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Equation Transformation

The nonlinear constant in these equations cannot be evaluated dkecdy by the methods previously described. Even forms such as these can be handled, however. For example, subtracting a trial value of a fromjy and taking logarithms transforms equation 97 into the linear form ... [Pg.246]

For other mechanisms, the particle-scale equation must be integrated. Equation (16-140) is used to advantage. For example, for external mass transfer acting alone, the dimensionless rate equation in Table 16-13 would be transformed into the ( — Ti, Ti) coordinate system and derivatives with respect to Ti discarded. Equation (16-138) is then used to replace cfwith /ifin the transformed equation. Furthermore, for this case there are assumed to be no gradients within the particles, so we have nf=nf. After making this substitution, the transformed equation can be rearranged to... [Pg.1527]

Tables of Laplace ti ansforms for a large number of functions have been calculated, and can be obtained from published data. In the present example, the transformed equation is... Tables of Laplace ti ansforms for a large number of functions have been calculated, and can be obtained from published data. In the present example, the transformed equation is...
The price of flexibility comes in the difficulty of mathematical manipulation of such distributions. For example, the 3-parameter Weibull distribution is intractable mathematically except by numerical estimation when used in probabilistic calculations. However, it is still regarded as a most valuable distribution (Bompas-Smith, 1973). If an improved estimate for the mean and standard deviation of a set of data is the goal, it has been cited that determining the Weibull parameters and then converting to Normal parameters using suitable transformation equations is recommended (Mischke, 1989). Similar estimates for the mean and standard deviation can be found from any initial distribution type by using the equations given in Appendix IX. [Pg.139]

The population balance in equation 2.86 employs the local instantaneous values of the velocity and concentration. In turbulent flow, there are fluctuations of the particle velocity as well as fluctuations of species and concentrations (Pope, 1979, 1985, 2000). Baldyga and Orciuch (1997, 2001) provide the appropriate generalization of the moment transformation equation 2.93 for the case of homogeneous and non-homogeneous turbulent particle flow by Reynolds averaging... [Pg.56]

At this point, we recall from elementary mechanics of materials the transformation equations for expressing stresses in an x-y coordinate system in temis of stresses in a 1-2 coordinate system. [Pg.74]

Tsai and Pagano [2-7] ingeniously recast the stiffness transformation equations to enable ready understanding of the consequences of rotating a lamina in a laminate. By use of various trigonometric identities between sin and cos to powers and sin and cos of multiples of the angle, the transformed reduced stiffnesses. Equation (2.85), can be written as... [Pg.85]

For each of the failure criteria, we will generate biaxial stresses by off-axis loading of a unidirectionally reinforced lamina. That is, the uniaxial off-axis stress at 0 to the fibers is transformed into biaxial stresses in the principal material coordinates as shown in Figure 2-35. From the stress-transformation equations in Figure 2-35, a uniaxial loading obviously cannot produce a state of mixed tension and compression in principal material coordinates. Thus, some other loading state must be applied to test any failure criterion against a condition of mixed tension and compression. [Pg.105]

Finally, for the off-axis composite material example of this section, substitution of the stress-transformation equations. [Pg.110]

Discuss wfhether this relation is valid for anisotropic materials. That is, denwistrate whether a a angle-ply laminate of the same anisotropic laminae that are symmetric geometrically is antisymmetric or not. The transformation equations for anisotropic materials are given in Section 2.7. [Pg.222]

The topic of invariant transformed reduced stiffnesses of orthotropic and anisotropic laminae was introduced in Section 2.7. There, the rearrangement of stiffness transformation equations by Tsai and Pagano [7-16 and 7-17] was shown to be quite advantageous. In particular, certain invariant components of the lamina stiffnesses become apparent and are heipful in determining how the iamina stiffnesses change with transformation to non-principal material directions that are essential for a laminate. [Pg.440]

Table 7-7 Transformation Equations for A,j (After Tsai and Pagano [7-17])... Table 7-7 Transformation Equations for A,j (After Tsai and Pagano [7-17])...
The reactions of fluorinated esters and amides to form, respectively, enol ethers [47] and enamines [4S] give high yields and are interesting synthetic transformations (equations 34 and 35) (Table 12)... [Pg.633]

A change of variables, from qi, pi ) to ( Qi, Pi ), is called a canonical transformation, if the transformed equations of motion have the same form as that given in equation 4,36, but with H = H( Qi, Pi )- In particular, if there exists a canonical transformation such that % = H Pi,P2,.., F ) only, then the equations... [Pg.188]

Recovery of Galilean Invariance There is a simple trick that is often used to transform equation 9.107 into the conventional Navier-Stokes equations. [Pg.501]

Solution Transform Equation (8.38) using the dimensionless independent variables = z/L and = y/Y ... [Pg.286]

Additional complications with regard to recognition of an insertion reaction may arise if the acyl produced defies isolation by undergoing a further transformation. Equations (17)-(19) 78, 134, 115) provide diversified examples of such behavior (the postulated CO insertion intermediates are enclosed in brackets). The intermediacy of acyl complexes in these reactions can sometimes be inferred through examination of the infrared or NMR spectra of reaction solutions. In a number of cases, however. [Pg.93]

Our next objective is to find the analytical forms for these simultaneous eigenfunctions. For that purpose, it is more convenient to express the operators Lx, Ly, Zz, and P in spherical polar coordinates r, 6, q> rather than in cartesian coordinates x, y, z. The relationships between r, 6, q> and x, y, z are shown in Figure 5.1. The transformation equations are... [Pg.138]

