A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
J. N E ˇ CAS J. S TARÁ R. Š VARC
Classical solution to a second order nonlinear elliptic system in R
3Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4
esérie, tome 5, n
o4 (1978), p. 605-631
<http://www.numdam.org/item?id=ASNSP_1978_4_5_4_605_0>
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Nonlinear Elliptic System in R3.
J.
NE010DAS (*) -
J.STARÁ (**) -
R.0160VARC (*)
dedicated to Jean
Leray
The paper is concerned with the
regularity properties
of weak solu- tions of a Dirichletboundary
valueproblem
for anelliptic
nonlinearsystem
of second order. It is well known that there exists a
unique
solution of thegiven problem
under suitable conditions on coefficients but this solution need be nor bounded nor continuous even if the coefficients areanalytic
functions
(see
J. L. Lions[1],
Ch. B.Morrey [2],
E.Giusti,
M. Miranda[3],
J. V. G.
Mazja [5]).
In this paper we shall consider coefficients defined
only
on a subset J~fof
Ram.
Similarproblem
arised instudying
the existence of solution in thetheory
ofhyperelasticity (see
J. Ne6as[4]).
The coefficientssatisfying
thecondition of
ellipticity
nonnecessarily uniformly
will besupposed
and theexistence of classical solution will be
proved
in thefollowing (briefly
andnon-exactly said)
sense: if ic is a classical solution of thegiven problem
with the
right-hand
sidei
and theboundary
conditionfo
and if weprescribe
a continuous
path
ofright-hand
andboundary
conditionsbeginning
inf and ico
then there areonly
twopossibilities:
eitherthere exists a continuous
path
ofregular
solutions on the whole(0, T)
orthere is a critical value
T)
where thepath
of solutionsends;
inthis case the
gradient Vu(t)
tends to theboundary
of .~ or to thepoint
where the
ellipticity
conditionsdegenerates
or the norms11 u
ast --~ to .
In the first
part-i 2-apriori
estimates will beproved.
If thegiven equation
is considered as Euler’sequation
of a functional0,
it ispossible
(*) Matematicko-fyzikální
fakulta UK, Malostransk6nim6sti,
Praha 1.(**) Matematicko-fyzikalni
fakulta UK,Sokolovska,
Praha 8.Pervenuto alla Redazione il 28
Giugno
1977.to say that the
apriori
estimates are based on the local behaviour of the fourth G,4teaux differentialof
0.In the second
part"§
3-regularity
results areproved by
means ofimplicit
function theorem.All the results are formulated for two
types
of domains-a bounded domain with aninfinitely
smoothboundary
and ahalf-space.
Theproof
of the
apriori
estimate for a half spaceis simpler
and showsclearly
itsbasic idea but the second
part (the implicit
functiontheorem) brings
somecomplications
causedby
the nonexistence ofcompact embeddings.
For abounded domain the
proofs
in the secondpart
are the standard ones and theproof
of theapriori
estimate isanalogous
to that for a half space, buta lot of difficulties is caused
by using
the suitablepartition
ofunity
andcomplicated
test functions.We shall consider
systems
of second order with coefficientsdependent only
on the
gradient
Vu.1. -
Notation.Let SZ be a domain in
B3
with aninfinitely
smoothboundary
and Mbe a domain in
Ram containing
theorigin.
Let us denoteby x
=(x,,
x2,x.,)
(respectively $ =
=1, 2, 3; r = 1, ... , m~
ageneric point
ofRa (re- spectively
with the normis the space of all functions with continuous and bounded first derivatives on S~ such that all these first derivatives can be
continuously
extended on
S2.
On the Cartesianproduct [Ol(Q)]3m
apseudonorm
will
be used.For a
bounded
domain Q we shall denoteby
or[1~’2(S~)]m
theusual Sobolev spaces with the norms
and
Let us remind that the norms
Ilullk.2
and1I’U11.2 ard equivalent
on thespace
W2.
