regularization of sweeping process old and new
play

Regularization of sweeping process: old and new Florent Nacry - PowerPoint PPT Presentation

Regularization of sweeping process: old and new Florent Nacry (Laboratoire IRMAR - INSA de Rennes) Joint work with Lionel Thibault (Institut Montpellirain Alexander Grothendieck) SEMINAIRE XLIM-MATHIS/MOD, UNIVERSITE DE LIMOGES March 27, 2018


  1. Regularization of sweeping process: old and new Florent Nacry (Laboratoire IRMAR - INSA de Rennes) Joint work with Lionel Thibault (Institut Montpelliérain Alexander Grothendieck) SEMINAIRE XLIM-MATHIS/MOD, UNIVERSITE DE LIMOGES March 27, 2018

  2. Table of contents 1. An introduction to Moreau’s sweeping process 2. Regularization: AC & BV convex cases 3. Prox-regular and α -far regularization 4. Sweeping process with truncated variation 1

  3. An introduction to Moreau’s sweeping process

  4. Notation • The letter H stands for a real Hilbert space endowed with an inner product �· , ·� and the associated norm �·� . • I := [0 , T ] is a compact interval of R for some given real T > 0. • C : I ⇒ H is a given multimapping with nonempty closed values (="moving set"). • Given S ⊂ H , ψ S is the indicator function of S , i.e., ψ S ( x ) = 0 if x ∈ S and ψ S ( x ) = + ∞ otherwise. 2

  5. Introduction in JDE Figure 1: Jean Jacques Moreau (1923-2014) "Given a ∈ C (0), the problem is that of finding a (single-valued) mapping u : I → H absolutely continuous on I such that u (0) = a and that − du dt ∈ ∂ψ C ( t ) ( u ( t )) a.e. t ∈ I . (1) [...] The evolution process defined by condition (1) may be depicted in a mechanical language, especially clear if C ( t ) possesses a nonempty interior. The moving point t �→ u ( t ) remains at rest as long as it happens to lie in this interior; when caught up by the boundary of the moving set, it can only proceed in an inward direction, as if pushed by this boundary, so as to go on belonging to C ( t )." 1 1 J.J. Moreau Evolution Problem Associated with a Moving Convex Set in a Hilbert space (Journal of Differential Equations, 26, 347-374, (1977)) 3

  6. Mechanical view 4

  7. Mechanical view Let u 0 ∈ C (0). The latter problem can be rewritten as: find absolutely continuous mappings u : I → H satisfying   u ( t ) ∈ ∂ ? ψ C ( t ) ( u ( t )) := N ? ( C ( t ); u ( t )) − ˙ λ -a.e. t ∈ I ,   u ( t ) ∈ C ( t ) for all t ∈ I ,    u (0) = u 0 . a ∋ C ⊂ H convex : ∂ψ C ( a ) := N ( C ; a ) := { ζ ∈ H : � ζ , x − a � ≤ 0 , ∀ x ∈ C } . 4

  8. Applications • Sweeping process appears in (non-exhaustive list): ◮ Planning procedure; ◮ Crowd motion; ◮ Elasto-plastic models; ◮ Non-regular electrical circuits; ◮ Evolution of sandpiles; ◮ Quasistatic evolution problems with friction, micromechanical damage models for iron materials. 5

  9. Through electrical circuits Two resistors R 1 , R 2 with voltage/current laws V R k = R k x k . � Two capacitors C 1 , C 2 with voltage/current laws V C k = C − 1 x k ( t ) dt . k Two ideal diodes with characteristics 0 ≤ − V D k ⊥ x k ≥ 0. 6

  10. Through electrical circuits Two resistors R 1 , R 2 with voltage/current laws V R k = R k x k . � Two capacitors C 1 , C 2 with voltage/current laws V C k = C − 1 x k ( t ) dt . k Two ideal diodes with characteristics 0 ≤ − V D k ⊥ x k ≥ 0. ⇒ Using Kirchhoff’s laws (˙ q i = x i and C ( t ) = [ c ( t ) , + ∞ [ × [0 , + ∞ [) � �� � � �� � C 1 + 1 1 − 1 ˙ R 1 0 q 1 q 1 C 2 C 2 ∈ − N ( C ( t ); ˙ + q ( t )) − 1 C 1 + 1 1 0 R 2 q 2 ˙ q 2 C 2 C 2 6

