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INDEX conservation equation

We shall begin by establishing the conservation equations. To this end we place a control surface O far from the flame we shall mark the quantities which pertain to this surface with the index 0 since they correspond to the initial state of the material. In the area where we have placed the surface O, at sufficient distance from the flame, all the gradients are also equal to zero. [Pg.336]

To investigate whether c, satisfies (25.52), we begin with the conservation equation using index notation... [Pg.1110]

The conservation equations (mass, momentum, energy) are primarily considered for fluids of uniform and homogeneous composition. Here, we examine how these conservation equations change when two or more species are present and when chemical reactions may also take place. In a multicomponent mixture, transfer of mass takes place whenever there is a spatial gradient in the mixture properties, even in the absence of body forces that act differently upon different species. In fluid flows, the mass transfer will generally be accompanied by a transport of momentum and may further be combined with a transport of heat. For a multicomponent fluid, conservation relations can be written for individual species. Let m, be the species velocities and Pi the species density where the index i, is used to represent the fth species. [Pg.105]

Basic Equations We make following assumptions that 1) the mass loss occurs steadily and 2) the flow is polytropic with index n within the secondary. In these assumptions, the energy conservation is given by... [Pg.215]

We will choose the second control surface such (position I, index 1) that between O and 1 the chemical reaction may be disregarded. In this case the fluxes of individual sorts of molecules are also conserved since in the interval of interest different kinds of molecules axe not transformed into others. Together with the equations written above the following g equations also hold... [Pg.337]

Problem 2-13. Derivation of Transport Equations. Consider the arbitrary fluid element depicted in the figure. If we have a flow containing several species that are undergoing reaction (a source/sink per unit volume) and diffusion (a flux of each species in addition to convection), derive the equation that governs the conservation of each species. The source of species i that is due to reaction is denoted as Rt (units of mass of i per unit time per unit volume) and the total mass flux of species i (diffusion and convection) is given by (p u + ji), in which p, is the mass of species i per unit volume, u is the total mass average velocity of the fluid and j, is the diffusive flux of species i. Note that both u and j, are vectors. We are not using index notation in this problem ... [Pg.101]

The required parameters in the calculation are Ushocked, t/s, and Wp. The shocked refi active index is given by the Gladstone-Dale equation nshocked=l+( -l)Pshocked/p, where p is the initial density of the PMMA (1.186 g/cm ) and n=1.487. Conservation of mass provides the shocked density pshocked=p/(l- Up / s) for a one-dimensional shock compression. Previous studies have validated the Gladstone-Dale model for shocked PMMA up to 22 GPa. [90-91]... [Pg.381]

In both equations the index does not refer to the wavelength of irradiation but to the degree of linear dependence between the different components according to the law of conservation of mass. [Pg.341]

In this paper, we derive an analogous finite-energy conservation relation for the quantum DOS for a particle in a nanoscale stepwise potential (Fig. lb,c), making use of the isomorphism between Helmholtz and Schrodinger equations and mutual correspondence between potential energy and refractive index [6]. [Pg.98]

For the one-dimensional unsteady problem the averaged equations of conservation of number, of mass, and the momentum equation are (with index g for gas and f for liquid)... [Pg.42]

Here n is the index of refraction at the final absorber surface relative to that just outside the collecting aperture. Equation (10) defines the ideal limiting concentration allowed by physical conservation laws for a dielectric secondary. For a focusing lens of focal ratio /, where... [Pg.144]

Fig. 5.5 Relationships between proteome conservation expressed as the averaged amino acid identity (AAI) index and the fraction of shared peptides (FSP) calculated for peptides of different length (L) by using the equation FSP=(AAI). (Reprinted with permission from Dworzanski et al. (2010, pp. 145-155). Copyright 2010 American Chemical Society)... Fig. 5.5 Relationships between proteome conservation expressed as the averaged amino acid identity (AAI) index and the fraction of shared peptides (FSP) calculated for peptides of different length (L) by using the equation FSP=(AAI). (Reprinted with permission from Dworzanski et al. (2010, pp. 145-155). Copyright 2010 American Chemical Society)...
Here p is the density, t the time, Xi the three Cartesian coordinates, and o,- the components of velocity in the respective directions of these coordinates. In equation 2, the index j may assume successively the values 1, 2, 3 gj is the component of gravitational acceleration in the j direction, and atj the appropriate component of the stress tensor (see below). (A third equation, describing the law of conservation of energy, can be omitted for a process at constant temperature the discussion in this chapter is limited to isothermal conditions.) Now, many experiments are purposely designed so that both sides of equation 1 are zero, and so that in equation 2 the inertial and gravitational forces represented by the first and last terms are negligible. In this case, the internal states of stress and strain can be calculated from observable quantities by the constitutive equation alone. For infinitesimal deformations, the appropriate relations for viscoelastic materials involve the same geometrical form factors as in the classical theory of equilibrium elasticity they are described in connection with experimental methods in Chapters 5-8 and are summarized in Appendix C. [Pg.4]


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INDEX conservation

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