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Transport three-dimensional

Elastic scattering is also the basis for Hdar, in which a laser pulse is propagated into a telescope s field of view, and the return signal is collected for detection and in some cases spectral analysis (14,196). The azimuth and elevation of the scatterers (from the orientation of the telescope), their column density (from the intensity), range (from the temporal delay), and velocity (from Doppler shifts) can be deterrnined. Such accurate, rapid three-dimensional spatial information about target species is useful in monitoring air mass movements and plume transport, and for tracking aerosols and pollutants (197). [Pg.318]

Laminar flame instabilities are dominated by diffusional effects that can only be of importance in flows with a low turbulence intensity, where molecular transport is of the same order of magnitude as turbulent transport (28). Flame instabilities do not appear to be capable of generating turbulence. They result in the growth of certain disturbances, leading to orderly three-dimensional stmctures which, though complex, are steady (1,2,8,9). [Pg.518]

Travis. J. R, K L. Lam, and T. L. Wilson, 1994, GASFLOW A Three-Dimensional Finite-Volume Fluid Dynamics Code for Calculating the Transport, Mixing, and Combustion of Flammable Gases in Geometrically Complex Domains, LA-UR-94-2270 Vol. 1,2, and 3 LANL, July. [Pg.490]

Figure 11. The [B2]X4 framework of an v4[B 2X4 spinel, e.g. A - MnO, with three dimensional pathways for lithium-ion transport. (The direction of transport perpendicular to the plane of the paper has not been marked by an arrow). Figure 11. The [B2]X4 framework of an v4[B 2X4 spinel, e.g. A - MnO, with three dimensional pathways for lithium-ion transport. (The direction of transport perpendicular to the plane of the paper has not been marked by an arrow).
Ionic transport in solid electrolytes and electrodes may also be treated by the statistical process of successive jumps between the various accessible sites of the lattice. For random motion in a three-dimensional isotropic crystal, the diffusivity is related to the jump distance r and the jump frequency v by [3] ... [Pg.532]

Heimann, M. and Keeling, C. D. (1989). A three-dimensional model of atmospheric CO2 transport based on observed winds 2. Model description and simulated tracer experiments. In "Aspects of Climate Variability in the Pacific and Western Americas," Geophys. Monogr. Ser. vol. 55 (D. H. Peterson, ed.), pp. 237-275, AGU, Washington, DC. [Pg.313]

Hunt, E. R. Jr., Piper, S. C., Nemani, R., Keeling, C. D., Otto, R. D. and Running, S. W. (1996). Global net carbon exchange and intra-annual atmospheric CO2 concentrations predicted by an ecosystem process model and three-dimensional atmospheric transport model. Global Biogeochem. Cycles 10, 431-456. [Pg.314]

Taguchi, S. (1996). A three-dimensional model of atmospheric CO2 transport based on analyzed winds Model description and simulation results for TRANSCOM, /. Geophys. Res. 101, 15099-15109. [Pg.320]

Models of atmospheric phenomena are similar to those of combustion and involve the coupling of exceedingly complex chemistry and physics with three-dimensional hydrodynamics. The distribution and transport of chemicals introduced into groundwater also involve a coupling of chemical reactions and transports through porous solid media. The development of groundwater models is critical to understanding the effects of land disposal of toxic waste (see Chapter 7). [Pg.155]

Keeling, C.D., Bacastow, R.B., Carter, A.F., Piper, S.C., Whorf T.P, Heimann, M., Mook, W.G. and Roeloffzen, H. 1989 A three-dimensional model of atmospheric COj transport based on observed winds 1. Analysis of observational data. Geophysical Monographs 55 165-236. [Pg.60]

The gas motion near a disk spinning in an unconfined space in the absence of buoyancy, can be described in terms of a similar solution. Of course, the disk in a real reactor is confined, and since the disk is heated buoyancy can play a large role. However, it is possible to operate the reactor in ways that minimize the effects of buoyancy and confinement. In these regimes the species and temperature gradients normal to the surface are the same everywhere on the disk. From a physical point of view, this property leads to uniform deposition - an important objective in CVD reactors. From a mathematical point of view, this property leads to the similarity transformation that reduces a complex three-dimensional swirling flow to a relatively simple two-point boundary value problem. Once in boundary-value problem form, the computational models can readily incorporate complex chemical kinetics and molecular transport models. [Pg.335]

Quintard, M, Diffusion in Isotropic and Anisotropic Porous Systems Three-Dimensional Cal-cnlations. Transport in Porons Media 11, 187, 1993. [Pg.619]


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