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Integration substitution method

Substitution Method The accumulated data from a kinetic study can be substituted in the integrated form of the various equations that describe reaction orders. When the values of one of the iterations remain constant, the reaction is considered to be of that order. [Pg.690]

Apply the integration by parts and substitution methods to integrate more complicated functions... [Pg.120]

In practice, we may find ourselves faced with more complicated functions, the solutions to which require us to use methods involving adaptation of some of the rules for differentiation. The choice of method more often than not involves some guesswork, but coming up with the correct guesses is all part of the fun In addition, it may be necessary to use a combination of several methods. In the following two sections, we discuss integration by parts and the substitution method... [Pg.128]

The second integration technique, known as the substitution method, derives from the inversion of the chain rule for differentiation described in Chapter 4. The objective here, once again, is to transform the integrand into a simpler or, preferably, a standard form. However, just like the integration by parts method, there is usually a choice of substitutions and although, in some cases, different substitutions yield different answers, these answers must only differ by a constant (remember that, for an indefinite integral, the answer is determined by inclusion of a constant). The substitution method is best illustrated using a worked problem. [Pg.129]

Note that within the framework of the integral equation method, the vectors E (r ) are still unknown and have to be determined by the solution of the corresponding equations. Substituting expansion (9.189) into the right-hand side of formula (9.180), we arrive at the discrete form of the operator equation ... [Pg.272]

There are a number of other methods which may be used to obtain approximate wave functions and energy levels. Five of these, a generalized perturbation method, the Wentzel-Kramers-Brillouin method, the method of numerical integration, the method of difference equations, and an approximate second-order perturbation treatment, are discussed in the following sections. Another method which has been of some importance is based on the polynomial method used in Section 11a to solve the harmonic oscillator equation. Only under special circumstances does the substitution of a series for 4 lead to a two-term recursion formula for the coefficients, but a technique has been developed which permits the computation of approximate energy levels for low-lying states even when a three-term recursion formula is obtained. We shall discuss this method briefly in Section 42c. [Pg.191]

Cross-enyne metathesis has also been applied to solid-phase synthesis by immobilizing either the alkyne or the alkene (498,499). By combination with a Diels-Alder reaction, this process has been used to create a combinatorial library of various six-membered ring structures (500). Within this theme, intermolecular enyne metathesis is the integral synthetic method used to produce novel amino acid derivatives (501, 502). To this end, the aromatic ring of highly substituted phenylalanines was synthesized through enyne crossmetathesis and cycloaddition. [Pg.427]

The convergence radius of the substitution method is similar to the one required for stability in an explicit method and is related to the product of the integration step and the maximum eigenvalue of the Jacobian. [Pg.108]

Thus, even though the implicit method adopted is very stable and allows a very large integration step, we are still forced to strongly reduce the integration step to prevent the substitution method from diverging. [Pg.108]

This is no longer true for the substitution method that converges only when the integration step is small for stiff problems, independent of the accuracy of the prediction. [Pg.109]

Obviously, the integration step influences the accuracy of the algorithm used for the integration of the system in both the cases of the substitution method and the Newton method for calculating the correction b. [Pg.109]

Adaptations of this method have been proposed in order to take into account the band displacement due either to substitution on the aromatic ring, or to chains of different lengths. The variations consist, instead of measuring the absorbance at maximum absorption, of an integration of the absorbance curve over a specified range (Oelert s method, 1971). More exact, this method is used less often mainly because the Brandes method is simpler... [Pg.61]

The use of selectively reduced integration to obtain accurate non-trivial solutions for incompressible flow problems by the continuous penalty method is not robust and failure may occur. An alternative method called the discrete penalty technique was therefore developed. In this technique separate discretizations for the equation of motion and the penalty relationship (3.6) are first obtained and then the pressure in the equation of motion is substituted using these discretized forms. Finite elements used in conjunction with the discrete penalty scheme must provide appropriate interpolation orders for velocity and pressure to satisfy the BB condition. This is in contrast to the continuous penalty method in which the satisfaction of the stability condition is achieved indirectly through... [Pg.76]

The problem of electrophilic substitution into the anilinium ion has been examined by the methods of m.o. theory. Attempts to simulate the --inductive effect in Hiickel M.o. theory by varying the Coulomb integral of C(j) (the carbon atom to which the NH3+ group is attached) remove 7r-electrons from the o- and -positions and add them to the... [Pg.174]

The Galerldn finite element method results when the Galerldn method is combined with a finite element trial function. The domain is divided into elements separated by nodes, as in the finite difference method. The solution is approximated by a linear (or sometimes quadratic) function of position within the element. These approximations are substituted into Eq. (3-76) to provide the Galerldn finite element equations. The element integrals are defined as... [Pg.477]

The hydrauhc diameter method does not work well for laminar flow because the shape affects the flow resistance in a way that cannot be expressed as a function only of the ratio of cross-sectional area to wetted perimeter. For some shapes, the Navier-Stokes equations have been integrated to yield relations between flow rate and pressure drop. These relations may be expressed in terms of equivalent diameters Dg defined to make the relations reduce to the second form of the Hagen-Poiseulle equation, Eq. (6-36) that is, Dg (l2SQ[LL/ KAPy. Equivalent diameters are not the same as hydraulie diameters. Equivalent diameters yield the correct relation between flow rate and pressure drop when substituted into Eq. (6-36), but not Eq. (6-35) because V Q/(tiDe/4). Equivalent diameter Dg is not to be used in the friction factor and Reynolds number ... [Pg.638]

After substituting (2.3) and (2.4) for (2.1), the integral can be evaluated with the method of steepest descents. The stationary point E = E is given by the equation derived by Miller and George [1972]... [Pg.12]

By de ult, Gaussian will substitute the in-core method for direct SCF when there is enough memory because it is fester. When we ran these computations, we explicitly prevented Gaussian from using the in-core method. When you run your jobs, however, the in-core method will undoubtedly be used for some jobs, and so your values may differ. An in-core job is identified by the following line in the output Two-electron integrals will be kept in memory. [Pg.31]

The CNDO method has been modified by substitution of semiempirical Coulomb integrals similar to those used in the Pariser-Parr-Pople method, and by the introduction of a new empirical parameter to differentiate resonance integrals between a orbitals and tt orbitals. The CNDO method with this change in parameterization is extended to the calculation of electronic spectra and applied to the isoelectronic compounds benzene, pyridine, pyri-dazine, pyrimidine and pyrazine. The results obtained were refined by a limited Cl calculation, and compared with the best available experimental data. It was found that the agreement was quite satisfactory for both the n TT and n tt singlet transitions. The relative energies of the tt and the lone pair orbitals in pyridine and the diazines are compared and an explanation proposed for the observed orders. Also, the nature of the lone pairs in these compounds is discussed. [Pg.150]

Values of Vm as a function of p are computed from an equation of state, substituted into equation (6.15). and numerically integrated. In principle, this method can be used to calculate o for any well-behaved equation of state. (It is essentially the method used at the beginning of this section to obtain from the m-BWR equation.)... [Pg.257]


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