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R E S E A R C H

Open Access

New

a posteriori

error estimates for

hp

version of finite element methods of

nonlinear parabolic optimal control problems

Zuliang Lu

1,2,3*

, Hongyan Liu

4

, Chunjuan Hou

5

and Longzhou Cao

1

*Correspondence:

[email protected]

1Key Laboratory of Signal and

Information Processing, Chongqing Three Gorges University, Chongqing, 404000, P.R. China

2Key Laboratory for Nonlinear

Science and System Structure, Chongqing Three Gorges University, Chongqing, 404000, P.R. China

3Research Center for Mathematics

and Economics, Tianjin University of Finance and Economics, Tianjin, 300222, P.R. China

Full list of author information is available at the end of the article

Abstract

In this paper, we investigate residual-baseda posteriorierror estimates for thehp

version of the finite element approximation of nonlinear parabolic optimal control problems. By using thehpfinite element approximation for both the state and the co-state variables and thehpdiscontinuous Galerkin finite element approximation for the control variable, we derivehpresidual-baseda posteriorierror estimates for both the state and the control approximation. Such estimates, which are apparently not available in the literature, can be used to construct a reliablehpadaptive finite element approximation for the nonlinear parabolic optimal control problems.

MSC: 49J20; 65N30

Keywords: residual-baseda posteriorierror estimates; nonlinear parabolic optimal control problems;hpversion of finite element method

1 Introduction

Recently, optimal control problems have attracted substantial interest due to their appli-cations in atmospheric pollution problems, exploration and extraction of oil and gas re-sources, and engineering. They must be solved with efficient numerical methods. The hpversion of the finite element method is an important numerical method for the opti-mal control problems governed by partial differential equations. There have been exten-sive studies of the convergence of the finite element approximation for optimal control problems. Let us mention two early papers devoted to linear optimal control problems by Falk [] and Geveci []. A systematic introduction of the finite element method for opti-mal control problems can be found in [–], but there are much less published results on this topic forhp-finite element methods for optimal control problems. The adaptive finite element method has been investigated extensively and became one of the most popular methods in the scientific computation and numerical modeling. In [], the authors studied a posteriorierror estimates for adaptive finite element discretizations of boundary control problems.A posteriorierror estimates and adaptive finite element approximation for pa-rameter estimation problems have been obtained in [, ]. The adaptive finite element approximation is among the most important means to boost the accuracy and efficiency of the finite element discretization. There are three main versions in adaptive finite ele-ment approximation,i.e., thep-version,h-version, andhp-version. Thep-version of finite

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element methods uses a fixed mesh and improves the approximation of the solution by increasing the degrees of piecewise polynomials. Theh-version is based on mesh refine-ment and piecewise polynomials of low and fixed degrees. In thehp-version adaptation, one has the option to split an element (h-refinement) or to increase its approximation or-der (p-refinement). Generally speaking, a localp-refinement is the more efficient method on regions where the solution is smooth, while a localh-refinement is the strategy suitable on elements where the solution is not smooth in []. There have been many theoretical studies as regards thehpfinite element method in [–].

To the best of our knowledge, there are manyh-versions of adaptive finite element meth-ods for optimal control problems in [, ]. In fact, comparable literature for high order elements such as thehp-version of the finite element method for optimal control prob-lems is rather limited. For the constrained optimal control problem governed by elliptic equations, the authors have deriveda posteriorierror estimates for thehpfinite element approximation in []. The purpose of this work is to derivehp a posteriorierror estimates for optimal control problems governed by nonlinear parabolic equations.

In this paper, we adopt the standard notationWm,p() for Sobolev spaces onwith a

norm · m,p given byvpm,p=

|α|≤mDαvpLp(), a semi-norm| · |m,p given by|v|pm,p=

|α|=mDαvpLp(). We set Wm,p() = {vWm,p() :v| = }. For p= , we denote

Hm() =Wm,(),Hm

() =W m,

 (), and · m= · m,, · = · ,. We denote by

Ls(,T;Wm,p()) the Banach space of allLsintegrable functions fromJintoWm,p() with

normvLs(J;Wm,p())= (T

v s

Wm,p()dt)

s fors∈[,∞), and the standard modification for

s=∞. Similarly, one can define the spacesH(J;Wm,p()) andCk(J;Wm,p()). The details

can be found in [].

