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Relaxation of functionals with linear growth: Interactions of emerging measures and free discontinuities

  • Stefan Krömer ORCID logo , Martin Kružík ORCID logo and Elvira Zappale ORCID logo EMAIL logo

Abstract

For an integral functional defined on functions ( u , v ) W 1 , 1 × L 1 featuring a prototypical strong interaction term between u and v, we calculate its relaxation in the space of functions with bounded variations and Radon measures. Interplay between measures and discontinuities brings various additional difficulties, and concentration effects in recovery sequences play a major role for the relaxed functional even if the limit measures are absolutely continuous with respect to the Lebesgue one.

MSC 2010: 49J45; 28A33

Communicated by Jan Kristensen


Award Identifier / Grant number: n. prot. U-UFMBAZ-2019-000458

Funding statement: E. Zappale is grateful to the Institute of Information Theory and Automation in Prague for its kind support and hospitality. She is a member of GNAMPA-INdAM, whose support is acknowledged. S. Krömer and M. Kružík are indebted to the Dipartimento di Ingegneria Industriale, University of Salerno (which E. Zappale was affiliated with during the course of this research) for support and hospitality during their stay there. The visit of S. Krömer at Dipartimento di Ingegneria Industriale, University of Salerno was partially sponsored by GNAMPA Project 2019 “Analisi ed Ottimizzazione di Strutture sottili”, coordinated by Marco Morandotti. Moreover, S. Krömer and M. Kružík were supported by the GAČR-FWF project 19-29646L.

A Proofs of auxiliary results

Here, we present the proofs of some of the auxiliary results collected in Section 2.

Proof of Proposition 2.6.

Clearly, it suffices to prove

¯ ( , , ) ¯ ( , , ) ,

the opposite inequality being trivial.

In order to achieve the desired conclusion, we argue as follows. For every A 𝒜 r ( Ω ¯ ) , denote by ¯ w the localized sequentially weak W 1 , 1 ( Ω A ; m ) × L 1 ( Ω A ; d ) lower semicontinuous envelope of F in (2.11). It was proved in [10] that for every A 𝒜 r ( Ω ¯ ) (so that A Ω can be any open subset of Ω),

¯ w ( u , v , A ) = Ω A ( f 1 ( u ) f 2 ( v ) + 𝒬 W ( u ) ) 𝑑 x for every  ( u , v ) W 1 , 1 ( Ω A ; m ) × L 1 ( Ω A ; d ) .

Since for every ( u , v ) W 1 , 1 ( Ω A ; m ) × L 1 ( Ω A ; d ) ,

¯ ( u , v , A ) ¯ w ( u , v , A ) ,

we infer that

¯ ( u , v , A ) = inf { lim inf k + ¯ ( u k , v k , A )
W 1 , 1 ( Ω A ; m ) × L 1 ( Ω A ; d ) ( u k , v k ) ( u , v )  in  BV ( Ω A ; m ) × ( A ; d ) }
inf { lim inf k + ¯ w ( u k , v k , A )
W 1 , 1 ( Ω A ; m ) × L 1 ( Ω A ; d ) ( u k , v k ) ( u , v )  in  BV ( Ω A ; m ) × ( A ; d ) }
= inf { lim inf k + A f 1 ( u k ) f 2 ( v k ) d x + A 𝒬 W ( u k ) d x |
W 1 , 1 ( Ω A ; m ) × L 1 ( Ω A ; d ) ( u k , v k ) ( u , v )  in  BV ( Ω A ; m ) × ( A ; d ) }

for every ( u , v ) BV ( Ω A ; m ) × ( A ; d ) , which concludes the proof. ∎

Proof of Proposition 2.7.

It suffices to show “ ”, as “ ” is trivial.

