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Metropolis Monte Carlo quantities

In general, Monte Carlo simulations are such calculations in which the values of some parameters are determined by the average of some randomly generated individuals.45-54 In chemistry applications, the most prevalent methods are the so called Metropolis Monte Carlo (MMC)55 and Reverse Monte Carlo (RMC) ones. The most important quantities in these methods are some kinds of U energy-type potentials (e.g. internal energy, enthalpy,... [Pg.182]

Another procedure to overcome the inefficiency of Metropolis Monte Carlo is adaptive importance sampling.194-196 In this technique, the partition function (and quantities derived from it, such as the probability of a given conformation) is evaluated by continually upgrading the distribution function (ultimately to the Boltzmann distribution) to concentrate the sampling in the region (s) where the probabilities are highest. [Pg.110]

Figure 6. Typical results of Metropolis-Monte Carlo calculations on the dependence on the number of straight segments per Kuhn length, k, of a mean quantity (the mean writhing number, Wr, see Section 4.3.2.1, in the particular case) for closed polymer chain. The data are from Vologodskii and Frank-Kamenetskii (1992) [81]. Figure 6. Typical results of Metropolis-Monte Carlo calculations on the dependence on the number of straight segments per Kuhn length, k, of a mean quantity (the mean writhing number, Wr, see Section 4.3.2.1, in the particular case) for closed polymer chain. The data are from Vologodskii and Frank-Kamenetskii (1992) [81].
Another simulation approach often used that does not offer a simple deterministic time evolution of the system is the Metropolis Monte Carlo [MMC] method. Based on the Metropolis-Hasting algorithm [3, 4], MMC methods are weighted sampling techniques in which particles are randomly moved about to obtain a statistical ensemble of atoms with a particular probability distribution for some quantity. This is usually the energy but can also be other quantities such as experimental inputs that can be quickly calculated from an atomic... [Pg.145]

These particular quantities were calculated for system of 108 particles using the Molecular Dynamics technique (Hentschke et al.), but Metropolis Monte Carlo could have used instead. [Pg.228]

In Chapters 3, 6 and 7, the two equivalent descriptions of Brownian motion the Langevin and Smoluchowski equations for an entanglement-free system have been studied in the cases where analytic solutions are obtainable the time-correlation function of the end-to-end vector of a Rouse chain and the constitutive equation of the Rouse model. When the Brownian motion of a more complicated model is to be studied, where an analytical solution cannot be obtained, the Monte Carlo simulation becomes a useful tool. Unlike the Monte Carlo simulation that is employed to calculate static properties using the Metropolis criterion, the simulation based on the Langevin equation can be used to calculate both static and dynamic quantities. [Pg.341]

The specific method devised by Metropolis et al to compute the properties of liquids is now known as the Monte Carlo (MC) method. In fact, this is a special procedure to compute multidimensional integrals numerically. Consider the computation of any average quantity, say in the T, V, N ensemble ... [Pg.296]

The steady-state dynamics is assumed to be governed by a Kawasaki-type particle-vacancy NN pair-exchange mechanism inside the system combined with a Glauber-type particle creation/annihilation mechanism at the two edges A and B. Hence, neither the particle number nor the total energy are conserved quantities. This implementation corresponds to a canonical ensemble inside the lattice and a grand canonical ensemble at the edges. The total density is hence a dependent variable which has to be calculated. The dynamical processes are subject to the conventional Monte Carlo Metropolis criterion. ... [Pg.344]

The Monte Carlo method, referred in this entry as Direct Monte Carlo (DMC), is a statistical sampling technique that has been originally developed by Stan Ulam, John von Neumann, Nick Metropolis (who actually suggested the name Monte Carlo (Metropolis 1987)), and their collaborators for solving the problem of neutron diffusion and other problems in mathematical physics (Metropolis and Ulam 1949). From a mathematical point of view, DMC allows to estimate the expected value of a quantity of interest. More specifically, suppose the goal is to evaluate [/i(x)], that is, an expectation of a function with respect to the PDF n x). [Pg.3674]

The statistical ensemble framework of equilibrium statistical mechanics gives us the tools to analyze experimental data and to make theoretical predictions. The concept of entropy, its maximization, and the ensuing definition of intensive quantities such as pressure and temperature reduces the complexity of a statistical system of 10 particles to manageable proportions. In principle, the problem of predicting the collective behavior of equilibrium systems starting from microscopic interactions is solved. In practice, exact calculations are rarities. Computational tools such as the Monte Carlo Metropolis method can, however, fill in this void a priori knowledge of the probability distribution of microstates is at the heart of the Metropolis algorithm. [Pg.190]

Molecular dynamics (MD) and Monte Carlo (MC) simulation techniques have been used now for decades to characterize aqueous solutions. The most basic elements that underlie these techniques, such as numerical integration algorithms and the Metropolis method, are discussed thoroughly else-where, " so they are not included here. Our intention here is to survey methods used for determining the thermodynamic and structural quantities most closely tied to hydrophobicity. [Pg.46]


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