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What Converges

There is an apparent contradiction which has been swept under the carpet in the previous few chapters. [Pg.115]


The development of an SC procedure involves a number of important decisions (1) What variables should be used (2) What equations should be used (3) How should variables be ordered (4) How should equations be ordered (5) How should flexibility in specifications be provided (6) Which derivatives of physical properties should be retained (7) How should equations be linearized (8) If Newton or quasi-Newton hnearization techniques are employed, how should the Jacobian be updated (9) Should corrections to unknowns that are computed at each iteration be modified to dampen or accelerate the solution or be kept within certain bounds (10) What convergence criterion should be applied ... [Pg.1286]

Gas liquid equilibria calculations at 1500 psia and 160°F have been completed for a black oil. Resulting compositions are given below. A convergence pressure of 5000 psia was used to obtain K-factors. What convergence pressure should have been used for this mixture at 160°F ... [Pg.411]

The above discussion represents a necessarily brief simnnary of the aspects of chemical reaction dynamics. The theoretical focus of tliis field is concerned with the development of accurate potential energy surfaces and the calculation of scattering dynamics on these surfaces. Experimentally, much effort has been devoted to developing complementary asymptotic techniques for product characterization and frequency- and time-resolved teclmiques to study transition-state spectroscopy and dynamics. It is instructive to see what can be accomplished with all of these capabilities. Of all the benclunark reactions mentioned in section A3.7.2. the reaction F + H2 —> HE + H represents the best example of how theory and experiment can converge to yield a fairly complete picture of the dynamics of a chemical reaction. Thus, the remainder of this chapter focuses on this reaction as a case study in reaction dynamics. [Pg.875]

Another option is a q,p) = p and b q,p) = VU q). This guarantees that we are discretizing a pure index-2 DAE for which A is well-defined. But for this choice we observed severe difficulties with Newton s method, where a step-size smaller even than what is required by explicit methods is needed to obtain convergence. In fact, it can be shown that when the linear harmonic oscillator is cast into such a projected DAE, the linearized problem can easily become unstable for k > . Another way is to check the conditions of the Newton-Kantorovich Theorem, which guarantees convergence of the Newton method. These conditions are also found to be satisfied only for a very small step size k, if is small. [Pg.285]

If the yield of each step is again 90%, what is the overall yield of this five step convergent synthesis ... [Pg.101]

After a number of iterations, the energy from one iteration may be the same as from the previous iteration. This is what chemists desire a converged solution. [Pg.193]

The solution oftheRHForUHFequationsisan iterative procedure with two principal issues. First is the question of what to use for an initial guess and second, whether the solutions will converge quickly or at all. The initial guess affects the convergence also, as an exact guess would immediately converge. [Pg.229]

The rate of flow of water in a 150 mm diameter pipe is measured with a venturi meter with a 50 mm diameter throat. When the pressure drop over the converging section is 121 mm of water, the flowrate is 2.91 kg/s. What is the coefficient for the converging cone of the meter at this flowrate ... [Pg.256]

The generality of a simple power series ansatz and an open-ended formulation of the dispersion formulas facilitate an alternative approach to the calculation of dispersion curves for hyperpolarizabilities complementary to the point-wise calculation of the frequency-dependent property. In particular, if dispersion curves are needed over a wide range of frequencies and for several optical proccesses, the calculation of the dispersion coefficients can provide a cost-efficient alternative to repeated calculations for different optical proccesses and different frequencies. The open-ended formulation allows to investigate the convergence of the dispersion expansion and to reduce the truncation error to what is considered tolerable. [Pg.114]

These results have converged to four decimal places. The output required about 2 s on what will undoubtedly be a slow PC by the time you read this. [Pg.43]

Figure 1.21. Monte Carlo simulation of six groups of eight normally distributed measurements each raw data are depicted as x,- vs. i (top) the mean (gaps) and its upper and lower confidence limits (full lines, middle) the confidence limits CL(s ) of the standard deviation converge toward a = 1 (bottom, Eq. 1.42). The vertical divisions are in units of 1 a. The CL are clipped to +5a resp. 0. .. 5ct for better overview. Case A shows the expected behavior, that is for every increase in n the CL(x,nean) bracket /r = 0 and the CL(i t) bracket a - 1. Cases B, C, and D illustrate the rather frequent occurrence of the CL not bracketing either ii and/or ff, cf. Case B n = 5. In Case C the low initial value (arrow ) makes Xmean low and Sx high from the beginning. In Case D the 7 measurement makes both Cl n = 7 widen relative to the n 6 situation. Case F depicts what happens when the same measurements as in Case E are clipped by the DVM. Figure 1.21. Monte Carlo simulation of six groups of eight normally distributed measurements each raw data are depicted as x,- vs. i (top) the mean (gaps) and its upper and lower confidence limits (full lines, middle) the confidence limits CL(s ) of the standard deviation converge toward a = 1 (bottom, Eq. 1.42). The vertical divisions are in units of 1 a. The CL are clipped to +5a resp. 0. .. 5ct for better overview. Case A shows the expected behavior, that is for every increase in n the CL(x,nean) bracket /r = 0 and the CL(i t) bracket a - 1. Cases B, C, and D illustrate the rather frequent occurrence of the CL not bracketing either ii and/or ff, cf. Case B n = 5. In Case C the low initial value (arrow ) makes Xmean low and Sx high from the beginning. In Case D the 7 measurement makes both Cl n = 7 widen relative to the n 6 situation. Case F depicts what happens when the same measurements as in Case E are clipped by the DVM.
Purpose Illustrate what happens when a series of measurements is evaluated for mean and standard deviation each time a new determination becomes available the mean converges towards zero and the SD towards 1.0. The CL(Xmean) and the CL(i c) normally enclose the expected values E x) = /r = 0, respectively E Sx) = a =. Due to the stochastic nature of the measured signal, it can happen that confidence limits do not bracket the expected value this fact is highlighted by a bold line. [Pg.366]

In what follows stability of differential schemes will be given special investigation irrelevant to approximation and convergence. [Pg.390]

For cr = 1 the maximum principle is in full force for any r and h, due to which the resulting scheme is uniformly stable with respect to the initial data and the right-hand side. What is more, the uniform convergence occurs with the rate 0(r - - h ). [Pg.498]

Where would you make the first disconnection to devise a convergent synthesis for (14), whose epoxide is the cecropia juvenile hormone What reaction and what starting materials might you use ... [Pg.478]

Although the minimization of the objective function might run to convergence problems for different NN structures (such as backpropagation for multilayer perceptrons), here we will assume that step 3 of the NN algorithm unambiguously produces the best, unique model, g(x). The question we would like to address is what properties this model inherits from the NN algorithm and the specific choices that are forced. [Pg.170]


See other pages where What Converges is mentioned: [Pg.115]    [Pg.116]    [Pg.118]    [Pg.115]    [Pg.116]    [Pg.118]    [Pg.256]    [Pg.2335]    [Pg.229]    [Pg.188]    [Pg.351]    [Pg.150]    [Pg.253]    [Pg.164]    [Pg.165]    [Pg.245]    [Pg.508]    [Pg.32]    [Pg.113]    [Pg.163]    [Pg.29]    [Pg.106]    [Pg.245]    [Pg.75]    [Pg.43]    [Pg.377]    [Pg.741]    [Pg.125]    [Pg.756]    [Pg.128]    [Pg.220]    [Pg.81]    [Pg.178]   


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