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
5and Longzhou Cao
1*Correspondence:
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
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() = {v∈Wm,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
y–ydL()+uL(
U)
dt
, (.)
yt–div(A∇y) +φ(y) =f+Bu, x∈,t∈(,T], (.)
y(x,t) = , x∈∂,t∈(,T], (.)
y(x, ) =y(x), x∈, (.)
whereandU are bounded open sets inRwith a Lipschitz boundary∂and∂U,
K is a set defined byK={v∈X:T
Uv dx dt≥}, andf,yd∈L
(,T;H),y
(x)∈V=
ξtAξ≥cξ,ξ ∈R. The functionφ(·)∈W,∞(–R,R) for anyR> ,φ(y)∈L() for
anyy∈H(), andφ(y)≥.
Let a(v,w) = (A∇v)· ∇w dx, ∀v,w∈ V, (f,f) =
ffdx, ∀f,f ∈ H, (v,w)U =
Uvw dx, ∀v,w∈U. 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,w∈Y.
Then a weak formula of the convex nonlinear parabolic optimal control problems (.)-(.) reads
min
u(t)∈K
T
y–ydL()+uL(
U)
dt
, (.)
wherey∈W,u∈X,u(t)∈K, subject to
(yt,w) +a(y,w) +
φ(y),w= (f+Bu,w), ∀w∈Y,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 p∈W such that the triplet (y,p,u) satisfies the following optimality conditions:
(yt,w) +a(y,w) +
φ(y),w= (f+Bu,w), ∀w∈Y,y() =y(x), (.)
–(pt,w) +a(q,p) +
φ(y)p,q= (y–yd,q), ∀q∈Y,p(T) = , (.) T
u+B∗p,v–uUdt≥, ∀v∈K, (.)
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,B∗p–B∗p,
where B∗p= T
UB∗p dx dt
T
Udx dt
denotes the integral average onU×[,T]of the function B∗p.
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 elementsτ∈T associated with each
elementτ, and an affine element mapFτ :τ →τ, where the reference elementτ is the
reference triangle
We consider the triangulationT which satisfies the standard conditions defined in [] and writehτ =diamτ. Additionally we assume that triangulationT isγ-shape regular,
i.e.,
h–τ FτL∞(τ)+hτF τ
–
L∞(τ)≤γ. (.)
This implies that there exists a constantC> that depends solely onγ such that
C–hτ≤hτ≤Chτ, τ,τ∈T withτ∩τ=∅, (.)
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 elementsτU∈TU, isγ-shape regular which satisfies the standard conditions
asT. Associated with each elementτUis an affine element mapFτU:τ→τU. We further
assume the triangulationT satisfies the relation between the patch and the reference patch in [].
For each elementτ∈T, we denoteE(τ) the set of edges ofτandN(τ) the set of vertices ofτ, and choose a polynomial degreepτ∈Nand collect these numbers in the polynomial
degree vector p= (pτ)τ∈T. Similarly, for each elementτU∈TU, we choose a polynomial
degree vector p= (pτU)τU∈TU(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 (V∈N(T), e∈E(T)):
N(e) =V∈N(T) :V∈e,
wV=
x∈:x∈τ andτ∩ {V} =∅,
we=
V∈N(e)
wV, wτ =
V∈N(τ)
wV,
hτU=diamτU, pe=max
pτ:e∈E(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) =v∈C() :v|
τ◦Fτ∈pτ(τ)
,
Up(T
U) =
v∈L(U) :v|τU◦FτU∈pτU(τ)
,
where we set
k(τ) = ⎧ ⎨ ⎩
Pk=span{xiyj: ≤i+j≤k}, ifτ =T,
Qk=span{xiyj: ≤i,j≤k}, ifτ =S.
We also assume that the polynomial degree vector psatisfies
Then we can introduce the finite dimensional spaces Khp=K∩Up(TU), Vhp=V ∩
Sp(T).
The semidiscretehpfinite element approximation of (.)-(.) is as follows:
min
uhp∈Khp
T
yhp–ydL()+uhpL(
U)
dt
, (.)
∂yhp
∂t ,whp
+a(yhp,whp) +
φ(yhp),w
= (f+Buhp,whp), ∀whp∈Vhp, (.)
yhp(x, ) =yhp(x), x∈, (.)
whereyhp∈H(,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-statephp∈Vhp
such that the triplet (yhp,php,uhp) satisfies the following optimality conditions:
∂yhp
∂t ,whp
+a(yhp,whp) +
φ(yhp),w
= (f+Buhp,whp), ∀whp∈Vhp, (.)
yhp(x, ) =yhp(x), x∈,
–
∂php
∂t ,qhp
+a(qhp,php) +
φ(yhp)php,qhp
= (yhp–yd,qhp), ∀whp∈Vhp, (.)
php(x,T) = , x∈,
uhp+B∗php,vhp–uhp
U≥, ∀vhp∈Khp. (.)
