Startseite Morley FEM for a Distributed Optimal Control Problem Governed by the von Kármán Equations
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Morley FEM for a Distributed Optimal Control Problem Governed by the von Kármán Equations

  • Sudipto Chowdhury , Neela Nataraj EMAIL logo und Devika Shylaja
Veröffentlicht/Copyright: 15. April 2020

Abstract

Consider the distributed optimal control problem governed by the von Kármán equations defined on a polygonal domain of 2 that describe the deflection of very thin plates with box constraints on the control variable. This article discusses a numerical approximation of the problem that employs the Morley nonconforming finite element method (FEM) to discretize the state and adjoint variables. The control is discretized using piecewise constants. A priori error estimates are derived for the state, adjoint and control variables under minimal regularity assumptions on the exact solution. Error estimates in lower-order norms for the state and adjoint variables are derived. The lower-order estimates for the adjoint variable and a post-processing of control leads to an improved error estimate for the control variable. Numerical results confirm the theoretical results obtained.

Award Identifier / Grant number: MTR/2017/000199

Funding statement: This work has been supported by DST SERB MATRICS grant MTR/2017/000199 titled Finite element methods for nonlinear plate bending problems and optimal control problems governed by nonlinear plates of the second author. The second author acknowledges the support of the IFCAM-project titled Analysis, control and homogenization of complex systems supported by DST-IISc-CNRS and Université Paul Sabatier Toulouse III.

A Appendix

This section proves a few technical results that are useful to establish the proof of Lemma 5.6 and concludes with a glossary of variables that are used throughout this paper.

Lemma A.1 (Maximum Norm Estimates).

Let Θ ¯ (resp. Θ ¯ M ) solve (2.5b) (resp. (5.2b)). Then, for a sufficiently small choice of the discretization parameter h, it holds that | | | Θ ¯ - Θ ¯ M | | | 𝐋 ( Ω ) h γ .

Proof.

Introduce intermediate terms, and use a triangle inequality (twice), Lemmas 3.1, 3.5 and Theorem 4.2 to obtain

| | | Θ ¯ - Θ ¯ M | | | 𝑳 ( Ω ) | | | Θ ¯ - I M Θ ¯ | | | 𝑳 ( Ω ) + | | | I M Θ ¯ - Θ ¯ M | | | 𝑳 ( Ω ) h γ + | | | I M Θ ¯ - Θ ¯ M | | | NC h γ + | | | I M Θ ¯ - Θ ¯ | | | NC + | | | Θ ¯ - Θ ¯ M | | | NC h γ .

Lemma A.2.

Let Θ ¯ solve (2.5b) with control u ¯ , and let P h : C ( Ω ¯ ) U h be defined as in Definition 5.2. Then, under the assumption that | Ω h 2 | h , it holds that

( P h Θ ¯ - Θ ¯ , 𝐮 h - P h 𝐮 ¯ ) 𝑳 2 ( Ω h 1 ) h 2 | | | 𝐮 h - P h 𝐮 ¯ | | | 𝑳 2 ( Ω h 1 ) ,
( P h Θ ¯ - Θ ¯ , 𝐮 h - P h 𝐮 ¯ ) 𝑳 2 ( Ω h 2 ) h 3 / 2 | | | 𝐮 h - P h 𝐮 ¯ | | | 𝑳 2 ( Ω h 2 ) .

Proof.

A use of the numerical integration property (see for example [30, Lemma 5.5], [25, Lemma 4]) of P h and the Cauchy–Schwarz inequality lead to

( P h Θ ¯ - Θ ¯ , 𝐮 h - P h 𝐮 ¯ ) 𝑳 2 ( Ω h 1 ) = T 𝒯 h 1 ( P h Θ ¯ - Θ ¯ , 𝐮 h - P h 𝐮 ¯ ) 𝑳 2 ( T ) h 2 | | | 𝐮 h - P h 𝐮 ¯ | | | 𝑳 2 ( Ω h 1 ) | | | Θ ¯ | | | 𝑯 2 ( Ω h 1 ) h 2 | | | 𝐮 h - P h 𝐮 ¯ | | | 𝑳 2 ( Ω h 1 ) .

