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Minimum necessary condition

Table 6 shows the minimum pasteurization conditions required by the USDA. It is necessary to pasteurize all egg products under these conditions, except for egg white which is to be dried. [Pg.459]

These are only necessary conditions, as point ti may be a minimum, maximum, or saddle point. [Pg.484]

We now regard the experimental data as fixed and treat the model parameters as the variables. The goal is to choose C, w, n, and r such that > Q achieves its minimum possible value. A necessary condition for to be a minimum is that... [Pg.256]

The necessary conditions for k to be the optimal parameter values corresponding to a minimum of the augmented objective function SLo(k,a)) are given by Edgar and Himmelblau (1988) and Gill et al. (1981) and are briefly presented here. [Pg.166]

To solve Equation 9.51, it is necessary to know the values of not only a ,-j and 9 but also x, d. The values of xitD for each component in the distillate in Equation 9.51 are the values at the minimum reflux and are unknown. Rigorous solution of the Underwood Equations, without assumptions of component distribution, thus requires Equation 9.50 to be solved for (NC — 1) values of 9 lying between the values of atj of the different components. Equation 9.51 is then written (NC -1) times to give a set of equations in which the unknowns are Rmin and (NC -2) values of xi D for the nonkey components. These equations can then be solved simultaneously. In this way, in addition to the calculation of Rmi , the Underwood Equations can also be used to estimate the distribution of nonkey components at minimum reflux conditions from a specification of the key component separation. This is analogous to the use of the Fenske Equation to determine the distribution at total reflux. Although there is often not too much difference between the estimates at total and minimum reflux, the true distribution is more likely to be between the two estimates. [Pg.167]

Examine the second term on the right-hand side of Equation (4.4) VTf(x ) Ax. Because Ax is arbitrary and can have both plus and minus values for its elements, we must insist that V/ (x ) = 0. Otherwise the resulting term added to/(x ) would violate Equation (4.5) for a minimum, or Equation (4.6) for a maximum. Hence, a necessary condition for a minimum or maximum of /(x) is that the gradient of/(x) vanishes at x ... [Pg.137]

With the second term on the right-hand side of Equation (4.4) forced to be zero, we next examine the third term (Axr) V2/(x )Ax. This term establishes the character of the stationary point (minimum, maximum, or saddle point). In Figure 4.17b, A and B are minima and C is a saddle point. Note how movement along one of the perpendicular search directions (dashed lines) from point C increases fix), whereas movement in the other direction decreases/(x). Thus, satisfaction of the necessary conditions does not guarantee a minimum or maximum. [Pg.137]

Recall that the first-order necessary condition for a local minimum is fix) = 0. Consequently, you can solve the equation/ ( ) = 0 by Newton s method to get... [Pg.158]

Let x be a local minimum or maximum for the problem (8.15), and assume that the constraint gradients Vhj(x ),j — 1,m, are linearly independent. Then there exists a vector of Lagrange multipliers A = (Af,..., A ) such that (x A ) satisfies the first-order necessary conditions (8.17)-(8.18). [Pg.271]

Examples illustrating what can go wrong if the constraint gradients are dependent at x can be found in Luenberger (1984). It is important to remember that all local maxima and minima of an NLP satisfy the first-order necessary conditions if the constraint gradients at each such optimum are independent. Also, because these conditions are necessary but not, in general, sufficient, a solution of Equations (8.17)-(8.18) need not be a minimum or a maximum at all. It can be a saddle or inflection point. This is exactly what happens in the unconstrained case, where there are no constraint functions hj = 0. Then conditions (8.17)-(8.18) become... [Pg.271]

The Kuhn-Tucker necessary conditions are satisfied at any local minimum or maximum and at saddle points. If (x, A, u ) is a Kuhn-Tucker point for the problem (8.25)-(8.26), and the second-order sufficiency conditions are satisfied at that point, optimality is guaranteed. The second order optimality conditions involve the matrix of second partial derivatives with respect to x (the Hessian matrix of the... [Pg.281]

Because — 2y is negative for all nonzero vectors in the set T, the second-order necessary condition is not satisfied, so (0, 0) is not a local minimum. [Pg.283]

Analytical solution. We set up the necessary conditions using calculus and also test to ensure that the extremum found is indeed a minimum. [Pg.465]

These give the necessary conditions for L to be minimum. The solution of the previous problem is... [Pg.119]

From the above, one can elicit that autopoiesis is not a necessary and sufficient condition for life. It is a necessary condition, but then it takes cognition, at least in the simplest stage, to arrive at the process of life. The union of autopoiesis and the most elementary form of cognition is the minimum that is needed for life. [Pg.171]

Now, it is useful to keep in mind our objective. The variational principle instructs us that as we get closer and closer to the true one-electron ground-state wave function, we will obtain lower and lower energies from our guess. Thus, once wc have selected a basis set, we would like to choose the coefficients a, so as to minimize the energy for all possible linear combinations of our basis functions. From calculus, we know that a necessary condition for a function (i.e., the energy) to be at its minimum is that its derivatives with respect to all of its free variables (i.e., the coefficients a,) are zero. Notationally, that is... [Pg.114]

Condition (22) is identical to the equation of the line (11) in Fig. 7 for large t. Analysis of the working conditions of current furnace chamber constructions falls outside the scope of the present paper. There are a number of indications that only in a small part of their total volume does intensive chemical reaction occur since it is only in this small part that necessary conditions of good mixing of air, fuel and hot reaction products are created. We may expect that, under these conditions, with the thermal intensity referred to the entire volume, the observed maximum and minimum values of the thermal intensity will prove to have been underestimated. [Pg.252]

NOTE Calcium carbonate is in fact sparingly soluble (typically the solubility ofCaCOi is to the extent of 15 to 20 ppm depending on temperature and other factors). If a decrease in cooling water pH occurs and there is a resultant increase in CO2. in excess of the minimum necessary to establish equilibrium, this can, under certain conditions, resolublize some or all of the calcium carbonate scale. [Pg.106]

Stationary points can be a (1) local maximum, (2) local minimum, or (3) saddle point. The existence of a stationary point is a necessary condition for an optimum. [Pg.135]

Nishida, N., Kobayashi, S. and Ichikawa, A., "Optimal Synthesis of Heat Exchange Systems. Necessary Conditions for Minimum Heat Transfer Area and their Application to Systems Synthesis," Chemical Engineering Science, Vol. 26, pp 1841-1856, 1971. [Pg.89]

Necessary Conditions for Stability. In a system with a fixed number of layers, such as the phospholipid bilayers, the equilibrium position (corresponding to the minimum of the free energy, F, of the whole system) is obtained when the free energy per unit area for the pair water/bilayer, f, is a minimum. This is no longer true when the number of pairs of layers is variable. In this case, at thermodynamic equilibrium one should use eq 3 c. From this equation, if the interactions between lamellae are known, one can calculate the surface tension y as a function... [Pg.316]


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