For every fixed k and u k BV ( Ω A ; m ) , we can choose a sequence ( w k , l ) l W 1 , 1 ( Ω A ; m ) such that, as l , we have w k , l * u k in BV ( Ω A ; m ) and

(A.1) Ω A 𝒬 W ( w k , l ) 𝑑 x = Ω A 𝑑 𝒬 W ( D u k ) ( x )

(any W 1 , 1 recovery sequence). For instance, since W 1 , 1 is dense in BV with respect to area strict convergence, there exists ( w k , l ) W 1 , 1 such that, as l , we have w k , l u k area-strictly, which yields (A.1) by Proposition 2.1. By (H3) (coercivity and growth of W), equation (A.1) implies that

lim sup l w k , l L 1 ( A ; m × n ) C ( 1 + | D u k | ( A ) )

with a constant C > 0 .

In addition, given any v k L 1 ( Ω A ; m ) , we also have that

Ω A f 1 ( w k , l ) f 2 ( v k ) 𝑑 x l Ω A f 1 ( u k ) f 2 ( v k ) 𝑑 x

by dominated convergence, also using that w k , l u k in L 1 , f 1 is bounded and f 2 ( v k ) L 1 ( Ω A ) .

If u k * u in BV and v k * v in , it is therefore possible to choose a diagonal sequence u ~ k := w k , l ( k ) , with l ( k ) fast enough as k , such that for

lim inf k Ω A f 1 ( u ~ k ) f 2 ( v k ) 𝑑 x + Ω A 𝒬 W ( u ~ k ) 𝑑 x
(A.2) = lim inf k Ω A f 1 ( u k ) f 2 ( v k ) 𝑑 x + Ω A 𝑑 𝒬 W ( D u k ) ( x ) ,

we have

lim sup k u ~ k L 1 ( Ω A ; m × n ) C ( 1 + lim sup k | D u k | ( Ω A ) )

and u ~ k u in L 1 ( Ω A ; m ) . In particular, u ~ k * u in BV ( Ω A ; m ) . This means that if

( u k , v k ) BV ( Ω A ; m ) × L 1 ( Ω A ; m )

is an arbitrary admissible sequence for the infimum defining ¯ in (2.13), then

( u ~ k , v k ) W 1 , 1 ( Ω A ; m ) × L 1 ( Ω A ; d )

is admissible, too. Hence, (A.2) yields the assertion. ∎

In the following, we will discuss the measure representation for the localized relaxed functionals, i.e., for A 𝒜 r ( Ω ¯ ) ,

¯ ( u , v , A ) := inf { lim inf k + F ( u k , v k , A ) ( u k , v k ) W 1 , 1 ( A ; m ) × L 1 ( A ; d ) ,
( u k , v k ) ( u , v )  in  BV ( A ; m ) × ( A ; d ) } .

Here, recall that by 𝒜 r ( Ω ¯ ) we denote the family of open subsets of Ω ¯ in the relative topology. The following result is a close relative of [1, Lemma 2.5].

Lemma A.1.

Let Ω ¯ be as above. Let λ : A r ( Ω ¯ ) [ 0 , + ) and μ be such that the following conditions hold:

  1. μ is a finite Radon measure on Ω ¯ .

  2. λ ( Ω ¯ ) μ ( Ω ¯ ) .

  3. λ ( A ) μ ( A ) for all A 𝒜 r ( Ω ¯ ) .

  4. (Subadditivity) λ ( A ) λ ( A U ¯ ) + λ ( B ) for all A , B , U 𝒜 r ( Ω ¯ ) such that U B A .

  5. For all A 𝒜 r ( Ω ¯ ) and ε > 0 , there exists U 𝒜 r ( Ω ¯ ) such that U A and λ ( A U ¯ ) < ε .

Then λ = μ on A r ( Ω ¯ ) .

Proof.

The inequality λ ( A ) μ ( A ) for every A 𝒜 r ( Ω ¯ ) follows from (iii).

For what concerns the other inequality, we can observe that, by the inner regularity of μ, we can find a relatively open subset of Ω ¯ , say A A , such that

μ ( A ) < ε + μ ( A ¯ )
= ε + μ ( Ω ¯ ) - μ ( Ω ¯ A ¯ )
ε + λ ( Ω ¯ ) - λ ( Ω ¯ A ¯ )
ε + λ ( A ) .