The paper is organized as follows. In Section , we shall construct thehpfinite element approximation for nonlinear parabolic optimal control problems. In Section , we derive hp a posteriorierror estimates for the optimal control problems. In the last section, we briefly give conclusions and some possible future work.

2 Thehpfinite element of nonlinear parabolic optimal control

In this section, we study thehpfinite element method and the backward Euler discretiza-tion approximadiscretiza-tion of convex optimal control problems governed by nonlinear parabolic equations. We shall take the state spaceW=L(,T;Y) withY=H

(), the control space

X=L(,T;U) withU=L(

U) andH=L() to fix the idea. LetBbe a linear

continu-ous operator fromXtoL(,T;Y). We are interested in the following nonlinear parabolic

optimal control problems:

min

u∈K

 

T

yydL()+uL(

U)

dt

, (.)

yt–div(Ay) +φ(y) =f+Bu, x,t∈(,T], (.)

y(x,t) = , x∂,t∈(,T], (.)

y(x, ) =y(x), x, (.)

whereandU are bounded open sets inRwith a Lipschitz boundaryand∂U,

K is a set defined byK={vX:T

Uv dx dt≥}, andf,ydL

(,T;H),y

(x)∈V=

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ξtAξcξ,ξ R. The functionφ(·)W,∞(–R,R) for anyR> ,φ(y)L() for

anyyH(), andφ(y).

Let a(v,w) = (Av)· ∇w dx, ∀v,wV, (f,f) =

ffdx, ∀f,f ∈ H, (v,w)U =

Uvw dx, ∀v,wU. It follows from the assumptions onAthat there are constants c

andC>  such that

a(v,v)≥cvH(), a(v,w) ≤C|v|H()|w|H(), ∀v,wY.

Then a weak formula of the convex nonlinear parabolic optimal control problems (.)-(.) reads

min

u(t)∈K

 

T

yydL()+uL(

U)

dt

, (.)

whereyW,uX,u(t)∈K, subject to

(yt,w) +a(y,w) +

φ(y),w= (f+Bu,w), ∀wY,t∈(,T], (.)

y(x, ) =y(x), x. (.)

It is well known (see,e.g., []) that the optimal control problem (.)-(.) has at least a solution (y,u), and if that a pair (y,u) is the solution of (.)-(.), then there is a co-state pW such that the triplet (y,p,u) satisfies the following optimality conditions:

(yt,w) +a(y,w) +

φ(y),w= (f+Bu,w), ∀wY,y() =y(x), (.)

–(pt,w) +a(q,p) +

φ(y)p,q= (yyd,q), ∀qY,p(T) = , (.) T

u+Bp,vuUdt≥, ∀vK, (.)

whereB∗is the adjoint operators ofB, and (·,·)Uis the inner product ofU, which will be

simply written as (·,·) in the rest of the paper when no confusion is caused.

Due to the special structure of the control constraint setK, we can derive a relation-ship between the control variable and the co-state variable of (.)-(.) in the following lemma.

Lemma . Let(y,p,u)be the solution of(.)-(.).Then we have

u=max,BpBp,

where Bp= T

UBp dx dt

T

Udx dt

denotes the integral average onU×[,T]of the function Bp.

Now, we consider thehpfinite element approximation for the nonlinear parabolic opti-mal control problems. We assume thatandUare polygonal. We consider the

triangu-lationT of the set⊂R, which is a collection of elementsτT associated with each

elementτ, and an affine element map :ττ, where the reference elementτ is the

reference triangle

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We consider the triangulationT which satisfies the standard conditions defined in [] and write =diamτ. Additionally we assume that triangulationT isγ-shape regular,

i.e.,

h–τ L(τ)+hτF τ

–

L∞(τ)γ. (.)

This implies that there exists a constantC>  that depends solely onγ such that

C–Chτ, τ,τT withττ=∅, (.)

and there exists a constantM∈Nthat depends solely onγ such that no more thanM elements share a common vertex. We assume that the triangulationTUofUwhich is a

collection of elementsτUTU, isγ-shape regular which satisfies the standard conditions

asT. Associated with each elementτUis an affine element mapFτU:ττU. We further

assume the triangulationT satisfies the relation between the patch and the reference patch in [].