Since Θ ¯ C 0 , 1 ( Ω ¯ ) , the definition of P h , the Cauchy–Schwarz inequality and the assumption | Ω h 2 | h lead to

( P h Θ ¯ - Θ ¯ , 𝐮 h - P h 𝐮 ¯ ) 𝑳 2 ( Ω h 2 ) T 𝒯 h 2 | | | Θ ¯ ( x T ) - Θ ¯ | | | 𝑳 ( T ) h | | | 𝐮 h - P h 𝐮 ¯ | | | 𝑳 2 ( T ) h | | | Θ ¯ | | | 1 , , Ω ( T 𝒯 h 2 | | | 𝐮 h - P h 𝐮 ¯ | | | 𝑳 2 ( T ) 2 ) 1 / 2 ( T 𝒯 h 2 h T 2 ) 1 / 2 h 3 / 2 | | | 𝐮 h - P h 𝐮 ¯ | | | 𝑳 2 ( Ω h 2 ) .

This concludes the proof. ∎

For a local regular solution ( Ψ ¯ , u ¯ ) of (2.1), the reduced control problem seeks a local solution u ¯ that satisfies inf u U ad 𝒪 ( u ¯ ) j ( u ) , where j : U ad 𝒪 ( u ¯ ) is the reduced cost functional defined by j ( u ) :- J ( G ( u ) , u ) and G ( u ) = Ψ u = ( ψ u , 1 , ψ u , 2 ) 𝐕 is the unique solution to (2.3) as defined in Theorem 2.1. Recall that G is of class C in 𝒪 ( u ¯ ) and thus j is of class C for every u 𝒪 ( u ¯ ) and v L 2 ( Ω ) (see [30, Section 2.3]). Also,

(A.1) j ( u ) v = Ω ( θ u , 1 + α u ) v d x , j ′′ ( u ) v 2 = Ω ( | 𝐳 v | 2 + [ [ 𝐳 v , 𝐳 v ] ] Θ u ) d x + α Ω | v | 2 d x ,

where 𝐳 v = ( z v , 1 , z v , 2 ) is the solution of (2.4), [ [ 𝐳 v , 𝐳 v ] ] :- ( [ z v , 1 , z v , 2 ] + [ z v , 2 , z v , 1 ] , - [ z v , 1 , z v , 1 ] ) , [ , ] being the von Kármán bracket, Θ u = ( θ u , 1 , θ u , 2 ) 𝐕 is the solution of the adjoint system and

(A.2) [ [ 𝐳 v , 𝐳 v ] ] Θ u :- ( [ z v , 1 , z v , 2 ] + [ z v , 2 , z v , 1 ] ) θ u , 1 - [ z v , 1 , z v , 1 ] θ u , 2 .

In a similar way, we can define the first-order j h and second-order j h ′′ derivatives for the reduced discrete cost functional j h .

The next lemma discusses results that are relevant to establish Lemma 5.6. Since several of the ideas of the proof are already repetitions from [25, Section 4], only a sketch of the proof is provided.

Lemma A.3.

Let u ¯ = ( u ¯ , 0 ) (resp. u ¯ h = ( u ¯ h , 0 ) ) be the optimal control in the optimality system (2.5) (resp. (5.1)) at the continuous (resp. discrete) level. Then the following estimates hold true.

  1. For u 1 , u 2 U ad and sufficiently close to u ¯ , and for v U h , ( j h ′′ ( u 1 ) - j h ′′ ( u 2 ) ) ( v 2 ) u 1 - u 2 v 2 .

  2. For v U h , ( j h ′′ ( u ¯ ) - j ′′ ( u ¯ ) ) ( v 2 ) h γ v 2 , γ ( 1 2 , 1 ] being the index of elliptic regularity.

  3. Let P h : C ( Ω ¯ ) U h be defined as in Definition 5.2 . Then ( j h ( P h u ¯ ) - j h ( u ¯ h ) , P h u ¯ - u ¯ h ) P h u ¯ - u ¯ h 2 .

