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Simulations stochastic

Next we will design a hybrid intelligent algorithm based on stochastic simulation to solve this model. [Pg.72]

Stochastic simulation, also known as Monte Carlo simulation, is a technology for system modeling which is used for random samples that obey a random distribution. Although the simulation only gives a statistic prediction rather than a precise result and is very time-consuming to be used to study problems, it is the only effective way for those complex problems [6, 9] that are impossible to find an analytic result. [Pg.72]

For uncertainty function U -. X) E F X,Pno,Wfio) in the model of this chapter, we use stochastic simulation technology to find an optimal solution within all possible range of random variable pno and Wno- [Pg.72]

The treatment for uncertainty function U2- (Y) E[G Y, Wno)] is similar to that for Up. (X). Here is the introduction of the process of the stochastic simulation of [Pg.72]

Step 4 Repeat Step 2 and Step 3 N times totally. Here N is an integer large enough  [Pg.73]


Before trying to solve the master equation for growth processes by direct stochastic simulation it is usually advisable to first try some analytical approximation. The mean-field approximation often gives very good results for questions of first-order phase transitions, and at least it provides a qualitative understanding for the interplay of the various model parameters. [Pg.864]

The relative fluctuations in Monte Carlo simulations are of the order of magnitude where N is the total number of molecules in the simulation. The observed error in kinetic simulations is about 1-2% when lO molecules are used. In the computer calculations described by Schaad, the grids of the technique shown here are replaced by computer memory, so the capacity of the memory is one limit on the maximum number of molecules. Other programs for stochastic simulation make use of different routes of calculation, and the number of molecules is not a limitation. Enzyme kinetics and very complex oscillatory reactions have been modeled. These simulations are valuable for establishing whether a postulated kinetic scheme is reasonable, for examining the appearance of extrema or induction periods, applicability of the steady-state approximation, and so on. Even the manual method is useful for such purposes. [Pg.114]

A final comment on the interpretation of stochastic simulations We are so accustomed to writing continuous functions—differential and integrated rate equations, commonly called deterministic rate equations—that our first impulse on viewing these stochastic calculations is to interpret them as approximations to the familiar continuous functions. However, we have got this the wrong way around. On a molecular level, events are discrete, not continuous. The continuous functions work so well for us only because we do experiments on veiy large numbers of molecules (typically 10 -10 ). If we could experiment with very much smaller numbers of molecules, we would find that it is the continuous functions that are approximations to the stochastic results. Gillespie has developed the stochastic theory of chemical kinetics without dependence on the deterministic rate equations. [Pg.114]

A further insight is that the best workflow depends on a combination of factors that can in many cases be expressed in closed mathematical form, allowing very rapid graphical feedback to users of what then becomes a visualization rather than a stochastic simulation tool. This particular approach is effective for simple binary comparisons of methods (e.g., use of in vitro alone vs. in silico as prefilter to in vitro). It can also be extended to evaluation of conditional sequencing for groups of compounds, using an extension of the sentinel approach [24]. [Pg.268]

Kovalyov EV, Elokhin VI, Myshlyavtsev AV. 2008. Stochastic simulation of physicochemical processes performance over supported metal nanoparticles. J Comput Chem 29 79-86. [Pg.559]

D. T. Gillespie, Exact stochastic simulation of coupled chemical reactions, J. Phys. Chem. 81, 2340 (1977). [Pg.143]

In Sect. 7.4.6, we discussed various stochastic simulation techniques that include the kinetics of recombination and free-ion yield in multiple ion-pair spurs. No further details will be presented here, but the results will be compared with available experiments. In so doing, we should remember that in the more comprehensive Monte Carlo simulations of Bartczak and Hummel (1986,1987, 1993,1997) Hummel and Bartczak, (1988) the recombination reaction is taken to be fully diffusion-controlled and that the diffusive free path distribution is frequently assumed to be rectangular, consistent with the diffusion coefficient, instead of a more realistic distribution. While the latter assumption can be justified on the basis of the central limit theorem, which guarantees a gaussian distribution for a large number of scatterings, the first assumption is only valid for low-mobility liquids. [Pg.300]

The WATS model is formulated in deterministic terms. However, an extension to include simple Monte-Carlo stochastic simulation is possible, taking into consideration a measured variability of the process parameters. [Pg.212]

Hewson, J. and A. R. Kerstein (2001). Stochastic simulation of transport and chemical kinetics in turbulent CO/H2/N2 flames. Combustion Theory and Modelling 5, 669-697. [Pg.415]