For each elementτT, we denoteE(τ) the set of edges ofτandN(τ) the set of vertices ofτ, and choose a polynomial degree∈Nand collect these numbers in the polynomial

degree vector p= ()τT. Similarly, for each elementτUTU, we choose a polynomial

degree vector p= (pτU)τUTU(pτU∈N).N(T) denotes the set of all vertices ofT,E(T)

denotes the set of all edges. Additionally, we introduce the following notation (VN(T), eE(T)):

N(e) =VN(T) :Ve,

wV=

x:xτ andτ∩ {V} =∅,

we=

V∈N(e)

wV, wτ =

V∈N(τ)

wV,

hτU=diamτU, pe=max

:eE(τ)

,

where χ denotes the interior of the setχ. Finally, we denote byhe the length of the

edgee.

Next, we define thehp-finite element spaceSp(T)H() and thehp-discontinuous Galerkin finite element spaceUp(T

U)⊂L(U) by

Sp(T) =vC() :v|

τ(τ)

,

Up(T

U) =

vL(U) :v|τUFτUpτU(τ)

,

where we set

k(τ) = ⎧ ⎨ ⎩

Pk=span{xiyj: ≤i+jk}, ifτ =T,

Qk=span{xiyj: ≤i,jk}, ifτ =S.

We also assume that the polynomial degree vector psatisfies

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Then we can introduce the finite dimensional spaces Khp=KUp(TU), Vhp=V

Sp(T).

The semidiscretehpfinite element approximation of (.)-(.) is as follows:

min

uhp∈Khp

 

T

yhpydL()+uhpL(

U)

dt

, (.)

∂yhp

∂t ,whp

+a(yhp,whp) +

φ(yhp),w

= (f+Buhp,whp), ∀whpVhp, (.)

yhp(x, ) =yhp(x), x, (.)

whereyhpH(,T;Vhp) andyhp ∈Vhpis an finite element approximation ofy.

It follows that the optimal control problems (.)-(.) has at least a solution (yhp,uhp)

and if that a pair (yhp,uhp) is the solution of (.)-(.), then there is a co-statephpVhp

such that the triplet (yhp,php,uhp) satisfies the following optimality conditions:

∂yhp

∂t ,whp

+a(yhp,whp) +

φ(yhp),w

= (f+Buhp,whp), ∀whpVhp, (.)

yhp(x, ) =yhp(x), x,

∂php

∂t ,qhp

+a(qhp,php) +

φ(yhp)php,qhp

= (yhpyd,qhp), ∀whpVhp, (.)

php(x,T) = , x,

uhp+Bphp,vhpuhp

U≥, ∀vhpKhp. (.)

Furthermore, we consider the fully discrete finite element approximation for the above semidiscrete problems by using the backward Euler scheme. Let  =t<t<· · ·<tM–<

tM=T,ki=titi–,i= , , . . . ,M,k=≤i≤Mmax{ki}.

Fori= , , . . . ,M, construct thehpfinite element approximation spacesVhpiH() (similar to Vhp) on theith time step. Similarly, we construct thehpfinite element

ap-proximation spaces KhpiL(

U) (similar toKhp) on theith time step. The fully

dis-cretehpfinite element approximation scheme (.)-(.) is to find (yi

hp,uihp)∈Vhpi ×Khpi ,

i= , , . . . ,M, such that

min

uihp∈Khpi

M

i=

 y

i

hpyd(x,ti)  L()+

 u

i hp

L(

U)

, (.)

yi hpyi–hp

ki

,whp

+ayihp,whp

+φyihp,whp

=f(x,ti) +Buihp,whp

, ∀whpVhpi , (.)

yhp(x) =yhp (x), x. (.)

It follows that the optimal control problem (.)-(.) has at least a solution (Yhpi ,Uhpi ), and if a pair (Yi

hp,Uhpi )∈Vhpi ×Khpi is the solution of (.)-(.), then there is a co-state

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optimality conditions:

Yi hpYhpi–

ki

,whp

+aYhpi ,whp

+φYhpi ,whp

=f(x,ti) +BUhpi ,whp

, (.)

whpVhpiV=H(), i= , , . . . ,M, Yhp(x) =y hp

 (x), x, Pi–

hpPihp

ki

,qhp

+aqhp,Pi–hp

+φYhpi–Pi–hp,qhp

=Yhpiyd(x,ti),qhp

, (.)

qhpVhpiV=H(), i=M, . . . , , , PMhp(x) = , x,

Uhpi +BPi–hp,vhpUhpi

U≥, ∀vhpK i

hp,i= , , . . . ,M. (.)

