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Convergence block

Figure 6 shows how the 5-representability is attained. Thus it can be seen from this hgure that the ofi Gaa fifi/spin-block converges very satisfactorily on a positive/negative semidehnite matrix. After twenty iterations the lowest/highest eigenvalue of these two matrices is —0.00010 and 0.00022, respectively. As was mentioned in Section II, these conditions are much more exacting than the well-known G-condition. [Pg.240]

Shown in Figure 7 is the comparison of the predicted resonance positions (3-channel-block converged results) for the six potentials considered. We notice that the results are sensitive to the potential energy surfaces used. In particular, the line widths predicted... [Pg.276]

For each iteration of the control block, converge only the units between the specified and adjusted variables solve the entire flowsheet after the adjust variable is converged. [Pg.1340]

The adaptive estimation of the pseudo-inverse parameters a n) consists of the blocks C and E (Fig. 1) if the transformed noise ( ) has unknown properties. Bloek C performes the restoration of the posterior PDD function w a,n) from the data a (n) + (n). It includes methods and algorithms for the PDD function restoration from empirical data [8] which are based on empirical averaging. Beeause the noise is assumed to be a stationary process with zero mean value and the image parameters are constant, the PDD function w(a,n) converges, at least, to the real distribution. The posterior PDD funetion is used to built a back loop to block B and as a direct input for the estimator E. For the given estimation criteria f(a,d) an optimal estimation a (n) can be found from the expression... [Pg.123]

Figure Bl.23.2. (a) Shadow cone of a stationary Pt atom in a 4 keV Ne ion beam, appearing with the overlapping of ion trajectories as a fiinction of the impact parameter. The initial position of the target atom that recoils in the collision is indicated by a solid circle, (b) Plot of the nonnalized ion flux distribution density across the shadow cone in (a). The flux density changes from 0 inside the shadow cone, to much greater than l in the focusing region, converging to 1 away from the shadow cone edge, (c) Blocking cones... Figure Bl.23.2. (a) Shadow cone of a stationary Pt atom in a 4 keV Ne ion beam, appearing with the overlapping of ion trajectories as a fiinction of the impact parameter. The initial position of the target atom that recoils in the collision is indicated by a solid circle, (b) Plot of the nonnalized ion flux distribution density across the shadow cone in (a). The flux density changes from 0 inside the shadow cone, to much greater than l in the focusing region, converging to 1 away from the shadow cone edge, (c) Blocking cones...
Note Because of its neglect of off-diagonal blocks, this optimizer can sometimes oscillate and fail to converge. In this case, use a conjugate gradicn t method. [Pg.60]

Earhest simulators determined the sequence of the calculations for the vatious unit operations from the expHcit iaput from the engineer or from the sequeace ia which the topological information about unit operations was entered. AH simulators today analyze the topology automatically and determine the sequence. Most of them, however, allow the user to alter this sequence through various techniques of creating hypothetical calculation units of convergence, recycle, and control blocks or units. [Pg.73]

Most flow sheets have one or mote recycles, and trial-and-ettot becomes necessary for the calculation of material and energy balances. The calculations in a block sequential simulator ate repeated in this trial-and-ettot process. In the language of numerical analysis, this is known as convergence of the calculations. There ate mathematical techniques for speeding up this trial-and-ettot process, and special hypothetical calculation units called convergence, or recycle, units ate used in calculation flow diagrams that invoke special calculation routines. [Pg.73]

Penicilloic acid 5, the substrate for the projected lactamization reaction, could be derived from the suitably protected intermediate 6. Retrosynthetic disassembly of 6, in the manner illustrated, provides D-penicillamine hydrochloride (7) and tert-butyl phthalimido-malonaldehydate (8) as potential building blocks. In the synthetic direction, it is conceivable that the thiol and amino groupings in 7 could be induced to converge upon the electrophilic aldehyde carbonyl in 8 to give thiazolidine 6 after loss of a molecule of water. [Pg.45]

Compound 16, the projected precursor of 15, could conceivably be assembled from bishomoallylic alcohol 17 via a pathway that features the oxidative functionalization of the A20,21 double bond with participation by the C-17 secondary hydroxyl. Compound 17 is an attractive retrosynthetic precursor for compound 16 because the A20-21 double bond, which could permit the introduction of the adjacent C-20 and C-21 stereocenters in 16, provides a convenient opportunity for significant molecular simplification. Thus, retrosynthetic cleavage of the A20 21 double bond in 17 furnishes compounds 18 and 19 as potential building blocks. The convergent union of the latter two compounds through a Wittig reaction would be expected to afford 17 stereoselectively. [Pg.193]

In another important class of cases, the matrix A is positive definite. When this is so, both the Gauss-Seidel iteration and block relaxation converge, but the Jacobi iteration may or may not. [Pg.61]


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See also in sourсe #XX -- [ Pg.516 ]




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