Figure 10. Stochastic simulations. In the starting structure (A) one C atom is attached to the catalyst only two events are possible propylene capture followed by the 1,2- or 2,1-insertion. For the structure B four events are taken into account isomerization to the tertiary carbon, 1,2- and 2,1-insertions, and a termination. For the structures C, D and E five events are considered two isomerizations, two insertions and a termination. The probabilities of these events are equal for the structures C and E (in both cases two different isomerizations lead to a primary or secondary carbon at the metal), and different for the structure D (for which both isomerizations lead to the structure with a secondary carbon attached to the metal). For clarity, the numbers [(1), (2), and (3)] labeling different atom types (primary, secondary, and tertiary, respectively) are shown. Figure 10. Stochastic simulations. In the starting structure (A) one C atom is attached to the catalyst only two events are possible propylene capture followed by the 1,2- or 2,1-insertion. For the structure B four events are taken into account isomerization to the tertiary carbon, 1,2- and 2,1-insertions, and a termination. For the structures C, D and E five events are considered two isomerizations, two insertions and a termination. The probabilities of these events are equal for the structures C and E (in both cases two different isomerizations lead to a primary or secondary carbon at the metal), and different for the structure D (for which both isomerizations lead to the structure with a secondary carbon attached to the metal). For clarity, the numbers [(1), (2), and (3)] labeling different atom types (primary, secondary, and tertiary, respectively) are shown.
Only deterministic models for cellular rhythms have been discussed so far. Do such models remain valid when the numbers of molecules involved are small, as may occur in cellular conditions Barkai and Leibler [127] stressed that in the presence of small amounts of mRNA or protein molecules, the effect of molecular noise on circadian rhythms may become significant and may compromise the emergence of coherent periodic oscillations. The way to assess the influence of molecular noise on circadian rhythms is to resort to stochastic simulations [127-129]. Stochastic simulations of the models schematized in Fig. 3A,B show that the dynamic behavior predicted by the corresponding deterministic equations remains valid as long as the maximum numbers of mRNA and protein molecules involved in the circadian clock mechanism are of the order of a few tens and hundreds, respectively [128]. In the presence of molecular noise, the trajectory in the phase space transforms into a cloud of points surrounding the deterministic limit cycle. [Pg.272]

Stochastic simulations confirm the existence of bifurcation values of the control parameters bounding a domain in which sustained oscillations occur. The effect of noise diminishes as the number of molecules increases. Only when the maximum numbers of molecules of mRNA and protein become smaller than a few tens does noise begin to obliterate the circadian rhythm. The robustness of circadian rhythms with respect to molecular noise is enhanced when the rate of binding of the repressor molecule to the gene promoter increases [128]. Conditions that enhance the resistance of genetic oscillators to random fluctuations have been investigated [130]. [Pg.273]

The irradiation of water is immediately followed by a period of fast chemistry, whose short-time kinetics reflects the competition between the relaxation of the nonhomogeneous spatial distributions of the radiation-induced reactants and their reactions. A variety of gamma and energetic electron experiments are available in the literature. Stochastic simulation methods have been used to model the observed short-time radiation chemical kinetics of water and the radiation chemistry of aqueous solutions of scavengers for the hydrated electron and the hydroxyl radical to provide fundamental information for use in the elucidation of more complex, complicated chemical, and biological systems found in real-world scenarios. [Pg.92]

Results of the stochastic simulations for the Lotka model are presented in Fig. 2.16. [Pg.104]

After years of experiments and the nonetheless effective use of these tools making it possible to refine and systematically optimise control of facilities, the tools due to increased performance and possibilities made available by software and other computer equipment, has been improved by increasing the calculation horizon, beyond two gas years by using adapted models (closer to classic reservoir models by taking into account a simplified physical representation). At the present stage with R D works still continuing, they now include more and more complexity (risk management, stochastic simulations, etc), and works are focused on ... [Pg.190]

Perkins MJ (1996) A radical reappraisal of Gif reactions. Chem Soc Rev 25 229-236 Phulkar S, Rao BSM, Schuchmann H-P, von Sonntag C (1990) Radiolysis of tertiary butyl hydroperoxide in aqueous solution. Reductive cleavage by the solvated electron, the hydrogen atom, and, in particular, the superoxide radical anion. Z Naturforsch 45b 1425-1432 Pimblott SM, LaVerne JA (1997) Stochastic simulation of the electron radiolysis of water and aqueous solutions. J Phys Chem A 101 5828-5838... [Pg.45]

Begusova M, Spotheim-Maurizot M, Sy D, MichalikV,Charlier M (2001b) RADACK.a stochastic simulation of hydroxyl radical attack on DNA. J Biomol Struc Dyn 19 141-158... [Pg.449]

The lowest-lying potential energy surfaces for the 0(3P) + CH2=C=CH2 reaction were theoretically characterized using CBS-QB3, RRKM statistical rate theory, and weak-collision master equation analysis using the exact stochastic simulation method. The results predicted that the electrophilic O-addition pathways on the central and terminal carbon atom are dominant up to combustion temperatures. Major predicted end-products are in agreement with experimental evidence. New H-abstraction pathways, resulting in OH and propargyl radicals, have been identified.254... [Pg.121]

The stochastic simulation technique creates 3-D realization of the non-woven carbon paper GDL based on structural inputs,... [Pg.262]

LifeLine Aggregate and cumulative stochastic Simulates daily pesticide exposures for periods from birth up to 85 years of pesticide applicators, residents of homes where pesticides are used, and the general population (dietary and tap water consumption) LifeLine Group (2005)... [Pg.138]

Doubtlessly, there are also other computational analyses to be performed in the future, such as stochastic simulations, stoichiometric network analysis, sensitivity analysis, etc. However, for this initial survey, we only take this absolute minimum into account, while listing additional features of the respective software tools. [Pg.74]

C. J. Brokaw. protein-protein ratchets stochastic simulation and application to processive enzymes. Biophys.J., 81 1333— 1344, 2001. [Pg.398]

We can, however, analyze these problems within the framework of the stochastic formulation by looking for an exact solution, or by using the probability generating functions, or the stochastic simulation algorithm. [Pg.264]

For linear systems, the differential equation for the jth cumulant function is linear and it involves terms up to the jth cumulant. The same procedure will be followed subsequently with other models to obtain analogous differential equations, which will be solved numerically if analytical solutions are not tractable. Historically, numerical methods were used to construct solutions to the master equations, but these solutions have pitfalls that include the need to approximate higher-order moments as a product of lower moments, and convergence issues [383]. What was needed was a general method that would solve this sort of problem, and that came with the stochastic simulation algorithm. [Pg.267]


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