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Vertices fitting

Vertical fit between partners. Olefines, such as ethylene and propylene, are the key raw materials for most petrochemical products. No fully efficient and liquid merchant markets for olefines exist yet in Europe, because of the traditional integration of petrochemical players and also because of transportation difficulties, which are worsened by the absence in Europe of an extensive pipeline network like that on the Gulf Coast of the United States. Such markets probably wiU not be developed in the short to medium term, especially for ethylene which is relatively hard to transport... [Pg.179]

Kauffman ([kauffSO], [kauffOOa]) has introduced a class of parametrizable fitness landscapes called NK-landscapes, that provide a formalism for studying the efficacy of GA evolution as a function of certain statistical properties of the landscape. Given N binary variables Xi = 1, so that x = (xi, X2, , Xjv) represents a vertex of an A -dimensional hypercube, an NK-landscape is defined by a fitness function, JF, of the form... [Pg.587]

KT1 does not have the NaTl structure because the K+ ions are too large to fit into the interstices of the diamond-like Tl- framework. It is a cluster compound K6T16 with distorted octahedral Tig- ions. A Tig- ion could be formulated as an electron precise octahedral cluster, with 24 skeleton electrons and four 2c2e bonds per octahedron vertex. The thallium atoms then would have no lone electron pairs, the outside of the octahedron would have nearly no valence electron density, and there would be no reason for the distortion of the octahedron. Taken as a closo cluster with one lone electron pair per T1 atom, it should have two more electrons. If we assume bonding as in the B6Hg- ion (Fig. 13.11), but occupy the t2g orbitals with only four instead of six electrons, we can understand the observed compression of the octahedra as a Jahn-Teller distortion. Clusters of this kind, that have less electrons than expected according to the Wade rules, are known with gallium, indium and thallium. They are called hypoelectronic clusters their skeleton electron numbers often are 2n or 2n — 4. [Pg.146]

With hexagons, there is no way to construct a regular polyhedron, since even three hexagons sharing a vertex lie in the same plane. With all higher poiyhedra not even three can be fitted together at a common vertex. [Pg.46]

Reconstruction of the vertex of low energy events is performed with an algorithm based on the time and position of hit PMTs. After the vertex is established, a separate fit is used to obtain the angle of the electron. The distribution of the events presented here is consistent with an uniform volume distribution. [Pg.339]

Fig. 4. Adenovirus and bacteriophage PRDl. Top On the left, a density isosurface representation of adenovirus at 25-A resolution is shown. The 5-fold axis, occupied by the protein penton, is marked with a pentagon. A trimer of hexon is marked with a triangle close by arrays of hexon extend outward in all directions from the pentagonal vertex, forming the flat faces of the virus. On the right, a close-up of the 5-fold axis is shown (top) and below that a close-up of the hexon trimer with it crystal structure fitted (Athappilly et at, 1994 Stewart et al, 1991). Bottom The Susl mutant of PRDl is shown... Fig. 4. Adenovirus and bacteriophage PRDl. Top On the left, a density isosurface representation of adenovirus at 25-A resolution is shown. The 5-fold axis, occupied by the protein penton, is marked with a pentagon. A trimer of hexon is marked with a triangle close by arrays of hexon extend outward in all directions from the pentagonal vertex, forming the flat faces of the virus. On the right, a close-up of the 5-fold axis is shown (top) and below that a close-up of the hexon trimer with it crystal structure fitted (Athappilly et at, 1994 Stewart et al, 1991). Bottom The Susl mutant of PRDl is shown...
The MTD-MC method is a modified version of the MTD method, accounting for the existence of several low-energy conformations of molecules used to derive the hypermolecule by overlap. Each molecule is described by a vector of binary variables Ii( )s equal to one if the 5th vertex of the hypermolecule is occupied by the ith molecule in the A th conformation. If more than one low-energy conformation is allowed for a molecule, the conformations considered will be the one which best fits the binding site cavity, i.e. the one with the lowest MTD value ... [Pg.293]

The important issue is We cannot draw a straight line which fits to all vertices of a triangle. There will always be one vertex which does not fit. We cannot fit a plane to all vertices of a tetrahedron. ... [Pg.226]

Assuming that such a relaxation procedure has been successfully carried out, we can analyze the resulting spatial structures using the same types of analysis that were used in Section III and IV. We have in fact done this for the topologically constrained model. Some typical results are shown in Fig. 86, namely the size distribution of sixfold-ordered clusters, n, for a 3584-vertex system at / = 1.4, r = 4, for = 6. This distribution represents an average over 100 configurations from a 10,000-sweep MC run. The fraction of broken bonds at this value of r and t is (f) = 0.11690 0.00011, which is comparable to the order parameter of the time-averaged WCA system at p = 0.83 and to that of the DRP system. The solid line represents a fit to Eq. (3.26), which yields a power law... [Pg.694]

Fig. 7.6. Simplex centroid design, with average responses for the mixtures represented by the points and contour curves for the special cubic model, Eq. (7.20). The three boxed response values close to each vertex were used to test the quality of the fit. Fig. 7.6. Simplex centroid design, with average responses for the mixtures represented by the points and contour curves for the special cubic model, Eq. (7.20). The three boxed response values close to each vertex were used to test the quality of the fit.
In short, we should stay with the quadratic model, whose contour curves are shown in Fig. 7A.1. The most intense absorbance values are obtained in the vicinity of the lower right vertex, which corresponds to ethanol-rich mixtures. The absence of significant interactions involving the third component (acetone) is reflected in the almost vertical contour curves. The graph of the predicted responses against the observed ones (Fig. 7A.2) visually confirms the quality of the fit. Note that the responses are stratified in five groups, corresponding to the five columns of points in Fig. 7A.1. [Pg.343]

The analysis of variance shows that the linear model is unsatisfactory, and that the other two models do not show lack of fit (Table 7A.4). This time, however, the special cubic model seems superior. The explained variation is larger, the MS of/MS ratio is smaller, and the cubic term is statistically significant. The contour curves for the cubic model are presented in Fig. 7A.3. The largest tensile strength values are obtained close to the base of the triangle, toward the left vertex, which corresponds to a blend that is predominantly PVDF, with httle or no polystyrene. [Pg.345]


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See also in sourсe #XX -- [ Pg.680 , Pg.681 , Pg.682 , Pg.683 ]




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