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Three-dimensional reactive flow

Because a detailed kinetic mechanism for conventional fuels consists of hundreds of species and thousands of elementary reactions, reduced mechanisms help to analyze three-dimensional reactive flows. [Pg.76]

This study is an example of how a fundamental study of a complicated three-dimensional reactive flow problem can result in sufficient increased understanding of the nature of the problem that a practicable engineering solution can be devised, kbar. It exhibits weak detonation behavior similar to that observed in X0233. [Pg.89]

Cheng, H. P. and G.T. Yeh, 1998, Development of a three-dimensional model of subsurface flow, heat transfer, and reactive chemical transport 3DHYDRO-GEOCHEM. Journal of Contaminant Hydrology 34,47-83. [Pg.513]

SIN s were prepared by adding the proper amount of oil prepolymer to the reactor and heating to 80°C. The styrene/DVB/BP mixture was charged to the reactor followed by purging with gas for 10 minutes. Next, the required amount of TDI needed to react with the remaining hydroxyl groups was added. The TDI crosslinks the reactive oligomers into a three-dimensional network. The reaction was carried out under a flow of N gas of 40 cm /min and the temperature maintained at 80°C. [Pg.239]

The characteristics of a reactive gas (a premixed gas) are dependent not only on the type of reactants, pressure, and temperature, but also on the flow conditions. When the flame front of a combustion wave is flat and one-dimensional in shape, the flame is said to be a laminar flame. When the flame front is composed of a large number of eddies, which are three-dimensional in shape, the flame is said to be a turbulent flame. In contrast to a laminar flame, the combustion wave of a turbulent flame is no longer one-dimensional and the reaction surface of the combustion wave is significantly increased by the eddies induced by the dynamics of the fluid flow. [Pg.42]

The Eulerian (bottom-up) approach is to start with the convective-diffusion equation and through Reynolds averaging, obtain time-smoothed transport equations that describe micromixing effectively. Several schemes have been proposed to close the two terms in the time-smoothed equations, namely, scalar turbulent flux in reactive mixing, and the mean reaction rate (Bourne and Toor, 1977 Brodkey and Lewalle, 1985 Dutta and Tarbell, 1989 Fox, 1992 Li and Toor, 1986). However, numerical solution of the three-dimensional transport equations for reacting flows using CFD codes are prohibitive in terms of the numerical effort required, especially for the case of multiple reactions with... [Pg.210]

Figure 5.7 Three-dimensional drawing of the experimental system used to assess the catalytic properties of the amorphous iron silicate smokes. The (smoke) catalyst is contained in the bottom of a quartz finger (attached to a 2L Pyrex bulb) that can be heated to a controlled temperature. A Pyrex tube brings reactive gas to the bottom of the finger. The gas then passes through the catalyst into the upper reservoir of the bulb and flows through a copper tube at room temperature to a glass-walled observation cell (with ZnSe windows) in an P iiR spectrometer. From there, a closed-cycle metal bellows pump returns the sample via a second 2L bulb and the Pyrex tube to the bottom of the catalyst finger to start the cycle over again (Hill and Nuth 2003). Figure 5.7 Three-dimensional drawing of the experimental system used to assess the catalytic properties of the amorphous iron silicate smokes. The (smoke) catalyst is contained in the bottom of a quartz finger (attached to a 2L Pyrex bulb) that can be heated to a controlled temperature. A Pyrex tube brings reactive gas to the bottom of the finger. The gas then passes through the catalyst into the upper reservoir of the bulb and flows through a copper tube at room temperature to a glass-walled observation cell (with ZnSe windows) in an P iiR spectrometer. From there, a closed-cycle metal bellows pump returns the sample via a second 2L bulb and the Pyrex tube to the bottom of the catalyst finger to start the cycle over again (Hill and Nuth 2003).
Srivastava, R. and Jim Yeh, T.C., A three-dimensional numerical model for water flow and transport of chemically reactive solute through porous media under variably saturated conditions, Adv. Water Resour., 15, 275, 1992. [Pg.88]

These redox cells can operate on a number of scales that depend on the length of the diffusion path from the point that the oxidised form becomes reduced to the point where it reduces another sediment constituent. In some pelagic cores these diffusion paths can be observed in linear portions of the pore-water profiles (e.g. Sawlan Murray, 1983). Here the sedimentation rate and the carbon burial rate are sufficiently low, relative to diffusion, to extend the processes of early diagenesis over tens of metres into the sediment. In coastal environments the sedimentation rate and the concentration and reactivity of the organic matter is often high, which results in a much more complex pattern. In this case, the distances between the cells are much shorter, since by definition the adjustment must occur more rapidly. Like laminar and turbulent flow, there may come a point where the flow of electrons downwards is better dispersed through eddies , which in this case are transitory micro-environments with small-scale three dimensional diffusion, rather than more stable... [Pg.114]

The PECVD or plasma polymerization represents a new technology that enables the production of thin films with manifold properties. Plasma polymerized layers are insoluble in organic solvents, indicative of the highly three dimensional crosslinked structure. The properties of such films can be influenced by parameters like pressure, flow rate, nature of monomer, carrier or reactive gases, power input, reactor configuration, substrate location, frequency (r.f. or microwave). In a "cold plasma" the particles are not in thermical equilibrium. The temperature of the electrons goes up to 10 °C, that of neutral particles and ions reaches about 300 C. The monomers get fragmented in the plasma and polymerize on the fibre surface. [Pg.288]

J.D. Kirtland, G.J. McGraw, A.D. Stroock, Mass transfer to reactive boundaries from steady three-dimensional flows in microchannels, Phys. Fluids, 2006, 18, 073602. [Pg.145]

Two-dimensional models realistically reproduce the in-channel fluid mechanical transport and, when coupled with detailed hetero-Z homogeneous chemistry, provide a powerful tool for both reactor design and fundamental research. Three-dimensional (3D) reactive flow models are necessary in complex geometries with nonstraight channels and cross-flow between channels used for achieving reactor radial uniformity. ZUthough 3D effects do play a role even for straight-channel honeycomb... [Pg.110]

The effect of two volume percent spherical air holes on the reaction zone was modeled using the three-dimensional Eulerian hydrodynamic code, 3DE. The air holes perturb the reaction zone flow. A complicated reaction region develops and is maintained by the reactive fluid dynamics. [Pg.28]

Numerical Solution of Three-Dimensional Eulerian Reactive Flow... [Pg.441]


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Numerical Solution of Three-Dimensional Eulerian Reactive Flow

Three-dimensional reactive flow models

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