0For Q
= Ri
= X3 >0 )
we shall denoteby [T~Y’2(.R3 )~m
the com-pletion
ofinfinitely
smooth functions withcompact support
inR3
withrespect
to the normBy ~~2’~R3 )~"Z
we shall denote thecompletion
of the space ofinfinitely
smooth functions with
compact support
inRi
withrespect
to the norm(respectively [~(-?3~)
is acompletion
of the space of all infi-nitely
smooth functions withcompact support
inR;
withrespect
to thenorm
(respectively ~~.2)’
Let F be a four times
continuously
differentiable real function definedon M and let us denote
Let we shall write
and denote the
graph
of thegradient by
We shall deal
with
theregularity properties
of a weak solution of aDirichlet
problem
for asystem
of the formBy
the weak solutiono f
thisproblem
we shall understand a vectorfunction
u E such that
(ii)
theequality
for
every2. -
Apriori
estimates..A. Estimate8 on
half -space.
In this
part
of Section 2 the domainwill be considered.
2.1. Let R be a
positive
number with thefollowing properties : (i)
(ii)
there existf unctions
800k
that, for
every we haveThen there exists a continuous
f unction
D :(0, .R) -~ (0, -[- oo)
such thatfor
every U EI W2 "(R’) 3
t1*2"(R+)]-, 3
which solves theequation (1.2)
with uo =0,
f
E[ W2(1~3 )]3’~
andsatis f ies
theinequality
the
inequality
holds.
PROOF.
Roughly
said the derivatives in the directions of the axis xl, x2 will be estimatedby choosing
suitable testfunctions,
then the normal deri- vative will be calculated from theequation.
Let us
fix e
E(0,
and deal with the terms with the first and second derivatives at first.The condition
(2.1) (ii) together
with = 0implies
Putting (1.2)
andusing (2.3),
weget
Let w’ denote the derivative of a function w in the
tangential
direc-tion, i.e.,
in the direction of one of the axes ri, x2. Let usand
put q; = 1p"
in(1.2). Integrating by parts
weget
and, putting again
= ~,Under the
assumption
on the function u theequation (1.2)
can be written on Q in the formfor
r = 1, - - ., m.
The matrix(b33)
isregular
with auniformly
boundedinverse and we can estimate
by
means of(2.6).
ThusLet us now
put q = 1p""
for the same function in theequation (1.2). Integrating
once moreby part,
we obtainLet us and consider the second
integral
on the left-hand side of(2.9). Integrating by parts
for the thirdtime,
we obtainbut the last
integral
is not less thanUsing
thedensity
of in the spaceW2(.R3 ),
we caneasily
provea
special
case of L.Nirenberg’s interpolation inequality.
2.2. LF,31MA. Let W E be ac bounded
f unction
onRN .
Then 2v’ EE and
(w’
has the samemeaning
as in theforegoing proof, i.e.,
the derivativeof w in any of the directions Xl’
...~~i).
Now we can estimate the first
integral
in(2.9) by (ii),
the secondintegral by (2.11), (2.12) (applied
to every function and(iv),
the third inte-gral by
Holder’sinequality.
Thus we havewhich
according
to(2.1) (iii) gives
an estimate for thetangential
deriva-tives in the form
The next
step
is the estimate of the derivatives of the formwhere
i, j
=1, 2,
and itimmediately
follows from2.3. Lr,,mlVIA. There exists a
positive
constant 0 such thatfor
everyfunc-
tion w E the
inequality
holds.
The
proof
of this lemma is an easy consequence of the Plancherel’s theoremapplied
to the function wprolonged
on the whole spaceJ~.
Thus
Let at least one of the
indices i, j
be less than 3. Thenaccording
toLemma
2.2,
The
L4-norm
ofa’ulax’ ,
can be calculated from thesystem (2.7)
as before.Differentiating
once more in(2.7)
in atangential direction,
weget
theequality
All the terms on the
right-hand
side areL2-functions
and the matrix(b33~
has a
uniformly
boundedinverse;
thereforeIf now ~/=
owjox3
in(2.17)
we canrepeat
all theprocedures
with the(2.18)
estimate instead of(2.16)
and weget
a bound for in the formwhich
together
with(2.18), (2.4),
and(2.8) accomplishes
theproof.
The
following
lemma deals with the sametype
of anapriori
estimate asLemma
2.I ;
we suppose there that u is a solution of anon-homogeneous
Dirichlet
boundary
valueproblem
and that it lies in aneighbourhood
of asmooth function ~.
2.4. LEMMA. and Let R be a
positive
number with the
following properties : (ii)
there existfunctions
such
that, for
every(iii) for
every ~o E(0, R), 3d(e) e2 c(~o).