Fori= , , . . . ,M, let

Yhp|(ti–,ti]=

(tit)Yhpi–+ (tti–)Yhpi

/ki,

Php|(ti–,ti]=

(tit)Phpi–+ (tti–)Pihp

/ki,

Uhp|(ti–,ti]=U

i hp.

For any functionwC(,T;L()), letwˆ(x,t)|t∈(ti–,ti]=w(x,ti),w˜(x,t)|t∈(ti–,ti]=w(x,ti–).

Then the optimality conditions (.)-(.) can be restated as

∂Yhp

∂t ,whp

+a(Yˆhp,whp) +

φ(Yˆhp),whp

= (fˆ+BUhp,whp), (.)

whpVhpiV=H(), t∈(ti–,ti],i= , , . . . ,M,

Yhp(x, ) =yhp(x), x,

∂Php

∂t ,qhp

+a(qhp,P˜hp) +

φ(Y˜hp)P˜hp,qhp

= (Yˆhpyˆd,qhp), (.)

qhpVhpiV=H(), t∈(ti–,ti],i=M, . . . , , ,

Php(x,T) = , x,

Uhp+BP˜hp,vhpUhp

U≥, (.)

vhpKhpi , t∈(ti–,ti],i= , , . . . ,M.

The following lemmas [, , ] are important in derivinga posteriorierror estimates of residual type.

Lemma . There exist a constant C> independent of v,hτU,and pτU and a mapping

πhτU

U :H(τU)→PUU)such thatvH(τU),τUTUthe following inequality is valid: vπhτU

UL

U)≤C

hτU

pτU

vH

U),

where we will write v∈PUU)if the following satisfied:v|τUFτUPpτU(τ)ifτU is a

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Lemma . Letpbe an arbitrary polynomial degree distribution satisfies(.).Then

there exists a linear operator E:H()→Sp(T)∩H(),and there exists a constant

C> depending solely onγ such that for every vH

()and all elementsτT and all

edges eE(T):

vEvL)+

(vEv)

L)C

vL(wτ),

vEvL(e)C

he

pe

vL(w

e).

Lemma . Letpbe an arbitrary polynomial degree distribution satisfying(.)and

≥, ∀τT. Then there exists a bounded linear operator E : H()∩H()→

Sp(T)H

(),and there exists a constant C> that depends solely onγ such that for

every vH()∩H()and all elementsτT and all edges eE(T):

vEvL)+

(vEv)L(τ)C

|v|H(wτ),

vEvL(e)C

he

pe

|v|H(w

e).

ForϕWh, we shall write

φ(ϕ) –φ(ρ) = –φ˜(ϕ)(ρ–ϕ) = –φ(ρ)(ρ–ϕ) +φ˜(ϕ)(ρ–ϕ), (.)

where

˜

φ(ϕ) =

φϕ+s(ρ–ϕ)ds, φ˜(ϕ) =

( –sρ+s(ϕ–ρ)ds

are bounded functions in¯ [].

3 A posteriori error estimates

In this section, we shall derive somea posteriorierror estimates for thehpfinite element approximation of the optimal control problems governed by nonlinear parabolic equa-tions.

Let

S(u) =  

yydL()+uL(

U)

, (.)

Shp(Uhp) =

 

YhpydL()+UhpL(

U)

. (.)

It can be shown [] that

S(u),v=u+Bp,v, (.)

S(Uhp),v

=Uhp+Bp(Uhp),v

, (.)

Shp (Uhp),v

=Uhp+BP˜hp,v

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It is clear thatSandShpare well defined and continuous onKandKhp. Also the

func-tionalShpcan be naturally extended onK. Then (.) and (.) can be represented as

min

u∈K

T

S(u)dt

(.)

and

min

Uhp∈Khp

T

Shp(Uhp)dt

. (.)

In many application,S(·) is uniform convex near the solutionu. The convexity ofS(·) is closely related to the second order sufficient conditions of the optimal control problems, which are assumed in many studies on numerical methods of the problem. For instance, in many applications, there is ac> , independent ofh, such that

T

S(u) –S(Uhp),uUhp

UdtcuUhp

L(J;L()). (.)

The following theorem is the first step to derivea posteriorierror estimates.

