries help moderately to reduce the matrix dimensions. On the other hand, two-dimensional periodicity can help drastically by reducing the number N to the number of atoms within a single two-dimensional unit cell with a depth perpendicular to the surface of a few times the electron mean free path. For surface crystallography this is, however, not yet sufficient, because surface structural determination requires repeating such calculations for hundreds of different geometrical models of the surface structure. [Pg.64]

Kevan L. (1979) Forbidden matrix proton spin flip satelites in 70 GHz ESP spectra of solvated electrons A geometrical model for the solvated electron in methanol glass. Chem Phys Lett 66 578-580. [Pg.54]

Associated with each eigenvalue (the length of the new axis in our geometric model) is a characteristic vector, the eigenvector, v = [vi,V2] defining the slope of the axis. Our eigenvalues, f, were defined as arising from a set of simultaneous equations. Equation (19), which can now be expressed, for a 2 x 2 matrix, as. [Pg.73]

An automatic version of MOLMEC has also been developed so that data sets with large numbers of molecules can be modelled without continuous supervision. The program consists of an input section, which reads the molecule s connection table and present coordinate matrix from the ADAPT disc files, a minimization section with all output suppressed, and a section which stores the final coordinate matrix. Good models can easily be obtained in this manner. However, before the coordinate matrices can be used for calculating descriptors, the structures are reviewed to make sure that the molecules are in acceptable conformations, Once modelling is complete, geometric descriptors can be derived. [Pg.150]

Once a weave coding is defined, an analysis of the weave matrix allows answering questions about mutual positions of the yams. Consider a warp yam between two intersections with weft. Which weft yams is it interacting with in these intersections What is its position vis-a-vis these yams An answer to these questions is evident for one-layer weave, but for multilayered weaves it needs analysing the weave code. Knowing these answers allows definition of interactions between warp and weft, which is needed for building a geometrical model of the unit cell based on mechanics of these interactions, and definition of contacts between the yam needed for creation of meso-level FE models. [Pg.24]

Neuts, M. F. 1981. Matrix-geometric solutions in stochastic models an algorithmic approach. Johns Hopkins series in the mathematical sciences 2. Baltimore, Johns Hopkins University Press 41-80. [Pg.595]

Another problem one could have with the geometrical model is that it would not be able to account for local differences in texture in different faces of the same cell, as are seen in epidermal cells of leaves. However there is no reason to suppose that a cell would not be able to regulate the cellulose to matrix ratio and, therefore, its wall texture in different wall facets. [Pg.194]

Emons A.M.C., Schel J.H.N., and Mulder B.M. 2002. The geometrical model for microfibril deposition and the influence of the cell wall matrix. Plant Biol 4 22-26. [Pg.196]

The character table of a point group can be derived in a rigorous manner using the concepts of matrix algebra and the geometric model of a molecule. Since this is not the purpose of this text, the following... [Pg.118]

The model for a filled system is different. The filler is, as before, represented by a cube with side a. The cube is coated with a polymer film of thickness d it is assumed that d is independent of the filler concentration. The filler modulus is much higher than that of the d-thick coat. A third layer of thickness c overlies the previous one and simulates the polymeric matrix. The characteristics of the layers d and c are prescribed as before, and the calculation is carried out in two steps at first, the characteristics of the filler (a) - interphase (d) system are calculated then this system is treated as an integral whole and, again, as part of the two component system (filler + interphase) — matrix. From geometric... [Pg.15]


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See also in sourсe #XX -- [ Pg.312 , Pg.313 ]




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