scieee Science in your language
[en] (orig)

Numerical approximation of a one-dimensional elliptic optimal design problem

Abstract

We address the numerical approximation by finite-element methods of an optimal design problem for a two phase material in one space dimension. This problem, in the continuous setting, due to high frequency oscillations, often does not have a classical solution, and a relaxed formulation is needed to ensure existence. On the contrary, the discrete versions obtained by numerical approximation have a solution. In this article we prove the convergence of the discretizations and obtain convergence rates. We also show a faster convergence when the relaxed version of the continuous problem is taken into account when building the discretization strategy. In particular it is worth emphasizing that, even when the original problem has a classical solution so that relaxation is not necessary, numerical algorithms converge faster when implemented on the relaxed version.

Read accessible full text

Numerical approximation of a one-dimensional elliptic optimal design problem

Author: Casado Díaz, Juan; Castro Barbero, Carlos Manuel; Luna Laynez, Manuel; Zuazua Iriondo, Enrique
Publisher: Society for Industrial and Applied Mathematics
Year: 2011
DOI: 10.1137/10081928X
Source: https://idus.us.es/bitstreams/44f99ed8-5bb7-4d14-bc09-5f5dfcf83afb/download
NUMERICAL APPROXIMATION OF A ONE-DIMENSIONAL
ELLIPTIC OPTIMAL DESIGN PROBLEM*
J. CASADO-DÍAZ†, C. CASTRO‡, M. LUNA-LAYNEZ†,AND E. ZUAZUA§
Abs ac . We add ess he nume ical app oxima ion by ini e-elemen me hods o an op imal design
p oblem o a wo phase ma e ial in one space dimension. This p oblem, in he con inuous se ing, due o high
equency oscilla ions, o en does no ha e a classical solu ion, and a elaxed o mula ion is needed o ensu e
exis ence. On he con a y, he disc e e e sions ob ained by nume ical app oxima ion ha e a solu ion. In his
a icle we p o e he con e gence o he disc e iza ions and ob ain con e gence a es. We also show a as e
con e gence when he elaxed e sion o he con inuous p oblem is aken in o accoun when building he dis-
c e iza ion s a egy. In pa icula i is wo h emphasizing ha , e en when he o iginal p oblem has a classical
solu ion so ha elaxa ion is no necessa y, nume ical algo i hms con e ge as e when implemen ed on he
elaxed e sion.
Key wo ds. con ol in he coe icien s, composi e op imal design, elaxa ion, nume ical app oxima ion,
ini e elemen s
AMS subjec classi ica ions. 49M25, 49J20
DOI. 10.1137/10081928X
1. In oduc ion. This pape is de o ed o he ini e-elemen nume ical analysis o
a p oblem o op imal mix u e o wo ( he mal o elec ical) ma e ials in o de o mini-
mize a gi en unc ional in one space dimension.
Le Ωbe a bounded open se o RN,N≥1(al hough ou analysis is limi ed o he
case N¼1, he p oblem makes sense in any space dimension), and conside he ollow-
ing op imiza ion p oblem:
Find ω0∈Usuch ha
Jðω0Þ¼min
ω∈U
JðωÞ:
ð1:1Þ
He e ω, he con ol, is a measu able subse o Ω,JðωÞ, he cos unc ional, is o he o m
JðωÞ¼Zω
F1ðx; u; ∇uÞdxþZΩ ω
F2ðx; u; ∇uÞdx;ð1:2Þ
whe e F1;F2∶Ω×R×RN→Ra e gi en unc ions, and u, he s a e, is he solu ion o
*Recei ed by he edi o s Decembe 23, 2010; accep ed o publica ion (in e ised o m) May 26, 2011;
published elec onically Sep embe 15, 2011.
h p://www.siam.o g/jou nals/mms/9-3/81928.h ml
†Dp o. de Ecuaciones Di e enciales y Análisis Numé ico, Facul ad de Ma emá icas, Uni e sidad de Se illa,
C. Ta ía s/n, 41012 Se illa, Spain ([email p o ec ed], [email p o ec ed]). The wo k o he i s and hi d au ho s
was pa ially suppo ed by p ojec MTM2008-00306 o he MICINN (Spain) and he esea ch g oup
FQM-309 o he CICE (Andalusia).
‡Dp o. de Ma emá icas e In o má ica, ETSI caminos, canales y pue os, Uni e sidad Poli écnica de Mad id,
Ciudad Uni e si a ia, 28040 Mad id, Spain ([email p o ec ed]). The wo k o he second au ho was
pa ially suppo ed by g an MTM2008-03541 o he MICINN (Spain).
§Basque Cen e o Applied Ma hema ics, Bizkaia Technology Pa k, Building 500. E-48160 De io, Basque
Coun y, Spain ([email p o ec ed]); IKERBASQUE, Basque Founda ion o Science, E-48011 Bilbao,
Basque Coun y, Spain. The wo k o he las au ho was pa ially suppo ed by ERC ad anced
g an FP7-246775 NUMERIWAVES, g an PI2010-04 o he Basque Go e nmen , ESF Resea ch
Ne wo king P og amme OPTPDE, and g an MTM2008-03541 o he MICINN (Spain).
1181
MULTISCALE MODEL.SIMUL.
Vol. 9, No. 3, pp. 1181–1216
© 2011 Socie y o Indus ial and Applied Ma hema ics
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
−di ððαχωþβð1−χωÞÞ∇uÞ¼ in Ω;
u¼0on∂Ω
ð1:3Þ
o some gi en sou ce e m ∶Ω→R. The posi i e cons an s α,β ep esen he wo
ma e ials, de e mining he coe icien s o he co esponding di usion ma ices. Some
es ic ions can and mus be imposed o he con ol ωdepending on he p oblem.
Fo example, an in e es ing case is when he ma e ial αis mo e e icien han he
ma e ial βbu i is also mo e expensi e. Then, i is usual o conside a es ic ion o
he o m jωj≤κ, limi ing he use o he ma e ial α. We include his es ic ion in
he admissible se o con ols U,
U¼ ω⊂Ω∶ωmeasu able;jωj≤κg:ð1:4Þ
The exis ence o an op imal se ω ul illing hese cons ain s, o which he unc ion
usolu ion o (1.3) minimizes J, does no hold in gene al (see [15], [16]). In hese cases, i
is na u al o look o minimizing sequences, i.e., sequences ωlg∞
l¼1⊂Usuch ha
lim
l→∞
JðωlÞ¼in
ω∈U
JðωÞ
since hey p o ide nea op imal designs. A usual p ocedu e o ind such sequences is o
in oduce a elaxed e sion o he p oblem o which a minimize exis s. Then, a sui able
app oxima ion o he minimize s p o ides minimizing sequences o he o iginal
p oblem.
Fo a sequen ially con inuous unc ional J, in he weak opology o he Sobole
space H1ðΩÞ(see [1], [13], [20]), his elaxa ion can be ob ained by eplacing in
(1.3) he unc ion χωwi h a measu able unc ion θ aking i s alues in he closed in e al
½0;1and he unc ion ðαχωþβð1−χωÞÞ wi h a ma ix unc ion Ain he se KðθÞo
ma ices cons uc ed by homogeniza ion (see, e.g., [17], [19], [21]) mixing he ma e ials α
and βwi h espec i e p opo ions θand 1−θ. Rema k ha he se KðθÞis known in he
case desc ibed abo e, co esponding o he mix u e o wo iso opic ma e ials (see [14],
[22]), bu no in o he in e es ing cases such as he mix u e o mo e han wo ma e ials,
aniso opic ma e ials, e c. Hence o h we deno e by ^
U he se o elaxed con ols ðθ;AÞ.
No e ha unc ionals o he o m (1.2) a e no sequen ially con inuous in he weak
opology o H1ðΩÞ, in gene al. In hose cases, o ob ain he elaxed e sion (see [6]) we
mus eplace he se o con ols χωand coe icien s ðαχωþβð1−χωÞÞ wi h he pai s
ðθ;AÞ∈^
Uas abo e, and he unc ional Jwi h ano he one o he o m
^
Jðθ;AÞ¼ZΩ
Hðx; u; ∇u; A∇u; θÞdx;ð1:5Þ
whe e uis solu ion o he homogenized p oblem
8
<
:
−di A∇u¼ in Ω;
u¼0on∂Ω:
ð1:6Þ
An explici exp ession o he unc ion His only known in some pa icula cases
(see he e e ences [2], [6], [7], [8], [11], [12], [18], [23]). I sa is ies
Hðx; u; ∇u; A∇u; θÞ¼F1ðx; u; ∇uÞχωþF2ðx; u; ∇uÞχΩ ω;i θ¼χω;
1182 CASADO-DÍAZ, CASTRO, LUNA-LAYNEZ, ZUAZUA
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
and A¼ðαχωþβð1−χωÞÞIand, so, he elaxed unc ional is in ac an ex ension o he
o iginal one o he la ge se o elaxed con ols. The elaxed con ol p oblem eads
Find ðθ0;A
0Þ∈^
Usuch ha
^
Jðθ0;A
0Þ¼ min
ðθ;AÞ∈^
U
^
Jðθ;AÞ:
ð1:7Þ
In p ac ical applica ions, in o de o sol e nume ically he abo e con ol p oblem
(1.1), i is necessa y o in oduce a disc e iza ion o bo h he con ol se and he unc-
ional. In he p esen con ex , we ha e a leas wo app oaches o his nume ical ap-
p oxima ion issue. One based on he disc e iza ion o he o iginal p oblem and one
elying on he disc e iza ion o he elaxed e sion. Recen ly, in [8] and [9], bo h disc e-
iza ion p ocedu es ha e been shown o con e ge. In hese a icles, some pa ially
