Optimality conditions for nonconvex multistate control problems in the coefficients
Abstract
The purpose of this paper is to attain some optimality conditions for the identification of a diffusion matrix (material) under several restrictions. Assuming that the set of such diffusion matrices is closed for the H-convergence, we give a method to obtain admissible directions which applies to a not-necessarily convex control set. Our results permit obtaining the diffusion matrix from the state functions.
Full text
OPTIMALITY CONDITIONS FOR NONCONVEX MULTISTATE
CONTROL PROBLEMS IN THE COEFFICIENTS∗
JUAN CASADO-D´
IAZ†, JULIO COUCE-CALVO†,AND JOS´
E D. MART´
IN-G´
OMEZ†
SIAM J. CONTROL OPTIM.c
2004 Socie y o Indus ial and Applied Ma hema ics
Vol. 43, No. 1, pp. 216–239
Abs ac . The pu pose o his pape is o a ain some op imali y condi ions o he iden ifica ion
o a diffusion ma ix (ma e ial) unde se e al es ic ions. Assuming ha he se o such diffusion
ma ices is closed o he H-con e gence, we gi e a me hod o ob ain admissible di ec ions which
applies o a no -necessa ily con ex con ol se . Ou esul s pe mi ob aining he diffusion ma ix
om he s a e unc ions.
Key wo ds. con ol in he coefficien s, admissible di ec ions, noncon ex con ol se
AMS subjec classifica ion. 49K20
DOI. 10.1137/S0363012902411714
1. In oduc ion. The p oblem we conside in he p esen pape is ela ed o
he choice o an op imal ma e ial unde se e al condi ions, o he iden ifica ion o a
ma e ial om a fini e numbe o obse a ions. In a ma hema ical se ing, we ha e he
model p oblem
min
A∈M(Ω) J(y1,... ,y
k),(1.1)
whe e yi=yi(A), 1 ≤i≤k, a e he solu ions o he equa ions
−di A∇yi= iin D(Ω),
yi∈H1
0(Ω),1≤i≤k.
(1.2)
He e Ω is a bounded open se o RN,Jis a smoo h objec i e unc ional in H1
0(Ω)k,
1,... ,
ka e kfixed elemen s o H−1(Ω), and M(Ω) is a gi en se o measu able
unc ions wi h alues in he space o symme ic ma ices o o de N. The elemen s
o M(Ω) a e uni o mly ellip ic and bounded. Clea ly, o he gene aliza ions can be
conside ed: Jdepending on A, o he bounda y condi ions, e c. A physical example
is he iden ifica ion o a ma e ial. Fo his pu pose, we apply a fini e numbe ko
ex e nal condi ions (in ou case hey a e ep esen ed by i) and in each case we ealize
a measu e o he co esponding s a e. Fo example, we gi e he alue zio he s a e
in a subse ω⊂Ω. Then he p oblem can be o mula ed as
min
k
i=1 ω|yi−zi|2dx,
whe e yia e he solu ions o (1.2).
Assuming Jis sequen ial lowe semicon inuous o he weak opology o H1
0(Ω)k
and M(Ω) is closed o he H-con e gence o he G-con e gence, because we a e
∗Recei ed by he edi o s July 22, 2002; accep ed o publica ion (in e ised o m) No embe 24,
2003; published elec onically June 15, 2004. This wo k has been pa ially suppo ed by he p ojec s
BFM 2002-00672 o he D.G.I. o he “Minis e io de Ciencia y Tecnolog´ıa” o Spain and FQM309 o
he “Jun a de Andaluc´ıa.”
h p://www.siam.o g/jou nals/sicon/43-1/41171.h ml
†Dep o. de Ecuaciones Di e enciales y An´alisis Num´e ico, Fac. de Ma em´a icas, Uni e sidad de
Se illa, C. Ta fia s/n, 41012 Se illa, Spain ([email p o ec ed], [email p o ec ed], [email p o ec ed]).
216
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NONCONVEX CONTROL PROBLEMS IN THE COEFFICIENTS 217
wo king wi h symme ic ma ices and hus he wo concep s a e equi alen (see, e.g.,
[22], [19], [18], [4], [25]), i is well known ha (1.1) has, a leas , a solu ion (see, e.g.,
[25], [17]). I M(Ω) does no sa is y his las condi ion and Jis sequen ial con inuous
o he weak opology o H1
0(Ω)k, we can ob ain a elaxed p oblem eplacing M(Ω)
by i s H-closu e. Thus, i is na u al o assume M(Ω) is H-closed. The calculus o
he H-closu e o a se is a e y difficul p oblem and he e a e a lo o wo ks in his
field (see, e.g., [23], [14], [13], [8], [25], [3], [16] and he e e ences in hem). In his
pape we a e in e es ed in ob aining some necessa y condi ions which mus sa is y he
op imal solu ion o (1.1). Fo k= 1, he p oblem has been s udied in [13], [20], [8],
[25], [3]. Fo k>1, he e a e ew esul s o ou knowledge (see [25], [6], [7], [3]).
The pape is o ganized as ollows:
In sec ion 3 we gi e a defini ion o admissible di ec ion (see Defini ion 3.1). Then
we p o e ha i Ais a solu ion o (1.1), y1,... ,y
k he co esponding s a e unc ions,
p1,... ,p
k he solu ions o (3.2) ( he adjoin s a es), and C he ma ix defined by
(3.3), we ha e
Ω
H:Cdx≤0(1.3)
o e e y admissible di ec ion H. Rela ed esul s can be ound, o example, in [8],
[13], [25], [3]. Howe e , in hese pape s, he admissible di ec ions a e o he o m
H=B−A, wi h Bin M(Ω), which needs some con exi y assump ions. When
k≤N−1 (in pa icula k= 1) and M(Ω) is ob ained by homogeniza ion, mixing a
fini e numbe o ma ices wi h fixed p opo ions, a esul o Ta a (see [25]) shows
ha al hough M(Ω) is no con ex, o e e y ξ1,... ,ξ
k∈RN, he se
{(Bξ1,... ,Bξ
k)/B∈M(Ω)}⊂L∞(Ω)k
(1.4)
is con ex, and hus he di ec ions H=B−Acan s ill be conside ed. Howe e , his
is no ue o k≥N(o , in p inciple, o o he choices o M(Ω) e en i k≤N−1).
This is he eason we ha e gi en a mo e gene al defini ion o admissible di ec ion.