Theorem . Let(y,u,p)and(Yhp,Php,Uhp)be the solutions of(.)-(.)and(.)

-(.),respectively.Assume that(Shp(Uhp))|τHs(τ),∀τTh(s= , ),and there is a vhp

Khpsuch that

Shp (Uhp),vhpuC

τTh

hτShp(Uhp)Hs)uUhpsL(τ). (.)

Then we have

uUhpL(J;L())+Cp(Uhp) –P˜hp

L(J;L()), (.)

where

η=

T

τ∈Th

h+sτ Uhp+BP˜hp +s H)dt,

and p(Uhp)is defined by the following equations:

∂ty(Uhp),w

+ay(Uhp),w

+φy(Uhp)

,w= (f+BUhp,w), ∀wV, (.)

y(Uhp)(x, ) =y(x), x,

∂tp(Uhp),q

+aq,p(Uhp)

+φy(Uhp)

p(Uhp),q

=y(Uhp) –yd,q

, ∀qV, (.)

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Proof It follows from (.) and (.) thatT(S(u),uv)dt≤,∀vK, andT(Shp(Uhp),

Uhpvhp)dt≤,∀vhpKhpK. Then it follows from the assumptions (.), (.), and

the Schwartz inequality that

cuUhpL(J;L())

T

S(u) –S(Uhp),uUhp

dt

T

Shp (Uhp),vhpu

+Shp (Uhp) –S(Uhp),uUhp

dt

C

T

τ∈Th

h+sτ Shp(Uhp) +s

Hs(τ)+Shp(Uhp) –S(Uhp)  L()

dt

+c

uUhp

L(J;L()). (.)

It is not difficult to show

Shp(Uhp) =Uhp+BP˜hp, S(Uhp) =Uhp+Bp(Uhp), (.)

wherep(Uhp) is defined in (.)-(.). Thanks to (.), it is easy to derive

Shp (Uhp) –S(Uhp)L()=p(Uhp) –P˜hpL(). (.)

Then by using the estimates (.) and (.) we can prove the requested result (.).

Next, we are in the position to estimate the errors Yhpy(Uhp)L(,T;H()) and

Phpp(Uhp)L(,T;H()).

Theorem . Let(Yhp,Php,Uhp)be the solutions of(.)-(.),let (y(Uhp),p(Uhp))be

defined by(.)-(.).Then we have

Yhpy(Uhp) 

L(,T;H())+Phpp(Uhp) 

L(,T;H())C

i=

ηi, (.)

where

η=

T

τ

hτ

pτ

τ

ˆ

f +BUhp+div(A∇ ˆYhp) –φ(Yˆhp) –

∂Yhp

∂t

dx dt,

η=

T

τ

hτ

pτ

τ

ˆ

Yhpyˆd+div

A∗∇ ˜Php

φ(Y˜hp)P˜hp+

∂Php

∂t

dx dt,

η=

T

e

e

he

pe

(A∇ ˆYhpn

de dt+

T

e

e

he

pe

A∗∇ ˜Php

·nde dt,

η=

T

A∇(YˆhpYhp) dx dt+ T

A∗∇(P˜hpPhp) dx dt,

η=YhpY˜hpL(,T;L())+YhpYˆhpL(,T;L())+ydyˆdL(,T;L())

(10)

where e=τ¯

e ∩ ¯τe,τe,τeare two neighboring elements inT, [A∇ ˆYhp·n]eand[A∗∇ ˜Php·n]e

are the A-normal and A-normal derivative jumps over the interior edge e,respectively, defined by

(A∇ ˆYhpn

e= (A∇ ˆYhp|τe–A∇ ˆYhp|τe)·n,

A∗∇ ˜Php

·ne=A∗∇ ˜Php|τe–A

∇ ˜P hp|τe

·n,

where n is the unit normal vector on e=τ¯e∩ ¯τeoutwardsτe.For later convenience,we define[A∇ ˆYhp·n]e= and[A∗∇ ˜Php·n]e= when e∂.

Proof Letrhp=p(Uhp) –PhpandEbe the linear operator defined in Lemma .. Note that

(p(Uhp) –Php)(x,T) = , hence

T

∂(p(Uhp) –Php)

∂t ,rhp

dt≥. (.)