Then there exists a continuousfunction
D :(0, B) -* (0, oo)
suchthat, for
every which solves theequation (1.2)
with theboundary
value u,, E[ W2~ (I~3 )]m
and theright-hand
side
f
E[ 1~2(.R3 )]3m
andsatisfies
theinequality
the estimate
holds.
PROOF.
Repeating
the firstpart
of theproof
of Lemma 2.1 with the test function u - uo insteadof u,
we obtain theinequality
The first difference is caused
by
the fact that theequality (2.10)
does nothold in such a
simple
form.Integrating by parts
in the secondintegral
in
(2.9),
y we obtainNow ’U - Uo
can be written in theequality
insteadof 99
andwhere
Substituting
y = u - uo into(2.9)
andusing (2.24)
and(ii),
we obtainIn this case
Nirenberg’s
lemma will be used for the function v = u - ~.Thus for every
positive E
weget
By
means ofNirenberg’s
lemma and the Fourier transform weget
thecontinuous
embedding
of the spaceW2 (R’)
into and thusUsing (2.26)
in theinequality (2.25),
we havewhere Z contains the terms on the
right-hand
side of(2.25)
and the second term on theright
hand side of(2.26).
The derivatives of the coefficientsb~!
areuniformly
bounded on9.
and we can estimate theright-hand
sideof
(2.25) by
Further,
y in virtue of(2.26),
In order to
get
a bound for11’1/," 11~12
we shall use asimple algebraic
lemma :2.5. LEMMA. Let a,, ..., an be
nonnegative
realnumbers,
Thenthe
inequality
implies
Choosing
asufficiently small 8,
I we obtainThe rest of the
proof
isquite analogous
to that of Lemma 2.1.B. Bounded domain
Q.
In the next
lemma,
S2 will be a bounded domain with aninfinitely
smooth
boundary
in Therequired
smoothness of theboundary
can bedescribed as follows:
The
boundary
8Q is described in aneighbourhood
of everypoint by
aninfinitely
differentiable function r which is defined on a ballin the
corresponding
coordinatesystem.
Theboundary
is coveredby
afinite number P of such
system, i.e.,
for every x E 8Q there exists a coordi- natesystem
in which x =(Xl’
X2,Ti(x,, X2)).
Let us supposefor
every i
=1,
..., P and a suitable or > 0. Let us add a domainVo
with aninfinitely
smoothboundary
and such thatLet be a
partition
ofunity corresponding
to thesystem i. e. ,
the
functions y (for i = 1, ..., P)
areinfinitely
differentiable and suppV~
U{.c
=(x’, ~i(x’ )) ;
x’ for i= 1~
... , P.Moreover,
allyQ
arenonnegative
andThe form of the
apriori
estimate for a bounded domain isquite
analo-gous to that for a half space. We include it for
completeness
andpoint
outthe different
part
in theproof.
2.6. LEMMA. Let’ 11 E
[ W2(S~)~m
and c Let R be apositive
numberswith the
following properties :
(ii)
there existfunctions
such
that, for
every.Then there exists a continuous
f unction
D :(0, R) -~ (0, -f- oo)
such thatfor
every u E which solves theequation ( 1.2 )
with theboundary
valueuo E
[ -W’(S2)]-
and theright-hand
sidef
E[W2(S2)] 3-
andsatisfies
the condition the estimateholes.
PROOF.
Apriori
estimate onYQ
will be obtainedby choosing
a suitabletest function of the form a
sufficiently large
K. Further we can transform the consideredpart
ofTTQ
into ahalf-space
and use the methods ofprevious
lemma.With
respect
to theequivalence
of the norms in the spaceW2(S~),
itis sufficient to bound the
highest
derivatives of u. The index Q will be fixedthroughout
theproof
and will be omitted.PART I. Estimates on VI.
Substituting
the testfunction 99
=(yO)2K.U
into(2.9),
we can dividethe left hand side into two
parts,
onepart containing
thehighest
deriva-tives of u and the second one with the derivatives of non-zero order of
(y°)2x.
The
symbol
w’ denotes here the first derivative of the function w in any direction. Thus _where
Z2
consists of the terms of the formand
Z3
contains theexpressions
with
1 n , 1 , .. n
Using
theequality (2.23)
for thisspecial
caseof 99
=(yl)2K.U,
we havethat the second
integral
in(2.35) equals
where
Z,
contains theexpressions
and Z5
theexpressions
where
and(2.36),
we obtain.