In sec ion 4, assuming M(Ω) local (see Defini ion 4.1) and closed o he H-
con e gence, we gi e an o iginal me hod o find admissible di ec ions ollowing ou
defini ion. As a consequence, we ob ain he main esul o he pape , Theo em 4.5,
whe e we p o e ha o e e y A, B ∈M(Ω), l∈{1,... ,N},W⊂RNlinea subspace
o dimension l, and e e y bounded measu able se To W, wi h l-dimensional posi i e
measu e, he ma ix Hdefined by
H(x)ei=(B(x)−A(x)) ei+1
|T|T∇W
zˆwi(x, z)d(z)
(1.5)
is an admissible di ec ion in A. He e e1,... ,e
Nis he s anda d basis o RN,∇W
z
deno es he g adien wi h espec o W, and ˆwiis he solu ion o he pa ial diffe en ial
p oblem gi en by (4.4). This di ec ion has he difficul y ha ˆwi(and hen H) canno
be explici ly ob ained. Howe e , we hink ha i can be in e es ing, o example, o
apply a descen me hod in o de o sol e nume ically p oblem (1.1), whe e we can
ob ain ˆwinume ically. Rela ed o his poin , an in e es ing ques ion, one ha we
wan o s udy in he u u e, is he op imal choice o Wand T o ob ain he s eepes
descen di ec ion. A c i e ion o de e mine his di ec ion (see Rema k 4.9) can be o
calcula e he maximum o H:Con he se o ma ices Hob ained by (1.5).
Al hough, as we ha e said abo e, i is no possible in gene al o ob ain ˆwiexplic-
i ly, we show in Theo em 4.12 ha his can be ca ied ou o a pa icula choice o
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218 J. CASADO-D´
IAZ, J. COUCE-CALVO, AND J. D. MART´
IN-G´
OMEZ
T(which p obably is no op imal). This pe mi s us o ob ain a amily o admissible
di ec ion, depending on he subspace Wchosen. Essen ially, hey a e o he o m
B−Aplus a e m which has a g ow h o o de wo in B−A o e e y B∈M(Ω).
When he dimension o Wis equal o 1, he co esponding admissible di ec ion comes
jus om a lamina ion. In his case he exp ession o His known and i can be ound,
o example, in [25] (i can also be ob ained om he esul s in [10]), bu o ou
knowledge i s u ili y o ob ain op imali y condi ions o p oblem (1.1) has no been
exploi ed. Mos o he consequences we ob ain in he p esen pape using Theo em
4.12 use only, in ac , l= 1. Howe e , we show ha in some cases (see Rema k 4.17)
i is be e o use a subspace o dimension g ea e han one. Using Theo em 4.12 we
p o e in Co olla y 4.18 ha o e e y B∈M(Ω), he condi ion
C:(A−B)≥0(1.6)
(which is he condi ion we find i he admissible di ec ions a e o he o m B−A) is s ill
ue on he se whe e Chas a nonposi i e eigen alue o whe e Ke (A−B)={0}.In
pa icula (see Co olla y 4.20) he condi ion (1.6) holds a.e. in Ω o e e y B∈M(Ω)
when k≤N−1. When M(Ω) comes om he mix u e o a fini e numbe o ma e ials
wi h fixed p opo ions, his esul can also be ob ained om he con exi y o he se
defined by (1.4), bu we no e ha ou se M(Ω) is mo e gene al.
In sec ion 5 we s udy he case whe e M(Ω) is in a iable by o a ions, which is a
na u al assump ion in he applica ions. Then we show ha condi ion (1.3) implies
ha Cand Aa e mu ually diagonalizable a.e. in Ω. Mo eo e , assuming u he
hypo heses (in pa icula i M(Ω) is H-closed and N≥3), we p o e in P oposi ion
5.4 ha he eigen alues o Aand Ca e mu ually o de ed.
As applica ion o he esul s s a ed abo e, i is possible o ob ain, in some si u-
a ions, he ma ix A om Cand hen o educe he se o op imali y condi ions o
a nonlinea pa ial diffe en ial sys em wi h a iables yi,pi,1≤i≤k. The main
p oblem o ca ying ou his poin is ha in gene al, he H-closu e o a gi en se is
unknown. In sec ion 6, we apply ou esul s o wo examples: The fi s one is he
mix u e o wo homogeneous iso opic ma e ials, which has also been s udied in [3]
(see also [25] o k= 1). In his case M(Ω) is con ex. In second p oblem we conside
a polyc ys al in dimension 2, whe e M(Ω) is no con ex.
2. No a ion. Fo a linea subspace W⊂RN, we define L(W, W ) as he space o
he linea applica ions om Win o Wand by Ls(W, W ) he subspace o he symme ic
applica ions. When W=RNwe w i e MN=L(RN,RN), Ms
N=Ls(RN,RN).
The o hogonal p ojec ion o RNin o Wis deno ed by PW.
Fo a ma ix A∈M
N, we define AW∈L(W, W )byAW=PWA|W.
The o hogonal subspace o Wis deno ed by W⊥.
Fo u:W→R, we deno e ∇Wu:W→W he g adien o uwi h espec o W,
i.e., ∇Wuis defined by
∇Wuξ=Dξu∀ξ∈W,
whe e Dξuis he de i a i e o uin he di ec ion ξ.
We deno e by {e1,... ,e
N} he s anda d basis o RN.
The g oup o he o hogonal ma ices in RNo de e minan 1 is deno ed by ON.
The scala p oduc o wo ma ices A, B ∈M
Nis w i en A:B.
The enso ial p oduc o wo ec o s ξ,η ∈RNis deno ed as ξ⊗η.
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NONCONVEX CONTROL PROBLEMS IN THE COEFFICIENTS 219
Fo a bounded open se Ω ⊂RN, we deno e by M(Ω) a fixed subse o he space
L∞(Ω,Ms
N) such ha he e exis α, β > 0 which sa is y
B(x)ξξ ≥α|ξ|2,|B(x)ξ|≤β|ξ|∀B∈M(Ω) a.e. x∈Ω.(2.1)
Fo a ma ix A∈M(Ω), KA(M(Ω)) and ¯
KA(M(Ω)) a e he cones o admissible
di ec ions o M(Ω) in A; see Defini ion 3.1.
Fo T⊂RNand ∈(0,N], we deno e by |T| he -dimensional Hausdo ff
measu e o T. The in eg al o a unc ion u:T→R, wi h espec o he -dimensional
Hausdo ff measu e, is w i en
T
u(z)dz.
When =N, we simpli y he no a ion by w i ing |T|and
T
u(z)dz.
We use he subindex o mean pe iodici y. Fo example, o a cube Y⊂RN,
H1
(Y) is he space o unc ions o H1
loc(RN) which a e Y-pe iodic.
3. Op imali y condi ions. In his sec ion we in oduce he defini ion o admis-
sible di ec ion. Using i , we ob ain he fi s op imali y esul o he con ol p oblem
(1.1).
