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contributor authorB. Friedland
date accessioned2017-05-08T23:44:13Z
date available2017-05-08T23:44:13Z
date copyrightJune, 1966
date issued1966
identifier issn0098-2202
identifier otherJFEGA4-27277#437_1.pdf
identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/113600
description abstractTo find the optimum control law u = u(x) for the process ẋ = f(x, u), the Hamiltonian H = p′ f is formed. The optimum control law can be expressed as u = u* = σ(p, x), where u* maximizes H. The transformation from the state x to the “costate” p entails the analytic solution of the nonlinear system: ẋ = f(x, σ(p, x)); ṗ = −fx′p with boundary conditions at two points. Since such a solution generally can not be found, we seek a quasi-optimum control law of the form u = σ(P + Mξ, x), where x = X + ξ with ‖ξ‖ small, and X, P are the solutions of a simplified problem, obtained by setting ξ = 0 in the above two-point boundary-value problem. We assume that P(X) is known. It is shown that the matrix M satisfies a Riccati equation, −Ṁ = MHXP + HPX M + MHPP M + HXX , and can be computed by solving a linear system of equations. A simple example illustrates the application of the technique to a problem with a bounded control variable.
publisherThe American Society of Mechanical Engineers (ASME)
titleA Technique of Quasi-Optimum Control
typeJournal Paper
journal volume88
journal issue2
journal titleJournal of Fluids Engineering
identifier doi10.1115/1.3645876
journal fristpage437
journal lastpage443
identifier eissn1528-901X
keywordsNonlinear systems
keywordsBoundary-value problems
keywordsEquations AND Linear systems
treeJournal of Fluids Engineering:;1966:;volume( 088 ):;issue: 002
contenttypeFulltext


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