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Basis functions node-based

Optimization of the PPR model is based on minimizing the mean-squares error approximation, as in back propagation networks and as shown in Table I. The projection directions a, basis functions 6, and regression coefficients /3 are optimized, one at a time for each node, while keeping all other parameters constant. New nodes are added to approximate the residual output error. The parameters of previously added nodes are optimized further by backfitting, and the previously fitted parameters are adjusted by cyclically minimizing the overall mean-squares error of the residuals, so that the overall error is further minimized. [Pg.39]

Fig. 4.6. Control points and Q nodes used to reconstruct A. The Qi basis function is a bilinear function equal to 1 at a Q node and zero at the surrounding Qi nodes. Four control points per cell were used. The derivatives of A were evaluated at each control point using a linear interpolation based on the neighboring data points... Fig. 4.6. Control points and Q nodes used to reconstruct A. The Qi basis function is a bilinear function equal to 1 at a Q node and zero at the surrounding Qi nodes. Four control points per cell were used. The derivatives of A were evaluated at each control point using a linear interpolation based on the neighboring data points...
Afterwards an update to the mesh deformation module is presented, which enables to represent the exact deflections for every CFD surface grid node, which are delivered by the coupling matrix. Performance limitations do not allow to use all points as input for the basic radial-basis-function based mesh deformation method. Then the FSI-loop to compute the static elastic equilibrium is described and the application to an industrial model is presented. Finally, a strategy how to couple and deflect control smfaces is shown. Therefore, a possible gapless representation by means of different coupling domains and a chimera-mesh representation is shown. This section describes the bricks, which are combined to a fluid-structure interaction loop. Most of the tools are part of the FlowSimulator software environment (Fig. 20.11). [Pg.591]

Given the set of x and y values for the nodes in the network, the allowable connections and the pipe diameter, d, (chosen from a discrete set) allocated to each possible connection, the evaluation of the objective function is based on identifying all the matches defined by the positions of the lines in the discrete space. This evaluation is deterministic and enables the identification of the network layout and the direct evaluation of the cost of the water distribution network. This objective function forms the basis of a discrete optimization problem in x, y, and d. [Pg.120]

Radial basis functions networks are good function approximation and classification as backpropagation networks but require much less time to train and don t have as critical local minima or connection weight freezing (sometimes called network paralysis) problems. Radial basis fimction CNNs are also known to be universal approximators and provide a convenient measure of the reliability and confidence of its output (based on the density of training data). In addition, the functional equivalence of these networks with fuzzy inference systems have shown that the membership functions within a rule are equivalent to Gaussian functions with the same variance (o ) and the munber of receptive field nodes is equivalent to the number of fuzzy if-then rules. [Pg.29]

Approximate linear dependence of AO-based sets is always a numerical problem, especially in 3D extended systems. Slater functions are no exceptions. We studied and recommended the use of mixed Slater/plane-wave (AO-PW) basis sets [15]. It offers a good compromise of local accuracy (nuclear cusps can be correctly described), global flexibility (nodes in /ik) outside primitive unit cell can be correct) and reduced PW expansion lengths. It seems also beneficial for GW calculations that need low-lying excited bands (not available with AO bases), yet limited numbers of PWs. Computationally the AOs and PWs mix perfectly mixed AO-PW matrix elements are even easier to calculate than those involving AO-AO combinations. [Pg.43]


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