De ini ion 3.1. Fo A∈M(Ω), le us define he cone o admissible di ec ions
¯
KA(M(Ω)) as he closu e in he weak-∗ opology o L∞(Ω,Ms
N)o he se KA(M(Ω)),
whe e KA(M(Ω)) is he se o H∈L∞(Ω,Ms
N)such ha he e exis a cons an c>0
and Aε∈M(Ω),ε>0, such ha
⎧
⎨
⎩
Aε−AL∞(Ω,Ms
N)≤cε,
lim
ε→0
Aε−A
ε=Ha.e. in Ω.
(3.1)
Theo em 3.2. We conside J:H1
0(Ω)k→R,F ´eche de i able, 1,... ,
k∈
H−1(Ω)k.Le A∈M(Ω) be a solu ion o (1.1) and y1,... ,y
k he solu ions o (1.2).
We define he adjoin s a es p1,... ,p
kas he solu ions o
−di (A∇pi)=∂iJ(y1,... ,y
k)in D(Ω),
pi∈H1
0(Ω),1≤i≤k,
(3.2)
and he ma ix C∈L1(Ω,Ms
N)by
C=1
2
k
i=1
(∇yi⊗∇pi+∇pi⊗∇yi).(3.3)
Then we ha e
Ω
H:Cdx≤0∀H∈¯
KA(M(Ω)).(3.4)
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220 J. CASADO-D´
IAZ, J. COUCE-CALVO, AND J. D. MART´
IN-G´
OMEZ
P oo . Le us fi s p o e he esul o H∈KA(M(Ω)). Fo ε>0 small enough,
we define y∗
i,ε,1≤i≤k, as he solu ion o
−di ((A+εH)∇y∗
i,ε)= iin D(Ω),
y∗
i,ε ∈H1
0(Ω).
(3.5)
Then i is easy o check ha o 1 ≤i≤k,weha e
lim
ε→0
y∗
i,ε −yi
ε=˙yiin H1
0(Ω),(3.6)
wi h ˙yi he solu ions o
−di (A∇˙yi+H∇yi)=0 inD(Ω),
˙yi∈H1
0(Ω).
(3.7)
Now, o ε>0, we conside Aε∈M(Ω) in he condi ions o (3.1). Then o
1≤i≤k, we define yi,ε as he solu ions o
−di (Aε∇yi,ε)= iin D(Ω),
yi,ε ∈H1
0(Ω).
(3.8)
Taking y∗
i,ε −yi,ε as es unc ion in he diffe ence o (3.5) and (3.8), and di iding by
ε,wege
1
εΩ
(A+εH)∇(y∗
i,ε −yi,ε)∇(y∗
i,ε −yi,ε)dx
=Ω
Aε−(A+εH)
ε∇(yi,ε −y∗
i,ε)∇(y∗
i,ε −yi,ε)dx(3.9)
+Ω
Aε−(A+εH)
ε∇y∗
i,ε∇(y∗
i,ε −yi,ε)dx.
By he ellip ici y o A+εH ( o εsmall enough) and (3.1), we deduce om (3.9) he
exis ence o c>0 such ha
1
εy∗
i,ε −yi,ε2
H1
0(Ω) ≤cy∗
i,ε −yi,εH1
0(Ω)µεL2(Ω),
wi h
µε=Aε−(A+εH)
ε∇y∗
i,ε.
F om (3.1), (3.6), and he Lebesgue-domina ed con e gence heo em, we deduce ha
µεcon e ges s ongly o ze o in L2(Ω)N. Thus,
lim
ε→0
y∗
i,ε −yi,ε
ε=0 inH1
0(Ω),
which, by (3.6), implies
lim
ε→0
yi,ε −yi
ε=˙yiin H1
0(Ω).(3.10)
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NONCONVEX CONTROL PROBLEMS IN THE COEFFICIENTS 221
On he o he hand, since Ais a solu ion o (1.1) and Aε∈M(Ω), we ha e
J(yε)−J(y)
ε≥0∀ε>0,
wi h yε=(y1,ε,... ,y
k,ε) and y=(y1,... ,y
k). F om (3.10) and he F ´eche de i -
abili y o J,wege
k
i=1∂iJ(y),˙yi= lim
ε→0
J(yε)−J(y)
ε≥0.(3.11)
Bu aking ˙yias he es unc ion in (3.2) and pias he es unc ion in (3.7), we ha e
k
i=1∂iJ(y),˙yi=
k
i=1 Ω
A∇pi∇˙yidx =−
k
i=1 Ω
H∇yi∇pidx.
This p o es
Ω
H:Cdx=
k
i=1 Ω
H∇yi∇pidx ≤0∀H∈KA(M(Ω)).(3.12)
Now le Hbe in ¯
KA(M(Ω)). Fo δ>0 we define
Gδ=M∈L∞(Ω,Ms
N)/Ω
C:(M−H)dx
<δ
.
Since Gδis a neighbo hood o Hin he weak-∗ opology o L∞(Ω,Ms
N), he e exis s
Hδin Gδ∩KA(M(Ω)) and hen, om (3.12), we ge
Ω
C:Hdx=Ω
C:Hδdx +Ω
C:(H−Hδ)dx<δ
o e e y δ>0. This p o es (3.4).
Rema k 3.3. The abo e heo em is s ill ue i he elemen s o M(Ω) a e no
necessa ily symme ic by changing A o A in he defini ion (3.2) o he unc ions pi
and aking
C=
k
i=1 ∇pi⊗∇yi.
Rema k 3.4. I M(Ω) is con ex, he condi ion (3.4) implies
Ω
A:Cdx= max Ω
B:Cdx/B∈M(Ω).(3.13)
Rema k 3.5. Theo em 3.2 s ill holds i we ake KA(M(Ω)) as he cone o ma ices
H∈L∞(Ω,Ms
N(Ω)) such ha o e e y sequence Φ1
ε,... ,Φk
ε,which espec i ely
con e ges in L2(Ω)N o Φ1,... ,Φk, he e exis s Aε∈M(Ω) such ha
Aε−A
εΦi
ε→HΦiin L2(Ω)N,i=1,... ,k.
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222 J. CASADO-D´
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IN-G´
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The ad an age o his defini ion is he ollowing: I M(Ω) is he se we ob ain by
mixing ma e ials wi h p opo ions fixed, hen o e e y ξ1,... ,ξ
N−1∈RN, he se
{(Bξ1,... ,Bξ
N−1)/B ∈M(Ω)}⊂L∞(Ω)N−1
is con ex (see [24], [25]). So, wi h his defini ion o KA(M(Ω)), he ma ices o he
o m B−Abelong o KA(M(Ω)) i k≤N−1. Thus, (3.13) s ill holds in his case.