elaxed e sions ha e also been s udied in which he class o con ols unde conside a ion
is enla ged bu no o he ex en o exhaus ing he class o he elaxed e sion o he
p oblem; we e e o [12] o a ela ed esul . We also e e o [26] o he nume ical s udy
o he elaxed o mula ion o a pa icula case o p oblem (1.1).
In his pape we compa e and ge con e gence a es o he sequences o disc e e
minimize s ob ained wi h bo h app oxima ion me hods. These issues a e add essed
in he simples one-dimensional se ing, whe e he pa ial di e en ial equa ion (1.3)
is educed o an o dina y di e en ial equa ion, he se KðθÞis well known o be educed
o he ha monic mean o αand βwi h espec i e p opo ions θand 1−θ, and he unc-
ion His explici ly known. No e ha in his case we can w i e ^
Jðθ;AÞ¼ ^
JðθÞin (1.5),
since Ais comple ely de e mined by θ, and ^
Uis jus he se o measu able unc ions
θ∶Ω→½0;1wi h in eg al less o equal han κ.
To make ou esul s p ecise, we i s conside he disc e iza ion o he se o con ols
bu no o he s a e equa ion (1.3). In he con ex o ini e-elemen app oxima ion me h-
ods, we can conside a decomposi ion o Ωin elemen s wi h maximum size and subse s
ωcons i u ed by unions o a subse o such elemen s. I we deno e by U he se o such
subse s, he disc e e p oblem eads
Find ω
0∈U such ha
Jðω
0Þ¼min
ω∈U JðωÞ:
ð1:8Þ
The disc e e space o con ols ob ained in his way U is compac in he s ong opology
o L1ðΩÞ, and he co esponding s a e unc ions a e compac in H1ðΩÞ. The e o e, he
disc e ized p oblem has a solu ion wi hou he need o a elaxed e sion.
In his way we ob ain a sequence o disc e e minimize s ω
0g ha a e likely o
cons i u e a minimizing sequence o Jin U,as →0. We show ha his is he case,
and we gi e con e gence a es o
Jðω
0Þ−in
ω∈U
JðωÞas →0:ð1:9Þ
On he o he hand, ins ead o disc e izing he o iginal con ol p oblem, we can dis-
c e ize he elaxed e sion. A e in oducing a decomposi ion o Ωin elemen s, wi h
maximal size , we can conside he se ^
U o unc ions θ∈^
Uwhich a e cons an on
each elemen . The disc e e elaxed p oblem eads
Find ^
θ
0∈^
U such ha
^
Jð^
θ
0Þ¼min
θ∈^
U
^
JðθÞ.
ð1:10Þ
APPROXIMATION OF AN OPTIMAL DESIGN PROBLEM 1183
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
As abo e, we show ha
^
Jð^
θ
0Þ−in
ω∈^
U∇
JðuÞ→0as →0;ð1:11Þ
and we gi e con e gence a es.
Once a disc e e elaxed minimize is known ^
θ
0we can cons uc a sequence
ωk; g∞
k¼1⊂Usuch ha
lim
k→∞
Jðωk; Þ¼ ^
Jð^
θ
0Þ:
This p o ides a minimizing sequence o he o iginal p oblem. As we show, he sequence
ωk; g∞
k¼1can be cons uc ed explici ly om ^
θ
0wi h almos no compu a ional cos .
Ou esul s show ha i is be e o disc e ize he elaxed p oblem, in he sense ha
we ge a as e con e gence a e, as →0, o (1.11) han he one ob ained o (1.9).
This is ue e en in he case whe e he o iginal p oblem has a solu ion, and so he e-
laxa ion is unnecessa y om a heo e ical poin o iew. Despi e his, he elaxed e sion
o he o iginal minimiza ion p oblem can always be o mula ed, and ou esul s show
ha i is indeed be e o app oxima e he op imal design p oblem nume ically in hese
cases as well.
F om a compu a ional poin o iew, besides disc e izing he se o con ols, we mus
also disc e ize he s a e equa ion (1.3) o (1.6). This equi es a second decomposi ion o
Ωcons i u ed by elemen s o maximum size h. A na u al assump ion is o conside his
new decomposi ion as a e inemen o he one used o he con ol se , o ice e sa.
In he con ex o he o iginal un elaxed con ol p oblem, deno ing by uh he
P1- ini e-elemen app oxima ion o he solu ion o (1.3), and de ining Jhas
JhðωÞ¼Zω
F1ðx; uh;∇uhÞdxþZΩ ω
F2ðx; uh;∇uhÞdx;
he ull disc e e con ol p oblem eads
Find ω ;h
0∈U such ha
Jhðω ;h
0Þ¼min
ω∈U JhðωÞ:
ð1:12Þ
Analogously, we can de ine a ull disc e iza ion o he elaxed p oblem by
conside ing
^
JhðθÞ¼ZΩ
Hðx; uh;∇uh;A∇uh;θÞdx;ð1:13Þ
whe e uhis he P1- ini e-elemen app oxima ion o (1.6). The ully disc e e elaxed
p oblem in his case is
Find ^
θ ;h
0∈^
U such ha
^
Jhð^
θ ;h
0Þ¼min
θ∈^
U
^
JhðθÞ:
ð1:14Þ
We ocus on he con e gence a es o he sequences ω ;h
0g ;h and ^
θ ;h
0g ;h ob ained
wi h he wo app oaches abo e, espec i ely. Mo e p ecisely, we compa e he sequences
1184 CASADO-DÍAZ, CASTRO, LUNA-LAYNEZ, ZUAZUA
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
Jðω ;h
0Þ−in
ω∈U
JðωÞand ^
Jð^
θ ;h
0Þ−in
ω∈U
JðωÞ;
as ; h →0.
The ollowing esul s a e p o en:
•Disc e izing he elaxed o mula ion, we show ha , sol ing he s a e equa ion
wi h he P1- ini e-elemen me hod in a mesh o size hand aking he con ol
θ o be piecewise cons an on elemen s o a coa se mesh o size ffiffiffi
h
p, he e o
is o o de h.
This cons i u es a big id o mul iscale s a egy, implemen ed on he elaxed
e sion, in he sense ha he disc e iza ion o he PDE and ha o he con ol
a e pe o med on wo di e en g ids. The PDE is disc e ized in he ine g id o
size h, while he con ol is disc e ized in he coa se one o size ffiffiffi
h
p.
•Disc e izing he o iginal un elaxed p oblem, sol ing he s a e equa ion wi h a
P1- ini e-elemen me hod in a mesh o size h, and aking he con ol χωpiece-
wise cons an in he elemen s o such mesh, we show ha he e o is o o de
h1−εwi h εa bi a ily small i he unc ions Fiin (1.2) do no depend on he
a iable uand ε¼1∕2o he wise.
A big id s a egy consis ing in disc e izing he PDE in he coa se g id (ins ead o
he ine one) can p oduce lack o con e gence o bo h he un elaxed and elaxed p o-
blems. In pa icula , he minimize s o he disc e e p oblem will possibly gi e a non-
minimizing sequence o he con inuous con ol p oblem, as ; h →0.
We also gi e an explici example in which he unc ional is independen o u, show-
ing ou es ima es a e nea ly sha p. To be mo e p ecise, ou example shows he op imali y
o he es ima es in he case in which he elaxed e sion o he p oblem is disc e ized,
while an o de ho con e gence is ob ained when he o iginal p oblem is disc e ized, hus
showing ha ou es ima es a e nea ly op imal.
The e o e he app oach based on he disc e iza ion o he elaxed o mula ion p o-
ides a be e app oxima ion and a as e con e gence a e wi h a lowe compu a ional
cos . The compu a ional cos and he complexi y o his app oach is lowe since he
con ols a e disc e ized in a mesh o o de ffiffiffi
h
pins ead o h. Fu he mo e, he minimize s
o he co esponding disc e e op imiza ion p oblems a e easie o ind nume ically.
Indeed, hanks o he con exi y o he elaxed con ol se , g adien -like algo i hms
can be implemen ed. This is in con as o he un elaxed p oblem, whe e he con ol
se is no con ex and we canno compu e a ia ions. Ins ead, much less e icien me hods
such as Mon e Ca lo o gene ic algo i hms should be used.
On he con a y, he ad an ages o disc e izing he o iginal p oblem di ec ly a e
ha , on one hand, one does no need o know he elaxed o mula ion and, on he o he
hand, i p o ides a physical con ol (i.e., a cha ac e is ic unc ion) ins ead o a elaxed
one. Howe e , his la e d awback can be o e come by app oxima ing he elaxed con-
ols by physical ones, wi h almos no compu a ional cos .
This pape p o ides a comple e analysis o he a e o con e gence o he ini e-
elemen app oxima ion o he op imal design p oblem unde conside a ion. Whe he
his classical enginee ing p ac ice leads o con e gen algo i hms is unknown in many
o he op imal design p oblems, excep in some o he pa icula examples as i occu s
when dealing wi h he op imal shape design o he domain o Di ichle Laplacian in
wo space dimensions (see [10]). No e, howe e , ha , in he la e , he e is no esul abou
he con e gence a e.
Al hough he p esen a icle is de o ed o he s udy o he 1−dop imal design
p oblem, some ema ks abou he N-dimensional case a e gi en in he las sec ion o
he pape . As abo e hese ema ks a e de o ed o he case o di usion coe icien s ha
APPROXIMATION OF AN OPTIMAL DESIGN PROBLEM 1185
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.