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=ti–ti–,i= , , . . . ,M,k=≤i≤Mmax{ki}.
Fori= , , . . . ,M, construct thehpfinite element approximation spacesVhpi ⊂H() (similar to Vhp) on theith time step. Similarly, we construct thehpfinite element
ap-proximation spaces Khpi ⊂L(
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
hp–yd(x,ti) L()+
u
i hp
L(
U)
, (.)
yi hp–yi–hp
ki
,whp
+ayihp,whp
+φyihp,whp
=f(x,ti) +Buihp,whp
, ∀whp∈Vhpi , (.)
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
optimality conditions:
Yi hp–Yhpi–
ki
,whp
+aYhpi ,whp
+φYhpi ,whp
=f(x,ti) +BUhpi ,whp
, (.)
∀whp∈Vhpi ⊂V=H(), i= , , . . . ,M, Yhp(x) =y hp
(x), x∈, Pi–
hp –Pihp
ki
,qhp
+aqhp,Pi–hp
+φYhpi–Pi–hp,qhp
=Yhpi –yd(x,ti),qhp
, (.)
∀qhp∈Vhpi ⊂V=H(), i=M, . . . , , , PMhp(x) = , x∈,
Uhpi +B∗Pi–hp,vhp–Uhpi
U≥, ∀vhp∈K i
hp,i= , , . . . ,M. (.)
Fori= , , . . . ,M, let
Yhp|(ti–,ti]=
(ti–t)Yhpi–+ (t–ti–)Yhpi
/ki,
Php|(ti–,ti]=
(ti–t)Phpi–+ (t–ti–)Pihp
/ki,
Uhp|(ti–,ti]=U
i hp.
For any functionw∈C(,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), (.)
∀whp∈Vhpi ⊂V=H(), t∈(ti–,ti],i= , , . . . ,M,
Yhp(x, ) =yhp(x), x∈,
–
∂Php
∂t ,qhp
+a(qhp,P˜hp) +
φ(Y˜hp)P˜hp,qhp
= (Yˆhp–yˆd,qhp), (.)
∀qhp∈Vhpi ⊂V=H(), t∈(ti–,ti],i=M, . . . , , ,
Php(x,T) = , x∈,
Uhp+B∗P˜hp,vhp–Uhp
U≥, (.)
∀vhp∈Khpi , 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
pτU :H(τU)→PpτU(τU)such that∀v∈H(τU),τU∈TUthe following inequality is valid: v–πhτU
pτUL(τ
U)≤C
hτU
pτU
vH(τ
U),
where we will write v∈PpτU(τU)if the following satisfied:v|τU◦FτU ∈PpτU(τ)ifτU is a
Lemma . Letp be 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 v∈H
()and all elementsτ∈T and all
edges e∈E(T):
v–EvL(τ)+
hτ
pτ
∇(v–Ev)
L(τ)≤C
hτ
pτ∇
vL(wτ),
v–EvL(e)≤C
he
pe
∇vL(w
e).
Lemma . Letp be an arbitrary polynomial degree distribution satisfying(.)and
pτ ≥, ∀τ ∈T. 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 v∈H()∩H()and all elementsτ ∈T and all edges e∈E(T):
v–EvL(τ)+
hτ
pτ
∇(v–Ev)L(τ)≤C
hτ
pτ
|v|H(wτ),
v–EvL(e)≤C
he
pe
|v|H(w
e).
Forϕ∈Wh, 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) =
( –s)φρ+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) =
y–ydL()+uL(
U)
, (.)
Shp(Uhp) =
Yhp–ydL()+UhpL(
U)
. (.)
It can be shown [] that
S(u),v=u+B∗p,v, (.)
S(Uhp),v
=Uhp+B∗p(Uhp),v
, (.)
Shp (Uhp),v
=Uhp+B∗P˜hp,v
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),u–Uhp
Udt≥cu–Uhp
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))|τ ∈Hs(τ),∀τ∈Th(s= , ),and there is a vhp∈
Khpsuch that
Shp (Uhp),vhp–u ≤C
τ∈Th
hτShp(Uhp)Hs(τ)u–UhpsL(τ). (.)
