On Uniqueness in Evolution Quasivariational Inequalities

Size: px
Start display at page:

Download "On Uniqueness in Evolution Quasivariational Inequalities"

Transcription

1 Journal of Convex Analysis Volume 11 24), No. 1, On Uniqueness in Evolution Quasivariational Inequalities Martin Brokate Zentrum Mathematik, TU München, D Garching b. München, Germany Pavel Krejčí Mathematical Institute, Academy of Sciences of the Czech Republic, Žitná 25, CZ Praha 1, Czech Republic Hans Schnabel Zentrum Mathematik, TU München, D Garching b. München, Germany Received July 4, 22 Revised manuscript received March 31, 23 We consider a rate independent evolution quasivariational inequality in a Hilbert space X with closed convex constraints having nonempty interior. We prove that there exists a unique solution which is Lipschitz dependent on the data, if the dependence of the Minkowski functional on the solution is Lipschitzian with a small constant and if also the gradient of the square of the Minkowski functional is Lipschitz continuous with respect to all variables. We exhibit an example of nonuniqueness if the assumption of Lipschitz continuity is violated by an arbitrarily small degree. Keywords: Evolution quasivariational inequality, uniqueness, sweeping process, hysteresis, play operator 2 Mathematics Subject Classification: 49J4, 34C55, 47J2 1. Introduction In 1973, Moreau has introduced the sweeping process, [1, 11]. It describes the movement ξ = ξt) of a point in a Hilbert space X induced by a time-dependent closed convex set C = Ct) according to ξt) N Ct) ξt)), ξ) = ξ, 1) where N K x) denotes the normal cone to a convex set K at a point x. The evolution variational inequality vt), w vt) ft), w vt) w Γ, vt) Γ, v) = v, 2) Supported by the Academy of Sciences of the Czech Republic. Supported by the DFG through SFB 438. Supported by the GAČR under Grant 21/2/158. Supported by the DFG under Grant BR 15/7 1. ISSN / $ 2.5 c Heldermann Verlag

2 112 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution... Γ H closed and convex, constitutes a special case of 1), if we set ξt) = vt) fs) ds, ξ = v, Ct) = Γ In the same manner, the evolution quasivariational inequality fs) ds. 3) vt), w vt) ft), w vt) w Γvt)), vt) Γvt)), v) = v, 4) becomes a special case of the implicit or state-dependent sweeping process if we set ξt) = vt) ξt) N Ct,ξt)) ξt)), ξ) = ξ, 5) fs) ds, ξ = v, Ct, ξ) = Γ ξ + ) fs) ds fs) ds. 6) An appropriate meaning has to be given to the time derivative if discontinuous processes are taken into consideration. The Young integral formulation was investigated in [5]. Another approach to nonsmooth evolution differential inclusions based on energy considerations was recently proposed by Mielke and Theil in [9]. While the sweeping process 1) has been an object of extensive study, see the survey [7], much less is known about the implicit process 5). The paper [2] seems to be the first result in this direction, in a more general setting actually, but restricted to the case dim X = 1. Kunze and Monteiro Marques [8] have proved existence for 5), if C satisfies a Lipschitz condition with respect to the Hausdorff distance, d H Ct, ξ), Cs, η)) L 1 t s + L 2 ξ η, 7) if L 2 < 1 and give examples for nonexistence if L 2 > 1. However, no matter how small L 2 is chosen, uniqueness may fail to hold; Ballard [1] has given an example in the context of quasi-static friction problems. Indeed, it is a general feature of quasivariational inequalities that the loss of monotonicity, as caused by the state dependence of the constraint C, is accompanied by a loss of uniqueness of their solution. On the other hand, there is no a priori reason why it should be impossible to enforce uniqueness if the constraint behaves in a sufficiently regular manner. We will show in this paper that uniqueness holds if the normal vectors to the constraint Ct, ξ) satisfy a Lipschitz condition with respect to t, ξ). Under the assumptions below this means that we require the gradient of the square of the Minkowski functional M of C to be Lipschitz continuous as a function of t, ξ), whereas 7) is under suitable hypotheses, see Lemma 3.2 below, equivalent to the Lipschitz continuity of M itself. Our proof of uniqueness and, incidentally, of existence at the same time) is based on the contraction principle, thus the possible loss of monotonicity does not play any role here. In order to obtain a contraction, results concerning time regularity for the solution operator f ξ of the standard variational inequality 1) are required which are stronger than the basic estimate ξ 1 t) ξ 2 t) ξ 1 ξ 2 + f 1 s) f 2 s) ds. 8)

3 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution Such stronger estimates have been provided within the context of hysteresis operators, see [4] for a recent exposition. However, to apply those results we need the constraint to be sandwiched uniformly between balls with fixed radius around zero. In particular, constraints with empty topological interior are excluded. In addition, we will relate the nonuniqueness in the quasivariational inequality to the generic nonuniqueness phenomenon for scalar ordinary differential equations. More precisely, to every concave increasing function ψ : R R with ψ) = which gives rise to a positive solution of the scalar problem y = ψy), y) =, 9) besides the trivial one, there corresponds a quasivariational inequality with nonunique solution, where the gradient with respect to the state ξ) of the Minkowski functional varies like ψ ξ ). 2. Problem statement We consider a separable Hilbert space X endowed with a scalar product,, a norm x = x, x for x X, and a family of bounded convex closed sets Zϱ) X parametrized by ϱ R Y, where Y is a reflexive Banach space endowed with a norm Y and R is a convex closed set with non-empty interior R. By Y we mean the dual of Y,, )) is the duality pairing between Y and Y, and Y, LX,Y ) denote natural norms in the corresponding spaces. Throughout the paper, with the exception of Section 4, we will assume that there exist < c C such that B c ) Zϱ) B C ) ϱ R. 1) We consider two problems, namely a variational inequality where the constraint Z depends on an additional given function Problem P )), and a quasivariational inequality Problem I )). For given functions u W 1,1, T ; X), r W 1,1, T ; R) and an initial condition x Zr)) we look for a function ξ W 1,1, T ; X) such that P ) i) ut) ξt) Zrt)) t [, T ], ii) u) ξ) = x, iii) ξt), ut) ξt) y y Zrt)) for a. e. t ], T [. Besides serving as the crucial tool for the solution of problem I ), problem P ) is of interest in itself consider, for example, a constitutive stress-strain law where the yield function depends on the temperature). Actually, problem P ) is a reformulation of 1). We reduce P ) to 1) if we set u =, rt) = t, x = ξ and C = Z, and we reduce 1) to P ) if we set Ct) = ut) Zrt)) and ξ = u) x. We now formulate problem I ). Let g : [, T ] X X R be a mapping satisfying Hypothesis G) stated below at the beginning of Section 6. For a given function u W 1,1, T ; X) and an initial condition x Zg, u), u) x )) for instance, any x B c ) satisfies this inclusion) we look for a solution ξ W 1,1, T ; X) of the implicit problem

4 114 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution... I ) i) ut) ξt) Zgt, ut), ξt))) t [, T ], ii) u) ξ) = x, iii) ξt), ut) ξt) y y Zgt, ut), ξt))) for a. e. t ], T [. The implicit sweeping process 5) becomes a special case of I ), if we set u =, gt, u, ξ) = t, ξ), x = ξ and C = Z. On the other hand, I ) becomes a special case of 5), if we set Ct, ξ) = ut) Zgt, ut), ξ)) and ξ = u) x. The quasivariational inequality 4) is subsumed under I ) either going through 6), or by setting ξt) = vt)+ut), ut) = fs) ds, x = v, Z = Γ, gt, u, ξ) = ξ u. 11) The formulation 5) certainly looks more compact than I ). However, in applications a driving function like u or its derivative f) often appears, and it is useful to study the dependence of ξ on u with respect to standard function spaces. In 5) one has to deal with metric properties of the set-valued mapping t Ct, ξ).) Our main results include the existence, uniqueness, and Lipschitz continuous input-output dependence for both Problems P ) and I ) in Sections 4 7. Before, we recall some basic notions from convex analysis as presented in [12, 4]. 3. Preliminaries: Convex sets Consider a Hilbert space X as in the previous section and a convex closed set Z X. The mapping M Z : X R + defined by the formula M Z x) = inf {s > ; x } s Z 12) is called the Minkowski functional associated with Z. The polar set Z to Z is defined by the formula Z = {x X ; x, y 1 y Z}. 13) We first summarize in Lemma 3.1 below some results of [4, Sections 3 and 6]. Lemma 3.1. Assume that there exist C > c > such that i) It holds B c ) Z B C ). 14) B 1/C ) Z B 1/c ), 15) x C M Zx) x c, 16) c x M Z x) C x. 17) ii) Let the derivative x M Z x) X exist for each x X \ {}, and set J Z ) =, J Z x) = M Z x) x M Z x) for x. Then the unit outward normal n Z x) to Z is uniquely determined at each point x Z, and we have n Z x) = J Zx) J Z x) x Z, 18)

5 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution M Z J Z x)) = M Z x) x Z. 19) Let moreover L > such that n Z x) n Z y) L x y x, y Z. 2) Then we have J Z x) J Z y) 1 c + L 2 c 1 + C ) ) 2 x y x, y X. 21) c We can measure the distance of two sets Z 1, Z 2 in the system C of all closed convex subsets Z of X either as the Hausdorff distance or the Minkowski distance d H Z 1, Z 2 ) = max{ sup z 1 Z 1 dist z 1, Z 2 ), sup z 2 Z 2 dist z 2, Z 1 )}, 22) d M Z 1, Z 2 ) = sup M Z1 x) M Z2 x). 23) x =1 We first show that these concepts are equivalent in the class of sets satisfying 14). Lemma 3.2. Let Z 1, Z 2 C be such that 14) holds for Z = Z i, i = 1, 2. Then we have Proof. c 2 d M Z 1, Z 2 ) d H Z 1, Z 2 ) C 2 d M Z 1, Z 2 ). 24) Assume first that there exists x Z 1 \ Z 2. Using 16) we obtain dist x, Z 2 ) x x M Z2 x) x 2 M Z1 x)m Z2 x) C 2 d M Z 1, Z 2 ), ) )) x x M Z2 M Z1 x x and reversing the roles of Z 1 and Z 2 we obtain the right inequality in 24). To prove the left estimate in 24), we divide the unit sphere B 1 ) into the sets A = {x B 1 ) ; M Z1 x) = M Z2 x)}, A 1 = {x B 1 ) ; M Z1 x) > M Z2 x)}, A 2 = {x B 1 ) ; M Z1 x) < M Z2 x)}. For x A 2 set x = x/m Z1 x), and let Q Z2 x be the orthogonal projection of x onto Z 2, that is, Q Z2 x Z 2, P Z2 x = dist x, Z 2 ), 25) where we denote P Z2 x = x Q Z2 x. We have M Z2 x) > M Z1 x) = 1, hence x / Z 2 and d := P Z2 x >. Put m = 1 + d/c. Then the vector 1 m x = c c + d Q Z 2 x + d cp Z2 x c + d d

