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Computation of the Integral

To compute we use the stationary point method. Using the inequality [Pg.291]

ImlifTs 0 and the asymptotic expressions of the spherical Hankel functions of the first kind [Pg.291]

To evaluate we pass to cylindrical coordinates, integrate over [Pg.291]


Computation of the Integrals Required for the Estimated Effects and the ANOVA Decomposition... [Pg.324]

Here, the expansion expressed in equation (4.4) with the functions defined as in equation (5.1) are needed in order to perform the computation of the integral (6.27), and one can write ... [Pg.204]

The computation of the integral molar entropy of adsorption at any coverage requires knowledge of the adsorption isotherm " = "(p) at a given temperature combined with the calorimetric isotherm Q = Q" (p). We must emphasize the fact that Q is measured by definition under reversible conditions. Therefore, when applying Eq. (48) to experimental data, the quasireversibility of the process must be verified. [Pg.161]

Practical computation of the integral (1) becomes computationally expensive when the involved density functions correspond to large molecules or have been calculated at high computational levels. Even concrete applications of MQSM have been carried out at the ab initio level, when several molecules are studied simultaneously, as in QSAR studies, MQSM need to be computed several times, preventing their usage at these stages. In order to overcome this problem, the promolecular atomic shell approximation (PASA) [34-38] has been defined as a model of the true ab initio density, devised as a linear combination of 15 functions, and mathematically expressed as ... [Pg.371]

View factors of many other simple cases may be found in a similar manner. More complicated cases, however, including all of the enclosures of Fig. 9.6, when they have a finite depth, require the use of Eq. (9.10). Computation of the integrals involved with. Eq. (9.10) will be illustrated here in terms of an example. [Pg.436]

Note how fast our computation of the integrals proceeds. The main job (zero or not zero—that is the question) is done by the group theory. [Pg.745]

The parallelization of a molecular quantum chemical code is at least in parts trivial. Especially the computation of the integrals (matrix elements)... [Pg.94]

Table 1 The Ratio of the Standard Deviation to the Average Time (a /p ), for the Computation of the Integrals in a Shell Quartet (for the Water Dimer) and Typical Values of the Average Effective Flop Counts (mi/K)... Table 1 The Ratio of the Standard Deviation to the Average Time (a /p ), for the Computation of the Integrals in a Shell Quartet (for the Water Dimer) and Typical Values of the Average Effective Flop Counts (mi/K)...
The principal part of the integral is taken and the integration must be done over all frequencies. In practice, the integration is often tenninated outside of the frequency range of interest. Once the frill dielectric fiinction is known, the reflectivity of the solid can be computed. [Pg.119]

Enforcing the molecular symmetry will also help orbital-based calculations run more quickly. This is because some of the integrals are equivalent by symmetry and thus need be computed only once and used several times. [Pg.75]

Computation of the overlap integrals in the atomic orbital basis set. [Pg.269]

Analysis of neutron data in terms of models that include lipid center-of-mass diffusion in a cylinder has led to estimates of the amplitudes of the lateral and out-of-plane motion and their corresponding diffusion constants. It is important to keep in mind that these diffusion constants are not derived from a Brownian dynamics model and are therefore not comparable to diffusion constants computed from simulations via the Einstein relation. Our comparison in the previous section of the Lorentzian line widths from simulation and neutron data has provided a direct, model-independent assessment of the integrity of the time scales of the dynamic processes predicted by the simulation. We estimate the amplimdes within the cylindrical diffusion model, i.e., the length (twice the out-of-plane amplitude) L and the radius (in-plane amplitude) R of the cylinder, respectively, as follows ... [Pg.488]


See other pages where Computation of the Integral is mentioned: [Pg.332]    [Pg.40]    [Pg.161]    [Pg.332]    [Pg.127]    [Pg.96]    [Pg.191]    [Pg.21]    [Pg.154]    [Pg.289]    [Pg.291]    [Pg.292]    [Pg.332]    [Pg.40]    [Pg.161]    [Pg.332]    [Pg.127]    [Pg.96]    [Pg.191]    [Pg.21]    [Pg.154]    [Pg.289]    [Pg.291]    [Pg.292]    [Pg.157]    [Pg.144]    [Pg.79]    [Pg.230]    [Pg.244]    [Pg.271]    [Pg.421]    [Pg.479]    [Pg.138]    [Pg.139]    [Pg.38]    [Pg.79]    [Pg.626]    [Pg.157]    [Pg.162]    [Pg.331]    [Pg.123]    [Pg.122]    [Pg.77]    [Pg.77]    [Pg.79]    [Pg.27]    [Pg.299]   


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Computer, the

Computing integrator

Integrity of the

The Integral

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