Equation (6.12) cannot be solved analytically when expressed in the cartesian coordinates x, y, z, but can be solved when expressed in spherical polar coordinates r, 6, cp, by means of the transformation equations (5.29). The laplacian operator in spherical polar coordinates is given by equation (A.61) and may be obtained by substituting equations (5.30) into (6.9b) to yield... [Pg.160]

As we have discussed in Chapter 8, this is a typical transformably linear system. Using the well-known Lineweaver-Burk transformation. Equation 17.2 becomes... [Pg.324]

If instead we use the Eadie-Hofstee transformation, Equation 17.2 becomes... [Pg.325]

The initial conditions are CD = CD(0) at t = 0 and CR = 0 at t = 0. Efforts to obtain analytical solutions are tedious and unnecessary. By applying the change in concentrations (or mass) in the donor and receiver solutions with time to the Laplace transforms of Eqs. (140) and (141), the inverse of the simultaneous transformed equations can be numerically calculated with appropriate software for best estimates of a, (3, and y. It is implicit here that P Pap, Pbh and Ke are functions of protein binding. Upon application of the transmonolayer flux model to the PNU-78,517 data in Figure 32, the effective permeability coefficients from the disappearance and appearance kinetics points of view are in good quantitative agreement with the permeability coefficients determined from independent studies involving uptake kinetics by MDCK cell monolayers cultured on a flat dish... [Pg.324]

Three steps are necessary to transform Equation 18 into an... [Pg.495]

It is seen that t can be 100 s and higher at vi0 = 10 10mol L 1 s 1 and less. When the period r is longer than the time of reactor heating, one can take it into account and transform Equation (4.33) into the following form ... [Pg.205]

Treatment of 1-pyridinium sulphonate with sodium or potassium hydroxide generates sodium or potassium salts of 5-hydroxy-2,4-pentadienal (glutaconaldehyde), which are starting materials for a variety of transformations (equation 178)171b 301. For example, the reaction of the potassium salt with a carbon electrophile has been used for the preparation of a dienol aldehyde (equation 179)mb which was an intermediate in the total synthesis of a mutagen, (S)-3-(dodeca-l,3,5,7,9-pentaenyloxy)propane-l,2-diol. [Pg.460]


See other pages where Equation Transformation is mentioned: [Pg.100]    [Pg.17]    [Pg.453]    [Pg.40]    [Pg.242]    [Pg.74]    [Pg.87]    [Pg.87]    [Pg.108]    [Pg.132]    [Pg.742]    [Pg.687]    [Pg.171]    [Pg.436]    [Pg.363]    [Pg.742]    [Pg.315]    [Pg.138]    [Pg.502]    [Pg.158]    [Pg.29]    [Pg.121]    [Pg.34]   
See also in sourсe #XX -- [ Pg.63 ]

See also in sourсe #XX -- [ Pg.63 ]




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Adiabatic-to-diabatic transformation equation

Balance equation of a transformation

Boltzmann equation Fourier transform

Classification methods and transformation of equations

Differential equations Laplace transform solution

Differential equations, Laplace transform

Differential equations, Laplace transform technique

Differential equations, solution with Laplace transforms

Diffusion equation Laplace transforms

Dilation equation transforms

Discretising the Transformed Equation

Distribution equations transformations

Equation Laplace transform

Fokker-Planck to Schrodinger Equation Transformation

Foldy-Wouthuysen Transformation of the Breit Equation

Fourier transform equation

Fourier transform of the free Dirac equation

Fundamental equation for the transformed Gibbs energy

Galilean transformation motion equations

Gibbs fundamental equation Legendre transformation

LaPlace transformation equation

Laplace Transform Technique for Partial Differential Equations (PDEs) in Finite Domains

Laplace transform Kramers equation

Laplace transform technique equations

Laplace transform technique for partial differential equations

Laplace transform technique ordinary differential equations

Laplace transform technique partial differential equations

Laplace transforms in solving differential equations

Laplace transforms, kinetic equations

Laplace transforms, kinetic equations solution

Legendre transforms Gibbs-Duhem equation

Legendre transforms internal energy equation

Master equations Laplace transform

Maxwell equations Fourier transform

Michaelis-Menten equation transformations

Moment Transformation of the Population Balance Equation

Navier-Stokes equation Fourier-transformed

Normalization transformation equations

Overall Rate of Transformation Johnson-Mehl and Avrami Equations

Partial differential equation similarity transformations

Partial differential equations Fourier transform

Partial differential equations Laplace transform

Partial differential equations standard Laplace transforms

Plane polar coordinates transformation equations

Poisson equations transformation

Population balance, equation moment transformation

Sieves transformation equations

Similarity transform equation

Similarity-transformed equation of motion

Similarity-transformed equation of motion coupled cluster

Solution of Differential Equations with Laplace Transforms

Solving First-Order Differential Equations Using Laplace Transforms

Stochastic differential equations Laplace transforms

Stochastic differential equations transformation

The transformed Dirac equation

Transformation Equations for Elastic Constants

Transformation equations for the

Transformation of the Model Equations

Transformation of the Plate Theory Elution Equation from Poisson to Gaussian Form

Transformation of the equations

Transformations of the Michaelis-Menten equation

Transformed Dirac Equation

Transformed Equations

Transformed equation-of-motion

Transforming the Hartree-Fock equation

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