Then we have
u–UhpL(J;L())≤Cη+Cp(Uhp) –P˜hp
L(J;L()), (.)
where
η=
T
τ∈Th
h+sτ Uhp+B∗P˜hp +s H(τ)dt,
and p(Uhp)is defined by the following equations:
∂
∂ty(Uhp),w
+ay(Uhp),w
+φy(Uhp)
,w= (f+BUhp,w), ∀w∈V, (.)
y(Uhp)(x, ) =y(x), x∈,
–
∂
∂tp(Uhp),q
+aq,p(Uhp)
+φy(Uhp)
p(Uhp),q
=y(Uhp) –yd,q
, ∀q∈V, (.)
Proof It follows from (.) and (.) thatT(S(u),u–v)dt≤,∀v∈K, andT(Shp(Uhp),
Uhp–vhp)dt≤,∀vhp∈Khp⊂K. Then it follows from the assumptions (.), (.), and
the Schwartz inequality that
cu–UhpL(J;L())≤
T
S(u) –S(Uhp),u–Uhp
dt
≤ T
Shp (Uhp),vhp–u
+Shp (Uhp) –S(Uhp),u–Uhp
dt
≤C
T
τ∈Th
h+sτ Shp(Uhp) +s
Hs(τ)+Shp(Uhp) –S(Uhp) L()
dt
+c
u–Uhp
L(J;L()). (.)
It is not difficult to show
Shp(Uhp) =Uhp+B∗P˜hp, S(Uhp) =Uhp+B∗p(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 Yhp – y(Uhp)L(,T;H()) and
Php–p(Uhp)L(,T;H()).
Theorem . Let(Yhp,Php,Uhp)be the solutions of(.)-(.),let (y(Uhp),p(Uhp))be
defined by(.)-(.).Then we have
Yhp–y(Uhp)
L(,T;H())+Php–p(Uhp)
L(,T;H())≤C
i=
ηi, (.)
where
η=
T
τ
h τ
p τ
τ
ˆ
f +BUhp+div(A∇ ˆYhp) –φ(Yˆhp) –
∂Yhp
∂t
dx dt,
η=
T
τ
h τ
p τ
τ
ˆ
Yhp–yˆd+div
A∗∇ ˜Php
–φ(Y˜hp)P˜hp+
∂Php
∂t
dx dt,
η=
T
e
e
he
pe
(A∇ ˆYhp)·n
de dt+
T
e
e
he
pe
A∗∇ ˜Php
·nde dt,
η=
T
A∇(Yˆhp–Yhp) dx dt+ T
A∗∇(P˜hp–Php) dx dt,
η=Yhp–Y˜hpL(,T;L())+Yhp–YˆhpL(,T;L())+yd–yˆdL(,T;L())
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∇ ˆYhp)·n
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∩ ¯τe outwardsτe.For later convenience,we define[A∇ ˆYhp·n]e= and[A∗∇ ˜Php·n]e= when e⊂∂.
Proof Letrhp=p(Uhp) –PhpandEbe 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 dt ≤ T
∇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˜hp–Php),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) ˜
Yhp–y(Uhp) ˜
Php,p(Uhp) –Php dt + T
φy(Uhp)
(P˜hp–Php),p(Uhp) –Php dt + T
∇rhp,A∗∇(P˜hp–Php)
dt. (.)
Connecting (.), (.), and (.), we have
crhpL(,T;H())
≤ T
∇(rhp–Erhp),A∗∇
p(Uhp) –P˜hp dt – T
∂(p(Uhp) –Php)
∂t ,rhp–Erhp
+
T
φy(Uhp)
p(Uhp) –φ(Y˜hp)P˜hp,rhp–Erhp dt – T
∂(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) ˜
Yhp–y(Uhp) ˜
Php,p(Uhp) –Php dt + T
φy(Uhp)
(P˜hp–Php),p(Uhp) –Php
dt+
T
∇rhp,A∗∇(P˜hp–Php) dt = T
y(Uhp) –yd+div
A∗∇ ˜Php
–φ(Y˜hp)P˜hp+
∂Php
∂t ,rhp–Erhp
dt + T e e
A∗∇ ˜Php
·n(rhp–Erhp)de dt
+
T
˜
φ(Y˜hp) ˜
Yhp–y(Uhp) ˜
Php,p(Uhp) –Php dt + T
y(Uhp) –Yˆhp,Erhp
dt+
T
(yˆd–yd,Erhp)dt
+
T
φy(Uhp)
(P˜hp–Php),p(Uhp) –Php dt + T
∇rhp,A∗∇(P˜hp–Php)
dt. (.)
