Titlebook: Classical Principles and Optimization Problems; B. S. Razumikhin Book 1987 Springer Science+Business Media Dordrecht 1987 Homotopy.Host.Le

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Charles P. O’Brien,George E. Woodyems described in Secs.7.2, 7.4 and 7.5 of the present chapter. We shall discuss models which differ among themselves only in the mechanical properties that cause constraints. In the first model these constraints are perfectly rigid and in others they are elastic. The problem under discussion constit

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Tolerance and Physical Dependence,s due not only to the necessity of solving problems involving a large number of variables of computers having a limited operational memory. The vital factor was that the decomposition methods for economic problems are essentially mathematical models of planning and controlling processes, where it is

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https://doi.org/10.1007/978-1-4899-1669-3ts own objectives, resources and budgets. Interactions among the constituent systems of the economy can take place in the form of the exchange. Physical analogues of such interactions are the processes of mass or energy transfer which are associated with the transition to the equilibrium stateoof th

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Richard A. Deitrich,Karen Spuhler of von Neumann’s classical model [33,16]. These problems are the problem of maximizing technological and minimizing economic growth rates, the problem of exit to the path of a balanced growth and the problem of minimizing transition time taken by the economy to reach a given set of terminal states

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