La e we will deduce his esul (see Co olla y 4.20) o mo e gene al choices o M(Ω),
using simply Defini ion 3.1 o admissible di ec ions.
4. Calculus o admissible di ec ions. In he ollowing, le us calcula e ex-
plici ely some admissible di ec ions by imposing addi ional hypo heses abou M(Ω).
De ini ion 4.1. We say ha M(Ω) is local i he e exis s a mul i alua ed appli-
ca ion F:x∈Ω→F(x)⊂M
s
Nsuch ha
M(Ω) = {B∈L∞(Ω,Ms
N)/B(x)∈F(x)a.e. x∈Ω},
whe e Fis measu able in he sense ha
{x∈Ω/F(x)∩G=∅} is measu able ∀G⊂M
s
Nopen.
As i is p o ed in [21], he local p ope y is sa isfied in se e al ypical examples
o M(Ω). A fi s consequence o assuming M(Ω) is local ollows.
P oposi ion 4.2. We assume M(Ω) is local. We conside A∈M(Ω),H1,... ,
Hm∈KA(M(Ω)),ω1,... ,ω
m⊂Ωmeasu able such ha |ωi∩ωj|=0i i=j. Then
he ma ix H=m
i=1 Hiχωibelongs o KA(M(Ω)).
P oo . By Defini ion 3.1, o e e y i∈{1,... ,m} he e exis s Ai
ε∈M(Ω) and
c>0 (which can be aken independen o i) such ha
Ai
ε−AL∞(Ω,Ms
N)≤cε, lim
ε→0
Ai
ε−A
ε=Hia.e. in Ω.
Taking hen
Aε=
m
i=1
Ai
εχωi+AχΩ ∪m
i=1ωi,
which belongs o M(Ω) because M(Ω) is local, we ha e
Aε−AL∞(Ω,Ms
N)≤cε, lim
ε→0
Aε−A
ε=Ha.e. in Ω,
and hen Hbelongs o KA(M(Ω)).
Rema k 4.3. I is no difficul o show ha he abo e esul emains ue i we
eplace KA(M(Ω)) by ¯
KA(M(Ω)).
Using P oposi ion 4.2, we ge he ollowing.
P oposi ion 4.4. In he assump ions o Theo em 3.2,i M(Ω) is local, we ha e
H:C≤0a.e. in Ω∀H∈¯
KA(M(Ω)).(4.1)
P oo . By P oposi ion 4.2, o e e y H∈KA(M(Ω)) and e e y ω⊂Ω measu able,
he ma ix Hχωbelongs o KA(M(Ω)). So, using (3.4), we ge
ω
H:Cdx≤0.(4.2)
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NONCONVEX CONTROL PROBLEMS IN THE COEFFICIENTS 223
Since ¯
KA(M(Ω)) is he closu e o KA(M(Ω)) in he weak-∗ opology o L∞(Ω,Ms
N),
we deduce ha (4.2) holds, in ac , o e e y H∈¯
KA(M(Ω)) and e e y ω⊂Ω
measu able, which implies (4.1).
Le us now see how assuming M(Ω) is local pe mi s us o ob ain admissible
di ec ions.
Theo em 4.5. We suppose ha M(Ω) is local and closed o he H-con e gence.
We conside a linea subspace W⊂RNo dimension and a measu able bounded
subse T⊂Wsuch ha |T|is posi i e. Then, o e e y A, B ∈M(Ω), he ma ix
H∈L∞(Ω,Ms
N)defined by
H(x)ei=(B(x)−A(x)) ei+1
|T|T∇W
zˆwi(x, z)d(z)
(4.3)
o 1≤i≤Nand a.e. x∈Ωbelongs o KA(M(Ω)).In(4.3), he unc ion ˆwiis
defined by
⎧
⎪
⎪
⎪
⎪
⎪
⎪
⎪
⎨
⎪
⎪
⎪
⎪
⎪
⎪
⎪
⎩
ˆwi(x, .)∈H1
loc(W),∇W
zˆwi(x, .)∈L2(W, W ),
W
(A(x)χW T+B(x)χT)∇W
zˆwi(x, .)∇W
zˆ d
(z)
=T
(A(x)−B(x))ei∇W
zˆ d
(z),
∀ˆ ∈H1
loc(W),∇W
zˆ ∈L2(W, W )a.e. x∈Ω.
(4.4)
P oo . We conside A,B,W, and Tas in he s a emen o he heo em. Fo an
o hono mal basis {e
1,... ,e
}o W, we deno e
Y=
i=1
λie
i/−1
2<λ
i<1
2,1≤i≤⊂W.
Fo ε>0 small enough, we deno e Tε=ε1
T⊂Y,˜
Tε=k∈Z(Tε+
i=1 kie
i), and
we define ˜
Aε:Ω×W→M
s
Nby
˜
Aε(x, y)=A(x)(1 −χ˜
Tε(y)) + B(x)χ˜
Tε(y).
Since M(Ω) is local and closed o he H-con e gence, he ma ix Aεob ained by ak-
ing, o εfixed, he H-limi when δ ends o ze o o he ma ices x→˜
Aε(x, 1
δPW(x))
belongs o M(Ω). Since he ma ices ˜
Aεa e a enso ial p oduc o unc ions which
only depend on xand unc ions which only depend on y, i is well known (see, e.g.,
[5], [2]) ha Aεis gi en by
Aε(x)ei=Y
˜
Aε(x, y)(∇W
ywi,ε +ei)d(y),(4.5)
whe e wi,ε is he unique solu ion o
⎧
⎪
⎪
⎨
⎪
⎪
⎩
wi,ε ∈L2(Ω,H1
(Y)/R),
Y
˜
Aε(x, y)(∇W
ywi,ε(x, y)+ei)∇W
y (y)d(y)=0
∀ ∈H1
(Y)/Ra.e. x∈Ω.
(4.6)
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224 J. CASADO-D´
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Le us s udy he asymp o ic beha io o Aε. Fi s , we ema k ha o e e y ∈
H1
(Y)/Rand a.e. x∈Ω, we ha e
Y
˜
Aε(x, y)ei∇W
y (y)d(y)=Y
A(x)ei∇W
y (y)d(y)
+Tε
(B(x)−A(x))ei∇W
y (y)d(y),
bu o a.e. x∈Ω, he fi s e m on he igh -hand side anishes. So, wi,ε sa isfies
⎧
⎪
⎪
⎪
⎪
⎨
⎪
⎪
⎪
⎪
⎩
Y
˜
Aε(x, y)∇W
ywi,ε(x, y)∇W
y (y)d(y)
=Tε
(A(x)−B(x))ei∇W
y (y)d(y)
∀ ∈H1
(Y)/Ra.e. x∈Ω.