Then we have
cp(Uhp) –PhpL(,T;H())
≤ T
ˆ
Yhp–yˆd+div
A∗∇ ˜Php
–φ(Y˜hp)P˜hp+
∂Php
∂t ,rhp–Erhp
dt + T e e
A∗∇ ˜Php
·n(rhp–Erhp)de dt
+
T
y(Uhp) –Yˆhp,rhp
dt+
T
(yˆd–yd,rhp)dt
+
T
∇rhp,A∗∇(P˜hp–Php) dt + T ˜
φ(Y˜hp) ˜
Yhp–y(Uhp) ˜
Php,p(Uhp) –Php dt + T
φy(Uhp)
(P˜hp–Php),p(Uhp) –Php dt ≡ i=
It follows from Lemma . that
I= T
ˆ
Yhp–yˆd+div
A∗∇ ˜Php
–φ(Y˜hp)P˜hp+
∂Php
∂t ,rhp–Erhp
dt
≤C(δ)
T
τ
h τ
p τ
τ
ˆ
Yhp–yˆd+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(rhp–Erhp)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)Yhp–YˆhpL(,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
(ˆyd–yd,rhp)dt
≤C(δ)yd–yˆdL(,T;L())+δp(Uhp) –PhpL(,T;H())
≤C(δ)η+δp(Uhp) –PhpL(,T;H()), (.)
and
I= T
∇rhp,A∗∇(P˜hp–Php)
dt
≤C(δ)
T
A∗∇(P˜
hp–Php)
dx dt+δ
T
|∇rhp|dx dt
≤C(δ)η+δp(Uhp) –Php
Similarly, we can obtain
I= T
˜
φ(Y˜hp) ˜
Yhp–y(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)Yhp–Y˜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˜hp–Php),p(Uhp) –Php
dt
≤C(δ)˜Php–PhpL(,T;L())+δp(Uhp) –Php
L(,T;H())
≤C(δ)
T
A∗∇(P˜hp–Php)
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
Ebe 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
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
A∇y(Uhp) –Yˆhp
,∇ehp
dt+
T
φy(Uhp)
–φ(Yˆhp),ehp dt + T
∂(y(Uhp) –Yhp)
∂t ,ehp
dt+
T
A∇(Yˆhp–Yhp),∇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 ,ehp–Eehp
dt + T e e
(A∇ ˆYhp)·n
(ehp–Eehp)de dt+ T
(f–fˆ,ehp)dt
+
T
A∇(Yˆhp–Yhp),∇ehp
dt+
y(x) –Yhp(x, )
L()
+
T
˜
φ(Yˆhp)(Yˆhp–Yhp),ehp
dt
≤C(δ)
T τ h τ p τ τ ˆ
f +BUhp+div(A∇ ˆYhp) –φ(Yˆhp) –
∂Yhp
∂t
dx dt
+C(δ)
T e e he pe
(A∇ ˆYhp)·n
de dt+C(δ)f–fˆL(,T;L())
+C(δ)
T
A∇(Yˆhp–Yhp)
dx dt+C(δ) ˆYhp–YhpL(,T;H())
+
y(x) –Yhp(x, )
L()+δy(Uhp) –Yhp
L(,T;H())
≤C(δ)
i=
ηi+δy(Uhp) –Yhp
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
y–YhpL(,T;H())+p–PhpL(,T;H())+u–UhpL(,T;L(
U))
≤C
i=
ηi, (.)
whereηi,i= , . . . , are defined in Theorem.and Theorem..
Proof It follows from Theorem . and Theorem . that
u–UhpL(,T;L(
U))≤Cη
+CP˜hp–p(Uhp)
L(,T;L())
≤Cη+C˜Php–PhpL(,T;L())
+CPhp–p(Uhp)
L(,T;L())
≤C
i=
ηi +C˜Php–PhpL(,T;L()). (.)
Note thatAis positive definite, it follows from the Poincaré inequality that
˜Php–PhpL(,T;L())≤
T
A∗∇(P˜hp–Php) dx dt
≤Cη. (.)
Then it follows from (.) and (.) that
u–UhpL(,T;L(
U))≤C
i=
ηi. (.)
Note that
y–YhpL(,T;H())≤y–y(Uhp)
L(,T;H())+y(Uhp) –Yhp
L(,T;H()), (.)
p–PhpL(,T;H())≤p–p(Uhp)
L(,T;H())+p(Uhp) –Php
and
y–y(Uhp)
L(,T;H())≤Cu–UhpL(,T;L(
U)), (.)
p–p(Uhp)
L(,T;H())≤y–y(Uhp)
L(,T;L())≤Cu–UhpL(,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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