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Computer simulations, pattern

Fig. 11. Computer-simulated recirculating patterns in a mixing tank with full baffles (a) elevation view shows circulation patterns generated by turbine blades (b) plane view shows the effect of the baffle on the radial velocity vectors above the turbine blades. Fig. 11. Computer-simulated recirculating patterns in a mixing tank with full baffles (a) elevation view shows circulation patterns generated by turbine blades (b) plane view shows the effect of the baffle on the radial velocity vectors above the turbine blades.
G. Schulz, M. Martin. Computer simulations of pattern formation in ionconducting systems. Solid State Ionics, Diffusion and Reactions 101-103AM,... [Pg.925]

Interstate pipelines also use computer simulation programs to calculate pipeline capacity, pressures, horsepower, fuel and other physical characteristics and properties of their systems. Using this information and incorporating variables such as ambient temperatures, facility outages, and changes in market patterns, transmission companies can run daily studies to determine how much natural gas their systems will deliver under expected operating conditions. [Pg.836]

We prepared microchannel reactor employing stainless steel sheet 400tan thick patterned microchannel by a wet chemical etching. The microchannel shape and dimension were decided by computer simulation of flow distribution and pressure drop of the reactants in the microchaimel sheet. Two different types of patterned plates with mirror image were prepared [5]. The plate has 21 straight microchannels which are 550/an wide, 230/an deep and 34mi long as revealed in Fig. 1(b). [Pg.654]

Figure 2.16. Computer simulation of spatio-temporal pattern formation in CO oxidation on a surface. [Adapted from R.J. Celten, A.P.J. Jansen, R.A. van Santen, j.j. Lukkien, j.P.L Segers and P.A.j. Hilbers,j. Chem. Phys. 108 (1998) 5921.]... Figure 2.16. Computer simulation of spatio-temporal pattern formation in CO oxidation on a surface. [Adapted from R.J. Celten, A.P.J. Jansen, R.A. van Santen, j.j. Lukkien, j.P.L Segers and P.A.j. Hilbers,j. Chem. Phys. 108 (1998) 5921.]...
Molecular spectra can be analyzed for spectrometric or for spectroscopic purposes. The term spectrometric usually refers to compound identification (linking a signal to a known structure) and to the determination of its concentration. The term spectroscopic stands for interpretation of the spectrum in terms of structure (chemical, electronic, nuclear, etc.). In this chapter we will look as some theoretical and practical aspects of a key spectrometric application of bioEPR, namely, the determination of the concentration of paramagnets, also known as spin counting. Subsequently, we consider the generation of anisotropic powder EPR patterns in the computer simulation of spectra, a basic technique that underlies both spectrometric and spectroscopic applications of bioEPR. [Pg.95]

Figure 2.6 High-resolution electron microscopic (HREM) image of ZSM-5/silicalite. The computer-simulated image is shown as an inset. The corresponding electron diffraction pattern and structural drawing are also given. Notice how the large channels ( 6.5 A diameter) as well as the small ones are revealed in the image. The zig-zag path of inversion symmetry lines joining the interchannel apertures is indicated by the bars drawn. (Courtesy of G.R. Millward J.M. Thomas. University of Cambridge.)... Figure 2.6 High-resolution electron microscopic (HREM) image of ZSM-5/silicalite. The computer-simulated image is shown as an inset. The corresponding electron diffraction pattern and structural drawing are also given. Notice how the large channels ( 6.5 A diameter) as well as the small ones are revealed in the image. The zig-zag path of inversion symmetry lines joining the interchannel apertures is indicated by the bars drawn. (Courtesy of G.R. Millward J.M. Thomas. University of Cambridge.)...
Over the last four decades or so, transport phenomena research has benefited from the substantial efforts made to replace empiricism by fundamental knowledge based on computer simulations and theoretical modeling of transport phenomena. These efforts were spurred on by the publication in 1960 by Bird et al. (6) of the first edition of their quintessential monograph on the interrelationships among the three fundamental types of transport phenomena mass transport, energy transport, and momentum transport. All transport phenomena follow the same pattern in accordance with the generalized diffusion equation (GDE). The unidimensional flux, or overall transport rate per unit area in one direction, is expressed as a system property multiplied by a gradient (5)... [Pg.91]