(4.7)
Fo 1 ≤i≤N, we ake wi,ε as he es unc ion in (4.7). Then we ge
Y
˜
Aε(x, y)∇W
ywi,ε(x, y)∇W
ywi,ε(x, y)d(y)=Tε
(A(x)−B(x))ei∇W
ywi,ε(x, y)d(y)
o a.e. x∈Ω. Using hen (2.1) and he Cauchy–Schwa z inequali y, we deduce he e
exis s c>0 such ha
Y|∇W
ywi,ε(x, y)|2d(y)≤c|Tε|=cε(4.8)
o ε>0 small enough and a.e. x∈Ω.
We define ˆwi,ε :Ω×(ε−1
Y)→Rby
ˆwi,ε(x, z)=ε−1
wi,ε(x, ε1
z).
F om (4.8), we deduce ha ∇W
zˆwi,ε χε−1
Yis bounded in L∞(Ω,L
2(W, W )). So
he e exis s a subsequence o ε, which we s ill deno e by ε, which con e ges weak-∗in
L∞(Ω,L
2(W, W )). Since he cu l o he limi is ze o, i is he g adien o a unc ion
ˆwi∈L∞(Ω,H1
loc(W)). Once we p o e ha ˆwiis he solu ion o (4.4), we conclude
ha he whole o he sequence con e ges.
We conside ˆ ∈D(W) and ε>0 small enough, such ha ε1
supp(ˆ )⊂Y, hen
we define ε∈H1
(Y)by
ε(y)=ε1
ˆ (ε−1
y) a.e. y∈Y.
Taking εas he es unc ion in (4.7), using he change o a iables z=ε−1
y, and
in eg a ing wi h espec o xin a measu able se ω,wege
ωε−1
lY
(A(x)χW T(z)+B(x)χT(z))∇W
zˆwi,ε(x, z)∇W
zˆ (z)d(z)dx
=ωT
(A(x)−B(x))ei∇W
zˆ (z)d(z)dx.
Passing o he limi in his equali y and aking in o accoun he a bi a iness o ˆ
and ω, and he densi y o D(RN)/Rin he ac o space o unc ions wi h g adien in
L2(RN) o e R(see, e.g., [9]), we show ha ˆwiis he solu ion o (4.4) o 1 ≤i≤N.
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NONCONVEX CONTROL PROBLEMS IN THE COEFFICIENTS 231
Now, i m−m−= 0, hen clea ly k+≥m−m−. In ano he case, we conside E=
Span({φ−
j/1≤j≤k}∪{φ−
j,φ
+
j/1≤j≤k}⊥), which has dimension m−+N−m.I
φ∈E⊥, hen, as abo e, s a emen (i) gi es ˜
Cjφφ ≥0, 1 ≤j≤k, and hen ˜
Cφφ ≥0.
Mo eo e , ˜
Cφφ =0iff ˜
Cjφφ =0,1≤j≤k, which, by s a emen (i), implies ha
φis o hogonal o φ−
j,φ+
j,1≤j≤k; i.e., φis in Eand so φ= 0. Thus, aking
i=m−+N−min (4.19) and using he compac ness o he uni a y ball in RN,we
ge
λm−+N−m+1 ≥min
φ∈E⊥
|φ|=1
˜
Cφφ > 0,
and hus k+≥m−m−.
The o he inequali ies in (4.18) ollow analogously.
As a consequence we ge he ollowing.
Co olla y 4.20. In he assump ions o Theo em 3.2,i M(Ω) is local and closed
o he H-con e gence and k≤N−1, hen condi ion (4.14) holds.
P oo . We apply Theo em 4.19 o ξi=∇yi(x), ηi=∇pi(x), 1 ≤i≤k, a.e. x∈Ω.
In his case ˜
C=C(x). Since, clea ly, he numbe m+which appea s in his esul is
less han o equal o k≤N−1, we deduce ha he numbe o posi i e eigen alues o
Cis less han o equal o N−1, and hen he e exis s a leas a nonposi i e eigen alue
o Ca.e. in Ω. Co olla y 4.18 gi es hen (4.14).
5. In a iabili y by o a ions. In he applica ions, i is a na u al hypo hesis
o assume ha M(Ω) is in a iable by o a ions. We show in his sec ion ha his
assump ion implies ha he eigen ec o s o Aand Cag ee.
De ini ion 5.1. We say ha M(Ω) is in a iable by o a ions i o e e y B∈
M(Ω) and e e y Q∈L∞(Ω,MN), wi h Q∈O
Na.e. in Ω, he ma ix QBQ belongs
o M(Ω).
We ha e he ollowing esul .
P oposi ion 5.2. In he assump ions o Theo em 3.2,i M(Ω) is in a iable by
o a ions, hen Aand Ca e mu ually diagonalizable a.e. in Ω.
P oo . Le us fi s p o e ha gi en a skew-symme ic ma ix Rand a measu able
se ω⊂Ω, he unc ion (RA +AR )χωbelongs o KA(M(Ω)). To his pu pose we
define G:MN→M
N×Rby G(M)=(MM ,de (M)). Since Ke (G(I)) coincides
wi h he space o skew-symme ic ma ices, i is known (see, e.g., [1]) ha o ε∈R
wi h |ε|small enough, he e exis s Pε∈M
Nsuch ha G(Pε)=G(I) o , equi alen ly,
Pε∈O
N, and (Pε−I)/ε con e ges o R. Defining hen
Aε=PεAP
εχω+AχΩ ω
and using ha M(Ω) is in a iable by o a ions, we deduce ha Aεbelongs o M(Ω)
and (Aε−A)/ε con e ges o (RA +AR )χωin L∞(Ω,Ms
N). Thus (RA +AR )χω
belongs o KA(M(Ω)).
Using now ha he se o skew-symme ic ma ices is a ec o ial space, condi ion
(3.4), and he a bi a iness o ω, we deduce
2(RA):C=(RA +AR ):C= 0 a.e. in Ω.
Fo i, j ∈{1,... ,N},i=j, we ake in he abo e equa ion Ras he ma ix
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232 J. CASADO-D´
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defined by
Rlk =⎧
⎪
⎨
⎪
⎩
1i l=i, k =j,
−1i l=j, k =i,
0 in ano he case.
Then we ge
(AC)ij −(CA)ij = 0 a.e. in Ω,
i.e., Aand Ccommu e, and hen hey a e mu ually diagonalizable.