According
to(2.33) (ii), (2.35),
andTo follow the method of the
proof
of Lemma 2.1 we have to overcome twotechnical difficulties. In the first
step
we mustreplace by v
= îi - uin order to
get sharp estimates,
y butNirenberg’s
lemma cannot be useddirectly
for the function because the powers ofy°
on theleft-hand side of
(2.37)
would not agree. We shall use thefollowing
modi-fication :
2.7. LEMMA. Let w be a bounded measurable
fonction
on a domainj
be apositive integer
less than orequal
to N.Suppose
that the derivativesexist in a weak sense and are square
integrable.
ILet 1p
ED(Q)
be a nonnega- tivef unetion.
I Then "1p EL4(Q)
andThe lemma can be
proved by
means of thesimple integration by parts
and the Holder’s
inequality.
If we
apply
Lemma 2.7 to the functions simulta-neously,
y we shall obtainHere
Z6
contains the termswith ,
Z7
contains theexpressions
and
Z.
the difference between the left-hand side of(2.37)
and the sameexpressions
with v instead of u.Returning
to the solution u on the left-hand side of(2.38),
weget
another additional term which can be included intoZg .
We shall now estimate
Zi by
means ofto the power less than 2 and the norms of
f, u,
1. Let us recall thatand
The function and the
equivalence
of the norms inthis space
implies
that there exists a constant C so thatand
we
get
forK>4To bound the
integrals
I andJn
we shall use thefollowing inequalities (which
can beproved integrating by parts)
and Lemma 2.5.2.8. LEMMA. Let h E
W2(S~)
be boundedby
a constant M and y ED(Q).
Then there exists a constant 0
depending only
on y and Q so thatand
40 - Annali della Scuota Norm. Sup. di Pisa
Putting ;
" we obtainand with
respect
to(2.38), (2.40)
and Lemma 2.5 weget finally
and
PART 2. Estimates on Vi.
Let us fix an index i =
1,
..., P and consider thecorresponding
coordi-nate
system.
Let x =Ø(x)
be the coordinates of apoint x
ERa
in thissystem.
We shall transform the set Vi into apart
of ahalf-space. Let y
be a
mapping
and z = Then the absolute value of Jacobi’s determinant
of x
isidentically equal
to 1. Let us writeLet us define
If we consider the test function in the
equality (1.2)
andwrite u =
uoX-1,
we can conclude that u solves theequation
of the formanalogous
to(1.2)
and theinteresting part
of theboundary 8£5
isa
part
of aplane. Especially
weget
that forNow the coefficients
ak satisfy
the conditions(2.33) (ii)
with the same con-stants
e(e)
and on theequally
transformed balls9,.
If we writeyi =
andKo = uooX-1
we shallrepeat
theproof
of Lemma 2.4choosing
the test
function = ()(2013 o)’ Combining
the estimates of Lemma 2.4 and2.6,
weget
and
using
theequivalence
of the norms, we haveAn additional term with the derivatives
2dlaxi
does not cause any diffi-culty
as areinfinitely
smooth functions. The functionsbelong
toL,(D) according
toNirenberg’s
lemma for all theindices k, j
such that k
+ j
5. The second derivative of K withrespect
tox3
can be calculateddirectly
from theequation
as in theproof
of Lemma 2.4.By
the same method the last third derivatives can be estimated. Thus we
get
the
inequality
Returning
to theoriginal
coordinatesystem,
we obtain the estimates for the solution u on the set Vi andsumming
these estimates for i =0, 1,..., P,
we
get
3. - Main theorem.
The main theorem will be
proved by
means of theimplicit
functiontheorem and the
apriori
estimates of the lastparagraph.
In this
part
thesymbol
Q denotes thehalf-space Rg
or a boundeddomain with a smooth
boundary,
ysimultaneously.
3.1. THEOREM. Let U E
[ W2 ~ (.~ )]m
be a solutiono f
theequation (1.2)
cor-responding
to theright-hand side i E [,W2(0)]"
and theboundary
conditionilo
E us suppose that there exists apositive
number Rsatisfying
the conditions
(2.33) of
Lemma 2.6.Then
for
every e E(0, R)
there existpositive
numbers8, 6
sothat, for
eachand
there exists a
unique
solutionof
theequations (1.2) corresponding
to theright
hand sidef
and theboundary
condition UO.