By using the assumption ofφ, (.), and (.), we obtain

crhpL(,T;H())

T

arhp,p(Uhp) –Php

dt+

T

φy(Uhp)

p(Uhp) –Php

,p(Uhp) –Php dtT

rhp,A∗∇

p(Uhp) –Php

dt

T

∂(p(Uhp) –Php)

∂t ,rhp

dt + T

φy(Uhp)

p(Uhp) –P˜hp

,p(Uhp) –Php dt + T

φy(Uhp)

(P˜hpPhp),p(Uhp) –Php dt = T

rhp,A∗∇

p(Uhp) –P˜hp

dt

T

∂(p(Uhp) –Php)

∂t ,rhp

dt + T

φy(Uhp)

p(Uhp) –φ(Y˜hp)P˜hp,p(Uhp) –Php dt + T˜

φ(Y˜hp) ˜

Yhpy(Uhp) ˜

Php,p(Uhp) –Php dt + T

φy(Uhp)

(P˜hpPhp),p(Uhp) –Php dt + T

rhp,A∗∇(P˜hpPhp)

dt. (.)

Connecting (.), (.), and (.), we have

crhpL(,T;H())

T

∇(rhpErhp),A∗∇

p(Uhp) –P˜hp dtT

∂(p(Uhp) –Php)

∂t ,rhpErhp

(11)

+

T

φy(Uhp)

p(Uhp) –φ(Y˜hp)P˜hp,rhpErhp dtT

∂(p(Uhp) –Php)

∂t ,Erhp

dt+

T

Erhp,A∗∇

p(Uhp) –P˜hp dt + T

φy(Uhp)

p(Uhp) –φ(Y˜hp)P˜hp,Erhp dt + T˜

φ(Y˜hp) ˜

Yhpy(Uhp) ˜

Php,p(Uhp) –Php dt + T

φy(Uhp)

(P˜hpPhp),p(Uhp) –Php

dt+

T

rhp,A∗∇(P˜hpPhp) dt = T

y(Uhp) –yd+div

A∗∇ ˜Php

φ(Y˜hp)P˜hp+

∂Php

∂t ,rhpErhp

dt + Te e

A∗∇ ˜Php

·n(rhpErhp)de dt

+

T

˜

φ(Y˜hp) ˜

Yhpy(Uhp) ˜

Php,p(Uhp) –Php dt + T

y(Uhp) –Yˆhp,Erhp

dt+

T

(yˆdyd,Erhp)dt

+

T

φy(Uhp)

(P˜hpPhp),p(Uhp) –Php dt + T

rhp,A∗∇(P˜hpPhp)

dt. (.)

Then we have

cp(Uhp) –PhpL(,T;H())

T

ˆ

Yhpyˆd+div

A∗∇ ˜Php

φ(Y˜hp)P˜hp+

∂Php

∂t ,rhpErhp

dt + Te e

A∗∇ ˜Php

·n(rhpErhp)de dt

+

T

y(Uhp) –Yˆhp,rhp

dt+

T

(yˆdyd,rhp)dt

+

T

rhp,A∗∇(P˜hpPhp) dt + T˜

φ(Y˜hp) ˜

Yhpy(Uhp) ˜

Php,p(Uhp) –Php dt + T

φy(Uhp)

(P˜hpPhp),p(Uhp) –Php dt ≡  i=

(12)

It follows from Lemma . that

I= T

ˆ

Yhpyˆd+div

A∗∇ ˜Php

φ(Y˜hp)P˜hp+

∂Php

∂t ,rhpErhp

dt

C(δ)

T

τ

hτ

pτ

τ

ˆ

Yhpyˆd+div

A∗∇ ˜Php

φ(Y˜hp)P˜hp+

∂Php

∂t

dx dt

+δ

T

rhpH()dt

=C(δ)η+δp(Uhp) –Php

L(,T;H()). (.)

Similarly,

I= T

e

e

A∗∇ ˜Php

·n(rhpErhp)de dt

C(δ)

T

e

e

he

pe

A∗∇ ˜Php

·nde dt+δ

T

rhpH()dt

C(δ)η+δp(Uhp) –PhpL(,T;H()). (.)

ForI-I, we have

I= T

y(Uhp) –Yˆhp,rhp

dt

C(δ)

T

y(Uhp) –Yˆhp

dx dt+δp(Uhp) –Php

L(,T;H())

C(δ)y(Uhp) –Yhp

L(,T;H())+C(δ)YhpYˆhpL(,T;L())

+δp(Uhp) –Php

L(,T;H())

C(δ)η+C(δ)y(Uhp) –Yhp

L(,T;H())+δp(Uhp) –Php

L(,T;H()), (.)

