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Inverse interpolation

There are many large molecules whose mteractions we have little hope of detemiining in detail. In these cases we turn to models based on simple mathematical representations of the interaction potential with empirically detemiined parameters. Even for smaller molecules where a detailed interaction potential has been obtained by an ab initio calculation or by a numerical inversion of experimental data, it is usefid to fit the calculated points to a functional fomi which then serves as a computationally inexpensive interpolation and extrapolation tool for use in fiirtlier work such as molecular simulation studies or predictive scattering computations. There are a very large number of such models in use, and only a small sample is considered here. The most frequently used simple spherical models are described in section Al.5.5.1 and some of the more common elaborate models are discussed in section A 1.5.5.2. section Al.5.5.3 and section Al.5.5.4. [Pg.204]

The described direct derivation of shape functions by the formulation and solution of algebraic equations in terms of nodal coordinates and nodal degrees of freedom is tedious and becomes impractical for higher-order elements. Furthermore, the existence of a solution for these equations (i.e. existence of an inverse for the coefficients matrix in them) is only guaranteed if the elemental interpolations are based on complete polynomials. Important families of useful finite elements do not provide interpolation models that correspond to complete polynomial expansions. Therefore, in practice, indirect methods are employed to derive the shape functions associated with the elements that belong to these families. [Pg.25]

When three-point interpolation fails to yield a convergent calculation, you can request a second accelerator for any SCFcalculation via the Semi-empirical Options dialog box and the Ab Initio Options dialog box. This alternative method. Direct Inversion in the Iterative Subspace (DIIS), was developed by Peter Pulay [P. Pulay, Chem. Phys. Lett., 73, 393 (1980) J. Comp. Chem., 3, 556(1982)]. DIIS relies on the fact that the eigenvectors of the density and Fock matrices are identical at self-consistency. At SCF convergence, the following condition exists... [Pg.230]

Interpolated from Vukalovich and Altunin s interpolation of data of Price, Ind. Eng. Chem., 47, 1691 (1955). Tl = lower inversion temperature, and Tu = upper inversion temperature. [Pg.178]

In analytical practice, fitting a model to data is only the first step in analogy to Eq. (2.19) an interpolation that uses y to estimate X(y ) is necessary. For many functional relationships y = f(x) finding an inverse, x=f (y), is difficult enough without confidence limits such a result is nearly worthless. [Pg.129]

The friction factor per base pair y for rotation of DNA around its symmetry axis was determined from FPA studies of restriction fragments containing N+ 1 =43 and 69 bp.(109) Both fragments are sufficiently short that a substantial amplitude of C (t), and also F (t), resides in their Uniform Mode Zones. Particular values of certain parameters were assumed, namely, the rise per base pair h = 3.4 A, the hydrodynamic radius b = 12 A for transverse motion in Eqs. (4.43)-(4.47) (which are quite insensitive to b), and D, = 1.8 x 106 s-1 for 43 bp and D = 4.8 x 105 s for 69 bp. The latter values were extrapolated or interpolated from the data of Elias and Eden using an inverse cubic relation between DL and L. They are close to the values calculated using the theory of Tirado and Garcia de la Torre.(129)... [Pg.176]

The DFT representation, however, allows a more convenient and faster interpolation of periodic data. To see how this can be, we shall write a few terms of the inverse DFT, which is a discrete Fourier series ... [Pg.274]

The abundances of krypton and xenon are determined exclusively from nucleosynthesis theory. They can be interpolated from the abundances of neighboring elements based on the observation that abundances of odd-mass-number nuclides vary smoothly with increasing mass numbers (Suess and Urey, 1956). The regular behavior of the s-process also provides a constraint (see Chapter 3). In a mature -process, the relative abundances of the stable nuclides are governed by the inverse of their neutron-capture cross-sections. Isotopes with large cross-sections have low abundance because they are easily destroyed, while the abundances of those with small cross-sections build up. Thus, one can estimate the abundances of krypton and xenon from the abundances of. v-only isotopes of neighboring elements (selenium, bromine, rubidium and strontium for krypton tellurium, iodine, cesium, and barium for xenon). [Pg.102]

