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Random simulations

The greater number of folds in larger proteomes is intuitively obvious simply because the functioning of more complex organisms is expected to require a greater structural diversity of proteins. From a different perspective, the increase of diversity follows from a stochastic model, which describes a proteome as a finite sample from an infinite pool of proteins with a particular distribution of fold fractions ( a bag of proteins ). A previous random simulation analysis suggested that the stochastic model significantly (about twofold) underestimates the number of different folds in the proteomes (Wolf et al., 1999). In other words, the structural diversity of real proteomes does not seem to follow... [Pg.268]

The mathematical model called diffusion-limited aggregation (DLA) was introduced by Witten and Sander in 1981 [46]. The model starts with a particle at the origin of a lattice. Another particle is allowed to walk at random (simulating Brownian motion) until it arrives at a site adjacent to the seed particle. At each time step, the traveling particle moves from one site to... [Pg.541]

Random Simulated Simulated Random Simulated Simulated Simulated... [Pg.594]

We wish to introduce next a topic of increasing importance to chemical engineers, stochastic (random) simulation. In stochastic models we simulate quite directly the random nature of the molecules. We will see that the deterministic rate laws and material balances presented in the previous sections can be captured in the stochastic approach by allowing the numbers of molecules in the simulation to become large. From this viewpoint, deterministic and stochastic approaches are complementary. Deterministic models and solution methods are quite efficient when the numbers of molecules are large and the random behavior is not important. The numerical methods for solution of the nonlinear differential equations of the deterministic models are... [Pg.97]

Perform several random simulations of the vims mode given in Equations 4.95 4.102. Perform enough simulations so that some of your trajectories lead to extinction of all three species cccDNA, rcDNA and envelope protein. [Pg.107]

In the hybrid intelligent algorithm, population size = 100, crossover probability Pc = 0.6, mutation probability = 0.5, number of iterations Gmax = 20,000, rank-based evaluation function a = 0.05 and there are 3000 random simulation. The main frequency of the PC for calculating is 2400 MHz, and all the algorithm program is realized by C++ language. [Pg.82]

Gmax = 16,000, in the rank-based evaluation function a = 0.05, and 3000 random simulations. Figure 4.7 shows the convergence process of the objective function of the example. Table 4.27 shows the objective function values at each stage and total profits of the supply chain. [Pg.84]

One example is fliermodynamics. The purely macroscopic theory is highly abstract and inaccessible. The statistical microscopic flieory is more easily interpreted, but seems to require difficult statistical arguments. Thirty years ago, in Nuffield Advanced Physics, we found a way through these difficulties, using random simulations. [Pg.62]

We have described a safety validation approach for SAA algorithms using multi-agent simulation and evolutionary search. Through experiments we have shown that our approach can reveal faults that random simulation takes a long time to find, and thus that our approach may accelerate the safety vaUdation process. In the process, we found some safety issues with the SVO algorithm. [Pg.47]

Table 1. The distribution function R(v, n) for the 3x3x3 Ising lattice. Each column gives the distribution of the number cf nearest neighbor contacts (g) for 2000 lattices generated by random simulation for a given value of the number of sites in state 2 (v). Zero s indicate conformations which are possible but which were not generated blank positions conformations which are not realizable... Table 1. The distribution function R(v, n) for the 3x3x3 Ising lattice. Each column gives the distribution of the number cf nearest neighbor contacts (g) for 2000 lattices generated by random simulation for a given value of the number of sites in state 2 (v). Zero s indicate conformations which are possible but which were not generated blank positions conformations which are not realizable...
Fig. 3.2 Random simulation of the switching of N molecules between two states A and B. The number of molecules in state A is plotted with blue, and the number of molecules in B is plotted with red. The plots in panels (a), (b), and (c) correspond to = 10, 100, 1,000 respectively... Fig. 3.2 Random simulation of the switching of N molecules between two states A and B. The number of molecules in state A is plotted with blue, and the number of molecules in B is plotted with red. The plots in panels (a), (b), and (c) correspond to = 10, 100, 1,000 respectively...

See other pages where Random simulations is mentioned: [Pg.188]    [Pg.26]    [Pg.102]    [Pg.416]    [Pg.6]    [Pg.98]    [Pg.131]    [Pg.194]    [Pg.3056]    [Pg.184]    [Pg.927]    [Pg.951]    [Pg.34]    [Pg.241]    [Pg.257]   
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