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Assessment and Future Directions of Nonlinear Model Predictive ...

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A Low Dimensional Contractive NMPC Scheme 527for a ball in R np centered at the origin. Consider the following open-loop optimalcontrol problem defined for some α>0<strong>and</strong>ε>0:Pα ε,∗ (x) : min J ∗ (x, q, p) =(q,p)∈{1,...,N}×P X‖F (qτ s ,x,p)‖ 2 + α q N · min{ ε 2 , ‖F q (·,x,p)‖ 2 ∞}. (8)Note that if all the functions involved in the definition <strong>of</strong> the problem (thesystem’s map f <strong>and</strong> the control parametrization) are continuous then the costfunction is continuous in p. This together with the compactness <strong>of</strong> the set P Xguarantee that the problem Pαε,∗ (x) admits a solution for all x ∈ X <strong>and</strong> henceis well posed. Therefore, let us denote the solution <strong>of</strong> (8) for some x ∈ X byˆq(x) ∈{1,...,N} <strong>and</strong> ˆp(x) ∈ P X . These solutions are then used to define thereceding horizon state feedback given by :u(kτ s + τ) =u 1 (ˆp(x(kτ s ))) ∀τ ∈ [0,τ s [. (9)The stability result associated to the resulting feedback strategy is stated in thefollowing proposition :Proposition 1. If the following conditions hold :1. The function f in (3) <strong>and</strong> the parametrization map are continuous <strong>and</strong> satisfythe strong contraction property (see definition 4). Moreover, the system(3) satisfies assumption 2.1.2. For all x ∈ X <strong>and</strong> all admissible u = U pwc (·,p), the solution <strong>of</strong> (3) is definedfor all t ∈ [0,Nτ s ] <strong>and</strong> all p ∈ P X . (No explosion in finite time shorter thanNτ s ).3. The control parametrization is translatable on P X in the sense <strong>of</strong> definition 2.Then, there exist sufficiently small ε>0 <strong>and</strong> α>0 such that the recedinghorizon state feedback (9) associated to the open-loop optimal control problem(8) is well defined <strong>and</strong> makes the origin x = 0 asymptotically stable for theresulting closed loop dynamics with a region <strong>of</strong> attraction that contains X. ♭Pro<strong>of</strong>. The fact that the feedback law is well defined directly results fromthe continuity <strong>of</strong> the functions being involved together with the compactness <strong>of</strong>P X . Let us denote by x cl (·) the closed loop trajectory under the receding horizonstate feedback law. Let us denote by V (x) the optimal value <strong>of</strong> the cost function,namely : V (x) =J ∗ (x, ˆq(x), ˆp(x)).♭ V is continuous V (x) can clearly be written as followsV (x) =inf{}V 1 (x),...,V N (x); V q (x) :=minp∈P XJ ∗ (x, q, p). (10)But for given q, J ∗ (x, q, p) is continuous in (x, p), therefore V q (·) isacontinuousfunction <strong>of</strong> x. SinceV is the sum <strong>of</strong> N continuous functions (V j ) j=1,...,N ,it is continuous itself.

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