  4. For u U ad sufficiently close to u ¯ , v 1 Ω h 1 , and v 2 Ω h 2 , j h ′′ ( u ) ( v 1 , v 2 ) v 1 L 1 ( Ω h 1 ) v 1 L 1 ( Ω h 2 ) .

Proof.

(i) For i = 1 , 2 ,

(A.3) j h ′′ ( u i ) ( v 2 ) = Ω | 𝐳 v , u i , M | 2 d x + T 𝒯 h T [ [ 𝐳 v , u i , M , 𝐳 v , u i , M ] ] Θ u i , M d x + α Ω | v | 2 d x ,

where 𝐳 v , u i , M satisfies the linearized von Kármán equation in the direction of v given by

(A.4) A NC ( 𝐳 v , u i , M , Φ M ) + B NC ( Ψ u i , M , 𝐳 v , u i , M , Φ M ) + B NC ( 𝐳 v , u i , M , Ψ u i , M , Φ M ) = ( 𝐯 , Φ M )

for all Φ M 𝐕 M . From (A.3) with i = 1 and i = 2 ,

(A.5) j h ′′ ( u 1 ) ( v 2 ) - j h ′′ ( u 2 ) ( v 2 ) = Ω ( | 𝐳 v , u 1 , M | 2 - | 𝐳 v , u 2 , M | 2 ) d x + T 𝒯 h T ( [ [ 𝐳 v , u 1 , M , 𝐳 v , u 1 , M ] ] Θ u 1 , M - [ [ 𝐳 v , u 2 , M , 𝐳 v , u 2 , M ] ] Θ u 2 , M ) d x .

Consider the first term on the right-hand side of (A.5). A use of the Cauchy–Schwarz inequality and the a priori bound for the solution of (A.4) yields

(A.6) Ω ( | 𝐳 v , u 1 , M | 2 - | 𝐳 v , u 2 , M | 2 ) d x ( Ω | 𝐳 v , u 1 , M - 𝐳 v , u 2 , M | 2 d x ) 1 / 2 ( Ω ( | 𝐳 v , u 1 , M | + | 𝐳 v , u 2 , M | ) 2 d x ) 1 / 2 | | | 𝐳 v , u 1 , M - 𝐳 v , u 2 , M | | | ( | | | 𝐳 v , u 1 , M | | | + | | | 𝐳 v , u 2 , M | | | ) | | | 𝐳 v , u 1 , M - 𝐳 v , u 2 , M | | | v .

Note that

(A.7) | | | 𝐳 v , u 1 , M - 𝐳 v , u 2 , M | | | = sup 𝟎 𝐩 𝑳 2 ( Ω ) ( 𝐳 v , u 1 , M - 𝐳 v , u 2 , M , 𝐩 ) | | | 𝐩 | | | .

Consider the auxiliary problem that seeks 𝝃 𝐩 , M 𝐕 M such that, for all Φ M 𝐕 M ,

(A.8) A NC ( 𝝃 𝐩 , M , Φ M ) + B NC ( Ψ u 1 , M , Φ M , 𝝃 𝐩 , M ) + B NC ( Φ M , Ψ u 1 , M , 𝝃 𝐩 , M ) = ( 𝐩 , Φ M ) .

Choose Φ M = 𝐳 v , u 1 , M - 𝐳 v , u 2 , M in (A.8), and use (A.4) to obtain

( 𝐩 , 𝐳 v , u 1 , M - 𝐳 v , u 2 , M ) = - B NC ( Ψ u 1 , M - Ψ u 2 , M , 𝐳 v , u 2 , M , 𝝃 𝐩 , M ) - B NC ( z v , u 2 , M , Ψ u 1 , M - Ψ u 2 , M , 𝝃 𝐩 , M ) .

A use of Lemma 3.6 (a), (3.16) and the a priori bounds for the solutions of (A.4) and (A.8), and then a substitution in (A.7) leads to | | | 𝐳 v , u 1 , M - 𝐳 v , u 2 , M | | | u 1 - u 2 v . Therefore, a substitution of this estimate in (A.6) yields

(A.9) Ω ( | 𝐳 v , u 1 , M | 2 - | 𝐳 v , u 2 , M | 2 ) d x u 1 - u 2 v 2 .