6 116 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution... is a convex combination of elements of Z 2, hence M Z2 x) m. This yields M Z2 x) M Z1 x) m 1 1 c dist x, Z 2) 1 c d HZ 1, Z 2 ). Using 16) we conclude that M Z2 x) M Z1 x) 1 c 2 d HZ 1, Z 2 ), and arguing similarly for x A A 1 we complete the proof. Another distance criterion for convex sets involving the mapping J Z introduced in Lemma 3.1 is used in Sections 5 and 7. Here, we derive the following estimate. Lemma 3.3. Let Z 1, Z 2 C be such x M Z x) exists for each x X \ {} and that 14) and 2) hold for Z = Z i, for Z = Z i, i = 1, 2. Let L J be the Lipschitz constant on the right-hand side of 21). Then J Z1 x) J Z2 x) 2 2 c d M Z 1, Z 2 ) cl J + d M Z 1, Z 2 ))) 1/2 x B 1 ). 26) Proof. Let x X with x = 1 and let J Z1 x) J Z2 x). We define x s = x + s J Z 2 x) J Z1 x) J Z2 x) J Z1 x) for s. 27) We may assume that x s x, x, otherwise we interchange Z 1 and Z 2. The functions λ i s) := 1 2 M 2 Z i x s ) are convex and satisfy Thus, λ i ) + sλ i) λ i s) λ i ) + sλ is) for s. 28) λ 2 s) λ 1 s) λ 2 ) λ 1 ) + s λ 2) λ 1s)) 29) = λ 2 ) λ 1 ) + s λ 2) λ 1)) + s λ 1) λ 1s)). Note that, because s M Zi x s ) is differentiable, the chain rule implies that λ J Z2 x) J Z1 x) is) = J Zi x s ), for s. J Z2 x) J Z1 x) Hence λ 2) λ 1) = J Z2 x) J Z1 x), 3) λ 1s) λ 1) J Z1 x s ) J Z1 x) sl J. 31) We further have by 16) for all s that recall that we have assumed x s x, x ) λ 2 s) λ 1 s) x s c M Z 2 x s ) M Z1 x s ) x s 2 c d M Z 1, Z 2 ) 1 + s2 c d M Z 1, Z 2 ). 32)

7 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution Combining 29) 32) we obtain for all s > that J Z2 x) J Z1 x) 2 + s2 sc d M Z 1, Z 2 ) + sl J. 33) The right-hand side attains its minimum for s = 2 d M Z 1, Z 2 )/cl J + d M Z 1, Z 2 )), and the assertion follows. We conclude this section with the following result as a simplified variant of [6, Lemma 3.2]. Lemma 3.4. Let Z X be an arbitrary convex closed set, and for θ > set Z θ = Z + B θ ). Then the outward unit normal n θ x) to Z θ is uniquely determined at each point x Z θ, and we have n θ x) n θ y) 1 θ x y x, y Z θ. 34) Proof. Let Q Z : X Z be the orthogonal projection onto Z. Putting P Z x = x Q Z x we have P Z x = dist x, Z) for each x X, and P Z x, Q Z x z x X, z Z. 35) For x Z θ and ˆx Z θ this yields P Z x = θ, P Z ˆx θ, and P Z x, x ˆx = P Z x, Q Z x Q Z ˆx + P Z x 2 P Z x, P Z ˆx. Let ñ be an arbitrary unit vector such that ñ, x x for every x Z θ. Putting x = Q Z x + θñ we obtain ñ, P Z x θ, hence ñ = 1/θ)P Z x = n θ x). From 35) it follows for all x, y X that P Z x P Z y, Q Z x Q Z y, hence P Z x P Z y x y, and 34) follows. 4. Existence and uniqueness for the explicit problem Since Problem P ) is equivalent to the classical sweeping process 1), the existence and uniqueness result for P ) can be deduced from the results of Moreau [11], if the set-valued function Z is Lipschitz continuous with respect to the Hausdorff metric, that is, if holds for some L Z >. d H Zϱ), Zσ)) L Z ϱ σ ϱ, σ R 36) It is obvious that if Problem P ) has a solution, it is unique. Indeed, if ξ, η are two solutions, then ξ, η ξ, η, ξ η, hence ξ η, ξ η and the assertion follows. Proposition 4.1. Let there exist L Z > such that 36) is satisfied. Then Problem P ) admits a unique solution ξ W 1,1, T ; X) for any given functions u W 1,1, T ; X), r W 1,1, T ; R) and any initial condition x Zr)).

8 118 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution... Proof. We consider the sweeping process 1) with Ct) = ut) Zrt)), ξ = u) x, which is equivalent to P ). By 36) we have d H Ct), Cτ)) ut) uτ) + L Z rt) rτ). Since u and r are absolutely continuous, so is C. By Proposition 3c in [11], 1) then has a solution ξ W 1,1, T ; X). Note that in Proposition 4.1 there is no assumption regarding the interior of the sets Zρ), in particular 1) is not needed. Concerning the dependence of u upon C in the sweeping process 1), the basic general result is of Hölder type, see Proposition 2g in [11] or Theorem 4 in [7]. Let ξ, η be the solutions of Problem P ) for the data u, r, x ) respectively v, s, y ). Then Theorem 4 in [7] implies, if u, r, v, s are Lipschitz continuous, ξt) ηt) 2 x y + u) v) ) 2 +L where uτ) vτ) +L Z rτ) sτ) dτ, 37) L = 2 u + v + L Z ṙ + ṡ )). 38) Because of the square in 37), this formula cannot serve as the basis of a contraction mapping argument for problem I ). 5. Lipschitz estimates Under the assumption 1), we denote by Z ϱ) the polar set to Zϱ) defined in 13) for ϱ R, and by M ϱ, ) its Minkowski functional. By Lemma 3.1 we have B 1/C ) Z ϱ) B 1/c ) for every ϱ R, and the inequalities x C Mϱ, x) x c, 39) c x M ϱ, x) C x 4) hold for every x X and ϱ R. The following conditions are assumed to hold: L1) The partial derivatives ϱ Mϱ, x) Y, x Mϱ, x) X exist for every x X \{} and ϱ R, and the mappings Jϱ, x) = Mϱ, x) x Mϱ, x) : R X \ {} X, 41) Kϱ, x) = Mϱ, x) ϱ Mϱ, x) : R X \ {} Y 42) admit continuous extensions to x = and ϱ R. L2) For every x, x B C ) and ϱ, ϱ R we have Kϱ, x) Y K, 43) Jϱ, x) Jϱ, x ) C J ϱ ϱ Y + x x ), 44) Kϱ, x) Kϱ, x ) Y C K ϱ ϱ Y + x x ) 45) with some fixed constants K, C J, C K >.

9 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution Lemma 5.1. Let 1), L1) and 43) hold. Then holds for all ϱ, σ R. Proof. By Lemma 3.2, By 39), if x = 1 we have 1 2 M 2 ϱ, x) 1 2 M 2 σ, x) d H Zϱ), Zσ)) C 3 K ϱ σ 46) d H Zϱ), Zσ)) C 2 sup Mϱ, x) Mσ, x). x =1 1 2 Mϱ, x) Mσ, x) Mϱ, x) + Mσ, x)) 1 Mϱ, x) Mσ, x), C and 46) follows from 43). Thus, Problem P ) has a unique solution by Proposition 4.1. The following two lemmas constitute the main steps towards the desired Lipschitz estimates. Lemma 5.2. Let L1) hold, let r, u) W 1,1, T ; R) W 1,1, T ; X) and x Zr)) be given, and let ξ W 1,1, T ; X) be the corresponding solution to Problem P ). For t ], T [ set A[r, u]t) = ξt), Jrt), xt)), B[r, u]t) = 1 2 M 2 rt), xt)), G[r, u]t) = ut), Jrt), xt)) + Krt), xt)), ṙt))), with xt) = ut) ξt). Then for a. e. t ], T [ we have either i) ξt) =, d B[r, u]t) = G[r, u]t) dt or ii) ξt), xt) Zrt)), A[r, u]t) = G[r, u]t) >, B[r, u]t) = max[,t ] B[r, u] = 1/2, d B[r, u]t) =, and dt ξt) = A[r, u]t) Jrt), xt)). 47) Jrt), xt)) 2 d Proof. Let L ], T [ be the set of Lebesgue points of all functions u, ṙ, ξ, B[r, u]. dt Then L has full measure in [, T ], and for t L we have d B[r, u]t) = ẋt), Jrt), xt)) + Krt), xt)), ṙt))). 48) dt

10 12 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution... If ξt) =, then ẋt) = ut), and i) follows from 48). If ξt), then xt) Zrt)), hence Mrt), xt)) = 1 = max s [,T ] Mrs), xs)). We therefore have B[r, u]t) = d 1/2 = max [,T ] B[r, u], B[r, u]t) =. As a consequence of P ) iii) we have ξt) = dt k nrt), xt)) with a constant k >, where nrt), xt)) is the unit outward normal to Zrt)) at the point xt), hence k = ξt), nrt), xt)), and 47) follows from Lemma 3.1 ii). Furthermore, 48) yields ẋt), Jrt), xt)) = Krt), xt)), ṙt))), hence ξt), Jrt), xt)) = ut), Jrt), xt)) ẋt), Jrt), xt)) and the proof is complete. = ut), Jrt), xt)) + Krt), xt)), ṙt))), In the situation of Lemma 5.2, we always have G[r, u]t) ut) Jrt), xt)) + K ṙt) Y, 49) ξt) ut) + CK ṙt) Y. 5) Indeed, 5) is trivial if ξt) = ; otherwise we have ξt) = A[r, u]t)/ Jrt), xt)) = G[r, u]t)/ Jrt), xt)) with xt) Zrt)). Lemma 3.1 then yields C Jrt), xt))) M rt), Jrt), xt))) = Mrt), xt)) = 1, and 5) follows from 49). Lemma 5.3. Let L1) and 43) hold, let r, u), s, v) W 1,1, T ; R) W 1,1, T ; X) and x Zr)), y Zs)) be given, let ξ, η W 1,1, T ; X) be the respective solutions to Problem P ), and set x = u ξ, y = v η. Then for a. e. t ], T [ we have A[r, u]t) A[s, v]t) + d B[r, u]t) B[s, v]t) G[r, u]t) G[s, v]t), 51) dt ξt) ηt) C ut) + CK ṙt) Y ) Jrt), xt)) Jst), yt)) 52) Proof. + C A[r, u]t) A[s, v]t). The assertion follows directly from Lemma 5.2 if ξt) = ηt) =. Assume now ξt), ηt). Then 51) is again an immediate consequence of Lemma 5.2. To prove 52), we use 47) and the elementary vector identity z z z 2 z 2 = 1 z z z z for z, z X \ {}, to obtain ξt) ηt) A[r, u]t) Jrt), xt)) Jrt), xt)) Jst), yt)) 2 Jst), yt)) 2 = + 1 A[r, u]t) A[s, v]t) Jst), yt)) 1 G[r, u]t) Jrt), xt)) Jst), yt)) Jrt), xt)) Jst), yt)) + 1 A[r, u]t) A[s, v]t). Jst), yt))