  11. Variants • Large number of variants: ◮ Stochastic (1973); ◮ State-dependent (1987/1998); ◮ Nonconvex (1988); ◮ With perturbations (1984); ◮ In Banach spaces framework (2010); ◮ Second order (Schatzman’s sense (1978), Castaing’s sense (1988)); ◮ In Wasserstein space (2016). 7

  12. How to handle Moreau’s sweeping processes? 8

  13. Catching-up algorithm Time discretization 0 = t n 0 < ... < t n p ( n ) = T + iterations of the form u n i ) ( u n i = proj C ( t n i − 1 ) (with u n 0 := u 0 where u 0 is the initial condition) + suitable interpolation ⇒ Sequence of mappings ( u n ( · )) ⇒ Convergence to a solution u ( · ). 9

  14. Reduction to unconstrained differential inclusion Assume that there is a Lipschitz mapping ζ : I → R wich allows to control the moving set C ( · ) in the following way: | d ( x , C ( t )) − d ( y , C ( s )) | ≤ � x − y � + | ζ ( t ) − ζ ( s ) | Idea: The following constrained differential inclusion is equivalent (under assumptions!)   − ˙ u ( t ) ∈ N ( C ( t ); u ( t )) λ -a.e. t ∈ I ,   u ( t ) ∈ C ( t ) for all t ∈ I ,    u (0) = u 0 , to the unconstrained one   u ( t ) ∈ ˙ − ˙ ζ ( t ) ∂ C d ( u ( t ) , C ( t )) λ -a.e. t ∈ I ,  u (0) = u 0 . 10

  15. Regularization of the normal cone To solve the differential inclusion   − ˙ u ( t ) ∈ N ( C ( t ); u ( t )) λ -a.e. t ∈ I ,   ( SP ) u ( t ) ∈ C ( t ) for all t ∈ I ,    u (0) = u 0 , Step 1: Find a family or ordinary differential equation   − ˙ u j ( t ) = f ( t , u j ( t )) ( E j )  u j (0) = u 0 . Step 2: Established a convergence ? u j ( · ) → u ( · ) . Step 3: Show that u ( · ) is a solution of ( SP ). 11

  16. Regularization: AC & BV convex cases

  17. Yosida approximation Let A : H → H be a maximal monotone operator, i.e., A is monotone � x ⋆ − y ⋆ , x − y � ≥ 0 for all x ⋆ ∈ A ( x ) , y ⋆ ∈ A ( y ) and no enlargement of its graph is possible in H 2 without destroying monotonicity. 12

  18. Yosida approximation Let A : H → H be a maximal monotone operator, i.e., A is monotone � x ⋆ − y ⋆ , x − y � ≥ 0 for all x ⋆ ∈ A ( x ) , y ⋆ ∈ A ( y ) and no enlargement of its graph is possible in H 2 without destroying monotonicity. Consider the Evolution Equation associated with Maximal Monotone Operator: find u : [0 , + ∞ [ → H such that u ( t ) + Au ( t ) ∋ 0 u (0) = u 0 . ˙ with initial condition ( EEMMO ) 12

  19. Yosida approximation Let A : H → H be a maximal monotone operator, i.e., A is monotone � x ⋆ − y ⋆ , x − y � ≥ 0 for all x ⋆ ∈ A ( x ) , y ⋆ ∈ A ( y ) and no enlargement of its graph is possible in H 2 without destroying monotonicity. Consider the Evolution Equation associated with Maximal Monotone Operator: find u : [0 , + ∞ [ → H such that u ( t ) + Au ( t ) ∋ 0 u (0) = u 0 . ˙ with initial condition ( EEMMO ) Yosida approximation of A with parameter λ > 0: A λ := ( λ I + A − 1 ) − 1 . It is maximal monotone, single-valued and Lipschitz continuous with λ − 1 -Lipschitz constant. To solve (EEMMO): Follow a regularization procedure with the family of ODE: u λ (0) = u 0 . u λ ( t ) + A λ u λ ( t ) = 0 ˙ with initial condition 12

