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Optimization iterative

Fig. 2.6. Evolutionary design of biopolymers in selection cycles. Properties of biomolecules, for example binding to a target or catalytic function, are optimized iteratively through selection cycles. Each cycle consists of three phases (i) amplification, (ii) diversification by replication with problem adjusted error rates (or random synthesis), and (iii) selection. Amplification and di-... Fig. 2.6. Evolutionary design of biopolymers in selection cycles. Properties of biomolecules, for example binding to a target or catalytic function, are optimized iteratively through selection cycles. Each cycle consists of three phases (i) amplification, (ii) diversification by replication with problem adjusted error rates (or random synthesis), and (iii) selection. Amplification and di-...
The plots of maximum temperature experienced within the composite in the die, the mean DOC as a function of the number of optimization iterations for these parameters are shown in Fig. 12.5 (Joshi et /.,2003). [Pg.395]

A trial-and-error statistical procedure is used to optimize the correlation between MTD and potency. One e assignment is changed at a time, and a new equation fitted. If the new equation has a higher statistical significance, the corresponding map is retained and subjected to further optimization iterations until no improvement can be made. This way the best map S is found. Because... [Pg.201]

Table 3. Number of training samples, parameters, and the resulting objective values for each of the adaptive optimization iteration steps. Table 3. Number of training samples, parameters, and the resulting objective values for each of the adaptive optimization iteration steps.
For the iteration algorithm (5) the optimal estimations (6) are directly used by a second back loop to block B (long dashed line in Fig. 1). [Pg.123]

A novel optimization approach based on the Newton-Kantorovich iterative scheme applied to the Riccati equation describing the reflection from the inhomogeneous half-space was proposed recently [7]. The method works well with complicated highly contrasted dielectric profiles and retains stability with respect to the noise in the input data. However, this algorithm like others needs the measurement data to be given in a broad frequency band. In this work, the method is improved to be valid for the input data obtained in an essentially restricted frequency band, i.e. when both low and high frequency data are not available. This... [Pg.127]

In many cases, the methods used to solve identification problems are based on an iterative minimization of some performance criterion measuring the dissimilarity between the experimental and the synthetic data (generated by the current estimate of the direct model). In our case, direct quantitative comparison of two Bscan images at the pixels level is a very difficult task and involves the solution of a very difficult optimization problem, which can be also ill-behaved. Moreover, it would lead to a tremendous amount of computational burden. Segmented Bscan images may be used as concentrated representations of the useful... [Pg.172]

In simple relaxation (the fixed approximate Hessian method), the step does not depend on the iteration history. More sophisticated optimization teclmiques use infonnation gathered during previous steps to improve the estimate of the minunizer, usually by invoking a quadratic model of the energy surface. These methods can be divided into two classes variable metric methods and interpolation methods. [Pg.2336]

Csaszar P and Pulay P 1984 Geometry optimization by direct inversion in the iterative subspace J. Moi. Struct. (Theochem) 114 31... [Pg.2356]

Hamilton T P and Pulay P 1986 Direct Inversion In the Iterative subspace (DNS) optimization of open-shell, excited-state and small multiconfiguratlonal SCF wavefunctlons J. Chem. Phys. 84 5728... [Pg.2357]

After an initial starting geometry has been generated and optimized (e.g., in a force field), the new conformation is compared with all the previously generated conformations, which are usually stored as a list of unique conformations. If a substantially different geometry is detected it is added to the list otherwise, it is rejected. Then a new initial structure is generated for the next iteration. Finally, a preset stop criterion, e.g., that a given number of loops has been performed or that no new conformations can be found, terminates the procedure. [Pg.105]

A transition structure is, of course, a maximum on the reaction pathway. One well-defined reaction path is the least energy or intrinsic reaction path (IRC). Quasi-Newton methods oscillate around the IRC path from one iteration to the next. Several researchers have proposed methods for obtaining the IRC path from the quasi-Newton optimization based on this observation. [Pg.154]


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