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Geometry graphs

Klein, D.J. (1997a). Graph Geometry, Graph Metrics, Wiener. MATCH (Comm.Math.Comp. Chem.),35,1-21. [Pg.601]

Klein, D.J. (1997) Graph geometry, graph metrics, and Wiener. MATCH Commun. Math. Comput. Chem., 35, 7-27. [Pg.1093]

Mathematics geometry graph theory set theory abstract algebra physics dimension theory knot theory. [Pg.1841]

Sketch the molecules on graph paper to help in determining the atomic coordinates. This is the first use of molecular geometry, a property that will become increasingly important as we go on. At this stage, the geometries are approximate the difference, for example, between cis and trans isomer s is ignored. [Pg.258]

Taking the concept of a master curve a step further, the relationships in Table 10.1 can also be incorporated into such curves so that graphs of z versus a characteristic dimension relative to X are plotted for various geometries. [Pg.707]

This value can be considerably smaller. It corresponds in Fig. 6-1 to the ordinate of the intersection of the resistance graph of slope cCq with a 7(f/-r) curve that deviates markedly to the left of that plotted. The maximum current density is an important quantity for the setting up of cathodic protection with galvanic anodes and is dependent on the anode geometry and conductivity of the medium. [Pg.185]

Read power number versus Reynolds number in turbulent region is based on geometry of the impellers. The lowest power number is less than l,for marine propellers. For flat bladed turbines in a turbulent region, the power number is equal to 6. The power graph is illustrated in Figure 6.6. [Pg.167]

It is feasible to carry out Hartree-Fock calculations on our available computer resources (an SGI Crimson Elan Workstation) using an STO-3G basis set with full geometry optimization of CeoMu but only partial geometry optimisations of the ChoMu isomers. Fig. 1 shows planar graphs of Ceo and C70 with the carbon atoms suitably labelled for future reference. [Pg.442]

The E-state is based solely on atom connectivity information obtained from the molecular graph, without any input from the molecular geometry or sophisticated quantum calculations. We start this chapter with a brief presentation of the relevant notions of graph theory and continue with the definitions of a couple of important graph matrices. Then the molecular connectivity indices are mentioned... [Pg.86]

Figure 6.16 Molecular graphs for some molecules in their equilibrium geometries. A bond critical point is denoted by a black dot. The molecule HCCH is ethyne, H2CO is methanal, and H2CCH2 is ethene. [Adapted with permission from Bader [1990], Fig. 2.8.]... Figure 6.16 Molecular graphs for some molecules in their equilibrium geometries. A bond critical point is denoted by a black dot. The molecule HCCH is ethyne, H2CO is methanal, and H2CCH2 is ethene. [Adapted with permission from Bader [1990], Fig. 2.8.]...
Graphs are shown for spheres and slabs separately, and with the modified Thiele modulus for all geometries and orders. [Pg.752]

This formula shows a smooth decrease of p toward the bulk magnetic moment with increasing N. However, the experimental results graphed in Figure 1 indicate that the variation of p with N has a more complex, oscillatory behavior. Its explanation requires a detailed consideration of the geometry of the cluster and a better treatment of its electronic structure. [Pg.198]

Then the graph must be interpreted and a trial geometry generated. [Pg.160]

Eontanella and co-workers studied the effect of high pressure variation on the conductivity as well as the H, H, and O NMR spectra of acid form Nafionl 17 membranes that were exposed to various humidities. Variation of pressure allows for a determination of activation volume, A V, presumably associated with ionic and molecular motions. Conductivities (a) were obtained from complex electrical impedance diagrams and sample geometry, and A V was determined from the slope of linear isothermal In a versus p graphs based on the equation A E = —kJ d In a/d/j] t, where p is the applied pressure. At room temperature, A Ewas found to be 2.9 cm mol for a sample conditioned in atmosphere and was 6.9 cm mol for a sample that was conditioned in 25% relative humidity, where the latter contained the lesser amount of water. [Pg.330]

Spellmeyee, D.C., Wong, A.K., Bower, M.J., and Bianey, J.M. Conformational analysis using distance geometry methods./. Mol. Graph. Model. 1997, 35, 18-36. [Pg.107]

The proof, as I understood it in 1972, can be found in Sections 2.3-2.6 of my book with V. I. Yukalov [1], which contains a misleading although minor error in Eq. (2.47). This mistake was corrected in 2002 in the paper [2], which also throws exciting light on the application of the RDM approach to the theory of condensed matter and to the complex geometry of the graph of the equation... [Pg.487]

Poutanen and Johnson (PI) show that the equation of a lituus (r = 1) resembled the true shape of a gas bubble forming at a submerged nozzle. They varied this geometry by using r 0 = 1, to describe such shapes quite accurately. Their method for calculating area involves a shape factor similar to that of Andreas et al. (A2), with a series of auxiliary graphs. Area becomes... [Pg.58]


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See also in sourсe #XX -- [ Pg.6 ]




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