If
we denoteby
G themapping of Ua( f )
XU.5(ilo)
intoUe(u)
suchthat
G(f, uo)
= u, then G is a continuousmapping from
PROOF. Let us
put
with the
topology
ofand let us define the in the
following
manner:where
The assertion of the Theorem 3.1 is an immediate consequence of the
implicit
function theoremapplied
to themapping
0. Toverify
the assump- tion of theimplicit
functiontheorem
we shall need anembedding
theoremof this
type:
and,
moreover,These theorems are well known
(see
J. Necas[6])
for a bounded domain Qwith a smooth
boundary.
For the case S~= RI
the firstinequality
can beproved by
means of Fourier transform and the second one is a consequenceof
(3.1)
and Lemma 2.2.’ Thus @ is an open subset of the Cartesian
product
Y x X andThe convergence of and in
~~W2’(S~)~m implies
the uniform con-vergence of their
gradients
andtogether
with thecontinuity
ofb~3
itgives
the
continuity
of themapping 0
on C~i.Let us prove that the
partial
differential~2
exists on Ci and it is a continuousmapping
of @ into the space of all continuous linearmappings
of X into Z. The above mentioned
embedding
theoremimplies
that theexpression
belongs
to thespace Z
for everyciently
near tou*,
Let us
write,
y for u suffl-Every component
of H is a sum of theexpressions
of thetype
After easy calculations
(the
mean valuetheorem)
weget
where 7: is a measurable vector function with
17:1 1.
Now the termin the brackets is of the order The norm
can
be estimatedquite analogously.
Let us prove the
continuity
ofø~.
Let~( f~,
uon,u,~)~,~ 1
be a sequence in 0152tending
to(f, uo, u)
andput
and
We
get immediately
But the convergence
of 1 implies
that 0 and thusAnalogously
weget
theinequality
and it
gives
therequired
result.The most
important part
of theproof
is that02(j, uo, u)
is a continuousone-to-one
mapping
of.
(v )
=0,
thenon S~ for r =
1,
..., m.Multiplying
everyequation by vr, integrating by parts
overQ,
andusing (2.33) (ii),
weget
and it
implies
that v = 0.In the next
part
we shall prove anapriori
estimate for a linearpartial
differential
equation
with continuous coefficientssaying
in fact that[Ø~]-l
is a continuousmapping
from Z in X. Such estimates can be obtainedby
themultiple
use ofregularity
theorems for linear differentialequations (see [7]).
We shall prove it here for com-pleteness by
a methodanalogous
to theproof
of Lemma 2.4. For a boundeddomain Q we shall use the
complete continuity
of theembedding
of thespace
W2(S~)
intoO(Q)
andW~(.Q)
intoL4(Q).
For ahalf-space
such anassertion does not hold and we
replace
itby
3.2. LEMMA. Let 8 be a
positive
real number. Then there exists a con-stant
C(8)
so eachPROOF.
Let g
be an extension of h on the whole spaceRa.
If wedenote
by ’
the Fourier transform of the function g, thenUsing
the Holder’sinequality
weget
for eachpositive
the relationThe second
integral
on the left-hand sideequals
to~r~-4. Using
Minkowski’sinequality
for the firstintegral
on the left-hand side of(3.10),
weget
We can choose the
function g
so that there exists a constant C’ so thatand
and it
gives, together
with(3.9)
and(3.11 ),
theinequality (3.7).
The ine-quality (3.8)
is an easy consequence of(3.7)
and Lemma 2.2.Let us now return to the
proof
of the Theorem 3.1. Let andand 99
EMultiplying
gby q
andintegrating by parts
weget
The condition
(2.33) (ii)
and theLax-Milgram
theoremgive
We shall
repeat
theprocedure
of theproofs
of Lemma2.4, respectively
2.6.Let D and let us
take cp = ’IjJ" for y
E(Here again y’ = ayaxi
for
i = 1, 2.) Integrating by parts
in(3.13),
we obtain theequality
Putting V
= v andusing (2.33) (ii)
and(3.8),
weget
The derivatives can be calculated from the
equation (3.12).
Letnow where y E and let us
integrate
once moreby parts
in(3.15). Putting x
= v andusing (2.33) (ii), (3.8)
and(3.7),
we shallhave
By
standard means we estimate the last third derivatives andget,
forsufficiently small E,
If Q is a bounded domain we have to return to the
partition
ofunity
andthe test functions as in the
proof
of Lemma 2.6 butbasically
theproof
remains without
changes.