As it will be discussed, while three maxima of the first derivative are observed, the second one is a consequence of the applied numerical method. Using the second derivative values in the last column, local inverse linear interpolation gives V = 3.74 ml and V = 7.13 ml for the two equivalence points. We will see later on how the false end point can be eliminated. [Pg.234]

Using inverse linear interpolation the two titration equivalence points are obtained as the zero-crossing points of the second derivative at V = 3.78 ml and V = 7.14 ml. On Fig. 4.4 the second derivative curve of the interpolating spline (SD = ) and that of the smoothing spline (SD = 8.25) are shown. The false zero-crossing of the second derivative present at interpolation is eliminated by smoothing. [Pg.245]

Interpolation and smoothing by addition of zeros. We may need to add zeros to the sample simply in order to obtain 2 1 points. The addition of zeros, however, also increases the length of the observation interval [0,T], and hence the number of frequences in the discrete spectrum. Smoothing the spectrum by an appropriate window and applying the inverse transformation then results in an... [Pg.253]

In the limit of very large viscosity, such as the one observed near the glass transition temperature, it is expected that rate of isomerization will ultimately go to zero. It is shown here that in this limit the barrier crossing dynamics itself becomes irrelevant and the Grote-Hynes theory continues to give a rate close to the transition theory result. However, there is no paradox or difficulty here. The existing theories already predict an interpolation scheme that can explain the crossover to inverse viscosity dependence of the rate... [Pg.183]

According to Kramers treatment, the proportionality of the Kramers rate to tj in the low viscosity limit turns over to the inverse proportionality in the high viscosity. The interpolating behavior for arbitrary rj was studied by Mel nikov and Meshkov [104]. [Pg.247]

A big advantage of this type of interpolation is that the matrices in the linear system of equations of coefficients,always have an inverse. A drawback is that in order to obtain the coefficients of the interpolation, we must solve very large systems of equations with full matrices. The most common radial functions are... [Pg.358]

This allows us to represent partial differential equations as found in the balance equations using the collocation method. Equation (11.47) is a solution to a partial differential equation represented by a system of linear algebraic equations, formed by the interpolation coefficients, oij, and the operated radial functions. The interpolation coefficients are solved for using matrix inversion techniques to approximately satisfy the partial differential equation... [Pg.569]

A method similar to the iterative, is the partial closure method [37], It was formulated originally as an approximated extrapolation of the iterative method at infinite number of iterations. A subsequent more general formulation has shown that it is equivalent to use a truncated Taylor expansion with respect to the nondiagonal part of T instead of T-1 in the inversion method. An interpolation of two sets of charges obtained at two consecutive levels of truncations (e.g. to the third and fourth order) accelerates the convergence rate of the power series [38], This method is no longer in use, because it has shown serious numerical problems with CPCM and IEFPCM. [Pg.61]

The interpolated gradient vector is p = p GDIIS algorithm, a currently updated estimate of the inverse Hessian is used to estimate a coordinate step based on these interpolated vectors. This gives... [Pg.31]


See other pages where Inverse interpolation is mentioned: [Pg.748]    [Pg.592]    [Pg.748]    [Pg.592]    [Pg.2337]    [Pg.2337]    [Pg.2340]    [Pg.452]    [Pg.751]    [Pg.335]    [Pg.370]    [Pg.176]    [Pg.303]    [Pg.427]    [Pg.53]    [Pg.308]    [Pg.84]    [Pg.218]    [Pg.61]    [Pg.104]    [Pg.274]    [Pg.138]    [Pg.228]    [Pg.241]    [Pg.52]    [Pg.30]    [Pg.90]    [Pg.375]    [Pg.105]    [Pg.256]   
See also in sourсe #XX -- [ Pg.13 , Pg.14 , Pg.16 , Pg.20 ]




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Inverse Rational Interpolation Method

Linear inverse interpolation

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