11 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution Lemma 3.1 yields Jrt), xt)) 1/C, Jst), yt)) 1/C. inequalities with 49) we obtain the assertion. Let us consider now the case ξt), ηt) =. Combining the above Then A[r, u]t) A[s, v]t) = A[r, u]t), B[r, u]t) B[s, v]t) = 1/2 B[s, v]t), hence A[r, u]t) A[s, v]t) + d dt B[r, u]t) B[s, v]t) = A[r, u]t) d B[s, v]t) dt hence 51) is fulfilled. We further have similarly as above that = G[r, u]t) G[s, v]t), ξt) ηt) = ξt) C A[r, u]t) = C A[r, u]t) A[s, v]t), hence 52) holds. The remaining case ξt) =, ηt) is analogous, and Lemma 5.3 is proved. We are now ready to prove the following crucial estimate. Proposition 5.4. Let L1), L2) hold, let r, u), s, v) W 1,1, T ; R) W 1,1, T ; X) and x Zr)), y Zs)) be given, let ξ, η W 1,1, T ; X) be the respective solutions to Problem P ), and set x = u ξ, y = v η. Then for a. e. t ], T [ we have ξt) ηt) + C d dt B[r, u]t) B[s, v]t) C c ut) vt) + CK ṙt) ṡt) Y 53) ) + C 2C J ut) + C K + CC J K ) ṙt) Y rt) st) Y + xt) yt) ). Proof. By Lemma 3.1 we have c Jrt), xt)) M rt), Jrt), xt))) = Mrt), xt)) 1, hence Jrt), xt)) 1/c for every t [, T ]. By Lemma 5.3, we can estimate the left-hand side of 53) by C ) G[r, u]t) G[s, v]t) + ut) + CK ṙt) Y ) Jrt), xt)) Jst), yt)) which together with the assumptions 43) 45) yields the assertion. 6. Implicit model We now consider Problem I ) under the following hypothesis on the mapping g. G) g : [, T ] X X Y is continuous and gt, u, ξ) R for each t, u, ξ)

12 122 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution... [, T ] X X. Its partial derivatives t g, u g, ξ g exist and satisfy the inequalities ξ gt, u, ξ) LX,Y ) γ, 54) u gt, u, ξ) LX,Y ) ω, 55) t gt, u, ξ) Y at), 56) ξ gt, u, ξ) ξ gt, v, η) LX,Y ) C g u v + ξ η ), 57) u gt, u, ξ) u gt, v, η) LX,Y ) C u u v + ξ η ), 58) t gt, u, ξ) t gt, v, η) Y bt) u v + ξ η ) 59) for every u, v, ξ, η X and a. e. t ], T [ with given functions a, b L 1, T ) and given constants γ, ω, C g, C u > such that where C, K are as in Hypotheses 1) and L2). δ = CK γ < 1, 6) Let us start our analysis with the following necessary condition. Lemma 6.1. Let Hypotheses L1), L2), and G) hold, and let ξ W 1,1, T ; X) be a solution to Problem I ) with some u W 1,1, T ; X) and x Zg, u), u) x )). Then we have ξt) 1 1 δ 1 + CK ω) ut) + CK at)) a. e. 61) Proof. Inequality 61) is an easy consequence of 5) with rt) = gt, ut),ξt)). Indeed, using 54), 55) we obtain ṙt) Y at) + ω ut) + γ ξt) and 61) follows. We now prove the converse as the main result of this section. Theorem 6.2. Let Hypotheses L1), L2), and G) hold. Then for every u W 1,1, T ; X) and every x Zg, u),u) x )) there exists a unique solution ξ W 1,1, T ; X) to Problem I ) in the set Ω = { η W 1,1, T ; X) ; ηt) CK 1 δ ω) ut) + CK at)) a. e. η) = u) x }. Proof. Let S : Ω W 1,1, T ; X) be the mapping which with each η Ω associates the solution ξ to Problem P ) with rt) = gt, ut), ηt)). By 5) we have ξt) ut) + CK ṙt) Y 1 + CK ω) ut) + CK at) + δ ηt) 62) 1 1 δ 1 + CK ω) ut) + CK at)), hence SΩ) Ω. The set Ω is convex and closed in W 1,1, T ; X). We now check that S : Ω Ω is a contraction with respect to a suitable norm in W 1,1, T ; X).

13 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution Let η 1, η 2 Ω be given. By Proposition 5.4, the functions ξ i = Sη i ) for i = 1, 2 satisfy almost everywhere the inequality ξ 1 t) ξ 2 t) + βt) δ η 1 t) η 2 t) 63) + C δ ut) + at) + bt)) η 1 t) η 2 t) + ξ 1 t) ξ 2 t) ) with βt) = C B[g, u,η 1 ), u]t) B[g, u,η 2 ), u]t), β) =, and with a constant C δ > independent of η 1, η 2. Let now ε > be chosen so small that and let us define an auxiliary function wt) = e 1 ε δ + εc δ 1 εc δ = δ < 1, 64) R t uτ) +aτ)+bτ)) dτ for t [, T ]. 65) We have wt) > for every t [, T ] and ẇt) a. e. We test the inequality 63) by wt) and integrate over [, T ]. Taking into account the relations βt) wt) dt = [βt) wt)] T βt) ẇt) dt, wt) ut) + at) + bt)) η 1 t) η 2 t) + ξ 1 t) ξ 2 t) ) dt ε ẇt) η 1 τ) η 2 τ) + ξ 1 τ) ξ 2 τ) ) dτ dt [ ] T = ε wt) η 1 τ) η 2 τ) + ξ 1 τ) ξ 2 τ) ) dτ + ε wt) η 1 t) η 2 t) + ξ 1 t) ξ 2 t) ) dt ε wt) η 1 t) η 2 t) + ξ 1 t) ξ 2 t) ) dt, we obtain from 63) that wt) ξ 1 t) ξ T 2 t) dt δ+εc δ ) wt) η 1 t) η 2 t) dt+εc δ wt) ξ 1 t) ξ 2 t) dt hence wt) ξ 1 t) ξ T 2 t) dt δ wt) η 1 t) η 2 t) dt. 66) We thus checked that S is a contraction on Ω with respect to the weighted norm η = η) + wt) ηt) dt, hence S admits a unique fixed point ξ which is a solution of I ).

14 124 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution Lipschitz continuity In this section we prove local Lipschitz continuity estimates for both Problems P ) and I ) as a combination of Proposition 5.4 and a Gronwall-type argument. Theorem 7.1. Let the assumptions of Proposition 5.4 be fulfilled. Then there exist positive constants C, C 1 such that for every R >, every r, u), s, v) W 1,1, T ; R) W 1,1, T ; X) with u + ṙ Y )dt R, v + ṡ Y )dt R, and every x Zr)), y Zs)), the respective solutions ξ, η W 1,1, T ; X) of problem P ) satisfy the inequality ξ η dt C 1 e C R x y + r) s) Y + ) u v + ṙ ṡ Y )dt. 67) Proof. By Proposition 5.4, there exists a constant C > such that ẋt) ẏt) + βt) C ut) vt) + ṙt) ṡt) Y 68) ) + ut) + ṙt) Y ) xt) yt) + rt) st) Y ) with βt) = C B[r, u]t) B[s, v]t). We argue similarly as in the proof of Theorem 6.2 and test 68) by the function This yields d w 1 t) dt Note that w 1 t) = e C R t u + ṙ Y ) dτ. ) ẋ ẏ dτ + w 1 t) βt) ) C w 1 t) ut) vt) + ṙt) ṡt) Y ẇ 1 t) x y + r) s) Y + 69) ) ṙ ṡ Y dτ. w 1 t) βt) dt = [w 1 t) βt)] T ẇ 1 t) βt) dt w 1 ) β) 7) C 2 M 2 r), x ) M 2 s), y ) CK r) s) Y + C ) c x y. On the other hand, integrating 69) from to T and using the fact that for every t [, T ] we have 1 w 1 t) w 1 T ) e C R we obtain e C R ẋ ẏ dt w 1 t) βt) dt + x y + r) s) Y 71) + C + 1) and the assertion follows from 7), 71). u v + ṙ ṡ Y ) dt,

15 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution Theorem 7.2. Let the assumptions of Theorem 6.2 be fulfilled. Then there exist positive constants C 2, C 3 such that for every R >, every u, v W 1,1, T ; X) with u dt R, v dt R, and every x Zg, u), u) x ), y Zg, v), v) y ), the respective solutions ξ, η W 1,1, T ; X) of problem I ) satisfy the inequality ξ η dt C 3 e C 2R ) x y + u) v) + u v dt. 72) Proof. We use Lemma 6.1 and Proposition 5.4 with rt) = gt, ut), ξt)), st) = gt, vt), ηt)), and find a constant C > such that 1 δ) ξt) ηt) + βt) C ut) vt) 73) ) + ut) + at) + bt)) ut) vt) + ξt) ηt) ) with βt) = C B[g, u, ξ), u]t) B[g, v, η), v]t). Repeating the procedure from the proof of Theorem 7.1 with we easily obtain the assertion. 8. Nonuniqueness C 2 = C 1 δ, w 2t) = e C R t 2 uτ) +aτ)+bτ)) dτ 74) Let ψ : [, 1] [, 1] be an increasing concave function with ψ) =. Then the initial value problem ẇ = δψw), w) =, 75) has a positive solution for any δ > in addition to the trivial one, if and only if Let us assume that 76) holds. Then 1 1 dε <. 76) ψε) ψε) lim ε + ψ ε) = lim ε + ε =. 77) Moreover assume that there exists K > such that ψ ε) K ε for a. e. ε ], 1[. 78) Then A typical example is ψε) = ε β, 1/2 β < 1. We denote ψε) 2K ε ε [, 1]. 79) θ = K 2 8)

