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Configuration, of systems

We have now defined a d-SoC for a given individual as a unique configuration of system of... [Pg.39]

In thermodynamics we are generally interested in stable or most stable configurations of systems, corresponding to lowest energy positions. According to the calculus, an extremum (maximum or minimum) is attained when... [Pg.93]

FIGURE 75.1 The Elemental Resource Model contains multiple hierarchical levels. Performance resources (i.e., the basic elements) at the basic element level are finite in number, as dictated by the finite set of human subsystems and the finite set of their respective dimensions of performance. At higher levels, new systems can be readily created by configuration of systems at the basic element level. Consequently, there are in infinite number of performance resources (i.e., higher-level elements) at these levels. However, rules of General Systems Performance Theory (refer to text) are applied at any level in the same way resulting in the identification of the system, its function, dimensions of performance, performance resource availabilities (system attributes), and performance resource demands (task attributes). [Pg.1229]

The role of the different parameters controlling the Ewald summation will now be considered in more detail. A single equilibrium configuration of System IV with Nm = 80 macroions will be used, but the outcome does not critically depend on the choice of system or configuration. Values of the potential energy for different truncations of the Ewald summation will be compared with essentially the exact value, the latter obtained from an Ewald siunmation with large values of J cut and cut. [Pg.144]

Fig. 13 Absolute truncation error of the reduced potential energy of the Ewald summation as a function of a the potential energy tolerance Si i/NkT at a = O.iR- and b a at 8toi/NkT = 2.5 X 10 with Rcat and cut evaluated using Eqs. 21 and 21 and the same equilibrium configuration of System IV as in Fig. 12 (symbols). The corresponding estimated truncation errors of the real-space and reciprocal-space terms of the reduced potential energy according to Eqs. 21 and 22, respectively (solid curves), and the values of Ucut are also shown... Fig. 13 Absolute truncation error of the reduced potential energy of the Ewald summation as a function of a the potential energy tolerance Si i/NkT at a = O.iR- and b a at 8toi/NkT = 2.5 X 10 with Rcat and cut evaluated using Eqs. 21 and 21 and the same equilibrium configuration of System IV as in Fig. 12 (symbols). The corresponding estimated truncation errors of the real-space and reciprocal-space terms of the reduced potential energy according to Eqs. 21 and 22, respectively (solid curves), and the values of Ucut are also shown...
MC simulations generate equilibrium configurations stochastically according to the probabilities rigorously known from statistical mechanics. Because it generates equilibrium states directly, one can use it to study the equilibrium configurations of systems that may be expensive or impossible to access via MD. The drawback of MC is that it cannot yield the kind of dynamic response information that leads directly to transport properties. [Pg.8]

A system state is the physical configuration of system hardware and software. Hardware and/or software are configured in a certain manner in order to perform a particular mode. A system state characterizes the particular physical configuration at any point in time. States identify conditions in which a system or subsystem can exist. A system or subsystem may be in only one state at a time. There is a connection between modes and states in that for every operational mode, there is one or more states the system can be in. For example, a stopwatch is a system that typically has modes such as on, off, timing, and reset. The on mode may go into the initialization state, which requires the initialization software package. [Pg.261]

Fig. 9.12 Typical configurations of systems of 50 chains of length N =50 grafted on a line at linear density (a) pm = 0.38, (b) 3.14, (c) 6.28 in a good solvent. The chains are projected on the plane perpendieular to the grafting lines. Note that these are not star polymers. (Results are from Ref. 104.)... Fig. 9.12 Typical configurations of systems of 50 chains of length N =50 grafted on a line at linear density (a) pm = 0.38, (b) 3.14, (c) 6.28 in a good solvent. The chains are projected on the plane perpendieular to the grafting lines. Note that these are not star polymers. (Results are from Ref. 104.)...

See other pages where Configuration, of systems is mentioned: [Pg.75]    [Pg.62]    [Pg.56]    [Pg.112]    [Pg.43]    [Pg.76]    [Pg.78]    [Pg.146]    [Pg.146]    [Pg.9]    [Pg.1062]    [Pg.107]   
See also in sourсe #XX -- [ Pg.9 ]




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