Rema k 5.3. F om P oposi ion 5.2, assuming ha he ma ix Cis known and ha
hei eigen alues a e all diffe en , we mus look o he op imal solu ion Aon he se o
ma ices o M(Ω) which ha e he same eigen ec o s as Ca.e. So i can be in e es ing
o w i e condi ion (4.13) assuming ha Bis also mu ually diagonalizable wi h C.I
we es ic ou sel es o he spaces Wwhich a e gene a ed by eigen ec o s o C,we
ge he ollowing esul : In he condi ions o P oposi ion 5.2, i ci,ai,i∈{1,... ,N},
a e, espec i ely, he eigen alues o Cand A, hen o e e y B∈M(Ω) mu ually
diagonalizable wi h Aand C, wi h eigen alues b1,... ,b
N,weha e
N
i=1
ci(ai−bi) + min
1≤≤Nmin
1≤i1<···<i≤N
j=1
cij(aij−bij)2
bij+(−1)aij≥0.(5.1)
We also no e ha by Rema k 4.16, o A,B,Cas abo e, he condi ion (5.1) implies
in pa icula (4.15).
Assuming s onge hypo heses, we can imp o e P oposi ion 5.2. P oposi ion 5.4
below is ela ed o a heo em due o Lewis [11], which applies o he op imiza ion o
a unc ion h:Ms
N→Rcon ex and in a iable by o a ions (see also [12], whe e he e
is a e iew o esul s co esponding o op imiza ion p oblems on symme ic ma ices).
P oposi ion 5.4. In he assump ions o Theo em 3.2, we assume M(Ω) in a i-
able by o a ions and a leas one o he ollowing hypo heses:
(i) M(Ω) is con ex.
(ii) M(Ω) is H-closed and N≥3.
(iii) M(Ω) is H-closed, N=2and k=1.
Then he e exis s Q∈L∞(Ω,MN), wi h Q∈O
Na.e. in Ω, such ha
QAQ = diag(a1,... ,a
N),
(5.2) QCQ = diag(c1,... ,c
N),
and a1≤···≤aN,c1≤···≤cN.
P oo . F om P oposi ion 5.2 he e exis s Q∈L∞(Ω,MN), wi h Q∈O
Na.e. in
Ω, such ha (5.2) holds. Clea ly, we can also assume c1≤···≤cNa.e. in Ω. We
conside i, j ∈{1,... ,N},i=j, and we ake L∈O
N, defined by
Lei=ej,Le
j=−ei,Le
l=el∀l=i, j.
Since M(Ω) is in a iable by o a ions, he ma ix B=(LQ) diag(a1,... ,a
N)LQ
belongs o M(Ω). Le us now see ha i one o he hypo heses (i), (ii) o (iii) hold,
hen
C:(A−B)≥0 a.e. in Ω.(5.3)
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NONCONVEX CONTROL PROBLEMS IN THE COEFFICIENTS 233
Fo his pu pose, we define ˜
M(Ω) as he con ex hull o
{SAS /S∈L∞(Ω,MN),S∈O
Na.e. in Ω},
i (i) holds and as he H-closu e o his se in cases (ii) and (iii). Then ˜
M(Ω) is
con ained in M(Ω) and Abelongs o ˜
M(Ω), so Ais also a solu ion o (1.1) wi h M(Ω)
eplaced by ˜
M(Ω).
In case (i), ˜
M(Ω) is con ex and local, so om (4.1) and B−Ain KA(M(Ω)), we
deduce (5.3).
In cases (ii) and (iii), ˜
M(Ω) is local and H-closed. Mo eo e , i (ii) holds, hen
Ke (B−A)= 0 a.e. in Ω, while i we ha e (iii) hen, om Theo em 4.19, Chas a
leas a nonposi i e eigen alue. So, in bo h si ua ions, we deduce (5.3) om (4.17).
F om (5.3) we ge
0≤C:(A−B)=ci(ai−aj)+cj(aj−ai)=(ci−cj)(ai−aj) a.e. in Ω.
This finishes he p oo o P oposi ion 5.4.
Rema k 5.5. As we ha e seen in he p oo o P oposi ion 5.4, he o de ela ion
be ween he eigen alues o Cand Ais a consequence o (5.3) wi h Bdefined as abo e.
So i N= 2 and M(Ω) is H-closed, by Co olla y 4.18, he hesis o P oposi ion 5.4
s ill holds on he se whe e Chas a leas a nonnega i e eigen alue. Whe e he wo
eigen alues a e posi i e, assuming c1<c
2, he condi ion (4.15) implies
a1<a
2o a1>a
2and c2a2≤c1a1.(5.4)
Rela ed o his inequali y, we also ema k ha i in he condi ions o P oposi ion
5.4 (ii) he e a e wo eigen alues o C,ci,cjsuch ha ci≤cj≤0, hen besides
ai≤aj,weha e|cj|aj≤|ci|ai.
6. Applica ions. In his sec ion le us show how he condi ion (3.4) and he
consequences we ha e ob ained om i can be used, in some cases, o ob ain A∇yi,
A∇pi,1≤i≤k, as explici unc ions o ∇yi,∇piand hen, om (1.2) and (3.2), o
educe he op imali y condi ions gi en in Theo em 3.2 o a nonlinea sys em in ∇yi,
∇pi. The main difficul y in ca ying ou his idea is ha ob aining he H-closu e o a
subse o L∞(Ω,MN) is a e y difficul p oblem, which has only been sol ed in some
pa icula cases (see [23], [14], [13], [8], [16], [25]). To simpli y he exposi ion, we ha e
chosen wo simple p oblems whe e he H-closu e is well known. The fi s consis s o
he mix u e o wo homogeneous iso opic ma e ials in dimension wo ( he p oblem
can also be s udied analogously o highe dimensions). This p oblem has also been
s udied in [3] and [7]. In his case he se M(Ω) is con ex. In he second p oblem we
conside a noncon ex si ua ion co esponding o a polyc ys al in dimension wo.
Fi s p oblem. We s a by ecalling he ollowing esul which has been p o ed
in [23] and [14].