16 126 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution... with K from 78), and consider for α and η 1 θ the system of convex sets in X = R 2, where Hη, α) is the half-plane V η, α) = B 1 θ ) Hη, α), 81) Hη, α) = {z R 2 ; z, ν α 1 θ η}, ν α = We further define two one-parametric families of convex sets ) 1. 82) α Zε) = V ε + θ 1 + ψ 2 ε) 1), ψε)), 83) Zε) = Zε) + B θ ), 84) for ε [, ε ], where ε ], 1] is chosen in such a way that for every ε ], ε ] we have θ ψ 2 ε)) ψ2 ε) ε + 2θ ε + θ 1 + ψ 2 ε) < 1, 85) 1 ε) ψ2 ε) ε + 1 ε 1 )) 1 ε 1 + ψ2 ε) 2 ε. 86) Let Λθ, ε) denote the left-hand side of 86). To see that condition 86) is meaningful, it suffices to use 79) which entails that ) ) 4K lim sup Λθ, ε) 4K 2 θ 2 + 2θ 1 + 6K ) = 2 1 < 2. 87) ε K 2 The set Zε) can also be characterized as z Zε) z 1 θ, z, νψε) 1 ε θ 1 + ψ2 ε), 88) see Figure 1. As the next step, we check that the segment { ) } x Sε) = z = ; x ψε)y = 1 ε, y θ ψε) y 89) satisfies Sε) Zε) ε [, ε ]. 9) The limit case ε = is easy: we have Z) = B 1 ), and S) contains only one element ) 1 e 1 =. For ε > and z Sε) we define z θ = z θ 1 + ψ2 ε) ν ψε). Then z θ z = θ, 91) zθ, ν ψε) = 1 ε θ 1 + ψ2 ε), 92)

17 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution z θ 2 = z 2 + θ 2 1 ε 2θ 1 + ψ2 ε), 93) where z 2 1 ε + θψ 2 ε)) 2 + θ 2 ψ 2 ε) by 89). Developing the computation and using 86) we obtain from 93) that z θ 2 1 ε) 2 + θ ψ 2 ε) + ψ 4 ε)) + 2θ 1 ε) ψ 2 1 ε ε) 2θ 1 + ψ2 ε) )) = 1 θ) 2 + θ ψ 2 ε)) ψ 2 ε) + 2θ 1 ε) ψ 2 1 ε ε) ε 2 2ε 1 + ψ2 ε) 1 θ) 2, hence z θ Zε) and z Zε). To see that z Zε), we notice using 88) that for arbitrary z Zε) we have z z 1 z z, νψε) θ. 1 + ψ2 ε) In other words, dist z, Zε)) = θ, and 9) is verified. y Zwt)) 1 θ Zwt)) vt) 1 x Figure 1. Trajectory of the nontrivial solution vt). We now construct the example of nonuniqueness for the evolution quasivariational inequality 4). Let w : [, t ] R be the positive solution to the initial value problem 75) for a fixed δ >, where we choose t sufficiently small such that We define vt) = wt ) ε, ) v1 t) with v 2 t) wt ) ψwt )) δ θ, δψwt )) < 1. 94) v 1 t) = 1 wt) + 1 δ wt)ψwt)), v 2t) = 1 wt), 95) δ

18 128 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution... and set Then Γv) = Zδv 2 ). 96) v 2 t) ψwt)) v 2t ) ψwt )) < θ, 97) hence vt) Swt)) Zwt)) = Γvt)) for all t [, t ], see Figure 1. We set ft) = f 1 t), ), f 1 t) = 1 + v 1 t), 98) then ft) vt) = ν ψwt)) vt)) N Γvt)) vt)), and f 1 t) > for t t. Therefore, both ) 1 vt) as defined and ˆvt) e 1 = are solutions of 4). Thus, there is nonuniqueness, despite the fact that the outward normal vectors n Zε) z) are Lipschitz continuous in z for every ε with a Lipschitz constant independent of ε as a consequence of Lemma 3.4. Moreover, the orthogonal projections Q Zε) of X onto Zε) and therefore also n Zε) by virtue of the argument in the proof of Lemma 3.4) depend Lipschitz-continuously on ε in each interval [ε 1, ε ] with < ε 1 < ε. For ε = there is indeed no problem in any direction different from e 1, as the boundary of Zε) does not move here for ε small. However, the dependence of J Zε) z) on ε is not globally Lipschitz and the Lipschitz constant behaves like ψε)/ε for z = e 1 near ε =. Indeed, for fixed ε > and z Sε) we have M Zε) z) = z, ν ψε) /1 ε). We easily find qε) > which guarantees that for every y B qε) ) we can find pε, y) > such that pε, y)e 1 + y) Sε). For all such y we thus have M Zε) e 1 + y) = e 1 + y, ν ψε) /1 ε), hence JZε) e 1 ) = ν ψε) /1 ε) 2. Obviously, J Z) x) = x for every x X, and we conclude that J Zε) e 1 ) J Z) e 1 ) = ψ2 ε) + ε 2 2 ε) 2 1 ε) 2, 99) where the right-hand side is of the order of ε β if for example ψε) = ε β, 1/2 β < 1. On the other hand, we will see that Zε) does depend Lipschitz-continuously on ε in the sense of the Hausdorff distance. This implies in turn that the map v Γv) is Lipschitz with an arbitrarily small constant similarly as in the example of [1] provided δ is chosen sufficiently small in fact, to make Figure 1 more transparent, we have chosen a trajectory of the solution vt) corresponding to a very large δ). We conclude the paper by establishing this Lipschitz continuity result as a separate lemma. Lemma 8.1. There exists a constant R > such that for every ε 2 < ε 1 ε we have i) Zε 1 ) Zε 2 ), ii) d H Zε 1 ), Zε 2 )) R ε 1 ε 2 ). It is interesting to compare formula 99) with Lemmas 3.2, 3.3, and 8.1. We see that the hypothesis 79) is sharp in the sense that if one sets ψε) = ε β with β < 1/2 in the example above, one cannot expect that d H Zε), Z)) remains Lipschitz continuous in ε. Proof. To prove i), let us consider an arbitrary z = ) x y Zε 1 ) and assume that

19 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution z / Zε 2 ). Then x ψε 2 )y > 1 ε 2 θ 1 + ψ 2 ε 2 ), 1) x ψε 1 )y 1 ε 1 θ 1 + ψ 2 ε 1 ), 11) For α [, ψε )] we define an auxiliary function x 1 θ. 12) Ψα) = ψ 1 α) + θ 1 + α 2 1) and set α i = ψε i ), i =, 1, 2. From 1) 12) it follows that Ψα 2 ) α 2 > y > Ψα 1) Ψα 2 ) α 1 α 2. 13) Since Ψ is convex, increasing, and Ψ) =, 13) is contradictory and we conclude that Zε 1 ) Zε 2 ), hence i) holds. It remains to prove the Lipschitz estimate in ii). Let z Zε 2 )\ Z ε 1 ) be arbitrary. With the above notation we have We find α [α 2, α 1 [ such that z, ν α2 1 θ Ψα 2 ), 14) z, ν α1 > 1 θ Ψα 1 ). 15) z, ν α = 1 θ Ψα ), 16) and put ε = ψ 1 α ), z 1 = z σν α1, where σ > is chosen in such a way that z 1, ν α1 = 1 θ Ψα 1 ), 17) that is, We have σ = 1 z, ν 1 + α1 2 α1 1 + θ + Ψα 1 )). z 1 2 = z 2 σ 2 ν α1 2 2σ 1 θ Ψα 1 )) < z 2 1 θ) 2, hence z 1 Zε 1 ). Our goal now is to find R > independent of ε 1, ε 2 such that z z 1 R ε 1 ε ), 18) and it will suffice to pass from Zε i ) to Zε i ), i = 1, 2, to complete the proof. Inequality 18) will follow from a series of estimates, where C 1, C 2,... will denote arbitrary positive constants depending only on K. First of all, we have z 1 θ)ν α ν α 2 ) 1 θ) 2 21 θ) 1 θ Ψα )) 19) 1 θ) α 2 + 2ψ 1 α ) ) C 1 ε.

20 13 M. Brokate, P. Krejčí, H. Schnabel / On Uniqueness in Evolution... On the other hand, we have z z 1 = σ ν α1 σ ν α1 2 = z z 1, ν α1 11) = z 1 θ)ν α, ν α1 ν α + 1 θ) ν α, ν α1 ν α + Ψα 1 ) Ψα ) C 1 ε ν α1 ν α + 1 θ να1 2 ν α 2) + Ψα 1 ) Ψα ) 2 C 2 ε α 1 α ) + ε 1 ε ) + α 2 1 α 2 ) ), where, by 78) 79), we have α 1 α 2K ε 1 ε ) and and 18) immediately follows. ε1 α1 2 α 2 = 2 ψε) ψ ε) dε 4K 2 ε 1 ε ), ε Acknowledgements. The authors thank one of the referees for the suggestion that Proposition 4.1 might follow directly from Moreau s results. This turned out to be right, as the exposition above shows. References [1] P. Ballard: A counter-example to uniqueness in quasi-static elastic contact problems with friction, Int. J. Eng. Sci ) [2] V. V. Chernorutskii, M. A. Krasnosel skii: Hysteresis systems with variable characteristics, Nonlinear Anal. TMA ) [3] R. E. Edwards: Functional Analysis, Holt, Rinehart and Winston, New York 1965). [4] P. Krejčí: Evolution variational inequalities and multidimensional hysteresis operators, in: Nonlinear Differential Equations, P. Drábek, P. Krejčí, P. Takáč eds.), Research Notes in Mathematics 44, Chapman & Hall/CRC, London 1999) [5] P. Krejčí, Ph. Laurençot: Generalized variational inequalities, J. Convex Analysis 9 22) [6] P. Krejčí, J. Sprekels: Singular limit in parabolic differential inclusions and the stop operator, Interfaces Free Bound. 4 22) [7] M. Kunze, M. Monteiro Marques: An introduction to Moreau s sweeping process, in: Impacts in Mechanical Systems - Analysis and Modelling, B. Brogliato ed.), Lecture Notes in Physics 551, Springer 2) 1 6. [8] M. Kunze, M. Monteiro Marques: On parabolic quasi-variational inequalities and statedependent sweeping processes, Topol. Methods Nonlinear Anal ) [9] A. Mielke, F. Theil: On rate-independent hysteresis models, Preprint #21/7, SFB 44, Universität Stuttgart, 21. [1] J.-J. Moreau: Problème d évolution associé à un convexe mobile d un espace hilbertien, C. R. Acad. Sci. Paris Sér. A-B ) A791 A794. [11] J.-J. Moreau: Evolution problem associated with a moving convex set in a Hilbert space, J. Diff. Eq ) [12] R. T. Rockafellar: Convex Analysis, Princeton University Press, Princeton 197).

