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Thin theory

However, by the thermally thin approximation, T(x,t) T(t) only. A control volume surrounding the thin material with the conservation of energy applied, Equation (3.45), gives (for a solid at equal pressure with its surroundings) [Pg.173]

The net heat flux is taken here to represent radiative heating in an environment at Tcx, with an initial temperature T,yj as well. From Equation (7.20) a more general form can apply if the flame heat flux is taken as constant. This nonlinear problem cannot yield an analytical solution. To circumvent this difficulty, the radiative loss term is approximated by a linearized relationship using an effective coefficient, hr  [Pg.173]

Note that the effect of cooling has been totally eliminated since we have implicitly considered the high heating case where qe ht(Tig — T0Q). Consider [Pg.174]

Therefore this approximation might prove valid for qe 5 kW/m2 at least. [Pg.174]

For long heating times, eventually at t — oo, the temperature just reaches Tig. Thus for any heat flux below this critical heat flux for ignition, gig crit, no ignition is possible by the conduction model. The critical flux is given by the steady state condition for Equation [Pg.174]


N. Flarfield and J. R. Bowler, Theory of thin-skin eddy-current interaction with surface cracks, J. Appl. Phys., 82(9), 4590 - 4603, 1997. [Pg.147]

It must also be realized that this thin surface region is in a very turbulent state. Since the liquid is in equilibrium with its vapor, then, clearly, there is a two-way and balanced traffic of molecules hitting and condensing on the surface from the vapor phase and of molecules evaporating from the surface into the vapor phase. From the gas kinetic theory, the number of moles striking 1 cm of surface per second is... [Pg.56]

The preceding treatment relates primarily to flocculation rates, while the irreversible aging of emulsions involves the coalescence of droplets, the prelude to which is the thinning of the liquid film separating the droplets. Similar theories were developed by Spielman [54] and by Honig and co-workers [55], which added hydrodynamic considerations to basic DLVO theory. A successful experimental test of these equations was made by Bernstein and co-workers [56] (see also Ref. 57). Coalescence leads eventually to separation of bulk oil phase, and a practical measure of emulsion stability is the rate of increase of the volume of this phase, V, as a function of time. A useful equation is... [Pg.512]

Stoyanov S and Kashchiev D 1981 Thin film nucleation and growth theories a confrontation with experiment Current... [Pg.954]

Vop D, Kruger P, Mazur A and Pollmann J 1999 Atomic and electronic structure of WSe from ah initio theory bulk crystal and thin film systems Phys. Rev. B 60 14 311... [Pg.2229]

In two-dimensional solids theory, the size of the solid in a fixed direction is assumed to be small as compared to the other ones. Therefore, all characteristics of the thin solid are referred to a so-called mid-surface, and one obtains the two-dimensional model. Let us give the construction of plate and shell models (Donnell, 1976 Vol mir, 1972 Lukasiewicz, 1979 Mikhailov, 1980). [Pg.5]

Fa.n Spra.ys, It was demonstrated around the 1950s that iastabiHty theory can be used to analyze the wave growth on a thin Hquid sheet (18). This analysis predicted the existence of an optimum wavelength at which a wave would grow rapidly. This optimum wavelength, X corresponds to a condition that leads to Hquid sheet disiategration. It can be expressed as ia equatioa 2 ... [Pg.329]

Dukler Theory The preceding expressions for condensation are based on the classical Nusselt theoiy. It is generally known and conceded that the film coefficients for steam and organic vapors calculated by the Nusselt theory are conservatively low. Dukler [Chem. Eng. Prog., 55, 62 (1959)] developed equations for velocity and temperature distribution in thin films on vertical walls based on expressions of Deissler (NACA Tech. Notes 2129, 1950 2138, 1952 3145, 1959) for the eddy viscosity and thermal conductivity near the solid boundaiy. According to the Dukler theoiy, three fixed factors must be known to estabhsh the value of the average film coefficient the terminal Reynolds number, the Prandtl number of the condensed phase, and a dimensionless group defined as follows ... [Pg.566]

Boundary layer flows are a special class of flows in which the flow far from the surface of an object is inviscid, and the effects of viscosity are manifest only in a thin region near the surface where steep velocity gradients occur to satisfy the no-slip condition at the solid surface. The thin layer where the velocity decreases from the inviscid, potential flow velocity to zero (relative velocity) at the sohd surface is called the boundary layer The thickness of the boundary layer is indefinite because the velocity asymptotically approaches the free-stream velocity at the outer edge. The boundaiy layer thickness is conventionally t en to be the distance for which the velocity equals 0.99 times the free-stream velocity. The boundary layer may be either laminar or turbulent. Particularly in the former case, the equations of motion may be simphfied by scaling arguments. Schhchting Boundary Layer Theory, 8th ed., McGraw-HiU, New York, 1987) is the most comprehensive source for information on boundary layer flows. [Pg.666]

Dwight, H.B., Theory for proximity effects in wires, thin tubes and sheaths , AIEE Trans. 42 (1923). [Pg.950]

The simplest system in which useful products are obtained by thermochemical processing involves the evaporahon of an element or elements in vacuum in order to produce thin hlms on a selected substrate. This process is usually limited to the production of thin hlms because of the low rates of evaporation of the elements into a vacuum under conditions which can be controlled. These rates can be calculated by the application of the kinetic theory of ideal gases. [Pg.4]

D. E. Aspnes. Thin Solid Films. 89, 249, 1982. A detailed review of effective medium theory and its use in studies of optical properties of solids. [Pg.410]

Most of the work, however, tend to give the impression of being somewhat esoteric, and of uncertain value in the practice of thin layer chromatography. A more detailed discussion of TLC theory can be found elsewhere. (4)... [Pg.453]


See other pages where Thin theory is mentioned: [Pg.172]    [Pg.126]    [Pg.172]    [Pg.126]    [Pg.50]    [Pg.143]    [Pg.1219]    [Pg.1800]    [Pg.2368]    [Pg.188]    [Pg.91]    [Pg.92]    [Pg.159]    [Pg.160]    [Pg.177]    [Pg.179]    [Pg.183]    [Pg.342]    [Pg.313]    [Pg.466]    [Pg.1416]    [Pg.2105]    [Pg.292]    [Pg.483]    [Pg.112]    [Pg.210]    [Pg.217]    [Pg.217]    [Pg.252]    [Pg.220]    [Pg.266]    [Pg.315]    [Pg.17]    [Pg.443]    [Pg.480]   


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