Can observe surface terrain at 1-2-mn definition occasionally atomic resolution, in solution. AFM particularly useful in observation of biosurfaccs Can be programmed to recognize patterns of behavior characteristic of certain mechanism sequences. Computer simulation is vital in, e.g., impedance spectroscopy... [Pg.545]

In this Chapter the kinetics of the Frenkel defect accumulation under permanent particle source (irradiation) is discussed with special emphasis on many-particle effects. Defect accumulation is restricted by their diffusion and annihilation, A + B — 0, if the relative distance between dissimilar particles is less than some critical distance 7 0. The formalism of many-point particle densities based on Kirkwood s superposition approximation, other analytical approaches and finally, computer simulations are analyzed in detail. Pattern formation and particle self-organization, as well as the dependence of the saturation concentration after a prolonged irradiation upon spatial dimension (d= 1,2,3), defect mobility and the initial correlation within geminate pairs are analyzed. Special attention is paid to the conditions of aggregate formation caused by the elastic attraction of particles (defects). [Pg.387]

Fig. 2.53 Computer simulation results, using lime-dependent Ginzburg-Landau dynamics, of a lattice model of an asymmetric copolymer forming a hex phase subject to a step-shear along the horizontal axis (Ohta et al. 1993), The evolution of the domain pattern after the application of the step-shear is shown, (a) t = 1 (the pattern immediately after the shear is applied) (b) t = 5000 (c) t = 10000 (d) t = 15 000. The time-scale corresponds to the characteristic time for motion of an individual chain, t = R M. [Pg.108]

Fig. 17. Sets of computed diffraction pattern simulations for different patterns of labeling of myosin heads on actin, defined by the head angular search range A9, the head axial search range AZ, and the actin target area angular size (twice the large number on each pattern), in each case with at least 98% of the available myosin heads bound to acdn. For details of parameters and regions A, B, and C, see text. (Based on Squire et at, 2005b.)... Fig. 17. Sets of computed diffraction pattern simulations for different patterns of labeling of myosin heads on actin, defined by the head angular search range A9, the head axial search range AZ, and the actin target area angular size (twice the large number on each pattern), in each case with at least 98% of the available myosin heads bound to acdn. For details of parameters and regions A, B, and C, see text. (Based on Squire et at, 2005b.)...
Figure 3.15 Experimental (a) and computer-simulated (b) X-band EPR spectra of a fulvic acid from an arable soil developed from base-rich parent material. Note the octet hyperfine structure patterns associated with the gB and gj features (from Cheshire et at., 1977). Figure 3.15 Experimental (a) and computer-simulated (b) X-band EPR spectra of a fulvic acid from an arable soil developed from base-rich parent material. Note the octet hyperfine structure patterns associated with the gB and gj features (from Cheshire et at., 1977).
Fig. 7.9 Computer simulations of a neuronal network (lOx 10 neurons) with nearest neighbor gap-junction coupling (see equations). The diagrams show the local mean field potentials (LFP) which are calculated as the mean potential values V of all neurons during continuously increasing coupling strength gc- Insets illustrate the different types of patterns in which the neurons originally operate (with randomly set initial values), (a) The network of tonic firing... Fig. 7.9 Computer simulations of a neuronal network (lOx 10 neurons) with nearest neighbor gap-junction coupling (see equations). The diagrams show the local mean field potentials (LFP) which are calculated as the mean potential values V of all neurons during continuously increasing coupling strength gc- Insets illustrate the different types of patterns in which the neurons originally operate (with randomly set initial values), (a) The network of tonic firing...

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Computational simulations

Computer simulation

Computer simulations, pattern formation

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