a e uni o mly ellip ic and bounded; he case whe e we conside ma ix di usions such
ha hei smalle and/o la ge eigen alues can app oxima e o ze o o in ini y, espec-
i ely, is mo e in ol ed. Indeed, e en he de ini ion o solu ion o he s a e equa ion is
no clea in his case, whe e in pa icula La en ie ’s phenomenon can occu ; i.e.,
smoo h unc ions canno be dense in he space o unc ions wi h bounded ene gy
(see, e.g., [25] and he e e ences he ein). In his sense, we ema k ha in o de o p o e
he con e gence o he ini e-elemen me hod, i is necessa y o ha e he densi y o he
Lipschi z unc ions in he space whe e we a e looking o he solu ion o he s a e equa-
ion. A ecip oca e o his esul has been ob ained in [5] o a calculus o a ia ions
p oblem wi hou es ic ions.
As we ha e al eady ema ked, con ol p oblem (1.1) does no ha e a solu ion in
gene al. To ha e a well-posed p oblem, such as we do in he p esen pape , an app oach
consis s o ob aining a elaxa ion o (1.1) by using homogeniza ion echniques. Howe e ,
he e exis o he app oaches, o ins ance, he il e ing echnique. Loosely speaking, he
idea o he il e ing echnique consis s o eplacing he se o con ols in (1.1) wi h a
smoo he class, de ined by mean o a con olu ion ope a o . Mo e p ecisely, in (1.3)
he cha ac e is ic unc ions χω, wi h ω∈U, a e eplaced by he smoo h unc ions
ρRθ, wi h θ∈L∞ðΩ;½0;1Þ sa is ying he olume es ic ion, whe e ρRis he ypical
molli ie unc ion ρRðxÞ¼ρðx∕RÞ∕RNwi h ρa ixed C∞nonnega i e unc ion wi h
suppo in he ball o cen e 0 and adius 1, and in eg al equals 1. Thus, we ob ain a new
p oblem ( il e ed p oblem) wi h a compac se o con ols in C∞ð¯
ΩÞ, which gua an ees
he exis ence o a solu ion when he cos unc ional Jis sequen ially lowe con inuous in
he weak opology o H1ðΩÞ. The il e ed p oblems a e hen smoo h app oxima ions o
(1.1) when R>0is small, a leas o mally. Gi en R ixed, he ini e-elemen app ox-
ima ion o he il e ed p oblem has been s udied in [4], in he amewo k o a con ol
p oblem in he coe icien s in elas ici y—namely he compliance p oblem. In [4], he
con e gence o he ini e-elemen app oxima ion, as he mesh size ends o ze o, is
p o ed bu wi hou explici a es.
Some de ini ions and no a ions:
•Fo a numbe ∈R, we deno e by ½  he in ege pa o .
•Fo a (Lebesgue) measu able subse Eo ð0;1Þ, wi h posi i e measu e, and a
unc ion win L1ð0;1Þ, we deno e he mean alue o win Eby
⨍E
wdx¼1
jEjZE
wdx:
•The se o unc ions o bounded a ia ion in ð0;1Þis deno ed by BVð0;1Þ.I ψis
in BVð0;1Þand Iis a subin e al o ½0;1, hen VIðψÞ ep esen s he o al a -
ia ion o ψin I.
•Th oughou he pape , αand βa e wo posi i e cons an s.
•Fo p∈½0;1, we deno e by MðpÞ∈R he ha monic mean o αand βwi h
p opo ions pand 1−p, espec i ely, gi en by
MðpÞ¼p
αþ1−p
β−1
¼αβ
ð1−pÞαþpβ:
No e ha Mð1Þ¼α,Mð0Þ¼β, and
α≤MðpÞ≤β∀p∈½0;1:ð1:15Þ
1186 CASADO-DÍAZ, CASTRO, LUNA-LAYNEZ, ZUAZUA
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
Fo e e y θ∈L∞ð0;1; ½0;1Þ we de ine Mθ∈L∞ðΩÞby
MθðxÞ¼MðθðxÞÞ o a:e:x∈ð0;1Þ:
•Fo a ma ix A∈RN×N, we deno e by EigðAÞ he se o i s eigen alues.
•Le Φbe a unc ion de ined in he in e al ð0;δÞ o some δ>0. The equali y
Φ¼oðhÞ(Landau symbol) means
lim
h→0
ΦðhÞ
h¼0:
•We deno e by Ca gene ic posi i e cons an ha can change om line o line.
2. Disc e iza ion and e o es ima es.
2.1. The main esul s. In his sec ion we s a e he main esul s o he pape . They
a e e e ed o he nume ical analysis o a con ol p oblem o he 1−dellip ic s a e
equa ion in Ω¼ð0;1Þbelow, he con ol being he space-dependen coe icien
(−d
dx ðαχωþβð1−χωÞÞdu
dx¼ inð0;1Þ;
uð0Þ¼uð1Þ¼0;
ð2:1Þ
whe e αand βa e wo ixed posi i e cons an s and a gi en unc ion in (a leas )
L1ð0;1Þ.
De ining, o a ixed cons an κ>0, he se o admissible con ols as (1.4), ou aim is
o choose ω∈Usuch ha he unique solu ion uω∈H1
0ð0;1Þo p oblem (2.1) minimizes
he unc ional J∶UR
!de ined as he 1−d e sion o (1.2); i.e.,
JðωÞ¼Zω
F1x; uω;duω
dx dxþZð0;1Þ ω
F2x; uω;duω
dx dx∀ω∈U:ð2:2Þ
He e F1;F2∶ð0;1Þ×R×R→Rsa is y
Fi∈W1;∞ðð0;1Þ×ð−R; RÞ×ð−R; RÞÞ ∀i∈ 1;2g∀R>0:ð2:3Þ
As we said in he in oduc ion, αand β ep esen wo ma e ials ha we wan o mix
in o de o minimize J. The cons an κis he maximum quan i y o ma e ial α ha can
be used in he mix u e. No e ha aking κ≥1would be equi alen o no imposing any
es ic ion in he se o admissible se s ω.
Rema k 1. In (2.1), we conside homogeneous Di ichle condi ions o ix ideas, bu
ou esul s also hold o nonhomogeneous Di ichle condi ions o o he bounda y
condi ions, such as Fou ie o Neumann ones. We can also conside he unc ions Fi
sa is ying weake assump ions han (2.3), bu hen he e o es ima es we ind o
he nume ical app oxima ions de ined below a e wo se.
I is well known ha he o iginal minimiza ion p oblem (1.1) does no ha e a solu-
ion in gene al (see [15], [16]). The e o e, i is necessa y o in oduce a elaxa ion. How-
e e , as we ha e men ioned in he in oduc ion, o nume ical pu poses i is o en
con enien o wo k in he elaxed e sion o he p oblem e en when he o iginal o mu-
la ion has a minimize . The elaxed e sion hus plays a key ole in he nume ical
analysis we de elop in his a icle.
The ollowing esul p o ides a cha ac e iza ion o he elaxa ion.
APPROXIMATION OF AN OPTIMAL DESIGN PROBLEM 1187
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
THEOREM 2.1. A elaxa ion o p oblem (1.1) is gi en by
Find θ0∈^
Usuch ha
^
Jðθ0Þ¼min
θ∈^
U
^
JðθÞ;
ð2:4Þ
whe e
^
U¼θ∈L∞ð0;1; ½0;1Þ∶Z1
0
θdx≤κ;ð2:5Þ
and ^
J∶^
U→Ris de ined by
^
JðθÞ¼Z1
0θF1x; uθ;Mθ
α
duθ
dx þð1−θÞF2x; uθ;Mθ
β
duθ
dx dxð2:6Þ
o e e y θ∈^
Uwi h u¼uθ he solu ion o
(−d
dx Mθdu
dx¼ in ð0;1Þ;
uð0Þ¼uð1Þ¼0:
ð2:7Þ
Rema k 2. Theo em 2.1 also holds ue o e e y ∈H−1ð0;1Þand mo e gene al
nonlinea i ies F1,F2. Indeed, i is enough o assume ha F1,F2a e wo Ca a héodo y
unc ions (measu able wi h espec o xand con inuous wi h espec o ðs; ξÞ) such ha
o e e y R>0, he unc ions φ1;R,φ2;R de ined as
φi;RðxÞ¼ sup
jsjþjξj≤RjFiðx; s; ξÞj o a:e:x∈ð0;1Þ∀i∈ 1;2g
belong o L1ð0;1Þ.
Rema k 3. Fo e e y ω⊂ð0;1Þmeasu able, we ha e
JðωÞ¼ ^
JðχωÞ:
The e o e, ^
Jis in ac an ex ension o he unc ional χω↦JðωÞde ined on he space
L∞ð0;1; 0;1gÞ o he elaxed con ol se L∞ð0;1; ½0;1Þ.
Rema k 4. Theo em 2.1 is a gene aliza ion o P oposi ion 4.1 and Theo em 4.3 in
[6], whe e he mul idimensional case is also conside ed.
In he p esen pape , we a e in e es ed mainly in he nume ical analysis o p oblem
(1.1). Fo his pu pose, hanks o Theo em 2.1, wo choices a e possible: o disc e ize
di ec ly p oblem (1.1) o o disc e ize he elaxed p oblem (2.4). Ou goal is o compa e
hese wo possibili ies.
To his aim, gi en >0, we ake a pa i ion P ¼ ykgm
k¼0o ½0;1, wi h m ∈N,
such ha
¼max
1≤k≤m ðyk−yk−1Þ:ð2:8Þ
Then, we de ine ^
U and U as he subse s o ^
Ugi en by
^
U ¼θ∈^
U∶θ¼X
m
k¼1
kχðyk−1;ykÞa:e:inð0;1Þwi h k∈½0;1;1≤k≤m ;ð2:9Þ
1188 CASADO-DÍAZ, CASTRO, LUNA-LAYNEZ, ZUAZUA
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
U ¼ ω⊂ð0;1Þ∶χω∈^
U g:ð2:10Þ
Associa ed o hese subse s we can conside he wo disc e iza ions o he con ol p o-
blem gi en by (1.10) and (1.8).
No e ha p oblem (1.8) is a disc e iza ion o he o iginal minimiza ion p oblem
(1.1), while (1.10) is a disc e iza ion o he elaxed p oblem (2.4).
The ollowing heo ems p o ide es ima es on he di e ence be ween hese p oblems
and (2.4). Some e sions o Theo em 2.2 can also be ob ained in he N-dimensional case;
see sec ion 8.
THEOREM 2.2. Assuming ∈L1ð0;1Þ, p oblem (1.10) has a solu ion o e e y >0,
and we ha e
0≤min
θ∈^
U
^
JðθÞ−min
θ∈^
U
^
JðθÞ¼oð Þ:ð2:11Þ
Mo eo e , i ∈L∞ð0;1Þand p oblem (2.4) has a solu ion θ0in BVð0;1Þ, hen
0≤min
θ∈^
U
^
JðθÞ−min
θ∈^
U
^
JðθÞ≤C 2:ð2:12Þ
THEOREM 2.3. Assuming ∈L1ð0;1Þ, p oblem (1.8) has a solu ion o e e y >0,
and we ha e
0≤min
ω∈U JðωÞ−in
ω∈U
JðωÞ≤C 1
2:ð2:13Þ
Mo eo e , i o some in ege l≥1, we ha e ha belongs o he space Wl;1ð0;1Þand
F1ðx; s; ξÞ,F2ðx; s; ξÞa e independen o sand belong o Cl;1
locð½0;1×RÞ; hen we ha e
0≤min
ω∈U JðωÞ−in
ω∈U
JðωÞ≤C lþ1
lþ2:ð2:14Þ
2.2. Op imali y. We now gi e an example showing ha he p e ious esul s a e
nea ly op imal.
Example 1. We conside p oblem (1.1) wi h α<β, ¼1,κ¼2∕3, and Jgi en by
JðωÞ¼−αZω
duω
dx 
2
dx−βZð0;1Þ ω
duω
dx 
2
dx:ð2:15Þ
Fo e e y n∈N, we de ine Pnas he pa i ion o ½0;1gi en by
Pn¼ k10−n∶0≤k≤10ng:
We de ine
^
Un¼θ∈^
U∶θ¼X
10n
k¼1
kχððk−1Þ10−n;k10−nÞwi h k∈½0;1∀k∈ 1; :::;10ng;ð2:16Þ
Un¼ ω∈U∶χω∈^
Ung:ð2:17Þ
We will p o e in sec ion 6 he ollowing esul .
APPROXIMATION OF AN OPTIMAL DESIGN PROBLEM 1189
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
Rema k 7. In Example 3 we a e disc e izing he s a e equa ion (2.1) o (2.7) using a
pa i ion o ½0;1o size hbigge han he size ¼h∕2employed in disc e izing he se o
con ols. S a emen (2.38) shows ha in his case he minimum o he disc e ized
p oblem does no end o he in imum o (1.1). Thus, his ype o disc e iza ion is
no con e gen in gene al.
3. P oo o he elaxa ion esul . This sec ion is de o ed o p o ing
Theo em 2.1, which cha ac e izes he elaxa ion o p oblem (1.1). To do i , we use
he ollowing lemma.
LEMMA 3.1. The unc ional ^
J∶^
U⊂L∞ð0;1Þ→Ris sequen ially con inuous o he
-weak opology o L∞ð0;1Þ.
P oo . Gi en a sequence θn∈^
Uwhich con e ges weakly-in L∞ð0;1Þ o a unc ion
θ∈^
U, we ha e o see ha ^
JðθnÞcon e ges o ^
JðθÞ. Fo a such sequence θn, we obse e
ha he co esponding solu ion uθno (2.7) is gi en by
uθnðxÞ¼−Zx
0
Fð Þ−cn
Mθn
d ¼−Zx
0ðFð Þ−cnÞαð1−θnð ÞÞþβθnð Þ
αβ d
wi h Fa p imi i e o in ð0;1Þand
cn¼Z1
0
d
Mθnð Þ−1Z1
0
Fð Þ
Mθnð Þd :
The e o e, i is immedia e o show ha
kuθnkW1;∞ð0;1Þ≤C; uθn→uθin C0ð½0;1Þ;M
θn
dun
dx −Mθ
duθ
dx →0inC0ð½0;1Þ
wi h uθ he unique solu ion o (2.7). Then, by (2.3) we ob ain
lim
n→∞
^
JðθnÞ
¼limn→∞Z1
0θnF1x; uθn;Mθn
α
duθn
dx þð1−θnÞF2x; uθn;Mθn
β
duθn
dx dx
¼Z1
0θF1x; uθ;Mθ
α
duθ
dx þð1−θÞF2x; uθ;Mθ
β
duθ
dx dx¼^
JðθÞ:▯
P oo o Theo em 2.1. Taking in o accoun ha he space o con ols ^
Ugi en by
(2.5) is sequen ially compac in he -weak opology o L∞ð0;1Þ, om Lemma 3.1 we
deduce ha p oblem (2.4) has a leas a solu ion. On he o he hand, by Rema k 3 i is
clea ha
in
ω∈U
JðωÞ¼ in
χω∈^
U
^
JðχωÞ≥min
θ∈^
U
^
JðθÞ:
The e o e, in o de o check ha p oblem (2.4) is a elaxa ion o (1.1), i is enough o
p o e ha o e e y θ∈^
U, he e exis s a sequence ωnin Usuch ha
1196 CASADO-DÍAZ, CASTRO, LUNA-LAYNEZ, ZUAZUA
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.

χωn⇀
θin L∞ð0;1Þ;ð3:1Þ
JðωnÞ→^
JðθÞ:ð3:2Þ
The exis ence o his sequence ωnis well known ( o example, i is a consequence o
Lemma 5.1 below), while by he con inui y p ope y o ^
Jp o ed in s ep 1, (3.2) is
a consequence o (3.1). So, he p oo o Theo em 2.1 is comple e. ▯
4. P oo o he con e gence es ima es o he disc e ized elaxed con ol
p oblem. In his sec ion we p o e Theo em 2.2 e e ed o he con e gence o he dis-
c e iza ion o p oblem (2.4) gi en by (1.10). No e ha we a e disc e izing he con ols
bu no he s a e equa ion. We also gi e he p oo o P oposi ion 2.5, which pe mi s us o
ob ain a physical con ol om a elaxed one.
Along his sec ion, we conside a pa i ion P ¼ ykgm
k¼0, wi h m ∈N, sa is ying
(2.8). The space ^
U is de ined by (2.9).
In o de o show Theo em 2.2, we will use he ope a o Π de ined by he ollowing.
DEFINITION 4.1. We de ine he p ojec ion ope a o Π ∶L1ð0;1Þ→^
U by
Π ψ¼X
m
k¼1⨍yk
yk−1
ψdsχðyk−1;ykÞ∀ψ∈L1ð0;1Þ:ð4:1Þ
The ollowing lemma es ima es he di e ence Π θ−θwhen ends o ze o.
LEMMA 4.2. Le θbe in L∞ð0;1; ½0;1Þ. Then, o e e y φ∈W1;1ð0;1Þ, i holds ha
Z1
0ðθ−Π θÞφdx¼oð Þ;ð4:2Þ
Z1
0Zx
0ðθð Þ−Π θð ÞÞφð Þd 
dx¼oð Þ:ð4:3Þ
Mo eo e , i θis in BVð0;1Þ, and φis in W1;∞ð0;1Þ, we ha e he ollowing imp o emen
o he p e ious es ima es:
Z1
0ðθ−Π θÞφdx
≤C



dφ
dx


L∞ð0;1Þ
2;ð4:4Þ
Z1
0Zx
0ðθð Þ−Π θð ÞÞφð Þd 
dx≤CkφkW1;∞ð0;1Þ 2:ð4:5Þ
P oo . We ake φ∈W1;1ð0;1Þ; o a gi en x∈½0;1, we conside yjde ined by
yj¼sup yk∶yk≤x; 0≤k≤m g:
Then, using he inequali y

φð Þ−⨍yk
yk−1
φds
≤



dφ
d 


L1ðyk−1;ykÞ
∀ ∈½yk−1;y
k
we ha e
APPROXIMATION OF AN OPTIMAL DESIGN PROBLEM 1197
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
Zx
0ðθ−Π θÞφd 
¼X
j
k¼1Zyk
yk−1θ−⨍yk
yk−1
θdsφd þZx
yjθ−⨍yk
yk−1
θdsφd
¼X
j
k¼1Zyk
yk−1ðθ−⨍yk
yk−1
θdsÞðφ−⨍yk
yk−1
φdsÞd
þZx
yjθ−⨍yk
yk−1
θdsφd
≤X
j
k¼1



dφ
dx


L1ðyk−1;ykÞkθ−Π θkL1ðyk−1;ykÞþkφkL∞ð0;1Þkθ−Π θkL1ðyj;xÞ:ð4:6Þ
In eg a ing his inequali y in ð0;1Þ,wege
Z1
0Zx
0ðθð Þ−Π θð ÞÞφð Þd 
dx
≤X
m
k¼1



dφ
dx


L1ðyk−1;ykÞkθ−Π θkL1ðyk−1;ykÞ
þkφkL∞ð0;1ÞX
m −1
j¼0Zyjþ1
yjkθ−Π θkL1ðyj;xÞdx
≤X
m
k¼1



dφ
dx


L1ðyk−1;ykÞkθ−Π θkL1ðyk−1;ykÞþkφkL∞ð0;1Þkθ−Π θkL1ð0;1Þ :ð4:7Þ
I φbelongs o W1;∞ð0;1Þand θbelongs o BVð0;1Þ, using in (4.7)




dφ
dx


L1ðyk−1;ykÞ
≤



dφ
dx


L∞ð0;1Þ
; kθ−Π θkL1ð0;1Þ≤Vð0;1ÞðθÞ ;ð4:8Þ
we deduce (4.5).
Inequali y (4.4) is a consequence o (4.6) wi h x¼1¼yjand (4.8).
In o de o show (4.2) and (4.3) we now ake a sequence φnin W1;∞ð0;1Þwhich
con e ges o φin W1;1ð0;1Þand a sequence θnin BVð0;1Þ, wi h 0≤θn≤1in ð0;1Þ,
which con e ges o θin L1ð0;1Þ. Then, we es ima e he igh -hand side o (4.7) as ollows:
X
m
k¼1



dφ
dx


L1ðyk−1;ykÞkθ−Π θkL1ðyk−1;ykÞþkφkL∞ð0;1Þkθ−Π θkL1ð0;1Þ
≤2



dðφ−φnÞ
dx 


L1ð0;1Þ
þkφkL∞ð0;1Þkθ−θn−Π ðθ−θnÞkL1ð0;1Þ
þX
m
k¼1



dφn
dx 


L1ðyk−1;ykÞkθ−Π θkL1ðyk−1;ykÞþkφkL∞ð0;1Þkθn−Π θnkL1ð0;1Þ
≤2



dðφ−φnÞ
dx 


L1ð0;1Þ
þkφkL∞ð0;1Þkθ−θn−Π ðθ−θnÞkL1ð0;1Þ
þ



dφn
dx 


L∞ð0;1Þ
Vð0;1ÞðθÞþkφkL∞ð0;1ÞVð0;1ÞðθnÞ 2:
1198 CASADO-DÍAZ, CASTRO, LUNA-LAYNEZ, ZUAZUA
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
Di iding his inequali y by and passing o he limi i s when ends o ze o and hen
when n ends o in ini y, we deduce (4.3). The p oo o (4.2) can be ob ained easoning in a
simila way wi h (4.6). ▯
Fo θ∈L∞ð0;1; ½0;1Þ, he ollowing lemma es ima es he di e ence be ween he
solu ion o (2.7) and he solu ion o he analogous p oblem when θis eplaced by Π θ.
LEMMA 4.3. Assume ∈L1ð0;1Þ. Fo θ∈L∞ð0;1; ½0;1Þ, we conside θ ¼Π θ.
Then, he solu ions uθand uθ o (2.7) o θand θ , espec i ely, sa is y
kuθ−uθ kL1ð0;1Þ≤oð Þ;ð4:9Þ




Mθ
duθ
dx −Mθ
duθ
dx 


L∞ð0;1Þ
≤oð Þ:ð4:10Þ
I is in L∞ð0;1Þand θis in BVð0;1Þ, hen in (4.9) and (4.10) we can ake
oð Þ¼CVð0;1ÞðθÞ 2:
P oo . The unc ions uθand uθ a e gi en by
uθðxÞ¼−Zx
0
g
Mθ
dsþcZx
0
1
Mθ
ds o a:e:x∈ð0;1Þ;ð4:11Þ
uθ ðxÞ¼−Zx
0
g
Mθ
dsþc Zx
0
1
Mθ
ds o a:e:x∈ð0;1Þð4:12Þ
wi h ga p imi i e o and c; c ∈Rde ined by
c¼Z1
0
1
Mθ
dx−1Z1
0
g
Mθ
dx; c ¼Z1
0
1
Mθ
dx−1Z1
0
g
Mθ
dx:ð4:13Þ
Using hese exp essions and aking in o accoun ha
min α;βg≤Mθ;Mθ ≤max α;βg;
we easily deduce
kuθ−uθ kL1ð0;1Þ≤CZ1
0ðθ−θ ÞgdxþZ1
0ðθ−θ Þdx
:
þZ1
0Zx
0ðθð Þ−θ ð ÞÞgð Þd 
dxþZ1
0Zx
0ðθð Þ−θ ð ÞÞd 
dx
and




Mθ
duθ
dx −Mθ
duθ
dx 


L∞ð0;1Þ
≤CZ1
0ðθ−θ ÞgdxþZ1
0ðθ−θ Þdx:
Lemma 4.3 is hen a simple consequence o Lemma 4.2. ▯
We a e now in posi ion o p o e he ollowing.
P oo o Theo em 2.2. The exis ence o solu ion o p oblem (1.10) is a simple con-
sequence o he compac ness o (2.9) in L1ð0;1Þ.
On he o he hand, using ha F1and F2a e locally Lipschi z, and ha he unc-
ions uθ,uθ de ined as in Lemma 4.2 a e bounded in W1;∞ð0;1Þindependen ly o ,
we ha e
APPROXIMATION OF AN OPTIMAL DESIGN PROBLEM 1199
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
j^
JðθÞ−^
Jðθ Þj
≤Z1
0
F1x; uθ;Mθ
α
duθ
dx ðθ−θ ÞdxþZ1
0
F2x; uθ;Mθ
α
duθ
dx ðθ−θ Þdx
þCZ1
0juθ−uθ jþMθ
duθ
dx −Mθ
duθ
dx dx:
Thanks o Lemma 4.3, we hen deduce (2.11) and (2.12). ▯
To inish his sec ion, we now gi e he p oo o P oposi ion 2.5.
P oo o P oposi ion 2.5. Reasoning as in he p oo o Theo em 2.2, we ha e ha
he esul is an immedia e consequence o he ollowing lemma, which is simila o
Lemma 4.2. ▯
LEMMA 4.4. Assume θand ωas in he s a emen o P oposi ion 2.5; hen o e e y
φ∈W1;∞ð0;1Þ, i holds ha
Z1
0ðθ−χωÞφdx
≤



dφ
dx


L∞ð0;1Þ
2;ð4:14Þ
Z1
0Zx
0ðθð Þ−χωð ÞÞφð Þd 
dx≤kφkW1;∞ð0;1Þ 2:ð4:15Þ
P oo . Since in each in e al ½yk−1þði−1Þsk;y
kþisk, wi h 1≤k≤m ,
1≤i≤jk, he unc ions θand χωha e he same in eg al, we can eason as in he p oo
o (4.6) o deduce ha o e e y x∈½0;1, we ha e
Zx
0ðθ−χωÞφd 
≤



dφ
dx


L∞ð0;1Þkθ−χωkL1ð0;1Þ 2þkφkL∞ð0;1Þkθ−χωkL1ðIÞ ;ð4:16Þ
whe e Iis an in e al o he o m ½yk−1þði−1Þsk;y
kþiskcon aining x. Taking x¼1
we ge (4.14). On he o he hand, since θand χωbelong o L∞ð0;1; ½0;1Þ, inequali y
(4.16) implies
Zx
0ðθ−χωÞφd 
≤ 2kφkW1;∞ð0;1Þ
o e e y x∈½0;1. This inequali y immedia ely p o es (4.15). ▯
5. P oo o he con e gence es ima es o he disc e ized un elaxed
con ol p oblem. Le us now p o e Theo em 2.3. As o Theo em 2.2, we will need
some p elimina y lemmas.
LEMMA 5.1. We conside θ∈L∞ð0;1Þand l∈N; hen, he e exis s ω⊂ð0;1Þmea-
su able such ha
Z1
0
jθð Þd ¼Zω
jd ∀j∈ 0; :::;lg:ð5:1Þ
Mo eo e ωcan be chosen in he ollowing way:
1200 CASADO-DÍAZ, CASTRO, LUNA-LAYNEZ, ZUAZUA
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
I l¼2n, wi h n∈N,
ω¼ð0;b
0Þ[[
m
i¼1ðai;b
iÞ;
whe e m≤nand 0≤b0<a1<b1<···<am<bm≤1.
I l¼2nþ1, wi h n∈N,
ω¼[
m
i¼1ðai;b
iÞ;
whe e m≤nþ1and 0≤a1<b1<···<am<bm≤1.
P oo . Le us p o e he esul in he case l¼2nþ1, he o he one being simila .
We de ine D⊂L1ð0;1Þas
D¼ϕ¼X
m
i¼1
χðai;biÞwi h m≤nþ1;0≤a1<b1<···<am<bm≤1
and Ψ∶D→Rby
ΨðϕÞ¼X
2nþ1
j¼0Z1
0
jðθð Þ−ϕð ÞÞd 2
∀ϕ∈D:
Since Dis compac in L1ð0;1Þand Ψis con inuous, we know ha Ψa ains i s minimum
in some unc ion
ϕ¼X
m
i¼1
χðai;biÞ∈D:
Then, we de ine he polynomial Pas
PðλÞ¼X
2nþ1
j¼0Z1
0
jðθð Þ−ϕð ÞÞd λj.
We ix k, wi h 1≤k≤m. Fo ε∈R, wi h jεjsmall (εmus also be posi i e i k¼1,
a1¼0), he unc ion
ϕε¼χ∪i≠kðai;biÞþχðakþε;bkÞ
belongs o D. Taking in o accoun ha
ΨðϕεÞ¼X
2nþ1
j¼0Z1
0
jðθð Þ−ϕð ÞÞd þZakþε
ak
jd 2
;
and ha ϕis a minimum poin o Ψ, he de i a i e o ΨðϕεÞwi h espec o εyields
PðakÞ¼0i ak≠0;Pða1Þ≥0i a1¼0:
Analogously, we can p o e
APPROXIMATION OF AN OPTIMAL DESIGN PROBLEM 1201
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.

PðbkÞ¼0i bk≠1;PðbmÞ≥0i bm¼1:
I Phas 2nþ2ze os, hen i is he ze o polynomial and we ob ain he conclusion o
he lemma. So, we assume in he ollowing ha Phas a mos 2nþ1ze os. By he abo e
p o ed we deduce ha
m¼nþ1;a
1¼0;and∕o bnþ1¼1;
o
m<nþ1:
Le us p o e ha in all hese cases Psa is ies
PðλÞ≥0in [
m
i¼1ðai;b
iÞ;PðλÞ≤0inð0;1Þ [
m
i¼1ðai;b
iÞ.ð5:2Þ
(i) Case m¼nþ1,a1¼0,bnþ1¼1. Since we a e supposing ha he numbe o
ze os o Pis s ic ly less han 2nþ2and P anishes in he 2npoin s akwi h
k¼2; :::;nþ1,bkwi h k¼1; :::;n, we ha e ha Phas 2no 2nþ1ze os
in ½0;1. I he numbe o ze os is 2nþ1, hen using ha Pð0Þ;Pð1Þ≥0,we
deduce ha he o he ze o o Pis in 0 o 1 and ha Psa is ies (5.2). I he
numbe o ze os is 2n, hen we ha e Pð0Þ;Pð1Þ>0and (5.2) is sa is ied.
(ii) Case m¼nþ1,a1¼0,bnþ1<1. In his case we ha e ha he 2nþ1ze os
o Pa e gi en by he poin s akwi h k¼2; :::;nþ1,bkwi h
k¼1; :::;nþ1. Since Pð0Þ≥0, we deduce (5.2).
(iii) Case m¼nþ1,a1>0,bnþ1¼1. I is simila o he case (ii).
(i ) Case m<nþ1. In his case, we ake a poin c∈ðai;b
iÞ o some
i∈ 1; :::mg. Then o ε>0, small enough, he unc ion
ϕε¼ϕ−χðc−ε;cþεÞ
belongs o D. Using ha
ΨðϕεÞ¼X
2nþ1
j¼0Z1
0
jðθð Þ−ϕð ÞÞd þZcþε
c−ε
jd 2
;
and de i ing wi h espec o ε, we deduce ha
PðcÞ≥0∀c∈[
m
i¼1ðai;b
iÞ:
Analogously, i c∈ð0;1Þ Sm
i¼1½ai;b
i, aking
ϕε¼ϕþχðc−ε;cþεÞ;
we deduce ha
1202 CASADO-DÍAZ, CASTRO, LUNA-LAYNEZ, ZUAZUA
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
PðcÞ≤0∀c∈ð0;1Þ [
m
i¼1½ai;b
i:
Thus, (5.2) is also p o en in his case.
To inish, le us p o e ha (5.2) implies he conclusion o he lemma. Fo his pu -
pose, we jus w i e
X
2nþ1
j¼0Z1
0
jðθð Þ−ϕð ÞÞd 2
¼Z1
0X
2nþ1
j¼0Z1
0
jðθð Þ−ϕð ÞÞd sjðθðsÞ−ϕðsÞÞds
¼Z1
0
PðsÞðθðsÞ−ϕðsÞÞds.ð5:3Þ
I s∈Sm
i¼1ðai;b
iÞ(i.e., ϕðsÞ¼1), hen by (5.2), PðsÞ≥0and since θðsÞ≤1, we ha e
PðsÞθðsÞ≤PðsÞϕðsÞ:
I s∈=Sm
i¼1ðai;b
iÞ(i.e., ϕðsÞ¼0), hen by (5.2), PðsÞ≤0and since θðsÞ≥0, we also
ha e
PðsÞθðsÞ≤PðsÞϕðsÞ:
The e o e he las in eg al in (5.3) is nonposi i e, which p o es
X
2nþ1
j¼0Z1
0
jðθð Þ−ϕð ÞÞd 2
¼0:
This p o es Lemma 5.1. ▯
As a consequence, we deduce he ollowing.
LEMMA 5.2. Le a,bbe in Rwi h a<band le ykgm
k¼0be a pa i ion o ½a; bo size
δ¼max
1≤k≤mðyk−yk−1Þ:
Le also θbe in L∞ða; b;½0;1Þ. Then o e e y l∈N, he e exis s I⊂ 1; :::;mgsuch
ha
~
ω¼[
k∈Iðyk−1;y
kÞð5:4Þ
sa is ies
j~
ωj≤Zb
a
θdx;ð5:5Þ
Zb
aðθ−χ~
ωÞφdx
≤Cðb−aÞlþ1kDlþ1φkL1ða;bÞþCδkφkL∞ða;bÞ∀φ∈Wlþ1;1ð0;1Þ;
ð5:6Þ
whe e Cis a posi i e cons an ha depends on l, bu i is independen o θ,δ,a, and b.
APPROXIMATION OF AN OPTIMAL DESIGN PROBLEM 1203
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
P oo . I is enough o show he case a¼0,b¼1. The gene al one ollows using a
ansla ion and a dila a ion which ans o ms ða; bÞin ð0;1Þ.
Fo a gi en l∈N, by Lemma 5.1 we know he e exis s ω⊂ð0;1Þsa is ying (5.1) and
such ha he numbe o discon inui y poin s o χωin ½0;1is a mos lþ1. We hen
de ine
I¼ k∈ 1; :::;mg∶ðyk−1;y
kÞ⊂ωg
and ~
ωby (5.4). By he de ini ion o ~
ω, we ha e ~
ω⊂ω, and hen using (5.1) when j¼0,
we ob ain (5.5). Mo eo e , using ha χωhas a mos lþ1discon inui y poin s in ½0;1,
we ha e
jω ~
ωj≤ðlþ1Þδ:ð5:7Þ
We now ix φ∈Wlþ1;1ð0;1Þ. Taking a polynomial po deg ee lsuch ha
Z1
0jφ−pjdx≤CkDlþ1φkL1ð0;1Þ
wi h Cindependen o φ( ake, o example, he Taylo polynomial o deg ee lo φ∈
Wlþ1;1ð0;1Þ⊂Clð½0;1Þ in some poin o ½0;1), we ge
Z1
0ðθ−χ~
ωÞφdx
≤Z1
0ðθ−χωÞðφ−pÞdxþZ1
0ðχω−χ~
ωÞφdx
≤CkDlþ1φkL1ð0;1Þþðlþ1ÞδkφkL∞ð0;1Þ:ð5:8Þ
This p o es (5.6) o a¼0,b¼1.▯
LEMMA 5.3. Fo >0small we ake a pa i ion P ¼ ykgm
k¼0wi h m ∈Nsuch ha
(2.8) is sa is ied. We de ine ^
Uby (2.5) and U by (2.10).
(a) Fo e e y θ∈^
U, he e exis s ω∈U such ha
Zx
0ðθ−χωÞφds
≤C 1
2kφkW1;1ð0;1Þ∀x∈½0;1;∀φ∈W1;1ð0;1Þ;ð5:9Þ
whe e Cis a posi i e cons an independen o θand .
(b) Fo e e y θ∈^
Uand e e y l∈N, he e exis s ω∈U such ha
Z1
0ðθ−χωÞφds
≤C lþ1
lþ2kφkWlþ1;1ð0;1Þ∀φ∈Wlþ1;1ð0;1Þ;ð5:10Þ
whe e Cis a posi i e cons an ha depends on l, bu i is independen o θand .
P oo . We ake l∈N,γ∈ð2 ; 1Þ, and a subpa i ion Pγ¼ zigmγ
i¼0⊂P o P
which sa is ies
γ− ≤zi−zi−1≤γ∀i∈ 1; :::;m
γ−1g; ≤zmγ−zmγ−1≤γ:
This implies in pa icula
mγ≤1
γ− þ1≤3
γ:ð5:11Þ
1204 CASADO-DÍAZ, CASTRO, LUNA-LAYNEZ, ZUAZUA
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
Using ha o e e y i∈ 1; :::;m
γ−1g he poin s ykwi h zi−1≤yk≤zia e a pa i ion
o ½zi−1;z
iwi h mesh , we can apply Lemma 5.2 in each in e al ½zi−1;z
i o cons uc a
se ω∈Usuch ha o e e y i∈ 1; :::;m
γ−1g, we ha e
Zzi
zi−1ðθ−χωÞφdx
≤Cðγlþ1kDlþ1φkL1ðzi−1;ziÞþkφkL∞ðzi−1;ziÞ Þð5:12Þ
o e e y φ∈Wlþ1;1ð0;1Þ.
Fo x∈½0;1, we ake he la ge jsuch ha zj≤x; hen, hanks o (5.12) and
(5.11), we ha e
Zx
0ðθ−χωÞφds¼Zzj
0ðθ−χωÞφdsþZx
zjðθ−χωÞφds
≤Cγlþ1kDlþ1φkL1ð0;1ÞþkφkL∞ð0;1Þ3
γþðx−zjÞ:ð5:13Þ
Fo l¼0, he abo e inequali y and x−zj<γp o e
Zx
0ðθ−χωÞφds
≤CγkD1φkL1ð0;1ÞþCkφkL∞ð0;1Þ
γþγ:
Minimizing in γ his quan i y, we deduce (5.9).
On he o he hand, o x¼1¼zjinequali y (5.13) gi es
Z1
0ðθ−χωÞφds
≤Cγlþ1kDlþ1φkL1ð0;1ÞþCkφkL∞ð0;1Þ
γ;
which minimizing in γp o es (5.10). ▯
Using Lemma 5.3 and easoning simila ly o Lemma 4.3, we easily deduce he
ollowing.
LEMMA 5.4. Le θbe in ^
Uand ∈L1ð0;1Þ. Then, o e e y >0, he e exis s ω∈U
such ha , de ining uθ,u as he solu ions o (2.7) o θand χω, espec i ely, we ha e he
ollowing:
(a)
kuθ−u kL1ð0;1Þ≤Cð1þk kL1ð0;1ÞÞ 1
2:ð5:14Þ
(b) I belongs o Wl;1ð0;1Þ, hen




Mθ
duθ
dx −Mχω
du
dx 


L∞ð0;1Þ
≤Cð1þk kWl;1ð0;1ÞÞ lþ1
lþ2:ð5:15Þ
LEMMA 5.5. Le ∈L1ð0;1Þand θbe in ^
U; hen o e e y >0, he e exis s ω∈U
such ha
j^
JðθÞ−JðωÞj ≤C 1
2ð1þk kL1ð0;1ÞÞ:ð5:16Þ
I o some l∈Nwe ha e ha belongs o Wl;1ð0;1Þ,F1ðx; s; ξÞ,F2ðx; s; ξÞa e
independen o sand belong o Cl;1
locð½0;1×RÞ; hen
APPROXIMATION OF AN OPTIMAL DESIGN PROBLEM 1205
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
This pe mi s us, o example, o subs i u e in he de ini ion o he elaxed con ol se ^
U
he se KðpÞby he (mo e simple) se o symme ic ma ices whose eigen alues a e com-
p essed be ween λðpÞand ΛðpÞ.
Rema k 9. De ining
E¼ ðξ;η;pÞ∈RN×RN×½0;1∶ðη−λðpÞξÞ·ðη−ΛðpÞξÞ≤0g;
he unc ion H ha appea s in (8.5) is a Ca a héodo y unc ion wi h domain Ω×R×E.
An explici exp ession o Hin he whole o i s domain is no known in gene al.
In he pa icula case whe e F1ðx; s; ξÞ,F2ðx; s; ξÞa e a ine unc ions in he a iable
ξ, we ha e
Hðx; s; ξ;η;pÞ¼pF1ðx; s; ξÞþð1−pÞF2ðx; s; ξÞ∀ðs; ξ;η;pÞ∈R×Ea:e:x∈Ω;
while o nonlinea unc ions Fiin he a iable ξ, an exp ession o His only known in
some pa icula cases (which essen ially a e conce ned wi h he nonlinea unc ion jξj2);
see [3], [6], [8], [11], and [18].
Howe e , an explici ep esen a ion is always known in he bounda y o i s domain
ðx; s; ξ;η;pÞ∶∈Ω×R×R×½0;1∶ðη−λðpÞξÞ·ðη−ΛðpÞξÞ¼0g;
whe e Hðx; s; ξ;η;pÞis gi en by
8
>
>
<
>
>
:
F1ðx; s; ξÞi p¼1;
F2ðx; s; ξÞi p¼0;
pF1x; s; βξ−η
pðβ−αÞþð1−pÞF2x; s; η−αξ
ð1−pÞðβ−αÞi p≠0;1:
ð8:7Þ
Obse e ha he las line can be aken as he gene al exp ession o H, aking he alues
o p¼0and p¼1by con inui y.
Analogously as we did in he one-dimensional case, in o de o nume ically sol e
p oblem (8.5), o >0we decompose Ωas
Ω¼[
m
i¼1
Ki;K
idisjoin ;measu able;diamðKiÞ< ; i ∈ 1; :::;m
g:ð8:8Þ
Then, we disc e ize p oblem (8.5) as
min ZΩ
Hðx; u; ∇u; M∇u; θÞdx
−di M∇u¼ in Ω;u¼0on∂Ω;
ðθ;MÞ∈^
U;ðθ;MÞcons an in Ki;1≤i≤m ;RΩθdx≤κ:
ð8:9Þ
As we said in Rema k 9 in he case whe e he unc ions Fiðx; s; ξÞa e nonlinea in he
a iable ξ, one o he main di icul ies o sol e p oblem (8.9) is ha His no known. To
sol e his di icul y we can eplace Hwi h ano he unc ion. The ollowing esul is
p o ed in [8] in he pa icula case F1ðx; s; ξÞ¼F2ðx; s; ξÞ¼FðξÞ. The gene al case
ollows simila ly.
1212 CASADO-DÍAZ, CASTRO, LUNA-LAYNEZ, ZUAZUA
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.

THEOREM 8.1. We conside a unc ion ^
H∶Ω×R×E→R∪ þ∞gsuch ha
^
Hð:; s; ξ;η;pÞis measu able in Ω∀ðs; ξ;η;pÞ∈R×E;ð8:10Þ
^
Hðx; :; :; :; :Þis lowe semicon inuous in R×E o a:e: x ∈Ω;ð8:11Þ
^
Hðx; s; ξ;αξ;1Þ¼F1ðx; s; ξÞ;^
Hðx; s; ξ;βξ;0Þ¼F2ðx; s; ξÞ;ð8:12Þ
^
Hðx; s; ξ;η;pÞ≥Hðx; s; ξ;η;pÞ∀ðs; ξ;η;pÞ∈R×E a:e: x ∈Ω:ð8:13Þ
Fo e e y >0, we decompose Ωby (8.9). Then, he p oblem
min ZΩ
^
Hðx; u; ∇u; M∇u; θÞdx
−di M∇u¼ in Ω;u¼0on∂Ω;
ðθ;MÞ∈^
U;ðθ;MÞcons an in Ki;1≤i≤m ;RΩθdx≤κ
ð8:14Þ
has a solu ion (no unique in gene al) ðθ ;M Þ. Taking u as he solu ion o
−di M ∇u ¼ inΩ;u
¼0on ∂Ω;
we ha e
∃lim
→0ZΩ
^
Hðx; u ;∇u ;M ∇u ;θ Þdx¼I
wi h I he minimum alue o p oblem de ined by (8.5). The sequence ðθ ;M ;u
Þis
bounded in L∞ðΩÞ×L∞ðΩ;RN×NÞ×H1
0ðΩÞ. E e y unc ion ðθ;M;uÞ∈L∞ðΩÞ×
L∞ðΩ;RN×NÞ×H1
0ðΩÞsuch ha he e exis s a subsequence o , s ill deno ed by ,
sa is ying
θ ⇀
θin L∞ðΩÞ;M
⇀
MinL
∞ðΩ;RN×NÞ;u
⇀uinH
1
0ðΩÞ
is such ha he unc ion ðθ;σ;uÞwi h σ¼M∇uis a solu ion o (8.6).
Rema k 10. A i s choice o unc ion ^
His o ake
^
Hðx; s; ξ;η;pÞ¼8
<
:
F1ðx; s; ξÞi p¼1;η¼αξ;
F2ðx; s; ξÞi p¼0;η¼βξ;
þ∞o he wise:
In his case, aking in o accoun ha ^
Hðx; u; ∇u; M∇u; θÞ<þ∞a.e. in Ωimplies ha θ
is a cha ac e is ic unc ion we ge ha p oblem (8.14) can be w i en as
min Zω
F1ðx; u; ∇uÞdxþZΩ ω
F2ðx; u; ∇uÞdx
−di ðαχωþβχΩ ωÞ∇u¼ in Ω;u¼0on∂Ω;
∃I⊂ 1; :::;m
gsuch ha ω¼S
i∈I
Ki;jωj≤κ:
The e o e, wi h his choice o unc ion ^
H, Theo em 8.1 gi es he con e gence o he nu-
me ical me hod consis ing in disc e izing di ec ly he o iginal (un elaxed) p oblem (8.1).
APPROXIMATION OF AN OPTIMAL DESIGN PROBLEM 1213
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
Thanks o (8.7), ano he possibili y o ^
His o ake ^
H¼Hin ∂DðHÞ, and ^
H¼þ∞,
o he wise. Fo his choice o unc ion ^
H, aking in o accoun ha o p≠0;1a ma ix
M∈KðpÞsa is ies
ðMξ−λðpÞξÞ·ðMξ−ΛðpÞξÞ¼ξ o some ξ≠0
⇔Mis a lamina ion o αI; βIwi h p opo ions pand 1 −p
⇔EigðMÞ¼ðλðpÞ;ΛðpÞ; :::;ΛðpÞÞ:
We can w i e p oblem (8.14) as
min ZΩpF1x; u; β∇u−M∇u
pðβ−αÞþð1−pÞF2x; u; M∇u−α∇u
ð1−pÞðβ−αÞdx
8
<
:
−di M∇u¼ in Ω;u¼0on∂Ω;
θ∈L∞ðΩ;½0;1Þ;Msymme ic;EigðMÞ¼ðλðθÞ;ΛðθÞ; :::;ΛðθÞÞa:e:in Ω;
θ;Mcons an s in Ki;i¼1; :::;m
;RΩθdx≤κ:
In his case, p oblem (8.14) consis s in disc e izing a pa ial elaxa ion o p oblem (8.1)
consis ing in conside ing no only he o iginal con ols bu also he ones ob ained by a
simple lamina ion.
Clea ly, when His known, ano he possibili y is o ake di ec ly ^
H¼H. In his case
we a e disc e izing he elaxed con ol p oblem (8.9).
Rema k 11. Al hough Theo em 8.1 gi es he con e gence o he disc e ized p oblem
(8.14), i does no p o ide any e o es ima e. In pa icula , i does no show which
choice o he unc ions ^
Hmen ioned in Rema k 10 is be e .
As we saw in he p oo o he es ima es o he one-dimensional p oblem, in o de o
ob ain an es ima e o he con e gence a e o he nume ical me hod, one idea is o con-
s uc om a elaxed con ol ðθ;MÞano he con ol ðθ ;M Þin he se o disc e ized
con ols such ha he solu ions o he s a e equa ions ela i e o ðθ;MÞand
ðθ ;M Þa e close. In he case whe e ^
H¼H(which can only be used i His known),
one idea is o ake ðθ ;M Þas he mean alue o ðθ;MÞin each elemen o he iangula-
ion. Deno ing by uand u he solu ions o
−di M∇u¼ in Ω;
u¼0on∂Ω;−di M ∇u ¼ in Ω;
u¼0on∂Ω
wi h in H−1ðΩÞand aking in o accoun ha
−di M ∇ðu−u Þ¼−di ðM −MÞ∇uin Ω;
we deduce ha
ZΩj∇ðu−u Þj2dx≤CZΩjðM −MÞ∇uj2dx;
which pe mi s o es ima e he di e ence o u−u depending on he smoo hness p ope -
ies o Mand uand hen o es ima e he e o o he disc e ized me hod.
When His no known and he e o e we need o disc e ize di ec ly he o iginal
p oblem o o conside some pa ial elaxa ion, he choice o ðθ ;M Þis no clea .
1214 CASADO-DÍAZ, CASTRO, LUNA-LAYNEZ, ZUAZUA
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
Rema k 12. In Theo em 8.1, we ha e disc e ized he se o con ols, bu he s a e
equa ion is di ec ly sol ed. I will be in e es ing o s udy he con e gence when we also
disc e ize his equa ion, and in pa icula o s udy wha he ela ion is ha we mus use
be ween he iangula ion chosen o he con ols and he one chosen o he esolu ion o
he s a e equa ion. A esul in his sense can be ound in [8], showing ha in some cases
he me hod con e ges using he same iangula ion o disc e ize he con ols and he
s a e equa ion.
Acknowledgmen . The au ho s a e g a e ul o he Basque Cen e o Applied
Ma hema ics o i s hospi ali y and suppo in se e al isi s.
REFERENCES
[1] G. ALLAIRE,Shape Op imiza ion by he Homogeniza ion Me hod, Appl. Ma h. Sci. 146, Sp inge -Ve lag,
New Yo k, 2002.
[2] G. ALLAIRE AND S. GUTIÉRREZ,Op imal design in small ampli ude homogeniza ion, ESAIM Ma h. Model.
Nume . Anal., 41 (2007), pp. 543–574.
[3] J. C. BELLIDO AND P. PEDREGAL,Explici quasicon exi ica ion o some cos unc ionals depending on
de i a i es o he s a e in op imal designing, Disc e e Con in. Dyn. Sys ., 8 (2002), pp. 967–982.
[4] B. BOURDIN,Fil e s in opology op imiza ion, In e na . J. Nume . Me hods Eng g., 50 (2001),
pp. 2143–2158.
[5] C. CARSTENSEN AND C. ORTHNER,Analysis o a class o penal y me hods o compu ing singula minimize s,
Compu . Me hods Appl. Ma h., 10 (2010), pp. 137–163.
[6] J. CASADO-DÍAZ,J.COUCE-CALVO,AND J. D. MARTÍN-GÓMEZ,Relaxa ion o a con ol p oblem in he coe i-
cien s wi h a unc ional o quad a ic g ow h in he g adien , SIAM J. Con ol Op im., 47 (2008),
pp. 1428–1459.
[7] J. CASADO-DÍAZ,J.COUCE-CALVO,AND J. D. MARTÍN-GÓMEZ,Relaxa ion o op imal design p oblems wi h
nonlinea unc ionals in he g adien , o appea .
[8] J. CASADO-DÍAZ,J.COUCE-CALVO,M.LUNA-LAYNEZ,AND J. D. MARTÍN-GÓMEZ,Op imal design
p oblems o a non-linea cos in he g adien : Nume ical esul s, Appl. Anal., 87 (2008),
pp. 1461–1487.
[9] J. CASADO-DÍAZ,J.COUCE-CALVO,M.LUNA-LAYNEZ,AND J. D. MARTÍN-GÓMEZ,Disc e iza ion o coe icien
con ol p oblems wi h a nonlinea cos in he g adien , in In eg al Me hods in Science and
Enginee ing, Compu a ional Me hods 2, C. Cons anda and M. E. Pé ez, eds., Bi khäuse , Bos on,
2010, pp. 55–63.
[10] D. CHENAIS AND E. ZUAZUA,Fini e elemen app oxima ion o 2D ellip ic op imal design, J. Ma h. Pu es
Appl. (9), 85 (2006), pp. 225–249.
[11] Y. GRABOVSKY,Op imal design o wo-phase conduc ing composi es wi h weakly discon inuous objec i e
unc ionals, Ad . in Appl. Ma h., 27 (2001), pp. 683–704.
[12] R. LIPTON AND A. P. VELO,Op imal design o g adien ields wi h applica ions o elec os a ics,in
Nonlinea Pa ial Di e en ial Equa ions and Thei Applica ions, Collège de F ance Semina
XIV, D. Cio anescu and J. L. Lions, eds., S ud. Ma h. Appl. 31, No h-Holland, Ams e dam,
2002, pp. 509–532.
[13] K. A. LURIE,Applied Op imal Con ol Theo y o Dis ibu ed Sys ems, Plenum P ess, New Yo k,
1993.
[14] K. A. LURIE AND A. V. CHERKAEV,Exac es ima es o he conduc i i y o a bina y mix u e o iso opic
ma e ials, P oc. Roy. Soc. Edinbu gh Sec . A, 104 (1986), pp. 21–38.
[15] F. MURAT,Un con e-example pou le p oblème du con ôle dans les coe icien s, C. R. Ma h. Acad. Sci.
Pa is, 273 (1971), pp. 708–711.
[16] F. MURAT,Théo èmes de non exis ence pou des p oblèmes de con ôle dans les coe icien s, C. R. Ma h.
Acad. Sci. Pa is, 274 (1972), pp. 395–398.
[17] F. MURAT AND L. TARTAR,H-con e gence, in Topics in he Ma hema ical Modelling o Composi e
Ma e ials, P og . Nonlinea Di e en ial Equa ions Appl. 31, L. Che kae and R. V. Kohn, eds.,
Bi khäuse , Bos on, 1998, pp. 21–43.
[18] P. PEDREGAL,Op imal design in wo-dimensional conduc i i y o a gene al cos depending on he ield,
A ch. Ra ion. Mech. Anal., 182 (2006), pp. 367–385.
APPROXIMATION OF AN OPTIMAL DESIGN PROBLEM 1215
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
[19] S. SPAGNOLO,Sulla con e genza di soluzioni di equazioni pa aboliche ed elli iche, Ann. Sc. No m. Supe .
Pisa Cl. Sci. (5), 22 (1968), pp. 571–597.
[20] L. TARTAR,P oblèmes de con ôle des coe icien s dan des équa ions aux dé i ées pa ielles, in Con ol
Theo y, Nume ical Me hods and Compu e Sys ems Modelling, Lec u es No es in Econ. and Ma h.
Sys ems 10, Sp inge -Ve lag, Be lin, 1975. English ansla ion: F. MURAT AND L. TARTAR,On he
con ol o coe icien s in pa ial di e en ial equa ions, in Topics in he Ma hema ical Modelling
o Composi e Ma e ials, P og . Nonlinea Di e en ial Equa ions Appl. 31, L. Che kae
and R. V. Kohn, eds., Bi khäuse , Bos on, 1998, pp. 1–8.
[21] L. TARTAR,Cou s Pecco , Collège de F ance, 1977, pa ly w i en in [17].
[22] L. TARTAR,Es ima ions ines de coe icien s homogénéisés, in Ennio de Gio gi Colloquium (Pa is 1983),
Res. No es Ma h. 125, P. K ee, ed., Pi man, London, 1985, pp. 168–187.
[23] L. TARTAR,Rema ks on op imal design p oblems, in Calculus o Va ia ions, Homogeniza ion and
Con inuum Mechanics, Se . Ad . Ma h. Appl. Sci. 18, G. Bu azzo, G. Bouchi e, and P. Suque ,
eds., Wo ld Scien i ic, Hackensack, NJ, 1994, pp. 279–296.
[24] L. TARTAR,An in oduc ion o he homogeniza ion me hod in op imal design, in Op imal Shape Design,
Lec u e No es in Ma h. 1740, A. Cellina and A. O nelas, eds., Sp inge -Ve lag, Be lin, 2000,
pp. 47–156.
[25] V. V. ZHIKOV,Weigh ed Sobole spaces, Sb. Ma h., 189 (1998), pp. 1139–1170.
[26] J. GOODMAN,R.V.KOHN,AND L. REYNA,Nume ical s udy o a elaxed a ia ional p oblem om op imal
design, Compu . Me hods Appl. Mech. Eng g., 57 (1986), pp. 107–127.
1216 CASADO-DÍAZ, CASTRO, LUNA-LAYNEZ, ZUAZUA
Copy igh ©by SIAM. Unau ho ized ep oduc ion o his a icle is p ohibi ed.
Rep oduced wi h pe mission o he copy igh owne . Fu he ep oduc ion p ohibi ed wi hou
pe mission.