Thus, letting ε 0 , we obtain the desired conclusion. ∎

Proof of Lemma 2.8.

In order to prove that ¯ ( u , v , A ) is the trace of a Radon measure, we refer to Lemma A.1, and define the increasing set function λ : 𝒜 r ( Ω ¯ ) [ 0 , + ] by

λ ( A ) := ¯ ( u , v , A ) .

By the definition of ¯ , we know that there exists a sequence ( u h , v h ) W 1 , 1 ( Ω ; m ) × L 1 ( Ω ; d ) such that u h u in BV ( Ω ; m ) and v h v in ( Ω ¯ ; d ) such that

¯ ( u , v , Ω ¯ ) = lim h + Ω ( f 1 ( u h ) f 2 ( v h ) + W ( u h ) ) 𝑑 x = λ ( Ω ¯ ) .

Next, denoting by λ h the measures ( f 1 ( u h ) f 2 ( v h ) + W ( u h ) n , we obtain that it converges weakly * in the sense of measures (duality with elements in C ( Ω ¯ ) ), up to a subsequence (due to the bounds) to a measure μ. Now, due to the lower semicontinuity with respect to the weak* convergence, we have

μ ( Ω ¯ ) lim inf h λ h ( Ω ¯ ) = λ ( Ω ¯ ) .

Then, by the definition of λ, we have, for every A 𝒜 r ( Ω ¯ ) ,

λ ( A ) lim inf h Ω A ( f 1 ( u h ) f 2 ( v h ) + W ( u h ) ) 𝑑 x μ ( A ¯ ) .

Now by the previous lemma, we would have that λ = μ if we prove inner regularity and subadditivity for ¯ ( u , v , ) .

For what concerns inner regularity (i.e., Lemma A.1 (v)), we employ the growth conditions in (H1)–(H3). It is enough to show that

(A.3) ¯ ( u , v , A ) β ( n ( A ) + | D u | ( A ) + | v | ( A ) ) ,

with some constant β > 0 , because if we substitute A U ¯ instead of A in (A.3), the inner regularity of the upper bound measures provides the asserted inner regularity for ¯ . By the definition of ¯ and the growth conditions from above, we have that

(A.4) ¯ ( u , v , A ) lim inf k β A ( 1 + | v k | + | u k | ) 𝑑 x

for any sequence ( v k , u k ) k L 1 ( A ; d ) × W 1 , 1 ( A ; m ) with v k * v in and u k * u in BV . It now suffices to choose ( v k , u k ) so that v k v strictly in ( A ; d ) , and u k u strictly in BV ( A Ω ; m ) , because then

A ( 1 + | v k | + | u k | ) 𝑑 x n ( A ) + | v | ( A ) + | D u | ( A ) as  k .

By the latter, (A.4) implies (A.3). Here, recall that we use the convention | D u | ( Ω ) := 0 , so that we have | D u | ( A ) = | D u | ( A Ω ) . By mollification similar to the classical approximation result of Meyers and Serrin, this choice of sequences is indeed possible even for arbitrary open A without boundary regularity; see, for instance, [3, Theorem 3.9] (to choose ( u k ) , while the choice of ( v k ) is easier and can be done similarly, or similarly to Lemma 2.5).

It remains to prove that ¯ ( u , v , ) is subadditive in the sense of Lemma A.1 (iv), i.e., it suffices to prove that

(A.5) ¯ ( u , v , A ) ¯ ( u , v , B ) + ¯ ( u , v , A U ¯ )

for all A , U , B 𝒜 r ( Ω ¯ ) with U B A , u BV ( Ω ; m ) and v ( Ω ¯ ; d ) (see, e.g., [7, Lemma 4.3.4]). Without loss of generality, in view of Proposition 2.6, we can assume f 2 convex and W quasiconvex. Fix η > 0 and find ( w h ) W 1 , 1 ( ( A U ¯ ) , m ) and ( v h ) L 1 ( A U ¯ , d ) such that w h u in BV ( ( A U ¯ ) , m ) , v h v in ( A U ¯ , d ) and

(A.6) lim sup h + A U ¯ ( f 1 ( w h ) f 2 ( v h ) + W ( w h ) ) 𝑑 x ¯ ( u , v , A U ¯ ) + η .