To estimate the second term on the right-hand side of (A.5), use the definition in (A.2), and consider the first term in the expansion. For 𝐳 v , u i , M = ( z v , u i , M , 1 , z v , u i , M , 2 ) and Θ u i , M = ( θ u i , M , 1 , θ u i , M , 2 ) , a simple manipulation, the generalized Hölder inequality, Lemma 3.5 and the a priori bound for the solutions of (A.4) lead to

(A.10) T 𝒯 h T ( [ z v , u 1 , M , 1 , z v , u 1 , M , 2 ] θ u 1 , M , 1 - [ z v , u 2 , M , 1 , z v , u 2 , M , 2 ] θ u 2 , M , 1 ) d x = T 𝒯 h T ( [ z v , u 1 , M , 1 - z v , u 2 , M , 1 , z v , u 1 , M , 2 ] + [ z v , u 2 , M , 1 , z v , u 1 , M , 2 - z v , u 2 , M , 2 ] ) θ u 1 , M , 1 d x + T 𝒯 h T [ z v , u 2 , M , 1 , z v , u 2 , M , 2 ] ( θ u 1 , M , 1 - θ u 2 , M , 1 ) d x | | | 𝐳 v , u 1 , M - 𝐳 v , u 2 , M | | | NC v θ u 1 , M , 1 NC + θ u 1 , M , 1 - θ u 2 , M , 1 NC v 2 .

Change the auxiliary problem (A.8) (resp. (A.4)) with duality pairing ( , ) 𝐕 M , 𝐕 M on the right-hand side, choose Φ M = 𝐳 v , u 1 , M - 𝐳 v , u 2 , M (resp. Φ M = Θ u 1 , M - Θ u 2 , M ), and modify the arguments to obtain

(A.11) | | | 𝐳 v , u 1 , M - 𝐳 v , u 2 , M | | | NC u 1 - u 2 v ( resp. | | | Θ u 1 , M - Θ u 2 , M | | | NC u 1 - u 2 ) .

A substitution of (A.11) in (A.10) leads to

(A.12) T 𝒯 h T ( [ z v , u 1 , M , 1 , z v , u 1 , M , 2 ] θ u 1 , M , 1 - [ z v , u 2 , M , 1 , z v , u 2 , M , 2 ] θ u 2 , M , 1 ) d x u 1 - u 2 v 2 .

The remaining terms that contribute to the right-hand side of (A.5) can be estimated in a similar way. A combination of (A.5), (A.9), (A.12) and (A.2) yields the desired result in (i).

(ii) A subtraction of the continuous and discrete second-order cost functionals leads to

( j h ′′ ( u ¯ ) - j ′′ ( u ¯ ) ) ( v 2 ) = Ω ( | 𝐳 v , u ¯ , M | 2 - | 𝐳 v , u ¯ | 2 ) d x + T 𝒯 h T [ [ 𝐳 v , u ¯ , M , 𝐳 v , u ¯ , M ] ] Θ u ¯ , M d x - Ω [ [ 𝐳 v , u ¯ , 𝐳 v , u ¯ ] ] Θ ¯ d x .

The proof then follows from arguments similar to (A.9) and (A.10) and by using Theorem 4.2 for Θ ¯ and Θ u ¯ , M (resp. 𝐳 v , u ¯ and 𝐳 v , u ¯ , M ).

(iii) The proof follows from [25, Lemma 6] together with (i), (ii), Lemma A.1 and [30, Lemma 4.4].