I= T

ydyd,rhp)dt

C(δ)ydyˆdL(,T;L())+δp(Uhp) –PhpL(,T;H())

C(δ)η+δp(Uhp) –PhpL(,T;H()), (.)

and

I= T

rhp,A∗∇(P˜hpPhp)

dt

C(δ)

T

A(P˜

hpPhp) 

dx dt+δ

T

|∇rhp|dx dt

C(δ)η+δp(Uhp) –Php

(13)

Similarly, we can obtain

I= T

˜

φ(Y˜hp) ˜

Yhpy(Uhp) ˜

Php,p(Uhp) –Php

dt

C(δ)

T

y(Uhp) –Y˜hp

dx dt+δp(Uhp) –Php

L(,T;H())

C(δ)y(Uhp) –Yhp

L(,T;H())+C(δ)YhpY˜hpL(,T;L())

+δp(Uhp) –Php

L(,T;H())

C(δ)η+C(δ)y(Uhp) –Yhp

L(,T;H())+δp(Uhp) –Php

L(,T;H()) (.)

and

I= T

φy(Uhp)

(P˜hpPhp),p(Uhp) –Php

dt

C(δ)˜PhpPhpL(,T;L())+δp(Uhp) –Php

L(,T;H())

C(δ)

T

A∗∇(P˜hpPhp) 

dx dt+δp(Uhp) –Php

L(,T;H())

C(δ)η+δp(Uhp) –Php

L(,T;H()). (.)

Then letδbe small enough, from (.)-(.), we derive

p(Uhp) –Php

L(,T;H())C(δ)

i=

ηi +C(δ)y(Uhp) –Yhp

L(,T;L()). (.)

Furthermore, we estimate the errory(Uhp) –YhpL(,T;L()). Letehp=y(Uhp) –Yhpand

Ebe the linear operator defined in Lemma .. Note that

T

∂(y(Uhp) –Yhp)

∂t ,ehp

dt

=

T

∂(y(Uhp) –Yhp)

∂t ehpdx dt

=

y(Uhp) –Yhp

(x,T)dx

y(Uhp) –Yhp

(x, )dx

T

∂(y(Uhp) –Yhp)

∂t ,ehp

dt.

Thus

T

∂(y(Uhp) –Yhp)

∂t ,ehp

dt+

y(x) –Yhp(x, )

L()≥. (.)

From (.), it is easy to see that

φy(Uhp)

φ(Yhp),ehp

=φ˜y(Uhp)

y(Uhp) –Yhp

,ehp

(14)

By using (.) and (.), we have

cehpL(,T;H())

T

ay(Uhp) –Yhp,ehp

dt+

T

φy(Uhp)

φ(Yhp),ehp

dt

T

ay(Uhp) –Yhp,ehp

dt+

T

φy(Uhp)

φ(Yˆhp),ehp dt + T

∂(y(Uhp) –Yhp)

∂t ,ehp

dt+

T

φ(Yˆhp) –φ(Yhp),ehp

dt

+

y(x) –Yhp(x, )

L()

=

T

Ay(Uhp) –Yˆhp

,∇ehp

dt+

T

φy(Uhp)

φ(Yˆhp),ehp dt + T

∂(y(Uhp) –Yhp)

∂t ,ehp

dt+

T

A∇(YˆhpYhp),∇ehp dt + T

φ(Yˆhp) –φ(Yhp),ehp

dt

+

y(x) –Yhp(x, )

L(). (.)

Connecting (.), (.), (.), and (.), we obtain

cehpL(,T;H())

T

ˆ

f+BUhp+div(A∇ ˆYhp) –φ(Yˆhp) –

∂Yhp

∂t ,ehpEehp

dt + Te e

(A∇ ˆYhpn

(ehpEehp)de dt+ T

(ffˆ,ehp)dt

+

T

A∇(YˆhpYhp),∇ehp

dt+

y(x) –Yhp(x, )

L()

+

T

˜

φ(Yˆhp)(YˆhpYhp),ehp

dt

C(δ)

Tτ hτ pτ τ ˆ

f +BUhp+div(A∇ ˆYhp) –φ(Yˆhp) –

∂Yhp

∂t

dx dt

+C(δ)

Te e he pe

(A∇ ˆYhpn

de dt+C(δ)ffˆL(,T;L())

+C(δ)

T

A∇(YˆhpYhp) 

dx dt+C(δ) ˆYhpYhpL(,T;H())

+

y(x) –Yhp(x, )

L()+δy(Uhp) –Yhp

L(,T;H())

C(δ)

i=

ηi+δy(Uhp) –Yhp

(15)

Hence, letδbe small enough, we have

y(Uhp) –YhpL(,T;H())C(δ)

i=

ηi. (.)