Extract a subsequence still denoted by n such that the above upper limit is a limit. Let B 0 be a relatively open subset of Ω ¯ with Lipschitz boundary such that U B 0 B . Then there exist ( u h ) W 1 , 1 ( B 0 , m ) and ( v ¯ h ) L 1 ( B 0 ; d ) such that u h u in BV ( B 0 , m ) , v ¯ h v in ( B ¯ 0 , d ) and

(A.7) ¯ ( u , v , B 0 ) = lim h + B 0 ( f 1 ( u h ) f 2 ( v ¯ h ) + W ( u h ) ) 𝑑 x .

Consider, for every D 𝒜 r ( Ω ¯ ) , the set function 𝒢 ( u , v , D ) := D ( 1 + | u | ) 𝑑 x + | v | ( D ) . Due to (H1)–(H3), we may extract a bounded subsequence, that we will not relabel, from the sequences of measures

ν h := 𝒢 ( w h , v h , ) + 𝒢 ( u h , v ¯ h , )

restricted to B 0 U ¯ , converging in the sense of distributions to some Radon measure ν defined on B 0 U ¯ . For every t > 0 , let

B t := { x B 0 dist ( x , B 0 ) > t } .

Define, for 0 < δ < η , the subsets

L δ := B η - 2 δ B η + δ .

Consider a smooth cut-off function φ δ C ( B η - δ , [ 0 , 1 ] ) such that φ δ = 1 on B η . As the thickness of the strip L δ is of order δ, we have an upper bound of the form φ δ L ( B η - δ ) C / δ . Define

w h ( x ) := φ δ ( x ( u ) h ( x ) + ( 1 - φ δ ( x ) ) w h ( x ) , v h ( x ) := φ δ ( x ) v ¯ h ( x ) + ( 1 - φ δ ( x ) ) v h ( x ) .

Clearly, the sequences w h and v h weakly* converge to u in BV ( A , d ) and to v in ( A ; m ) as h + , respectively, and

w h = φ δ u h + ( 1 - φ δ ) w h + φ δ ( u h - w h ) .

By the growth conditions (H1)–(H3), we have the estimate

A ( f 1 ( w h ) f 2 ( v h ) + W ( w h ) ) 𝑑 x
B η ( f 1 ( u h ) f 2 ( v ¯ h ) + W ( u h ) ) 𝑑 x + A B η - δ ¯ ( f 1 ( w h ) f 2 ( v h ) + W ( w h ) ) 𝑑 x
    + C ( 𝒢 ( u n , v ¯ h , L δ ) + 𝒢 ( w h , v h , L δ ) ) + 1 δ L δ | w h - u h | 𝑑 x
B 0 ( f 1 ( u h ) f 2 ( v ¯ h ) + W ( u h ) ) 𝑑 x + A U ¯ ( f 1 ( w h ) f 2 ( v h ) + W ( w h ) ) 𝑑 x
    + C ( 𝒢 ( u h , v ¯ h , L δ ) + 𝒢 ( w h , v h , L δ ) ) + 1 δ L δ | w h - u h | 𝑑 x .

Thus, passing to the limit as n + and making use of the lower semicontinuity of ¯ ( , , A ) (which is a consequence of its definition (2.12)), (A.6) and (A.7), we obtain

¯ ( u , v , A ) ¯ ( u , v , B 0 ) + ¯ ( u , v , A U ¯ ) + η + C ν ( L δ ¯ )
¯ ( u , v , B ) + ¯ ( u , v , A U ¯ ) + η + C ν ( L δ ¯ ) .

Now passing to the limit as δ 0 + , we get

¯ ( u , v , A ) ¯ ( u , v , B ) + ¯ ( u , v , A U ¯ ) + η + C ν ( B η ) .

It suffices to choose a subsequence { η h } such that η h 0 + and ν ( B η h ) = 0 , to conclude the proof of (A.5). ∎

References

[1] E. Acerbi, G. Bouchitté and I. Fonseca, Relaxation of convex functionals: The gap problem, Ann. Inst. H. Poincaré Anal. Non Linéaire 20 (2003), no. 3, 359–390. 10.1016/s0294-1449(02)00017-3Search in Google Scholar

[2] L. Ambrosio and G. Dal Maso, On the Relaxation in B V ( Ω ; m ) of quasi-convex integrals, J. Funct. Anal. 109 (1992), 76–97. 10.1016/0022-1236(92)90012-8Search in Google Scholar

[3] L. Ambrosio, N. Fusco and D. Pallara, Functions of Bounded Variation and Free Discontinuity Problems, Oxford Math. Monogr., Oxford University, Oxford, 2000. 10.1093/oso/9780198502456.001.0001Search in Google Scholar

[4] J.-F. Babadjian, E. Zappale and H. Zorgati, Dimensional reduction for energies with linear growth involving the bending moment, J. Math. Pures Appl. (9) 90 (2008), no. 6, 520–549. 10.1016/j.matpur.2008.07.003Search in Google Scholar

[5] M. Baía, S. Krömer and M. Kružík, Generalized W 1 , 1 -Young measures and relaxation of problems with linear growth, SIAM J. Math. Anal. 50 (2018), no. 1, 1076–1119. 10.1137/16M1103464Search in Google Scholar

[6] G. Bouchitté and G. Buttazzo, New lower semicontinuity results for nonconvex functionals defined on measures, Nonlinear Anal. 15 (1990), no. 7, 679–692. 10.1016/0362-546X(90)90007-4Search in Google Scholar

[7] G. Bouchitté, I. Fonseca and L. Mascarenhas, A global method for relaxation, Arch. Ration. Mech. Anal. 145 (1998), no. 1, 51–98. 10.1007/s002050050124Search in Google Scholar

[8] G. Bouchitté, I. Fonseca and M. L. Mascarenhas, Bending moment in membrane theory, J. Elasticity 73 (2004), no. 1–3, 75–99. 10.1023/B:ELAS.0000029996.20973.92Search in Google Scholar

[9] J. W. Cahn and F. Lärché, Surface stress and the chemical equilibrium of small crystals–II. Solid particles embedded in a solid matrix, Acta Metall. 30 (1981), 51–56. 10.1016/0001-6160(82)90043-8Search in Google Scholar

[10] G. Carita, A. M. Ribeiro and E. Zappale, Relaxation for some integral functionals in W w 1 , p × L w q , Bol. Soc. Port. Mat., Special Issue (2010), 47–53. Search in Google Scholar

[11] G. Carita and E. Zappale, A relaxation result in B V × L p for integral functionals depending on chemical composition and elastic strain, Asymptot. Anal. 100 (2016), no. 1–2, 1–20. 10.3233/ASY-161383Search in Google Scholar

[12] G. Carita and E. Zappale, Integral representation results in 𝖡𝖵 × 𝖫 𝗉 , ESAIM Control Optim. Calc. Var. 23 (2017), no. 4, 1555–1599. 10.1051/cocv/2016065Search in Google Scholar

[13] B. Dacorogna, Direct Methods in the Calculus of Variations, 2nd ed., Appl. Math. Sci. 78, Springer, New York, 2008. Search in Google Scholar

[14] G. Dal Maso, An Introduction to Γ-Convergence, Progr. Nonlinear Differential Equations Appl. 8, Birkhäuser, Boston, 1993. 10.1007/978-1-4612-0327-8Search in Google Scholar

[15] A. DeSimone and G. Dolzmann, Existence of minimizers for a variational problem in two-dimensional nonlinear magnetoelasticity, Arch. Ration. Mech. Anal. 144 (1998), no. 2, 107–120. 10.1007/s002050050114Search in Google Scholar

[16] I. Fonseca, D. Kinderlehrer and P. Pedregal, Relaxation in BV × L of functionals depending on strain and composition, Boundary Value Problems for Partial Differential Equations and Applications, RMA Res. Notes Appl. Math. 29, Masson, Paris (1993), 113–152. Search in Google Scholar

[17] I. Fonseca, D. Kinderlehrer and P. Pedregal, Energy functionals depending on elastic strain and chemical composition, Calc. Var. Partial Differential Equations 2 (1994), no. 3, 283–313. 10.1007/BF01235532Search in Google Scholar

[18] I. Fonseca and S. Krömer, Multiple integrals under differential constraints: Two-scale convergence and homogenization, Indiana Univ. Math. J. 59 (2010), no. 2, 427–457. 10.1512/iumj.2010.59.4249Search in Google Scholar

[19] I. Fonseca and G. Leoni, Modern Methods in the Calculus of Variations: L p Spaces, Springer, New York, 2007. Search in Google Scholar

[20] I. Fonseca and S. Müller, Quasi-convex integrands and lower semicontinuity in L 1 , SIAM J. Math. Anal. 23 (1992), no. 5, 1081–1098. 10.1137/0523060Search in Google Scholar

[21] I. Fonseca and S. Müller, Relaxation of quasiconvex functionals in B V ( Ω ; p ) for integrands f ( x , u , u ) , Arch. Ration. Mech. Anal. 123 (1993), 1–49. 10.1007/BF00386367Search in Google Scholar

[22] I. Fonseca, S. Müller and P. Pedregal, Analysis of concentration and oscillation effects generated by gradients, SIAM J. Math. Anal. 29 (1998), no. 3, 736–756. 10.1137/S0036141096306534Search in Google Scholar

[23] D. Henrion, M. Kružík and T. Weisser, Optimal control problems with oscillations, concentrations and discontinuities, Automatica J. IFAC 103 (2019), 159–165. 10.1016/j.automatica.2019.01.030Search in Google Scholar

[24] A. Kałamajska, S. Krömer and M. Kružík, Weak lower semicontinuity by means of anisotropic parametrized measures, Trends in Applications of Mathematics to Mechanics, Springer INdAM Ser. 27, Springer, Cham (2018), 23–51. 10.1007/978-3-319-75940-1_2Search in Google Scholar

[25] A. Kałamajska and M. Kružík, Oscillations and concentrations in sequences of gradients, ESAIM Control Optim. Calc. Var. 14 (2008), no. 1, 71–104. 10.1051/cocv:2007051Search in Google Scholar

[26] J. Kristensen and F. Rindler, Characterization of generalized gradient Young measures generated by sequences in W 1 , 1 and BV, Arch. Ration. Mech. Anal. 197 (2010), no. 2, 539–598. 10.1007/s00205-009-0287-9Search in Google Scholar

[27] A. M. Ribeiro and E. Zappale, Relaxation of certain integral functionals depending on strain and chemical composition, Chin. Ann. Math. Ser. B 34 (2013), no. 4, 491–514. 10.1007/s11401-013-0784-xSearch in Google Scholar

[28] A. M. Ribeiro and E. Zappale, Lower semicontinuous envelopes in W 1 , 1 × L p , Calculus of Variations and PDEs, Banach Center Publ. 101, Polish Academy of Sciences, Warsaw (2014), 187–206. 10.4064/bc101-0-15Search in Google Scholar

[29] F. Rindler and G. Shaw, Liftings, Young measures, and lower semicontinuity, Arch. Ration. Mech. Anal. 232 (2019), no. 3, 1227–1328. 10.1007/s00205-018-01343-8Search in Google Scholar

[30] W. P. Ziemer, Weakly Differentiable Functions, Grad. Texts in Math. 120, Springer, New York, 1989. 10.1007/978-1-4612-1015-3Search in Google Scholar

Received: 2021-07-27
Revised: 2021-11-15
Accepted: 2021-11-19
Published Online: 2022-01-06
Published in Print: 2023-10-01

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