(iv) Since 𝒯 h 1 𝒯 h 2 = , v 1 Ω h 1 (resp. v 2 Ω h 2 ), we have Ω v 1 v 2 d x = 0 . Hence a use of the definition of j h ′′ ( u ) ( v 1 , v 2 ) yields

j h ′′ ( u ) ( v 1 , v 2 ) = Ω ( z v 1 , M , 1 z v 2 , M , 1 + z v 1 , M , 2 z v 2 , M , 2 ) d x + T 𝒯 h T ( [ z v 1 , M , 1 , z v 2 , M , 2 ] + [ z v 1 , M , 2 , z v 2 , M , 1 ] ) θ u , M , 1 d x - T 𝒯 h T [ z v 1 , M , 1 , z v 2 , M , 1 ] θ u , M , 2 d x ,

where 𝐳 v i , M = ( z v i , M , 1 , z v i , M , 2 ) solves (A.4) with 𝐯 = 𝐯 i for i = 1 , 2 . The bound 𝐳 v i , M NC 𝐯 i L 1 ( Ω h i ) for i = 1 , 2 would now lead to the desired estimate. ∎

Table 3

Glossary of variables.

Variables Description
Ψ = ( ψ 1 , ψ 2 ) State variables, ψ 1 and ψ 2 correspond to displacement and Airy stress
𝐮 = ( u , 0 ) Control variable
Ψ u Solution to the state equation that corresponds to the control u
γ Elliptic regularity index that belongs to ( 1 2 , 1 ]
Θ = ( θ 1 , θ 2 ) Adjoint variables
𝐮 ¯ = ( u ¯ , 0 ) Optimal control
Ψ ¯ = ( ψ ¯ 1 , ψ ¯ 2 ) State variables that correspond to optimal control 𝐮 ¯
Θ ¯ = ( θ ¯ 1 , θ ¯ 2 ) Adjoint variables that correspond to optimal control 𝐮 ¯
Ψ u , M = ( ψ u , M , 1 , ψ u , M , 2 ) Morley FEM approximation of Ψ u
𝝃 = ( ξ 1 , ξ 2 ) Solution to the biharmonic system
𝝃 M = ( ξ M , 1 , ξ M , 2 ) Morley FE approximation of 𝝃
Θ u , M = ( θ u , M , 1 , θ u , M , 2 ) Morley FE approximation of the adjoint variable Θ u
𝝌 𝒈 Solution of the dual problem with respect to the adjoint equation
𝝌 𝒈 , M Morley FE approximation of 𝝌 𝒈
u h Discrete control
Ψ M = ( ψ M , 1 , ψ M , 2 ) Morley FE approximation of state equation with respect to u h
Θ M = ( θ M , 1 , θ M , 2 ) Morley FE approximation of adjoint equation with respect to u h
u ¯ h Discrete optimal control
Ψ ¯ M = ( ψ ¯ M , 1 , ψ ¯ M , 2 ) Discrete optimal state variables with respect to u ¯ h
Θ ¯ M = ( θ ¯ M , 1 , θ ¯ M , 2 ) Discrete optimal adjoint variables with respect to u ¯ h
u ¯ ~ h Post-processed control

Sketch of the proof of Lemma 5.6.

The proof of Lemma 5.6 follows from [25, Lemmas 9 and 10] together with Theorem 4.2, Proposition 5.10, Lemmas A.2 and A.3. We will sketch the steps of the proof.

A use of the pointwise version of the continuous optimality condition with x = S T and u = u ¯ h ( S T ) leads to

( Θ ¯ ( S T ) + α 𝐮 ¯ ( S T ) ) ( 𝐮 ¯ h ( S T ) - 𝐮 ¯ ( S T ) ) 𝑳 2 ( T ) 0 for all T 𝒯 h 1 .

Apply the above variational inequality to T 𝒯 h 2 with x T instead of S T to obtain

( Θ ¯ ( x T ) + α 𝐮 ¯ ( x T ) ) ( 𝐮 ¯ h ( x T ) - 𝐮 ¯ ( x T ) ) 𝑳 2 ( T ) 0 for all T 𝒯 h 2 .

An integration of the above two inequalities over T, a summation over all T 𝒯 h and the definition of P h yield

(A.13) ( P h Θ ¯ + α P h 𝐮 ¯ , 𝐮 ¯ h - P h 𝐮 ¯ ) 0 .

Since P h u ¯ U h , ad , choose 𝐮 h = P h 𝐮 ¯ in the discrete optimality condition (5.2) to obtain

(A.14) ( Θ ¯ M + α 𝐮 ¯ h , P h 𝐮 ¯ - 𝐮 ¯ h ) 0 .