Obstacle problems and isotonicity

Obstacle problems and isotonicity Obstacle problems and isotonicity Thomas I. Seidman Revised version for NA-TMA: NA-D-06-00007R1+ [June 6, 2006] Abstract For variational inequalities of an abstract obstacle type, a comparison principle

More information

Lebesgue-Stieltjes measures and the play operator

Lebesgue-Stieltjes measures and the play operator Lebesgue-Stieltjes measures and the play operator Vincenzo Recupero Politecnico di Torino, Dipartimento di Matematica Corso Duca degli Abruzzi, 24, 10129 Torino - Italy E-mail: vincenzo.recupero@polito.it

More information

Functional Analysis. Martin Brokate. 1 Normed Spaces 2. 2 Hilbert Spaces The Principle of Uniform Boundedness 32

Functional Analysis. Martin Brokate. 1 Normed Spaces 2. 2 Hilbert Spaces The Principle of Uniform Boundedness 32 Functional Analysis Martin Brokate Contents 1 Normed Spaces 2 2 Hilbert Spaces 2 3 The Principle of Uniform Boundedness 32 4 Extension, Reflexivity, Separation 37 5 Compact subsets of C and L p 46 6 Weak

More information

NONTRIVIAL SOLUTIONS FOR SUPERQUADRATIC NONAUTONOMOUS PERIODIC SYSTEMS. Shouchuan Hu Nikolas S. Papageorgiou. 1. Introduction

NONTRIVIAL SOLUTIONS FOR SUPERQUADRATIC NONAUTONOMOUS PERIODIC SYSTEMS. Shouchuan Hu Nikolas S. Papageorgiou. 1. Introduction Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 34, 29, 327 338 NONTRIVIAL SOLUTIONS FOR SUPERQUADRATIC NONAUTONOMOUS PERIODIC SYSTEMS Shouchuan Hu Nikolas S. Papageorgiou

More information

Some Properties of the Augmented Lagrangian in Cone Constrained Optimization

Some Properties of the Augmented Lagrangian in Cone Constrained Optimization MATHEMATICS OF OPERATIONS RESEARCH Vol. 29, No. 3, August 2004, pp. 479 491 issn 0364-765X eissn 1526-5471 04 2903 0479 informs doi 10.1287/moor.1040.0103 2004 INFORMS Some Properties of the Augmented

More information

Hysteresis rarefaction in the Riemann problem

Hysteresis rarefaction in the Riemann problem Hysteresis rarefaction in the Riemann problem Pavel Krejčí 1 Institute of Mathematics, Czech Academy of Sciences, Žitná 25, 11567 Praha 1, Czech Republic E-mail: krejci@math.cas.cz Abstract. We consider

More information

An introduction to Mathematical Theory of Control

An introduction to Mathematical Theory of Control An introduction to Mathematical Theory of Control Vasile Staicu University of Aveiro UNICA, May 2018 Vasile Staicu (University of Aveiro) An introduction to Mathematical Theory of Control UNICA, May 2018

More information

LOCAL FIXED POINT THEORY INVOLVING THREE OPERATORS IN BANACH ALGEBRAS. B. C. Dhage. 1. Introduction

LOCAL FIXED POINT THEORY INVOLVING THREE OPERATORS IN BANACH ALGEBRAS. B. C. Dhage. 1. Introduction Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 24, 24, 377 386 LOCAL FIXED POINT THEORY INVOLVING THREE OPERATORS IN BANACH ALGEBRAS B. C. Dhage Abstract. The present

More information

ON WEAKLY NONLINEAR BACKWARD PARABOLIC PROBLEM

ON WEAKLY NONLINEAR BACKWARD PARABOLIC PROBLEM ON WEAKLY NONLINEAR BACKWARD PARABOLIC PROBLEM OLEG ZUBELEVICH DEPARTMENT OF MATHEMATICS THE BUDGET AND TREASURY ACADEMY OF THE MINISTRY OF FINANCE OF THE RUSSIAN FEDERATION 7, ZLATOUSTINSKY MALIY PER.,

More information

PERIODIC PROBLEMS WITH φ-laplacian INVOLVING NON-ORDERED LOWER AND UPPER FUNCTIONS

PERIODIC PROBLEMS WITH φ-laplacian INVOLVING NON-ORDERED LOWER AND UPPER FUNCTIONS Fixed Point Theory, Volume 6, No. 1, 25, 99-112 http://www.math.ubbcluj.ro/ nodeacj/sfptcj.htm PERIODIC PROBLEMS WITH φ-laplacian INVOLVING NON-ORDERED LOWER AND UPPER FUNCTIONS IRENA RACHŮNKOVÁ1 AND MILAN

More information

Institut für Mathematik

Institut für Mathematik U n i v e r s i t ä t A u g s b u r g Institut für Mathematik Martin Rasmussen, Peter Giesl A Note on Almost Periodic Variational Equations Preprint Nr. 13/28 14. März 28 Institut für Mathematik, Universitätsstraße,

More information

AW -Convergence and Well-Posedness of Non Convex Functions

AW -Convergence and Well-Posedness of Non Convex Functions Journal of Convex Analysis Volume 10 (2003), No. 2, 351 364 AW -Convergence Well-Posedness of Non Convex Functions Silvia Villa DIMA, Università di Genova, Via Dodecaneso 35, 16146 Genova, Italy villa@dima.unige.it

More information

SYNCHRONIZATION OF NONAUTONOMOUS DYNAMICAL SYSTEMS

SYNCHRONIZATION OF NONAUTONOMOUS DYNAMICAL SYSTEMS Electronic Journal of Differential Equations, Vol. 003003, No. 39, pp. 1 10. ISSN: 107-6691. URL: http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu login: ftp SYNCHRONIZATION OF

More information

Stability for solution of Differential Variational Inequalitiy

Stability for solution of Differential Variational Inequalitiy Stability for solution of Differential Variational Inequalitiy Jian-xun Zhao Department of Mathematics, School of Science, Tianjin University Tianjin 300072, P.R. China Abstract In this paper we study

More information

The local equicontinuity of a maximal monotone operator

The local equicontinuity of a maximal monotone operator arxiv:1410.3328v2 [math.fa] 3 Nov 2014 The local equicontinuity of a maximal monotone operator M.D. Voisei Abstract The local equicontinuity of an operator T : X X with proper Fitzpatrick function ϕ T

More information

A Concise Course on Stochastic Partial Differential Equations

A Concise Course on Stochastic Partial Differential Equations A Concise Course on Stochastic Partial Differential Equations Michael Röckner Reference: C. Prevot, M. Röckner: Springer LN in Math. 1905, Berlin (2007) And see the references therein for the original

More information

2 Statement of the problem and assumptions

2 Statement of the problem and assumptions Mathematical Notes, 25, vol. 78, no. 4, pp. 466 48. Existence Theorem for Optimal Control Problems on an Infinite Time Interval A.V. Dmitruk and N.V. Kuz kina We consider an optimal control problem on

More information

Locally Lipschitzian Guiding Function Method for ODEs.

Locally Lipschitzian Guiding Function Method for ODEs. Locally Lipschitzian Guiding Function Method for ODEs. Marta Lewicka International School for Advanced Studies, SISSA, via Beirut 2-4, 3414 Trieste, Italy. E-mail: lewicka@sissa.it 1 Introduction Let f

More information

The Bang-Bang theorem via Baire category. A Dual Approach

The Bang-Bang theorem via Baire category. A Dual Approach The Bang-Bang theorem via Baire category A Dual Approach Alberto Bressan Marco Mazzola, and Khai T Nguyen (*) Department of Mathematics, Penn State University (**) Université Pierre et Marie Curie, Paris

More information

ON WEAK SOLUTION OF A HYPERBOLIC DIFFERENTIAL INCLUSION WITH NONMONOTONE DISCONTINUOUS NONLINEAR TERM

ON WEAK SOLUTION OF A HYPERBOLIC DIFFERENTIAL INCLUSION WITH NONMONOTONE DISCONTINUOUS NONLINEAR TERM Internat. J. Math. & Math. Sci. Vol. 22, No. 3 (999 587 595 S 6-72 9922587-2 Electronic Publishing House ON WEAK SOLUTION OF A HYPERBOLIC DIFFERENTIAL INCLUSION WITH NONMONOTONE DISCONTINUOUS NONLINEAR

More information

On the Well-Posedness of the Cauchy Problem for a Neutral Differential Equation with Distributed Prehistory

On the Well-Posedness of the Cauchy Problem for a Neutral Differential Equation with Distributed Prehistory Bulletin of TICMI Vol. 21, No. 1, 2017, 3 8 On the Well-Posedness of the Cauchy Problem for a Neutral Differential Equation with Distributed Prehistory Tamaz Tadumadze I. Javakhishvili Tbilisi State University

More information

2. Dual space is essential for the concept of gradient which, in turn, leads to the variational analysis of Lagrange multipliers.

