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Space scales, multiple

Errors and confusion in modelling arise because the complex set of coupled, nonlinear, partial differential equations are not usually an exact representation of the physical system. As examples, first consider the input parameters, such as chemical rate constants or diffusion coefficients. These input quantities, used as submodels in the detailed model, must be derived from more fundamental theories, models or experiments. They are usually not known to any appreciable accuracy and often their values are simply guesses. Or consider the geometry used in a calculation. It is often one or two dimensions less than needed to completely describe the real system. Multidimensional effects which may be important are either crudely approximated or ignored. This lack of exact correspondence between the model adopted and the actual physical system constitutes the basic problem of detailed modelling. This problem, which must be overcome in order to accurately model transient combustion systems, can be analyzed in terms of the multiple time scales, multiple space scales, geometric complexity, and physical complexity of the systems to be modelled. [Pg.333]

Input Errors. Errors in model input often constitute one of the most significant causes of discrepancies between observed data and model predictions. As shown in Figure 2, the natural system receives the "true" input (usually as a "driving function") whereas the model receives the "observed" input as detected by some measurement method or device. Whenever a measurement is made possible source of error is introduced. System inputs usually vary continuously both in space and time, whereas measurements are usually point values, or averages of multiple point values, and for a particular time or accumulated over a time period. Although continuous measurement devices are in common use, errors are still possible, and essentially all models require transformation of a continuous record into discrete time and space scales acceptable to the model formulation and structure. [Pg.157]

Y.L. Bai et al Statistical mesomechanics of solid, linking coupled multiple space and time scales. App. Mech. Rev. 58, 372-388 (2005)... [Pg.131]

We believe that devising a way to handle this difficult problem of strongly coupled multiple time and space scales is the challenge we currently face. [Pg.354]

The analysis of multiple-time-scale systems can, however, be carried out by extending the methods used for analyzing two-time-scale systems presented in Section 2.2. In analogy with two-time-scale systems, in the limiting case as e —> 0, the dimension of the state space of the system in Equations (B.l) collapses... [Pg.229]

Note that this method ultimately leads to a set of state-space realizations for the reduced-order models for each time scale of a multiple-time-scale system, but does not identify the slow and fast variables associated with the individual... [Pg.234]

Now we will see how this simple fact can be used to our advantage, to help alleviate the multiple time scales problem. Let us concentrate on an atomic system molecules can be treated by a simple extension of this approach [41]. Subdividing the space allows us to treat the electrons as... [Pg.59]

We continue in the ensuing chapters with several tutorials tied together by the theme of how to exploit and/or treat multiple length scales and multiple time scales in simulations. In Chapter 5 Thomas Beck introduces us to real-space and multigrid methods used in computational chemistry. Real-space methods are iterative numerical techniques for solving partial differential equations on grids in coordinate space. They are used because the physical responses from many chemical systems are restricted to localized domains in space. This is a situation that real-space methods can exploit because the iterative updates of the desired functions need information in only a small area near the updated point. [Pg.550]

Usually refers to a method of solving Newton s equations of classical mechanics numerically, in order to propagate the positions and velocities of a system of molecules forward in time and thus to explore the phase space of the system. See Molecular Dynamics and Hybrid Monte Carlo in Systems with Multiple Time Scales and Long-range Forces Reference System Propagator Algorithms Molecular Dynamics DMA Molecular Dynamics Simulations of Nucleic Acids Molecular Dynamics Studies of Lipid Bilayers and Molecular Dynamics Techniques and Applications to Proteins. [Pg.1614]

Systems in which problems of multiple time scales and of "bottlenecks in phase space" occur are hardly exceptional, and promising methods of theory and discrete-event simulation have been developed recently in several important areas. In a marriage of molecular dynamics (and Monte Carlo methods) to transition state theory (2 j, for example, Bennett (22J has developed a general simulation method for treating arbitrarily infrequent dynamical events (e.g., an enzyme-catalyzed reaction process). [Pg.233]

Dust Separation It is usuaUy necessaiy to recover the solids carried by the gas leaving the disengaging space or freeboard of the fluidized becl GeneraUy, cyclones are used to remove the major portion of these sohds (see Gas-Sohds Separation ). However, in a few cases, usuaUy on small-scale units, filters are employed without the use of cyclones to reduce the loading of solids in the gas. For high-temperature usage, either porous ceramic or sintered metal has been employed. Multiple units must be provided so that one unit can be blown back with clean gas while one or more are filtering. [Pg.1570]

The scaling function, (f)(x), has either local support or decays very fast to zero. For all practical purposes, it is a local function. By translating and dilating that function we are able to cover the entire input space in multiple resolutions, as it is required. [Pg.184]


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Multiple scales

Space scales

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