Then (.) follows from (.) and (.).

Finally, collecting Theorems .-., we derive the following residual-baseda posteriori error estimates.

Theorem . Let(y,p,u)and(Yhp,Php,Uhp)are the solutions of(.)-(.)and(.)

-(.)respectively.Assume that all the conditions in Theorem.are valid.Then

yYhpL(,T;H())+pPhpL(,T;H())+uUhpL(,T;L(

U))

C

i=

ηi, (.)

whereηi,i= , . . . , are defined in Theorem.and Theorem..

Proof It follows from Theorem . and Theorem . that

uUhpL(,T;L(

U))≤

+CP˜hpp(Uhp) 

L(,T;L())

+C˜PhpPhpL(,T;L())

+CPhpp(Uhp) 

L(,T;L())

C

i=

ηi +C˜PhpPhpL(,T;L()). (.)

Note thatAis positive definite, it follows from the Poincaré inequality that

˜PhpPhpL(,T;L())

T

A∗∇(P˜hpPhp) dx dt

. (.)

Then it follows from (.) and (.) that

uUhpL(,T;L(

U))≤C

i=

ηi. (.)

Note that

yYhpL(,T;H())yy(Uhp) 

L(,T;H())+y(Uhp) –Yhp

L(,T;H()), (.)

pPhpL(,T;H())pp(Uhp) 

L(,T;H())+p(Uhp) –Php

(16)

and

yy(Uhp)

L(,T;H())CuUhpL(,T;L(

U)), (.)

pp(Uhp) 

L(,T;H())yy(Uhp) 

L(,T;L())CuUhpL(,T;L(

U)). (.)

Therefore, we obtain (.) from (.) and (.)-(.).

4 Conclusion and future work

In this paper, we present thehpversion of the finite element approximation for the opti-mal control problems governed by nonlinear parabolic equations. By using thehpfinite element approximation for both the state and the co-state variables and thehp discontinu-ous Galerkin finite element approximation for the control variable, we derivehp residual-baseda posteriorierror estimates for the nonlinear parabolic optimal control problems. To the best of our knowledge in the context of optimal control problems, these residual-baseda posteriorierror estimates for the nonlinear parabolic optimal control problems are new.

In future, we shall consider thehpversion of the finite element method for hyperbolic optimal control problems. Furthermore, we shall considera posteriorierror estimates and the superconvergence of the hpfinite element solutions for hyperbolic optimal control problems.

Competing interests

The authors declare that they have no competing interests.

Authors’ contributions

ZL and LC have participated in the sequence alignment and drafted the manuscript. HL and CH have made substantial contributions to the conception and design. All authors read and approved the final manuscript.

Author details

1Key Laboratory of Signal and Information Processing, Chongqing Three Gorges University, Chongqing, 404000, P.R.

China.2Key Laboratory for Nonlinear Science and System Structure, Chongqing Three Gorges University, Chongqing,

404000, P.R. China.3Research Center for Mathematics and Economics, Tianjin University of Finance and Economics,

Tianjin, 300222, P.R. China.4Chongqing Wanzhou Long Bao Middle School, Chongqing, 404001, P.R. China.5Huashang

College, Guangdong University of Finance, Guangzhou, 511300, P.R. China.

Acknowledgements

The authors express their thanks to the referees for their helpful suggestions, which led to improvements of the presentation. This work is supported by National Science Foundation of China (11201510), China Postdoctoral Science Foundation (2015M580197), Chongqing Research Program of Basic Research and Frontier Technology

(cstc2015jcyjA20001), Ministry of education Chunhui projects (Z2015139) and Science and Technology Project of Wanzhou District of Chongqing (2013030050).

Received: 17 June 2015 Accepted: 1 February 2016 References

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(17)

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References

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