2. Dual space is essential for the concept of gradient which, in turn, leads to the variational analysis of Lagrange multipliers. Chapter 3 Duality in Banach Space Modern optimization theory largely centers around the interplay of a normed vector space and its corresponding dual. The notion of duality is important for the following

More information

On the wellposedness of the Chaboche model

On the wellposedness of the Chaboche model On the wellposedness of the Chaboche model Martin Brokate Mathematisches Seminar Universität Kiel 24098 Kiel Germany Pavel Krejčí nstitute of Mathematics Academy of Sciences Žitná 25 11567 Praha Czech

More information

LECTURE 15: COMPLETENESS AND CONVEXITY

LECTURE 15: COMPLETENESS AND CONVEXITY LECTURE 15: COMPLETENESS AND CONVEXITY 1. The Hopf-Rinow Theorem Recall that a Riemannian manifold (M, g) is called geodesically complete if the maximal defining interval of any geodesic is R. On the other

More information

LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS. S. G. Bobkov and F. L. Nazarov. September 25, 2011

LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS. S. G. Bobkov and F. L. Nazarov. September 25, 2011 LARGE DEVIATIONS OF TYPICAL LINEAR FUNCTIONALS ON A CONVEX BODY WITH UNCONDITIONAL BASIS S. G. Bobkov and F. L. Nazarov September 25, 20 Abstract We study large deviations of linear functionals on an isotropic

More information

Neighboring feasible trajectories in infinite dimension

Neighboring feasible trajectories in infinite dimension Neighboring feasible trajectories in infinite dimension Marco Mazzola Université Pierre et Marie Curie (Paris 6) H. Frankowska and E. M. Marchini Control of State Constrained Dynamical Systems Padova,

More information

Epiconvergence and ε-subgradients of Convex Functions

Epiconvergence and ε-subgradients of Convex Functions Journal of Convex Analysis Volume 1 (1994), No.1, 87 100 Epiconvergence and ε-subgradients of Convex Functions Andrei Verona Department of Mathematics, California State University Los Angeles, CA 90032,

More information

Extremal Solutions of Differential Inclusions via Baire Category: a Dual Approach

Extremal Solutions of Differential Inclusions via Baire Category: a Dual Approach Extremal Solutions of Differential Inclusions via Baire Category: a Dual Approach Alberto Bressan Department of Mathematics, Penn State University University Park, Pa 1682, USA e-mail: bressan@mathpsuedu

More information

An Integral-type Constraint Qualification for Optimal Control Problems with State Constraints

An Integral-type Constraint Qualification for Optimal Control Problems with State Constraints An Integral-type Constraint Qualification for Optimal Control Problems with State Constraints S. Lopes, F. A. C. C. Fontes and M. d. R. de Pinho Officina Mathematica report, April 4, 27 Abstract Standard

More information

A convergence result for an Outer Approximation Scheme

A convergence result for an Outer Approximation Scheme A convergence result for an Outer Approximation Scheme R. S. Burachik Engenharia de Sistemas e Computação, COPPE-UFRJ, CP 68511, Rio de Janeiro, RJ, CEP 21941-972, Brazil regi@cos.ufrj.br J. O. Lopes Departamento

More information

FINITE-DIFFERENCE APPROXIMATIONS AND OPTIMAL CONTROL OF THE SWEEPING PROCESS. BORIS MORDUKHOVICH Wayne State University, USA

FINITE-DIFFERENCE APPROXIMATIONS AND OPTIMAL CONTROL OF THE SWEEPING PROCESS. BORIS MORDUKHOVICH Wayne State University, USA FINITE-DIFFERENCE APPROXIMATIONS AND OPTIMAL CONTROL OF THE SWEEPING PROCESS BORIS MORDUKHOVICH Wayne State University, USA International Workshop Optimization without Borders Tribute to Yurii Nesterov

More information

SOME PROPERTIES ON THE CLOSED SUBSETS IN BANACH SPACES

SOME PROPERTIES ON THE CLOSED SUBSETS IN BANACH SPACES ARCHIVUM MATHEMATICUM (BRNO) Tomus 42 (2006), 167 174 SOME PROPERTIES ON THE CLOSED SUBSETS IN BANACH SPACES ABDELHAKIM MAADEN AND ABDELKADER STOUTI Abstract. It is shown that under natural assumptions,

More information

BIHARMONIC WAVE MAPS INTO SPHERES

BIHARMONIC WAVE MAPS INTO SPHERES BIHARMONIC WAVE MAPS INTO SPHERES SEBASTIAN HERR, TOBIAS LAMM, AND ROLAND SCHNAUBELT Abstract. A global weak solution of the biharmonic wave map equation in the energy space for spherical targets is constructed.

More information

Singularities and Laplacians in Boundary Value Problems for Nonlinear Ordinary Differential Equations

Singularities and Laplacians in Boundary Value Problems for Nonlinear Ordinary Differential Equations Singularities and Laplacians in Boundary Value Problems for Nonlinear Ordinary Differential Equations Irena Rachůnková, Svatoslav Staněk, Department of Mathematics, Palacký University, 779 OLOMOUC, Tomkova

More information

Nontrivial Solutions for Boundary Value Problems of Nonlinear Differential Equation

Nontrivial Solutions for Boundary Value Problems of Nonlinear Differential Equation Advances in Dynamical Systems and Applications ISSN 973-532, Volume 6, Number 2, pp. 24 254 (2 http://campus.mst.edu/adsa Nontrivial Solutions for Boundary Value Problems of Nonlinear Differential Equation

More information

Functional Analysis. Franck Sueur Metric spaces Definitions Completeness Compactness Separability...

Functional Analysis. Franck Sueur Metric spaces Definitions Completeness Compactness Separability... Functional Analysis Franck Sueur 2018-2019 Contents 1 Metric spaces 1 1.1 Definitions........................................ 1 1.2 Completeness...................................... 3 1.3 Compactness......................................

More information

NONLINEAR DIFFERENTIAL INEQUALITY. 1. Introduction. In this paper the following nonlinear differential inequality

NONLINEAR DIFFERENTIAL INEQUALITY. 1. Introduction. In this paper the following nonlinear differential inequality M athematical Inequalities & Applications [2407] First Galley Proofs NONLINEAR DIFFERENTIAL INEQUALITY N. S. HOANG AND A. G. RAMM Abstract. A nonlinear differential inequality is formulated in the paper.

More information

On Discontinuous Differential Equations

On Discontinuous Differential Equations On Discontinuous Differential Equations Alberto Bressan and Wen Shen S.I.S.S.A., Via Beirut 4, Trieste 3414 Italy. Department of Informatics, University of Oslo, P.O. Box 18 Blindern, N-316 Oslo, Norway.

More information

On smoothness properties of optimal value functions at the boundary of their domain under complete convexity

On smoothness properties of optimal value functions at the boundary of their domain under complete convexity On smoothness properties of optimal value functions at the boundary of their domain under complete convexity Oliver Stein # Nathan Sudermann-Merx June 14, 2013 Abstract This article studies continuity

More information

On intermediate value theorem in ordered Banach spaces for noncompact and discontinuous mappings

On intermediate value theorem in ordered Banach spaces for noncompact and discontinuous mappings Int. J. Nonlinear Anal. Appl. 7 (2016) No. 1, 295-300 ISSN: 2008-6822 (electronic) http://dx.doi.org/10.22075/ijnaa.2015.341 On intermediate value theorem in ordered Banach spaces for noncompact and discontinuous

More information

Subdifferential representation of convex functions: refinements and applications

Subdifferential representation of convex functions: refinements and applications Subdifferential representation of convex functions: refinements and applications Joël Benoist & Aris Daniilidis Abstract Every lower semicontinuous convex function can be represented through its subdifferential

More information

ASYMPTOTICALLY NONEXPANSIVE MAPPINGS IN MODULAR FUNCTION SPACES ABSTRACT

ASYMPTOTICALLY NONEXPANSIVE MAPPINGS IN MODULAR FUNCTION SPACES ABSTRACT ASYMPTOTICALLY NONEXPANSIVE MAPPINGS IN MODULAR FUNCTION SPACES T. DOMINGUEZ-BENAVIDES, M.A. KHAMSI AND S. SAMADI ABSTRACT In this paper, we prove that if ρ is a convex, σ-finite modular function satisfying

More information

Nonlinear Analysis 71 (2009) Contents lists available at ScienceDirect. Nonlinear Analysis. journal homepage:

Nonlinear Analysis 71 (2009) Contents lists available at ScienceDirect. Nonlinear Analysis. journal homepage: Nonlinear Analysis 71 2009 2744 2752 Contents lists available at ScienceDirect Nonlinear Analysis journal homepage: www.elsevier.com/locate/na A nonlinear inequality and applications N.S. Hoang A.G. Ramm

More information

UNCERTAINTY FUNCTIONAL DIFFERENTIAL EQUATIONS FOR FINANCE

UNCERTAINTY FUNCTIONAL DIFFERENTIAL EQUATIONS FOR FINANCE Surveys in Mathematics and its Applications ISSN 1842-6298 (electronic), 1843-7265 (print) Volume 5 (2010), 275 284 UNCERTAINTY FUNCTIONAL DIFFERENTIAL EQUATIONS FOR FINANCE Iuliana Carmen Bărbăcioru Abstract.

More information

Parameter Dependent Quasi-Linear Parabolic Equations

Parameter Dependent Quasi-Linear Parabolic Equations CADERNOS DE MATEMÁTICA 4, 39 33 October (23) ARTIGO NÚMERO SMA#79 Parameter Dependent Quasi-Linear Parabolic Equations Cláudia Buttarello Gentile Departamento de Matemática, Universidade Federal de São

More information

AN EFFECTIVE METRIC ON C(H, K) WITH NORMAL STRUCTURE. Mona Nabiei (Received 23 June, 2015)

AN EFFECTIVE METRIC ON C(H, K) WITH NORMAL STRUCTURE. Mona Nabiei (Received 23 June, 2015) NEW ZEALAND JOURNAL OF MATHEMATICS Volume 46 (2016), 53-64 AN EFFECTIVE METRIC ON C(H, K) WITH NORMAL STRUCTURE Mona Nabiei (Received 23 June, 2015) Abstract. This study first defines a new metric with

More information

56 4 Integration against rough paths

56 4 Integration against rough paths 56 4 Integration against rough paths comes to the definition of a rough integral we typically take W = LV, W ; although other choices can be useful see e.g. remark 4.11. In the context of rough differential

More information

Robustness for a Liouville type theorem in exterior domains

Robustness for a Liouville type theorem in exterior domains Robustness for a Liouville type theorem in exterior domains Juliette Bouhours 1 arxiv:1207.0329v3 [math.ap] 24 Oct 2014 1 UPMC Univ Paris 06, UMR 7598, Laboratoire Jacques-Louis Lions, F-75005, Paris,

More information

Nonlinear D-set contraction mappings in partially ordered normed linear spaces and applications to functional hybrid integral equations

Nonlinear D-set contraction mappings in partially ordered normed linear spaces and applications to functional hybrid integral equations Malaya J. Mat. 3(1)(215) 62 85 Nonlinear D-set contraction mappings in partially ordered normed linear spaces and applications to functional hybrid integral equations Bapurao C. Dhage Kasubai, Gurukul

More information

Geometry and topology of continuous best and near best approximations

Geometry and topology of continuous best and near best approximations Journal of Approximation Theory 105: 252 262, Geometry and topology of continuous best and near best approximations Paul C. Kainen Dept. of Mathematics Georgetown University Washington, D.C. 20057 Věra

More information

EXISTENCE OF PURE EQUILIBRIA IN GAMES WITH NONATOMIC SPACE OF PLAYERS. Agnieszka Wiszniewska Matyszkiel. 1. Introduction

EXISTENCE OF PURE EQUILIBRIA IN GAMES WITH NONATOMIC SPACE OF PLAYERS. Agnieszka Wiszniewska Matyszkiel. 1. Introduction Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 16, 2000, 339 349 EXISTENCE OF PURE EQUILIBRIA IN GAMES WITH NONATOMIC SPACE OF PLAYERS Agnieszka Wiszniewska Matyszkiel

More information

Vector hysteresis models

Vector hysteresis models Euro. Jnl. Appl. Math. 2 (99), 28 292 Vector hysteresis models Pavel Krejčí Matematický ústav ČSAV, Žitná 25 5 67 Praha, Czechoslovakia Key words: vector hysteresis operator, hysteresis potential, differential

More information

The Fitzpatrick Function and Nonreflexive Spaces

The Fitzpatrick Function and Nonreflexive Spaces Journal of Convex Analysis Volume 13 (2006), No. 3+4, 861 881 The Fitzpatrick Function and Nonreflexive Spaces S. Simons Department of Mathematics, University of California, Santa Barbara, CA 93106-3080,

More information

From now on, we will represent a metric space with (X, d). Here are some examples: i=1 (x i y i ) p ) 1 p, p 1.

From now on, we will represent a metric space with (X, d). Here are some examples: i=1 (x i y i ) p ) 1 p, p 1. Chapter 1 Metric spaces 1.1 Metric and convergence We will begin with some basic concepts. Definition 1.1. (Metric space) Metric space is a set X, with a metric satisfying: 1. d(x, y) 0, d(x, y) = 0 x

More information

On the Midpoint Method for Solving Generalized Equations

On the Midpoint Method for Solving Generalized Equations Punjab University Journal of Mathematics (ISSN 1016-56) Vol. 40 (008) pp. 63-70 On the Midpoint Method for Solving Generalized Equations Ioannis K. Argyros Cameron University Department of Mathematics

More information

The small ball property in Banach spaces (quantitative results)

The small ball property in Banach spaces (quantitative results) The small ball property in Banach spaces (quantitative results) Ehrhard Behrends Abstract A metric space (M, d) is said to have the small ball property (sbp) if for every ε 0 > 0 there exists a sequence

More information

INITIAL AND BOUNDARY VALUE PROBLEMS FOR NONCONVEX VALUED MULTIVALUED FUNCTIONAL DIFFERENTIAL EQUATIONS

INITIAL AND BOUNDARY VALUE PROBLEMS FOR NONCONVEX VALUED MULTIVALUED FUNCTIONAL DIFFERENTIAL EQUATIONS Applied Mathematics and Stochastic Analysis, 6:2 23, 9-2. Printed in the USA c 23 by North Atlantic Science Publishing Company INITIAL AND BOUNDARY VALUE PROBLEMS FOR NONCONVEX VALUED MULTIVALUED FUNCTIONAL

More information

for all subintervals I J. If the same is true for the dyadic subintervals I D J only, we will write ϕ BMO d (J). In fact, the following is true

for all subintervals I J. If the same is true for the dyadic subintervals I D J only, we will write ϕ BMO d (J). In fact, the following is true 3 ohn Nirenberg inequality, Part I A function ϕ L () belongs to the space BMO() if sup ϕ(s) ϕ I I I < for all subintervals I If the same is true for the dyadic subintervals I D only, we will write ϕ BMO

More information

On Friedrichs inequality, Helmholtz decomposition, vector potentials, and the div-curl lemma. Ben Schweizer 1

On Friedrichs inequality, Helmholtz decomposition, vector potentials, and the div-curl lemma. Ben Schweizer 1 On Friedrichs inequality, Helmholtz decomposition, vector potentials, and the div-curl lemma Ben Schweizer 1 January 16, 2017 Abstract: We study connections between four different types of results that

More information

ẋ = f(x, y), ẏ = g(x, y), (x, y) D, can only have periodic solutions if (f,g) changes sign in D or if (f,g)=0in D.

ẋ = f(x, y), ẏ = g(x, y), (x, y) D, can only have periodic solutions if (f,g) changes sign in D or if (f,g)=0in D. 4 Periodic Solutions We have shown that in the case of an autonomous equation the periodic solutions correspond with closed orbits in phase-space. Autonomous two-dimensional systems with phase-space R

More information

ON THE ANALYSIS OF A VISCOPLASTIC CONTACT PROBLEM WITH TIME DEPENDENT TRESCA S FRIC- TION LAW

ON THE ANALYSIS OF A VISCOPLASTIC CONTACT PROBLEM WITH TIME DEPENDENT TRESCA S FRIC- TION LAW Electron. J. M ath. Phys. Sci. 22, 1, 1,47 71 Electronic Journal of Mathematical and Physical Sciences EJMAPS ISSN: 1538-263X www.ejmaps.org ON THE ANALYSIS OF A VISCOPLASTIC CONTACT PROBLEM WITH TIME

More information

On duality theory of conic linear problems

On duality theory of conic linear problems On duality theory of conic linear problems Alexander Shapiro School of Industrial and Systems Engineering, Georgia Institute of Technology, Atlanta, Georgia 3332-25, USA e-mail: ashapiro@isye.gatech.edu

More information

Observer design for a general class of triangular systems

Observer design for a general class of triangular systems 1st International Symposium on Mathematical Theory of Networks and Systems July 7-11, 014. Observer design for a general class of triangular systems Dimitris Boskos 1 John Tsinias Abstract The paper deals

More information

KRASNOSELSKII-TYPE FIXED POINT THEOREMS UNDER WEAK TOPOLOGY SETTINGS AND APPLICATIONS

KRASNOSELSKII-TYPE FIXED POINT THEOREMS UNDER WEAK TOPOLOGY SETTINGS AND APPLICATIONS Electronic Journal of Differential Equations, Vol. 21(21), No. 35, pp. 1 15. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu KRASNOSELSKII-TYPE FIXED

More information

Differentiability of Convex Functions on a Banach Space with Smooth Bump Function 1

Differentiability of Convex Functions on a Banach Space with Smooth Bump Function 1 Journal of Convex Analysis Volume 1 (1994), No.1, 47 60 Differentiability of Convex Functions on a Banach Space with Smooth Bump Function 1 Li Yongxin, Shi Shuzhong Nankai Institute of Mathematics Tianjin,

More information

EXISTENCE OF SOLUTIONS TO A BOUNDARY-VALUE PROBLEM FOR AN INFINITE SYSTEM OF DIFFERENTIAL EQUATIONS

EXISTENCE OF SOLUTIONS TO A BOUNDARY-VALUE PROBLEM FOR AN INFINITE SYSTEM OF DIFFERENTIAL EQUATIONS Electronic Journal of Differential Equations, Vol. 217 (217, No. 262, pp. 1 12. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu EXISTENCE OF SOLUTIONS TO A BOUNDARY-VALUE

More information

On a general definition of transition waves and their properties

On a general definition of transition waves and their properties On a general definition of transition waves and their properties Henri Berestycki a and François Hamel b a EHESS, CAMS, 54 Boulevard Raspail, F-75006 Paris, France b Université Aix-Marseille III, LATP,

More information

A NOTE ON ALMOST PERIODIC VARIATIONAL EQUATIONS

A NOTE ON ALMOST PERIODIC VARIATIONAL EQUATIONS A NOTE ON ALMOST PERIODIC VARIATIONAL EQUATIONS PETER GIESL AND MARTIN RASMUSSEN Abstract. The variational equation of a nonautonomous differential equation ẋ = F t, x) along a solution µ is given by ẋ

More information

Nonlinear Control Systems

Nonlinear Control Systems Nonlinear Control Systems António Pedro Aguiar pedro@isr.ist.utl.pt 3. Fundamental properties IST-DEEC PhD Course http://users.isr.ist.utl.pt/%7epedro/ncs2012/ 2012 1 Example Consider the system ẋ = f

More information

Centre d Economie de la Sorbonne UMR 8174

Centre d Economie de la Sorbonne UMR 8174 Centre d Economie de la Sorbonne UMR 8174 On alternative theorems and necessary conditions for efficiency Do Van LUU Manh Hung NGUYEN 2006.19 Maison des Sciences Économiques, 106-112 boulevard de L'Hôpital,

More information

The Skorokhod problem in a time-dependent interval

The Skorokhod problem in a time-dependent interval The Skorokhod problem in a time-dependent interval Krzysztof Burdzy, Weining Kang and Kavita Ramanan University of Washington and Carnegie Mellon University Abstract: We consider the Skorokhod problem

More information

EXISTENCE AND UNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH LINEAR PROGRAMS EMBEDDED

EXISTENCE AND UNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH LINEAR PROGRAMS EMBEDDED EXISTENCE AND UNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH LINEAR PROGRAMS EMBEDDED STUART M. HARWOOD AND PAUL I. BARTON Key words. linear programs, ordinary differential equations, embedded

More information

EXISTENCE OF THREE WEAK SOLUTIONS FOR A QUASILINEAR DIRICHLET PROBLEM. Saeid Shokooh and Ghasem A. Afrouzi. 1. Introduction

EXISTENCE OF THREE WEAK SOLUTIONS FOR A QUASILINEAR DIRICHLET PROBLEM. Saeid Shokooh and Ghasem A. Afrouzi. 1. Introduction MATEMATIČKI VESNIK MATEMATIQKI VESNIK 69 4 (217 271 28 December 217 research paper originalni nauqni rad EXISTENCE OF THREE WEAK SOLUTIONS FOR A QUASILINEAR DIRICHLET PROBLEM Saeid Shokooh and Ghasem A.

More information

On a Class of Multidimensional Optimal Transportation Problems

On a Class of Multidimensional Optimal Transportation Problems Journal of Convex Analysis Volume 10 (2003), No. 2, 517 529 On a Class of Multidimensional Optimal Transportation Problems G. Carlier Université Bordeaux 1, MAB, UMR CNRS 5466, France and Université Bordeaux

More information

Threshold solutions and sharp transitions for nonautonomous parabolic equations on R N

Threshold solutions and sharp transitions for nonautonomous parabolic equations on R N Threshold solutions and sharp transitions for nonautonomous parabolic equations on R N P. Poláčik School of Mathematics, University of Minnesota Minneapolis, MN 55455 Abstract This paper is devoted to

More information

The first order quasi-linear PDEs

The first order quasi-linear PDEs Chapter 2 The first order quasi-linear PDEs The first order quasi-linear PDEs have the following general form: F (x, u, Du) = 0, (2.1) where x = (x 1, x 2,, x 3 ) R n, u = u(x), Du is the gradient of u.