  20. Let us go back to the Moreau’s sweeping process with A t ( · ) := N ( C ( t ); · ): u ( t ) + A t u ( t ) ∋ 0 u (0) = u 0 . ˙ 13

  21. Let us go back to the Moreau’s sweeping process with A t ( · ) := N ( C ( t ); · ): u ( t ) + A t u ( t ) ∋ 0 u (0) = u 0 . ˙ • f ∈ Γ 0 ( H ) ⇒ ∂ f : H ⇒ H defined by � � � � ζ , x ′ − x ∀ x ′ ∈ H ≤ f ( x ′ ) − f ( x ) ∂ f ( x ) := ζ ∈ H : . is a maximal monotone operator. 13

  22. Let us go back to the Moreau’s sweeping process with A t ( · ) := N ( C ( t ); · ): u ( t ) + A t u ( t ) ∋ 0 u (0) = u 0 . ˙ • f ∈ Γ 0 ( H ) ⇒ ∂ f : H ⇒ H defined by � � � � ζ , x ′ − x ∀ x ′ ∈ H ≤ f ( x ′ ) − f ( x ) ∂ f ( x ) := ζ ∈ H : . is a maximal monotone operator. • For each t > 0, A t ( · ) = ∂ψ C ( t ) ( · ) is a maximal monotone operator (convex subdifferential of a proper lower semi-continuous function !) How to compute Yosida approximation of A t ? 13

  23. Moreau envelope Let f : H → R ∪{ + ∞ } a function, λ > 0. The λ -Moreau envelope of f is the function e λ f : H → R ∪{− ∞ , + ∞ } defined by y ∈ H ( f ( y ) + 1 2 λ � y − x � 2 ) for all x ∈ H . e λ f ( x ) := inf 14

  24. Moreau envelope Let f : H → R ∪{ + ∞ } a function, λ > 0. The λ -Moreau envelope of f is the function e λ f : H → R ∪{− ∞ , + ∞ } defined by y ∈ H ( f ( y ) + 1 2 λ � y − x � 2 ) for all x ∈ H . e λ f ( x ) := inf ◮ J.J. Moreau, Fonctions convexes duales et points proximaux dans un espace hilbertien , CRAS 1962. ◮ Term coined by R.T. Rockafellar and R.J.B. Wets in Variational Analysis , 1998. 14

  25. Few words about Moreau envelope 2 λ �·� 2 where � is the The λ -Moreau envelope of f is given by e λ f = f � 1 inf-convolution/epi-sum (J.J. Moreau, 1963) y ∈ H ( g ( y ) + h ( x − y )) . ( g � h )( x ) := inf First properties of e λ f Let f ∈ Γ 0 ( H ), x ∈ H . Then, one has: ( i ) ∀ λ > 0, e λ f is convex, real-valued, continuous and exact at only one point. ( ii ) The net ( e λ f ( x )) λ > 0 is decreasing. ( iii ) e λ f ( x ) ↑ f ( x ) as λ ↓ 0 and e λ f ( x ) ↓ inf f ( H ) as λ ↑ + ∞ . ( iv ) e λ f is differentiable on H with gradient λ − 1 -Lipschitz. 15

  26. Aim: Compute Yosida approximation ( A t ) λ where A t ( · ) := ∂ψ C ( t ) ( · ) = N ( C ( t ); · ) . (Moreau envelope-Yosida regularization) Let f ∈ Γ 0 ( H ). Then, the Yosida regularization of ∂ f for any λ > 0 is the gradient mapping ∇ e λ f associated with the Moreau envelope e λ f . 16

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend