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Research article Special Issues

Griffith energies as small strain limit of nonlinear models for nonsimple brittle materials

  • Received: 24 June 2019 Accepted: 15 September 2019 Published: 26 November 2019
  • We consider a nonlinear, frame indifferent Griffith model for nonsimple brittle materials where the elastic energy also depends on the second gradient of the deformations. In the framework of free discontinuity and gradient discontinuity problems, we prove existence of minimizers for boundary value problems. We then pass to a small strain limit in terms of suitably rescaled displacement fields and show that the nonlinear energies can be identified with a linear Griffith model in the sense of Γ-convergence. This complements the study in [39] by providing a linearization result in arbitrary space dimensions.

    Citation: Manuel Friedrich. Griffith energies as small strain limit of nonlinear models for nonsimple brittle materials[J]. Mathematics in Engineering, 2020, 2(1): 75-100. doi: 10.3934/mine.2020005

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  • We consider a nonlinear, frame indifferent Griffith model for nonsimple brittle materials where the elastic energy also depends on the second gradient of the deformations. In the framework of free discontinuity and gradient discontinuity problems, we prove existence of minimizers for boundary value problems. We then pass to a small strain limit in terms of suitably rescaled displacement fields and show that the nonlinear energies can be identified with a linear Griffith model in the sense of Γ-convergence. This complements the study in [39] by providing a linearization result in arbitrary space dimensions.


    In 1940, Ulam [20] suggested a problem of stability on group homomorphisms in metric groups. Hyers is the first mathematician who answered the question of Ulam in 1941. He demonstrated the following theorem in [8].

    Theorem 1.1. Let X and Y be two Banach spaces and f:XY be a mapping such that

    f(x+y)f(x)f(y)δ

    for some δ>0 and all x,yX. Next there is an exclusive additive mapping A:XY such that

    f(x)A(x)δ

    for all xX.

    The Hyers' stability theorem was developed by other mathematicians. Recently, numerous consequences concerning the stability of various functional equations in different normed spaces and various control functions have been obtained. The problem of stability of some functional equations have been widely explored by direct methods and there are numerous exciting outcomes regarding this problem ([4,7,9,10,11,13,15,17]). The fixed point approach has been used in other Hyers-Ulam stability investigations. The relationship between Hyers-Ulam stability and fixed point theory has been defined in ([5,6,14,16]).

    The first definition of Riesz spaces was done by Riesz in 1930. In [18], Riesz introduced the vector lattice spaces and their properties. A Riesz space (vector lattice) is a vector space which is also a lattice, so that the two structures are compatible in a certain natural way. If, in addition, the space is a Banach space (and, again, a certain natural compatibility axiom is satisfied), it is a Banach lattice. We present some of the terms and concepts of the Riesz spaces used in this article, concisely. However, we relegate the reader to [1,12,19,24], for the fundamental notions and theorems of Riesz spaces and Banach lattices.

    A real vector space X is supposed to be a partially orderly vector space or an ordered vector space, if it is equipped with a partial ordering "≤" that satisfies

    1. xx for every xX.

    2. xy and yx implies that x=y.

    3. xy and yz implies that xz.

    A Riesz space (or vector lattice) is an ordered vector space in which for all x,yX the infimum and supremum of {x,y}, denoted by xy and xy respectively, exist in X. The negative part, the positive part, and the absolute value of xX, are defined by x:=x0,x+:=x0,and|x|:=xx, respectively. Let X be a Riesz space. X is called Archimedean if inf{xn:nN}=0 for all xX+. If |x||y| implies xy for all x,yX, then . is called a lattice norm or Riesz norm on X.

    1. x+y=xy+xy,(xy)=xy.

    2. x+(yz)=(x+y)(x+z),x+(yz)=(x+y)(x+z).

    3. |x|=x++x,|x+y||x|+|y|.

    4. xy is equivalent to x+y+ and yx.

    5. (xy)z=(xy)(yz),(xy)z=(xy)(yz).

    Let X be a Riesz space. The sequence {xn} is called uniformly bounded if there exists an element eX+ and sequence {an}l1 such that xnane. A Riesz space X is called uniformly complete if sup{ni=1xi:nN} exists for every uniformly bounded sequence xnX+. Let X and Y be Banach lattices. Then the function F:XY is called a cone-related function if F(X+)={F(|x|):xX}Y+.

    Theorem 1.2. [1] For a mapping F:XY defined between two Riesz spaces, the following statements are equivalent:

    1. F is a lattice homomorphism.

    2. F(x)+=F(x+) for all xX.

    3. F(x)F(y)=F(xy), for all x,yX.

    4. If xy=0 in X, then F(x)F(y)=0 in Y.

    5. F(|x|)=|F(x)|, for every xX.

    Definition 1.3. [23] The (real) vector lattice (Riesz space) X is named a lattice ordered algebra (Riesz algebra, concisely, l-algebra) if it is a linear algebra (not essentially associative) so that if a,bX+, then abX+. The latter property is equal to every of the following declarations:

    (ⅰ) |ab||a||b| for all a,bX;

    (ⅱ) (ab)+a+b++ab for all a,bX;

    (ⅱ) (ab)a+b+ab+ for all a,bX.

    Definition 1.4. [2] Assume that X be an l-algebra.

    (ⅰ) If for all a,bX, ab=0 implies ab=0, then X is named an almost f-algebra.

    (ⅱ) If c(ab)=cacb and (ab)c=acab for all a,bX and cX+, then X is named a d-algebra.

    (ⅲ) If ab=0 implies cab=acb=0 for all a,bX and cX+, then X is named an f-algebra.

    Proposition 1.5. [2] For an l-algebra X, the following statements are equivalent:

    (i) X is a d-algebra;

    (ii) c|a|=|ca| and |a|c=|ac| for all aX and cX+;

    (iii) for all a,bX and cX+, c(ab)=cacb and (ab)c=acbc.

    Definition 1.6. [21] Any lattice ordered algebra X that is meantime a Banach lattice is named a Banach lattice algebra when abab keeps for all a,bX+. Moreover, if X is an f-algebra next it is named a Banach lattice f-algebra, explicitly, X is next a (real) Banach algebra.

    It is explicit that every f-algebra is an almost f-algebra and a d-algebra. Every Archimedean f-algebra is commutative and associative. It turns out that every Archimedean almost f-algebra is commutative but not necessarily associative [2].

    Theorem 1.7. For an l-algebra A with unit element e>0, the following are equivalent:

    (i) A is an f-algebra.

    (ii) A is a d-algebra.

    (iii) A is an almost f-algebra.

    (iv) e is a weak order unit (i.e., ae implies a=0).

    (v) For all aA, aa+0.

    (vi) For all aA, a20.

    We gather several simple f-algebra properties. Let A be an f-algebra. In this case, for every a,bA, we have the following:

    (1) |ab|=|a||b|.

    (2) ab implies that ab=0.

    (3) a2=(a+)2+(a)20.

    (4) 0(a+)2=aa+.

    (5) (ab)(ab)=ab.

    (6) If a2=0, then ab=0.

    (7) If A is semiprime (i.e., the only nilpotent element in A is 0 or, equivalently, a2=0 in A implies a=0), then a2b2 if and only if |a||b|.

    (8) If A is semiprime, then ab if and only if ab=0.

    (9) Every unital f-algebra is semiprime.

    See [3,22,23] for consider more properties of f-algebras.

    Definition 1.8. Let X and Y be Banach f-algebras and F:XY be a cone-related function. We describe the following:

    (P1) Supremum preserving functional equation:

    F(|x|)F(|y|)=F(|x||y|),for allx,yX.

    (P2) Multiplication preserving functional equation:

    F(|x|)F(|y|)=F(|x||y|),for allx,yX.

    (P3) Semi-homogeneity:

    F(τ|x|)=τF(|x|),for allxXandτ[0,).

    (P4) Positive Cauchy additive functional equation:

    F(|x|)+F(|y|)=F(|x|+|y|),for allx,yX.

    Definition 1.9. [16] A function d:X×X[0,] is named a generalized metric on set X if d satisfies the following conditions:

    (a) for each x,yX, d(x,y)=0 iff x=y;

    (b) for all x,yX, d(x,y)=d(y,x);

    (c) for all x,y,zX, d(x,z)d(x,y)+d(y,z).

    Notice that the just generalized metric significant difference from the metric is that the generalized metric range contains the infinite.

    Theorem 1.10. [16] Let (X,d) be a complete generalized metric space and J:XX be a contractive mapping with Lipschitz constant L<1. Then for every xX, either

    d(Jn+1x,Jnx)=

    for all nonnegative integers n or there exists an integer n0>0 such that

    (a) For all nn0, d(Jnx,Jn+1x)<;

    (b) Jn(x)y, where y is a fixed point of J;

    (c) y is the unique fixed point of J in the set Y={yX:d(Jn0(x),y)<};

    (d) For each yY, d(y,y)11Ld(Jy,y).

    In this part, we will investigate the stability of lattice multiplication functional equation in Banach f-algebra by using the fixed point method.

    Lemma 2.1. Let X and Y be Riesz spaces and F:XY be a cone-related mapping such that

    F(|x|+|z|2|y|)2F(|z||x||y|)=F(|z|)F(|y|) (2.1)

    or

    F(|x|+|z|2|y|)2F(|z||x||y|)=F(|y|+|z||x|)F(|z|+|y||x|) (2.2)

    for all x,y,zX. Then F satisfies (P1).

    Proof. It is easy to indicate that F(0)=0. Replacing z by x in (2.1), we get

    F(|x||y|)2F(0|y|)=F(|x|)F(|y|),

    which means that F satisfies (P1). By the same reasoning, we can show that if (2.2) holds, then F satisfies (P1).

    Lemma 2.2. Let X and Y be Riesz spaces. If F:XY is a cone-related mapping, which satisfies

    F(|x||y||x|+|z|)+F(|y||z||x|)=2F(|y|)+F(|z|) (2.3)

    or

    F(|x|+|y||z|)+2F(|x||y||z|)=F(|x|)+F(|z|) (2.4)

    or

    F(|x||y|+|z|)+F(|x||y||z|)=F(|x|)+2F(|z|) (2.5)

    for all x,y,zX, then F:XY satisfies (P4).

    Proof. Letting y=x in (2.3), we have

    F(|x|+|z|)+F(|x|)=2F(|x|)+F(|z|),

    for all x,y,zX and so F is a positive Cauchy additive mapping. Letting x=y=z=0 in (2.4), we get F(0)=0. Now putting z=y in (2.4), we show that F satisfies (P2). Finally, letting y=x in (2.5), we obtain that F is a positive Cauchy additive mapping.

    Theorem 2.3. Let X and Y be two Banach lattices. Consider a cone-related function F:XY with F(0)=0, that is,

    F(τ|x|+ν|z|2η|y|)2F(ν|z|τ|x|η|y|)νF(|z|)ηF(|y|)φ(τ|x|,η|y|,ν|z|) (2.6)

    for all x,y,zX and τ,η,ν[1,). Suppose that a function φ:X3[0,) satisfies

    φ(|x|,|y|,|z|)(την)α3φ(|x|τ,|y|η,|z|ν) (2.7)

    for all x,y,zX, τ,η,ν[1,) and there is a number α[0,13). Then there is an individual cone-related mapping T:XY which satisfies the properties (P1), (P3) and

    T(|x|)F(|x|)τατταφ(|x|,|x|,|x|) (2.8)

    for all xX and τ[1,).

    Proof. Letting x=y=z and τ=η=ν in (2.6), we get

    F(τ|x|)τF(|x|)φ(τ|x|,τ|x|,τ|x|).

    By (2.7), we have

    F(τ|x|)τF(|x|)ταφ(|x|,|x|,|x|).

    Dividing by τ in the above inequality, we get

    1τF(τ|x|)F(|x|)τα1φ(|x|,|x|,|x|)

    for all xX, τ1 and α[0,13).

    Consider the set

    Δ:={G|G:XY,G(0)=0}

    and the generalized metric on Δ defined by

    d(G,H)=inf{cR+:G(|x|)H(|x|)cφ(|x|,|x|,|x|)for allxX},

    where, as common, inf=. It is easy to demonstrate that (Δ,d) is a complete generalized metric space (see [6,Theorem 3.1]).

    Now, we define the operator J:ΔΔ by

    JG(|x|)=1τG(τ|x|)for allxX.

    Given G,HΔ, let c[0,) be a desired constant with d(G,H)c, that means

    G(|x|)H(|x|)cφ(|x|,|x|,|x|).

    Then we have

    JG(|x|)JH(|x|)=1τG(τ|x|)H(τ|x|)1τcφ(τ|x|,τ|x|,τ|x|)=τα1cφ(|x|,|x|,|x|).

    By Theorem 1.10, there is a mapping T:XY such that the following hold.

    (1) T is a fixed point of J, that means

    T(τ|x|)=τT(|x|) (2.9)

    for all xX. Also the mapping T is an individual fixed point of J in the set

    Z={GΔ;d(G,T)<},

    this implies that T is an individual mapping satisfying (2.9) such that there exists c(0,) satisfying

    T(|x|)F(|x|)cφ(|x|,|x|,|x|)

    for all xX.

    (2) d(JnF,T)0, as n. This implies the equality

    limnF(τn|x|)τn=T(|x|)

    for all xX.

    (3) d(F,T)11Ld(JF,F), which implies the inequality

    d(F,T)τα11τα1=ταττα.

    So we obtain

    F(|x|)T(|x|)τατταφ(|x|,|x|,|x|)

    for all xX, τ1 and α[0,13). Accordingly the inequality (2.8) holds.

    Next, we show that (P1) is satisfied. Putting τ=η=ν:=τn in (2.6), we get

    F(τn|x|+τn|z|2τn|y|)2F(τn|z|τn|x|τn|y|)τnF(|z|)τnF(|y|)φ(τn|x|,τn|y|,τn|z|)

    and so

    F(τn(|x|+|z|2|y|))2F(τn(|z||x||y|))τnF(|z|)τnF(|y|)τ3nαφ(|x|,|y|,|z|).

    Substituting x,y,z by τny,τny,τnz, respectively, in the above inequality, we get

    F(τn(τn|x|+τn|z|2τn|y|))2F(τn(τn|z|τn|x|τn|y|))τnF(τn|z|)τnF(τn|y|)τ3nαφ(τn|x|,τn|y|,τn|z|)

    and thus

    F(τ2n(|x|+|z|2|y|))2F(τ2n(|z||x||y|))τnF(τn|z|)τnF(τn|y|)τ6nαφ(|x|,|y|,|z|) (2.10)

    for all x,y,zX, τ1 and α[0,13). Dividing both sides of (2.10) by τ2n, we obtain

    1τ2nF(τ2n(|x|+|z|2|y|))2τ2nF(τ2n(|z||x||y|))1τnF(τn|z|)1τnF(τn|y|)τ6nα2nφ(|x|,|y|,|z|).

    Since lattice operations are continuous, by (1.2), as n, we get

    T(|x|+|z|2|y|)2T(|z||x||y|)T(|z|)T(|y|)0.

    Therefore,

    T(|x|+|z|2|y|)2T(|z||x||y|)=T(|z|)T(|y|)

    for all x,y,zX. Accordingly, by Lemma 2.1, T satisfies (P1).

    Theorem 2.4. Let F:XY be a cone-related mapping with F(0)=0 in two uniformly complete Banach f-algebras X and Y. Assume that

    F(τ|x|+ν|z|2η|y|)2F(ν|z|τ|x|η|y|)νF(|z|)ηF(|y|)φ(τ|x|,η|y|,ν|z|)

    and

    F(|x||y|)F(|x|)F(|y|)ψ(|x|,|y|),

    where φ:X3[0,) and ψ:X2[0,) satisfy

    φ(τ|x|,η|y|,ν|z|)(την)α3φ(|x|,|y|,|z|)

    and

    ψ(τn|x|,τn|y|)=O(τ2n) (2.11)

    for all x,y,zX, τ,η,ν[1,), α[0,13). Then there exists an individual cone-related mapping T:XY satisfying (P1),(P2),(P3) and

    F(|x|)T(|x|)τατταφ(|x|,|x|,|x|). (2.12)

    Proof. In the previous theorem, we proved that there exists an individual cone-related mapping T:XY such that

    T(|x|)=limnF(τn|x|)τn,F(|x|)T(|x|)τατταφ(|x|,|x|,|x|) (2.13)

    for all xX and τ[1,). Moreover, we showed that T satisfies (P1) and (P3). It follows from (2.11), (2.12) and (2.13) that

    T(|x||y|)T(|x|)T(|y|)=limnF(τ2n|x||y|)τ2nF(τn|x|)τnF(τn|y|)τn=limn1τ2nF(τ2n|x||y|)F(τn|x|)F(τn|y|)limn1τ2nψ(τn|x|,τn|y|)=0.

    Thus T satisfies (P2).

    Corollary 2.5. Suppose that τ>1, α<13 and θ<1 are nonnegative real numbers. Let X and Y be two uniformly complete Banach f-algebras and F:XY be a cone-related mapping with F(0)=0. If F satisfies

    F(τ|x|+ν|z|2η|y|)2F(ν|z|τ|x|η|y|)νF(|z|)ηF(|y|)θ(xα+yα+zα)

    and

    F(|x||y|)F(|x|)F(|y|)θ(xα+yα)

    for all x,y,zX and τ,η,ν[0,), then there exists an individual cone-related mapping T:XY satisfying (P1), (P2), (P3) and

    T(|x|)F(|x|)2θτατταx

    for all xX.

    Proof. Letting

    φ(x,y,z)=θ(xα+yα),ψ(x,y)=θ(xα+yα)

    in the above theorem, we get the desired result.

    Theorem 2.6. Suppose that r,θ,τ,η and ν are nonnegative real numbers with θ>0, r[0,13) and τ,η,ν[1,). If X is a Banach lattice and Y is Banach f-algebra and F:XY is a mapping such that

    F(τ|x|η|y|τ|x|+ν|z|)+F(η|y|ν|z|τ|x|)2ηF(|y|)νF(|z|)θτxrηyrνzr (2.14)

    for all x,y,zX, then there exists an individual mapping T:XY such that the next properties hold:

    (1) For all xX,

    F(|x|)T(|x|)τ3rθτ3τr+2xr.

    (2) T:XY satisfies (P4).

    Proof. By induction on n, we can easily show that the following inequality holds.

    1τnF(τn|x|)F(|x|)τ2θni=3τi(r1)xr. (2.15)

    Moreover, for all xX, we have

    1τnF(τn|x|)1τmF(τm|x|)=τm1τnmF(τnmF(τm|x|))F(τm|x|)θτ2mnmi=3τi(r1)τmxr=θτ2ni=m+3τi(r1)xr

    for all m,nN with nm and all xX. As m, the right side term in the above inequality tends to 0 and so the sequence {1τnF(τn|x|)} is a Cauchy sequence. Hence it converges since Y is complete. Therefore we can define an operator T:XY by

    T(|x|):=limn1τnF(τn|x|) (2.16)

    for all xX. Then we obtain

    T(|x|)F(|x|)τ3rθτ3τr+2xr

    by (2.15).

    Next, we show that (2) is satisfied. Putting τ=ν=η=τn in (2.14), we have

    F(τn(|x||y||x|+|z|))+F(τn(|y||z||x|))2τnF(|y|)τnF(|z|)θτ3nrxryrzr.

    Replacing x by τnx, y by τny and z by τnz in the above inequality, we obtain

    F(τ2n(|x||y||x|+|z|))+F(τ2n(|y||z||x|))2τnF(τn|y|)τnF(τn|z|)θτ6nrxryrzr.

    Dividing the last inequality by τ2n, we have

    1τ2nF(τ2n(|x||y||x|+|z|))+1τ2nF(τ2n(|y||z||x|))21τnF(τn|y|)1τnF(τn|z|)θτ2n(3r1)xryrzr.

    Since lattice operations are continuous, as n we obtain

    T(|x||y||x|+|z|)+T(|y||z||x|)=2T(|y|)T(|z|)

    by (2.16). Therefore, by Lemma 2.2, T is a positive Cauchy additive mapping.

    Corollary 2.7. Suppose that r<13 and θ are nonnegative real numbers and that X,Y are Banach f-algebras. If F:XY is a cone related mapping satisfying (2.14) such that

    F(|x||y|)F(|x|)F(|y|)θxryr (2.17)

    for all x,yX, then there is an individual cone-related mapping T:XY such that satisfies (P2) and (P4).

    Proof. In the above proof, we demonstrate that T:XY exists and satisfies (P4). It follows from (2.16) and (2.17) that

    T(|x||y|)T(|x|)T(|y|)=limnF(τ2n|x||y|)τ2nF(τn|x|)τn.F(τn|y|)τn=limn1τ2nF(τ2n|x||y|)F(τn|x|)F(τn|y|)limnθτ2n(r1)xryr=0.

    Thus T(|x||y|)=T(|x|)T(|y|) and so T satisfies (P2).

    In this paper, we have proved the Hyers-Ulam stability of supremum, infimum and multiplication preserving functional equations in Banach f-algebras.

    The authors equally conceived of the study, participated in its design and coordination, drafted the manuscript, participated in the sequence alignment, and read and approved the final manuscript.

    The authors declare that they have no competing interests.



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