More information

GENERAL NONCONVEX SPLIT VARIATIONAL INEQUALITY PROBLEMS. Jong Kyu Kim, Salahuddin, and Won Hee Lim

GENERAL NONCONVEX SPLIT VARIATIONAL INEQUALITY PROBLEMS. Jong Kyu Kim, Salahuddin, and Won Hee Lim Korean J. Math. 25 (2017), No. 4, pp. 469 481 https://doi.org/10.11568/kjm.2017.25.4.469 GENERAL NONCONVEX SPLIT VARIATIONAL INEQUALITY PROBLEMS Jong Kyu Kim, Salahuddin, and Won Hee Lim Abstract. In this

More information

Relative Controllability of Fractional Dynamical Systems with Multiple Delays in Control

Relative Controllability of Fractional Dynamical Systems with Multiple Delays in Control Chapter 4 Relative Controllability of Fractional Dynamical Systems with Multiple Delays in Control 4.1 Introduction A mathematical model for the dynamical systems with delayed controls denoting time varying

More information

A TWO PARAMETERS AMBROSETTI PRODI PROBLEM*

A TWO PARAMETERS AMBROSETTI PRODI PROBLEM* PORTUGALIAE MATHEMATICA Vol. 53 Fasc. 3 1996 A TWO PARAMETERS AMBROSETTI PRODI PROBLEM* C. De Coster** and P. Habets 1 Introduction The study of the Ambrosetti Prodi problem has started with the paper

More information

Variational and Topological methods : Theory, Applications, Numerical Simulations, and Open Problems 6-9 June 2012, Northern Arizona University

Variational and Topological methods : Theory, Applications, Numerical Simulations, and Open Problems 6-9 June 2012, Northern Arizona University Variational and Topological methods : Theory, Applications, Numerical Simulations, and Open Problems 6-9 June 22, Northern Arizona University Some methods using monotonicity for solving quasilinear parabolic

More information

Laplace s Equation. Chapter Mean Value Formulas

Laplace s Equation. Chapter Mean Value Formulas Chapter 1 Laplace s Equation Let be an open set in R n. A function u C 2 () is called harmonic in if it satisfies Laplace s equation n (1.1) u := D ii u = 0 in. i=1 A function u C 2 () is called subharmonic

More information

In this paper we study periodic solutions of a second order differential equation

In this paper we study periodic solutions of a second order differential equation Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 5, 1995, 385 396 A GRANAS TYPE APPROACH TO SOME CONTINUATION THEOREMS AND PERIODIC BOUNDARY VALUE PROBLEMS WITH IMPULSES

More information

Asymptotic behavior of Ginzburg-Landau equations of superfluidity

Asymptotic behavior of Ginzburg-Landau equations of superfluidity Communications to SIMAI Congress, ISSN 1827-9015, Vol. 3 (2009) 200 (12pp) DOI: 10.1685/CSC09200 Asymptotic behavior of Ginzburg-Landau equations of superfluidity Alessia Berti 1, Valeria Berti 2, Ivana

More information

Extreme points of compact convex sets

Extreme points of compact convex sets Extreme points of compact convex sets In this chapter, we are going to show that compact convex sets are determined by a proper subset, the set of its extreme points. Let us start with the main definition.

More information

Approximating solutions of nonlinear second order ordinary differential equations via Dhage iteration principle

Approximating solutions of nonlinear second order ordinary differential equations via Dhage iteration principle Malaya J. Mat. 4(1)(216) 8-18 Approximating solutions of nonlinear second order ordinary differential equations via Dhage iteration principle B. C. Dhage a,, S. B. Dhage a and S. K. Ntouyas b,c, a Kasubai,

More information

PATA TYPE FIXED POINT THEOREMS OF MULTIVALUED OPERATORS IN ORDERED METRIC SPACES WITH APPLICATIONS TO HYPERBOLIC DIFFERENTIAL INCLUSIONS

PATA TYPE FIXED POINT THEOREMS OF MULTIVALUED OPERATORS IN ORDERED METRIC SPACES WITH APPLICATIONS TO HYPERBOLIC DIFFERENTIAL INCLUSIONS U.P.B. Sci. Bull., Series A, Vol. 78, Iss. 4, 216 ISSN 1223-727 PATA TYPE FIXED POINT THEOREMS OF MULTIVALUED OPERATORS IN ORDERED METRIC SPACES WITH APPLICATIONS TO HYPERBOLIC DIFFERENTIAL INCLUSIONS

More information

Some Applications to Lebesgue Points in Variable Exponent Lebesgue Spaces

Some Applications to Lebesgue Points in Variable Exponent Lebesgue Spaces Çankaya University Journal of Science and Engineering Volume 7 (200), No. 2, 05 3 Some Applications to Lebesgue Points in Variable Exponent Lebesgue Spaces Rabil A. Mashiyev Dicle University, Department

More information

OPTIMAL SOLUTIONS TO STOCHASTIC DIFFERENTIAL INCLUSIONS

OPTIMAL SOLUTIONS TO STOCHASTIC DIFFERENTIAL INCLUSIONS APPLICATIONES MATHEMATICAE 29,4 (22), pp. 387 398 Mariusz Michta (Zielona Góra) OPTIMAL SOLUTIONS TO STOCHASTIC DIFFERENTIAL INCLUSIONS Abstract. A martingale problem approach is used first to analyze

More information

COUNTEREXAMPLES IN ROTUND AND LOCALLY UNIFORMLY ROTUND NORM

COUNTEREXAMPLES IN ROTUND AND LOCALLY UNIFORMLY ROTUND NORM Journal of Mathematical Analysis ISSN: 2217-3412, URL: http://www.ilirias.com Volume 5 Issue 1(2014), Pages 11-15. COUNTEREXAMPLES IN ROTUND AND LOCALLY UNIFORMLY ROTUND NORM F. HEYDARI, D. BEHMARDI 1

More information

arxiv: v1 [math.oc] 22 Sep 2016

arxiv: v1 [math.oc] 22 Sep 2016 EUIVALENCE BETWEEN MINIMAL TIME AND MINIMAL NORM CONTROL PROBLEMS FOR THE HEAT EUATION SHULIN IN AND GENGSHENG WANG arxiv:1609.06860v1 [math.oc] 22 Sep 2016 Abstract. This paper presents the equivalence

More information

Functional Differential Equations with Causal Operators

Functional Differential Equations with Causal Operators ISSN 1749-3889 (print), 1749-3897 (online) International Journal of Nonlinear Science Vol.11(211) No.4,pp.499-55 Functional Differential Equations with Causal Operators Vasile Lupulescu Constantin Brancusi

More information

HAIYUN ZHOU, RAVI P. AGARWAL, YEOL JE CHO, AND YONG SOO KIM

HAIYUN ZHOU, RAVI P. AGARWAL, YEOL JE CHO, AND YONG SOO KIM Georgian Mathematical Journal Volume 9 (2002), Number 3, 591 600 NONEXPANSIVE MAPPINGS AND ITERATIVE METHODS IN UNIFORMLY CONVEX BANACH SPACES HAIYUN ZHOU, RAVI P. AGARWAL, YEOL JE CHO, AND YONG SOO KIM

More information

EXISTENCE RESULTS FOR QUASILINEAR HEMIVARIATIONAL INEQUALITIES AT RESONANCE. Leszek Gasiński

EXISTENCE RESULTS FOR QUASILINEAR HEMIVARIATIONAL INEQUALITIES AT RESONANCE. Leszek Gasiński DISCRETE AND CONTINUOUS Website: www.aimsciences.org DYNAMICAL SYSTEMS SUPPLEMENT 2007 pp. 409 418 EXISTENCE RESULTS FOR QUASILINEAR HEMIVARIATIONAL INEQUALITIES AT RESONANCE Leszek Gasiński Jagiellonian

More information

Pseudo-Poincaré Inequalities and Applications to Sobolev Inequalities

Pseudo-Poincaré Inequalities and Applications to Sobolev Inequalities Pseudo-Poincaré Inequalities and Applications to Sobolev Inequalities Laurent Saloff-Coste Abstract Most smoothing procedures are via averaging. Pseudo-Poincaré inequalities give a basic L p -norm control

More information

ON THE ESSENTIAL BOUNDEDNESS OF SOLUTIONS TO PROBLEMS IN PIECEWISE LINEAR-QUADRATIC OPTIMAL CONTROL. R.T. Rockafellar*

ON THE ESSENTIAL BOUNDEDNESS OF SOLUTIONS TO PROBLEMS IN PIECEWISE LINEAR-QUADRATIC OPTIMAL CONTROL. R.T. Rockafellar* ON THE ESSENTIAL BOUNDEDNESS OF SOLUTIONS TO PROBLEMS IN PIECEWISE LINEAR-QUADRATIC OPTIMAL CONTROL R.T. Rockafellar* Dedicated to J-L. Lions on his 60 th birthday Abstract. Primal and dual problems of

More information

Appendix B Convex analysis

Appendix B Convex analysis This version: 28/02/2014 Appendix B Convex analysis In this appendix we review a few basic notions of convexity and related notions that will be important for us at various times. B.1 The Hausdorff distance

More information

ON CONTINUITY OF MEASURABLE COCYCLES

ON CONTINUITY OF MEASURABLE COCYCLES Journal of Applied Analysis Vol. 6, No. 2 (2000), pp. 295 302 ON CONTINUITY OF MEASURABLE COCYCLES G. GUZIK Received January 18, 2000 and, in revised form, July 27, 2000 Abstract. It is proved that every

More information

Boundedly complete weak-cauchy basic sequences in Banach spaces with the PCP

Boundedly complete weak-cauchy basic sequences in Banach spaces with the PCP Journal of Functional Analysis 253 (2007) 772 781 www.elsevier.com/locate/jfa Note Boundedly complete weak-cauchy basic sequences in Banach spaces with the PCP Haskell Rosenthal Department of Mathematics,

More information

b i (µ, x, s) ei ϕ(x) µ s (dx) ds (2) i=1

b i (µ, x, s) ei ϕ(x) µ s (dx) ds (2) i=1 NONLINEAR EVOLTION EQATIONS FOR MEASRES ON INFINITE DIMENSIONAL SPACES V.I. Bogachev 1, G. Da Prato 2, M. Röckner 3, S.V. Shaposhnikov 1 The goal of this work is to prove the existence of a solution to

More information

On Semicontinuity of Convex-valued Multifunctions and Cesari s Property (Q)

On Semicontinuity of Convex-valued Multifunctions and Cesari s Property (Q) On Semicontinuity of Convex-valued Multifunctions and Cesari s Property (Q) Andreas Löhne May 2, 2005 (last update: November 22, 2005) Abstract We investigate two types of semicontinuity for set-valued

More information