Theo em 6.1. We assume N=2.Fo 0<α≤βand θ∈L∞(Ω) wi h 0≤θ≤1
a.e. in Ω, he se Mθ(Ω) o he H-limi s o he sequences αI χωn+β(1−χωn)I, such
ha ωn⊂Ωa e measu able se s and sa is y χωncon e ges weakly-∗in L∞(Ω) o θ,
is cha ac e ized as ollows:
Mθ⊂L∞(Ω,Ms
2)is he se o ma ices such ha hei eigen alues λ1,λ2sa is y
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234 J. CASADO-D´
IAZ, J. COUCE-CALVO, AND J. D. MART´
IN-G´
OMEZ
he ollowing inequali ies a.e. in Ω:
⎧
⎪
⎪
⎪
⎪
⎪
⎪
⎪
⎨
⎪
⎪
⎪
⎪
⎪
⎪
⎪
⎩
λ−≤λ1,λ
2≤λ+,
2
i=1
1
λi−α≤1
λ−−α+1
λ+−α,
2
i=1
1
β−λi≤1
β−λ−+1
β−λ+,
(6.1)
whe e λ−,λ+a e gi en by
λ+=αθ +β(1 −θ),λ
−=θ
α+1−θ
β−1
.(6.2)
Le us see how he esul s ob ained in he p e ious sec ions pe mi us o ob ain
A om C, and hen om ∇yi,∇pi,1≤i≤k, o some choices o M(Ω) ela ed o
Mθ(Ω).
In he ollowing, we define
ˇ
Ω={x∈Ω/(c1(x),c
2(x)) =(0,0)},(6.3)
whe e c1,c2a e he eigen alues o he ma ix C.
P oposi ion 6.2. In he assump ions o Theo em 3.2,i M(Ω) is he se o
ma ices defined in Theo em 6.1 o a fixed unc ion θand c1,c2,c1≤c2, a e he
eigen alues o C, hen he e exis s an associa ed basis {µ1,µ
2}o eigen ec o s o C
such ha a.e. in Ω, we ha e
Aµi=aiµi,i=1,2,(6.4)
whe e a.e. in ˇ
Ω, he unc ions a1,a2a e gi en by he ollowing:
I c2<0and c2
c1≥α
α+(β−α)θ⇒⎧
⎪
⎪
⎪
⎨
⎪
⎪
⎪
⎩
a1=α+α(β−α)(1 −θ)
2α+(β−α)θ1+c2
c1,
a2=α+α(β−α)(1 −θ)
2α+(β−α)θ1+c1
c2.
I c1>0and c2
c1≤β
α+(β−α)θ⇒⎧
⎪
⎪
⎪
⎨
⎪
⎪
⎪
⎩
a1=β−β(β−α)θ
α+β+(β−α)θ1+c2
c1,
a2=β−β(β−α)θ
α+β+(β−α)θ1+c1
c2.
In ano he case a1=λ−,a2=λ+, whe e λ−,λ+a e defined by (6.2).
P oo . In his case, he se M(Ω) is local, con ex, and in a iable by o a ions.
So we can apply P oposi ion 5.4 and (4.14), which imply ha a.e. in Ω, Asa isfies
(6.4) o a basis o eigen ec o s o C, and a1c1+a2c2is he maximum o λ1c1+λ2c2,
wi h λ1,λ2in he se defined by (6.1). Sol ing his maximum p oblem we ge he
exp essions a1and a2gi en in P oposi ion 6.2.
The abo e esul assumes ha θis known, bu clea ly his is no a ealis ic
si ua ion. Nex , we conside wo examples whe e θalso a ies. In he fi s one we
impose he condi ion
1
|Ω|Ω
θdx=s,(6.5)
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NONCONVEX CONTROL PROBLEMS IN THE COEFFICIENTS 235
wi h s∈(0,1). This means we know he p opo ion o he ma e ials defined by αand
βbu no i s local dis ibu ion. This usually holds when one ma e ial is be e han
he o he bu i is also mo e expensi e. In he second si ua ion we conside he case
whe e we do no ha e any es ic ion on θ.
P oposi ion 6.3. In he assump ions o Theo em 3.2, i o s∈(0,1) gi en,
M(Ω) is he se o ma ices defined in Theo em 6.1, wi h θ∈L∞(Ω),0≤θ≤1a.e.
in Ωand such ha (6.5) holds, hen he ma ix Asa isfies he hesis o P oposi ion
6.2, whe e he co esponding unc ion θis such ha defining F∈L∞(ˇ
Ω) by
F(x)=
⎧
⎪
⎪
⎪
⎪
⎪
⎪
⎪
⎨
⎪
⎪
⎪
⎪
⎪
⎪
⎪
⎩
α(β2−α2)(√−c1−√−c2)2
(2α+(β−α)θ)2i c2<0and c2
c1≥α
α+(β−α)θ,
−β(β2−α2)(√c1+√c2)2
(α+β+(β−α)θ)2i c1>0and c2
c1≤β
α+(β−α)θ,
−(β−α)αβ
(α+(β−α)θ)2c1+c2in ano he case,
he e exis s ∈Rwhich sa isfies
⎧
⎨
⎩
F(x)≤ a.e. in {θ=0}∩ˇ
Ω,
F(x)= a.e. in {0<θ<1}∩ˇ
Ω,
F(x)≥ a.e. in {θ=1}∩ˇ
Ω.
(6.6)
P oo . We ema k ha i θis he co esponding unc ion associa ed wi h Ain
he defini ion o he elemen s o M(Ω) and we define Mθ(Ω) as in he s a emen o
Theo em 6.1, hen Ais also he solu ion o (1.1) wi h M(Ω) eplaced by Mθ(Ω). So
P oposi ion 6.2 applies.
Le us now a y θ. Fo e e y θ∗∈L∞(Ω) such ha 0 ≤θ∗≤1 a.e. in Ω,
1
|Ω|Ω
θ∗dx =s,
and θ∗=θa.e. in Ω ˇ
Ω, we define Aθ∗∈M(Ω) as he unc ion gi en by P oposi ion
6.2 applied o θ∗a.e. in ˇ
Ω and Aθ∗=Aa.e. in Ω ˇ
Ω. De i ing Aθ∗wi h espec o
θ∗, we ob ain an admissible di ec ion. Then, using condi ion (3.4), we ge
Ω
Fϑdx≤0(6.7)
o e e y ϑ∈L∞(Ω) such ha ϑ= 0 a.e. in Ω ˇ
Ω, ϑ≥0 a.e. in {θ=0}∩ˇ
Ω, ϑ≤0
a.e. in {θ=1}∩ˇ
Ω, and
Ω
ϑdx=0.
I is easy o check ha his implies he exis ence o ∈R, which sa isfies he s a emen
o he p oposi ion.
Rema k 6.4. The exp ession o Fis s ic ly dec easing wi h espec o θ. Then,
om (6.6), i is possible o ob ain θas a unc ion o c1,c2and .
Rema k 6.5. In P oposi ion 6.3, i ≥0, hen θ= 0 a.e. in he se
{c1>0}c2
c1≤β
α∩ˇ
Ω.
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236 J. CASADO-D´
IAZ, J. COUCE-CALVO, AND J. D. MART´
IN-G´
OMEZ
Analogously, i ≤0, hen θ= 1 a.e. in he se
{c2<0}c2
c1≥α
β∩ˇ
Ω.
