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Path Approach

Morison (1984) and Vassialidis (1993) developed sequential model solution and optimisation strategy which is commonly known as Feasible Path Approach. [Pg.135]

In this approach, the ODE or DAE process models are discretised into a set of algebraic equations (AEs) using collocation or other suitable methods and are solved simultaneously with the optimisation problem. Application of the collocation techniques to ODEs or DAEs results in a large system of algebraic equations which appear as constraints in the optimisation problem. This approach results in a large sparse optimisation problem. [Pg.135]

Cuthrell and Biegler (1987) and Renfro et al. (1987) developed dynamic optimisation methods based on the infeasible path approach. The main advantage of this approach is that it avoids repetitive simulations during iteration of the [Pg.135]

Chen (1988) provided detailed accounts on feasible and infeasible path approaches in optimisation. [Pg.136]

Nonlinear Programming (NLP) Based Dynamic Optimisation Problem-Feasible Path Approach [Pg.136]


Related to the previous method, a simulation scheme was recently derived from the Onsager-Machlup action that combines atomistic simulations with a reaction path approach ([Oleander and Elber 1996]). Here, time steps up to 100 times larger than in standard molecular dynamics simulations were used to produce approximate trajectories by the following equations of motion ... [Pg.74]

Since most compressors operate along a polytropic path approaching the adiabatic, compressor calculations are generally based on the adiabatic cui ve. [Pg.915]

Note that the funnel requirement is attenuated to the degree that the path approaches reversibility. Actually for a reversible path, the phase spaces of successive states along the path will be almost identical (cf. Fig. 6.1b). [Pg.210]

An example of a Gaussian distribution pair is shown in Fig. 6.9. As the switching path approaches reversibility, f(W) and g(W) becomes closer to each other and their variance decreases. Both the bias and variance of the free energy estimate also decrease. Finally, at reversibility, the two distributions coincide at x IF = AA, and converge at a single point (x = AA, f(x) = g(x) = 1), as predicted from the second law of thermodynamics. [Pg.225]

Elber, R. Meller, J. Olender, R., Stochastic path approach to compute atomically detailed trajectories application to the folding of C peptide, J. Phys. Chem. B 1999, 103, 899-911... [Pg.319]

Fig. 26.2. Kinetic reaction of quartz and cristobalite with water at 25 °C. In calculation A the fluid is originally in equilibrium with quartz, in B with cristobalite. The top diagram shows how the SiChlaq) concentration varies with time, and the bottom plot shows the change in quartz saturation. The reaction paths approach a steady state in which the fluid... Fig. 26.2. Kinetic reaction of quartz and cristobalite with water at 25 °C. In calculation A the fluid is originally in equilibrium with quartz, in B with cristobalite. The top diagram shows how the SiChlaq) concentration varies with time, and the bottom plot shows the change in quartz saturation. The reaction paths approach a steady state in which the fluid...
A feasible path optimization approach can be very expensive because an iterative calculation is required to solve the undetermined model. A more efficient way is to use an unfeasible path approach to solve the NLP problem however, many of these large-scale NLP methods are only efficient in solving problems with few degrees of freedom. A decoupled SQP method was proposed by Tjoa and Biegler (1991) that is based on a globally convergent SQP method. [Pg.187]

For a molecule at RTP this is of the order of a few hundred molecular diameters. In our ideal gas there is a distribution of velocities of the molecules about a mean value c. The mean free path defines a length scale in gases. As the density of the gas is increased and the mean free path approaches the molecular dimensions, a short-range molecular order develops and the material condenses to a liquid. The diffusional length scale is now much shorter range as a molecule encounters its... [Pg.99]

Using this nonlinear programming approach (also termed the embedded model or feasible path approach), we denote as x the vector of parameters representing l/(t) as well as the parameters x. For example, if U t) is assumed piecewise constant over a variable distance, we include w, and t in x. Problem... [Pg.218]

The distinction between reversible and irreversible work is one of the most important in thermodynamics. We shall first illustrate this distinction by means of a specific numerical example, in which a specified system undergoes a certain change of state by three distinct paths approaching the idealized reversible limit. Later, we introduce a formal definition for reversible work that summarizes and generalizes what has been learned from the path dependence in the three cases. In each case, we shall evaluate the integrated work w 2 from the basic path integral,... [Pg.71]

In this section the application of the optimal path approach to the problem of escape from a nonhyperbolic and from a quasihyperbolic attractor is examined. We discuss these two different types of chaotic attractor because it is known [160] that noise does not change very much the structure and properties of quasi-hyperbolic attractors, but that the structure of non-hyperbolic attractors is abruptly changed in the presence of noise, with a strong dependence on noise intensity. Note that for optical systems both types of chaotic attractor [161-163] (nonhyperbolic and quasihyperbolic) are observed, but a nonhyperbolic attractor is much more typical. [Pg.501]

In this approach, the process variables are partitioned into dependent variables and independent variables (optimisation variables). For each choice of the optimisation variables (sometimes referred to as decision variables in the literature) the simulator (model solver) is used to converge the process model equations (described by a set of ODEs or DAEs). Therefore, the method includes two levels. The first level performs the simulation to converge all the equality constraints and to satisfy the inequality constraints and the second level performs the optimisation. The resulting optimisation problem is thus an unconstrained nonlinear optimisation problem or a constrained optimisation problem with simple bounds for the associated optimisation variables plus any interior or terminal point constraints (e.g. the amount and purity of the product at the end of a cut). Figure 5.2 describes the solution strategy using the feasible path approach. [Pg.135]

NLP Based Dynamic Optimisation Problem- Infeasible Path Approach... [Pg.139]

The quantitized classical path approach (Hwang and Warshel, 1996) was applied to the analysis of quantum mechanical nuclear motion in enzyme catalysis. According to this approach the rate constant of the process... [Pg.58]

Fig. 11.1. Heatup path for S02, 02, N2 gas descending a catalyst bed. The S02 and 02 in feed gas react to form S03, Eqn. (1.1). The gas is heated by the exothermic heat of reaction. The result is a path with increasing % S02 oxidized and increasing gas temperature. Notice how the feed gas s heatup path approaches its Chapter 10 equilibrium curve. Fig. 11.1. Heatup path for S02, 02, N2 gas descending a catalyst bed. The S02 and 02 in feed gas react to form S03, Eqn. (1.1). The gas is heated by the exothermic heat of reaction. The result is a path with increasing % S02 oxidized and increasing gas temperature. Notice how the feed gas s heatup path approaches its Chapter 10 equilibrium curve.

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