An addition of (A.13) and (A.14), and introduction of intermediate terms yield

(A.15) 0 ( ( P h Θ ¯ - Θ ¯ ) + ( Θ ¯ - Θ u ¯ , M ) + ( Θ u ¯ , M - Θ P h u ¯ , M ) , 𝐮 ¯ h - P h 𝐮 ¯ ) + ( ( Θ P h u ¯ , M - Θ ¯ M ) + α ( P h 𝐮 ¯ - 𝐮 ¯ h ) , 𝐮 ¯ h - P h 𝐮 ¯ ) .

Lemma A.2, the Cauchy–Schwarz inequality, Theorem 4.2 (c) and Proposition 5.10 lead to an estimate for the first term in (A.15) as ( ( P h Θ ¯ - Θ ¯ ) + ( Θ ¯ - Θ u ¯ , M ) + ( Θ u ¯ , M - Θ P h u ¯ , M ) , 𝐮 ¯ h - P h 𝐮 ¯ ) h 3 / 2 | | | P h 𝐮 ¯ - 𝐮 ¯ h | | | . This and (A.15) result in

(A.16) ( Θ P h u ¯ , M + α P h 𝐮 ¯ , P h 𝐮 ¯ - 𝐮 ¯ h ) - ( Θ ¯ M + α 𝐮 ¯ h , P h 𝐮 ¯ - 𝐮 ¯ h ) h 3 / 2 | | | P h 𝐮 ¯ - 𝐮 ¯ h | | | .

The term on the left-hand side of (A.16) is estimated using the discrete version of (A.1) and Lemma A.3 (iii) to obtain ( Θ P h u ¯ , M + α P h 𝐮 ¯ , P h 𝐮 ¯ - 𝐮 ¯ h ) - ( Θ ¯ M + α 𝐮 ¯ h , P h 𝐮 ¯ - 𝐮 ¯ h ) | | | P h 𝐮 ¯ - 𝐮 ¯ h | | | 2 . A substitution of this estimate in (A.16) leads to | | | P h 𝐮 ¯ - 𝐮 ¯ h | | | h 3 / 2 helps to deduce

(A.17) | | | P h 𝐮 ¯ - 𝐮 ¯ h | | | L 2 ( Ω h 2 ) h 3 / 2 .

For Ω h 1 , follow the same steps up to (A.16) with L 2 ( Ω ) replaced with L 2 ( Ω h 1 ) to obtain

(A.18) ( Θ P h u ¯ , M + α P h 𝐮 ¯ , P h 𝐮 ¯ - 𝐮 ¯ h ) 𝑳 2 ( Ω h 1 ) - ( Θ ¯ M + α 𝐮 ¯ h , P h 𝐮 ¯ - 𝐮 ¯ h ) 𝑳 2 ( Ω h 1 ) h 2 γ | | | P h 𝐮 ¯ - 𝐮 ¯ h | | | 𝑳 2 ( Ω h 1 ) .

The left-hand side of (A.18) is estimated as

( Θ P h u ¯ , M + α P h 𝐮 ¯ , P h 𝐮 ¯ - 𝐮 ¯ h ) 𝑳 2 ( Ω h 1 ) - ( Θ ¯ M + α 𝐮 ¯ h , P h 𝐮 ¯ - 𝐮 ¯ h ) 𝑳 2 ( Ω h 1 ) | | | P h 𝐮 ¯ - 𝐮 ¯ h | | | 𝑳 2 ( Ω h 1 ) 2 .

For the details of this proof (that uses the second-order sufficient optimality conditions [30, Theorem 2.17] and Lemma A.3), see [25, Lemma 10]. The last inequality substituted in (A.18) and (A.17) concludes the proof. ∎

A glossary of several variables which are used throughout the paper is given in Table 3.

Acknowledgements

The authors also thank Prof. J. P. Raymond for the fruitful discussions during his visit to IIT Bombay.

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Received: 2020-03-15
Accepted: 2020-03-16
Published Online: 2020-04-15
Published in Print: 2021-01-01

© 2021 Walter de Gruyter GmbH, Berlin/Boston

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