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Quadratic first function

Another limitation is perhaps not so much a limitation as, perhaps, a strange characteristic, albeit one that can catch the unwary. To demonstrate, we consider the simplest S-G derivative function, that for the first derivative using a 5-point quadratic fitting function. The convolution coefficients (after including the normalization factor) are... [Pg.364]

Index 7-point smoothing with quartic fitting function 5-point first derivative with cubic fitting function 5-point second derivative, quadratic fitting function... [Pg.377]

For comparison 2, we find one case five-point first derivative versus five-point second derivative, both using a quadratic fitting function. Here again, the noise multiplier increased with increasing derivative order. [Pg.377]

First, let us consider the perfectly scaled quadratic objective function /(x) = x + x, whose contours are concentric circles as shown in Figure 6.6. Suppose we calculate the gradient at the point xT = [2 2]... [Pg.191]

LP software includes two related but fundamentally different kinds of programs. The first is solver software, which takes data specifying an LP or MILP as input, solves it, and returns the results. Solver software may contain one or more algorithms (simplex and interior point LP solvers and branch-and-bound methods for MILPs, which call an LP solver many times). Some LP solvers also include facilities for solving some types of nonlinear problems, usually quadratic programming problems (quadratic objective function, linear constraints see Section 8.3), or separable nonlinear problems, in which the objective or some constraint functions are a sum of nonlinear functions, each of a single variable, such as... [Pg.243]

The quadratic response function is obtained as the third derivative of the time-averaged quasi-energy. The program is then to expand the energy to third order in the first-order parameters ... [Pg.176]

Mikkelsen reviews recent advances of the MCSCF/MM method. This approach has been developed in order to obtain frequency-dependent molecular properties for a solute perturbed by solvent interactions. He defines the Hamiltonian for the total system. It involves three components the first describes the quantum mechanical (QM) system, the second, the classical (MM) system and the third their interaction. He describes the energy functional, the MCSCF wave function and the linear and quadratic response functions. [Pg.687]

At the moment of writing very few implementations of the theory of molecular properties at the 4-component relativistic molecular level, beyond expectation values at the closed-shell Hartree-Fock level, have been reported. The first implementation of the linear response function at the RPA level in a molecular code appears to be to MO-based module reported by Visscher et al. [97]. Quiney and co-workers [98] have reported the calculation of second-order properties at the uncoupled Hartree-Fock level (see section 5.3 for terminology). Saue and Jensen [99] have reported an AO-driven implementation of the linear response function at the RPA level and this work has been extended to quadratic response functions by Norman and Jensen [100]. Linear response functions at the DFT/LDA-level have been reported by Saue and Helgaker [101]. In this section we will review the calculation of linear and quadratic response functions at the closed-shell 4-component relativistic Hartree-Fock level. We will follow the approach of Saue and Jensen [99] where the reader is referred for further details. [Pg.379]

In the following sections we will derive the first order response of the wave function as well as the linear and quadratic response functions at the Hartree-Fock level using the above parameterization. The results may be compared with those for exact states obtained using Rayleigh-Schrbdinger perturbation theory in section 2.2. Alternatively, the results of that section may be rederived using the exponential parameterization (203) replacing k t) by... [Pg.383]

We see that the evaluation of the quadratic response function involves the contraction of the third derivative tensor with respect to Hq with three first order response vectors as well as the contraction of three property Hessians with two response vectors. The daggers appearing in the above expression determines... [Pg.391]

The quadratic response function is imaginary. In the static case to = 0 the quadratic response function is zero, as there are then no anti-Hermitian contribution to the first order response vectors. [Pg.393]

It can be seen that the evaluation of the quadratic response function involves the one-index transformation of various Fock-like matrices generated in the determination of the first order response of the wave function as well as the generation of the (two-electron) Fock-matrix with modified density. [Pg.393]

The final classification involved a hierarchy of quadratic discriminant functions (QDFs). The first hierarchical level separated the six fuels into three fuel-groups (oil coal series oil shale/Czech black coal), whilst the second hierarchical level used separate QDFs to separate each fuel group into its component fuel-types. Some fuel separations proved to be very good with oil, oil shale, Czech black coal and brown coal being 94.1%, 89.3%, 86.0% and 84.1% correctly allocated to their fuel-types, respectively. The coal-series and, in particular peat and coal, showed considerable overlap and were less effectively separated. In total, of those particles allocated to a fuel-type, over 80% were allocated correctly. [Pg.340]

Figure 11 Effect of reactant consumption on the stability ofa first-order exothermic reaction, heat loss (a) against reciprocal adiabatic flame temperature (B ). Curve (a). Adler-Enig temperature-concentration inflection criterion curve (b) Bowes-Thomas temperature-time inflection criterion curve (c) Gray-Sherrington quadratic Uapunov function curve (d). Frank-Kamenetskii s empirical criterion (the curves show a )... Figure 11 Effect of reactant consumption on the stability ofa first-order exothermic reaction, heat loss (a) against reciprocal adiabatic flame temperature (B ). Curve (a). Adler-Enig temperature-concentration inflection criterion curve (b) Bowes-Thomas temperature-time inflection criterion curve (c) Gray-Sherrington quadratic Uapunov function curve (d). Frank-Kamenetskii s empirical criterion (the curves show a )...
There exist circumstances that sometimes facilitate the search. In fact the Hamiltonians appearing in mechanics and physics are usually quadratic (bilinear) functions. Therefore one should first examine the linear subspace of quadratic functions contained in a commutative Lie algebra V. As a rule, this examination is rather simple, and we will demonstrate it on concrete examples. [Pg.189]

The second-order steady drift force is derived directly from the first-order potential. Therefore, the steady drift force is computed by the pressure-area method within the linear diffraction/radiation program. The low or high frequency force calculations are much more complex in terms of a quadratic transfer function, which is extremely time-consuming. In order to reduce the computation effort for routine application in a design, simplified assumptions are often applied using fewer frequency pairs around the resonance frequency. This type of approximation is a common design practice. [Pg.679]

Quadratic response function in the adiabatic four-component Kohn-Sham approximation has been formulated and implemented by Henriksson et al Applications to dihalosubstituted benzenes illustrate the significance of this work to describe heavy atom effects on the polarizability and first hyperpolarizability. In particular, using the CAM-B3LYP XC functional, relativity reduces the EFISHG nP response by 62% and 75% for meta- and urt/ju-dibromobenzene, and enhances the same response by 17% and 21% for meta- and or/ o-diiodobenzene, respectively. Moreover, these results have further evidenced that correlation and relativistic effects are not additive. [Pg.24]

The first electric dipole hyperpolarizability, given by the quadratic response function... [Pg.383]

Including these first-order corrections to the ground- and excited-state wave functions in the expression for the dipole transition moment, we find that the first-order nonvanishing contribution to the dipole transition moment between a singlet and a triplet state may be written in terms of a residue of a quadratic response function (Olsen and Jorgensen 1995 Vahtras et al. 1992a) ... [Pg.426]

For MPC based on linear process models, both linear and quadratic objective functions can be used (Maciejowski, 2002 Qin and Badgwell, 2003). To demonstrate the MPC control calculations, consider a quadratic objective function J based on the first two types of deviations ... [Pg.397]


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See also in sourсe #XX -- [ Pg.421 ]




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