We finish wi h he ollowing esul .
P oposi ion 6.6. In he assump ions o Theo em 3.2, le M(Ω) be he se
o ma ices defined in Theo em 6.1, whe e θis any unc ion in L∞(Ω) such ha
0≤θ≤1a.e. in Ω, and deno e by c1,c2,c1≤c2, he eigen alues o C. Then he e
exis s an associa ed basis {µ1,µ
2}o eigen ec o s o Csuch ha a.e. in Ωwe ha e
(6.4). Mo eo e , a.e. in ˇ
Ω, he unc ions a1,a2a e gi en by he ollowing:
I 0≤c1≤c2, hen a1=a2=β.
I c1≤c2≤0, hen a1=a2=α.
I c1<0<c
2, hen
⎧
⎪
⎪
⎪
⎪
⎪
⎪
⎨
⎪
⎪
⎪
⎪
⎪
⎪
⎩
α
β≥−c1
c2⇒a1=a2=β,
β
α>−c1
c2
>α
β⇒a1=−αβc2
c1
,a
2=α+β−−αβc1
c2
,
−c1
c2≥β
α⇒a1=a2=α.
P oo . We p oceed simila ly o P oposi ion 6.3, bu now, in he condi ion (6.7),
he unc ion ϑdoes no necessa ily sa is y
Ω
ϑdx=0.
This implies ha he unc ion Fgi en in P oposi ion 6.3 sa isfies (6.6) wi h =0,
which easily gi es he esul .
Second p oblem. Gi en a diagonal ma ix Λ = diag(α, β) wi h 0 <α<β, le
us now conside he op imiza ion p oblem (1.1) when M(Ω) is he H-closu e o he
ma ices o he o m R(x)ΛR(x) , whe e Ris measu able, and R(x) belongs o O2 o
a.e. x∈Ω (obse e ha o assume Λ diagonal is no a es ic ion). This se M(Ω)
is known (see, e.g., [25], [16]) and ag ees wi h he se o unc ions B∈L∞(Ω,Ms
2)
such ha o a.e. x∈Ω, he eigen alues b1(x) and b2(x)o B(x) sa is y α≤b1(x),
b2(x)≤β,b1(x)b2(x)=αβ. Fo his choice o M(Ω), we ha e he ollowing esul .
P oposi ion 6.7. In he assump ions o Theo em 3.2,i c1and c2, wi h c1≤c2,
a e he eigen alues o C, hen he e exis s an associa ed basis {µ1,µ
2}o eigen ec o s
o Csuch ha a.e. in Ω, we ha e
Aµi=aiµi,i=1,2,(6.8)
whe e a.e. in he se ˇ
Ωdefined by (6.3), he unc ions a1,a2a e gi en by
c2<0and c2
c1
>α
β⇒⎧
⎪
⎪
⎨
⎪
⎪
⎩
a1=αβc2
c1
,
a2=αβc1
c2
.
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NONCONVEX CONTROL PROBLEMS IN THE COEFFICIENTS 237
I c1>0and c2
c1≤β
α, hen he e exis h ee possibili es:
a1=α,
a2=β, o a1=β,
a2=α, o ⎧
⎪
⎪
⎨
⎪
⎪
⎩
a1=√αβc2
c1
,
a2=√αβc1
c2
.
In ano he case a1=α,a2=β.
P oo . Since he se M(Ω) is in a iable by o a ions, we can apply P oposi ion
5.2 o deduce ha o a.e. x∈Ω, he e exis s a basis {µ1(x),µ
2(x)}o R2such ha
C(x)µi(x)=ci(x)µi(x),A(x)µi(x)=ai(x)µi(x),i=1,2,
wi h c1(x)≤c2(x), a1(x),a
2(x)∈R. F om he defini ion o M(Ω), we also ha e ha
o a.e. x∈Ω, he e exis s ∗(x)∈[1,β
α] such ha
a1(x)=α ∗(x),a
2(x)= β
∗(x).
Mo eo e , om (5.1), we deduce ha ∗sa isfies
( ∗(x)− )αc1(x)−βc2(x)
∗(x)
(6.9)
+( ∗(x)− )2min αc1(x)
,βc2(x)
( ∗(x))2 ,1
∗(x)+ αc1(x)+βc2(x)
∗(x) ≥0
o e e y ∈[1,β
α] and a.e. x∈Ω. In he se whe e ∗(x)=1,weha e ∗(x)− <0
o e e y ∈(1,β
α]. So, di iding by 1 − and aking con e ging o 1 on he igh ,
we deduce
αc1−βc2≤0 a.e. in {x∈Ω: ∗(x)=1}.(6.10)
Analogously, we deduce
βc1−αc2≥0 a.e. in x∈Ω: ∗(x)=β
α,(6.11)
αc1−βc2
( ∗(x))2= 0 a.e. in x∈Ω: 1<
∗(x)<β
α,(6.12)
whe e he s a emen (6.12) implies
c1c2>0,
∗=βc2
αc1
a.e. in x∈ˇ
Ω: 1<
∗(x)<β
α.(6.13)
Analyzing he diffe en cases which appea depending on he sign o c1o c2, we easily
conclude om (6.10), (6.11), and (6.13) he p oo o P oposi ion 6.7.
Rema k 6.8. We ha e deduced (6.10), (6.11), and (6.13) om inequali y (6.9).
One could conjec u e ha his inequali y gi es, in ac , mo e in o ma ion. Howe e , a
simple calculus shows ha he s a emen s (6.10), (6.11), and (6.13) also imply (6.9).
Rema k 6.9. P oposi ion 6.7 does no gi e he exp essions o a1and a2in he se
whe e c1>0 and c2
c1≤β
α; i gi es h ee possibili ies. The possibili y a1=α,a2=β
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238 J. CASADO-D´
IAZ, J. COUCE-CALVO, AND J. D. MART´
IN-G´
OMEZ
seems o be he mos na u al in o de o s ick con inuously wi h he alues o a1and
a2in he o he zones. We also no e ha i M(Ω) was con ex hen, using ha B−A
is an admissible di ec ion o e e y B∈M(Ω), we should ob ain in place o (6.9) ha
α ∗+β
∗= max α +β
: ∈1,β
α,
which implies ha ∗= 1 (and hen a1=α,a2=β) a.e. on he se whe e c1>0 and
c2
c1≤β
αas well as he exp essions o a1and a2gi en in P oposi ion 6.7 in he o he
cases. Howe e , since M(Ω) is no con ex, his easoning is no good and hus he
only conclusion we ob ain is ha s a ed in P oposi ion 6.7.
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