Lemma 3.2 will bereplaced by
J. L. Lion’s lemma for spaces with thecompletely
continuousembedding
The
equality 0’(X)
= Z will beproved by
thehomotopy
method. Letus define
for every
t c- 0, 1> - At
is a one-to-one continuous linearmapping
of Xinto Z. It is well known that
Ao(X )
= Z. LetQ
be maximum of the con-stant C of
(3.18)
and the norm of themapping
Let usput
Then is a closed subset of
{v,.,}
is a bounded sequence in the Hilbertspace X
and thus there existsa
subsequence (let
us denote itby fv"}, too)
and an element v E X so that convergesweakly
to v. Theembedding inequalities imply
thatin Z and thus
According
to(3.21),
and is an open subset in
~0, 1~ :
Letg E Z,
Let us define a
mapping
B: X -> X in thefollowing
manner:!~2013~o!!3.2~}’
Let us prove that themapping B
has afixed
point
in ? for asufficiently
smallIt - tol.
But ? isweakly compact
and B is
weakly
continuous.Moreover,
where
, and
with ~S that
depends
on and does notdepend
on v and t. There exists apositive
s(it
does notdepend
ong)
sothat,
forIt - tol
E,B(St)
and B has a fixedpoint
v but such a function solves theequation A,(v)
= g.3.3. THEOREM. Let U E
[W~‘(S2)]m
be the solutionof
theequation (1. 2) corresponding
to theright-hand
side and theboundary
vaclu eU E
[ -W3’ (92)]’.
Let us suppose that there exists apositive
number R sactis -fying
the condition(2.33) o f
.Lemmac 2.6. Let F be ac continuousmapping of o, T)
into Y such thatF(O)
=[1, uoJ.
Then there exists aunique
contin-uous
mapping
Uof
Si) c~0, T)
into X so thatU(t)
solves(1.2)
with theright-hand
sidef (t)
and theboundary
condition
uo(t)
such that[f(t), uo(t)]
=F(t) for
every t c- Z .Moreover there are
only
twopossibilities of
theshape of
the domain ~J : either Z =0, T)
or there exists a critical valueto
> 0 80 that0, to )
andPROOF. Theorem 3.1
implies immediately
that the domain of therequired
« solutionpath >>
is open.Clearly
0 E ~. Let us consider the com-ponent ~1
of Dcontaining
thepoint
0. If =~0, T)
then the con-tinuity
of U follows from Theorem 3.1. Let0, T)
and let usput
~1
=o, to).
It remains to prove the condition(3.24).
Lettn
E0, to),
and
Then c
KR-r¡/2
for asufficiently large
n, andusing
thecontinuity
of F at the
point to
and Lemma 2.4 or2.6,
weget
the boundfor all
sufficiently large
n.According
to the weakcompactness
of a ballin
X,
there exists asubsequence {U(t.,,)l
and a function u E X so thatconverges
weakly
to u inBy
the usuallimiting
processwe
get
that u solves theequation (1.2)
with theright-hand
sidef (to )
andthe
boundary
conditionuo(to)
and theuniqueness implies
that u =U(to).
With
respect
to Theorem 3.1 weget
the continuation of U on the intervalto, + e),
which is a contradiction with theassumption
on the domain 3.4. THEOREM..Let M =R,
let Ù E[ W2~ (S~)]m
be the solutionof
theequation (1.2) corresponding
to theright-hand
sidef
E and theboundary
valueÙo
E us s2cppose that there exists a continuousf unction
c:0, -~- oo)
so thatfor
all71, ~
ERam
theinequality
holds.
Let F be a continuous
mapping of 0, T)
into Y such thatF(O)
=[1,
Then there exists a continuous
mapping
Uof 0, T ~
into X so that(3.26) U(t)
solves theequation (1.2)
with theright-hand
sidef(t)
and theboundary
value such that[ f (t), uo(t)]
=F(t) for
every tMoreover,
there areonly
twopossibilities of
theshape of
the domain ’Z:either
0, T)
or there exist8 a criticalpoint to
> 0 so that~0, to)
andPROOF. Let
~1
andto
be defined as in theproof
of Theorem 3.3. LetThen we can choose a sequence and a so that
U (tn)
2013~in
[ W2’ (S)’. According
to theembedding theorems, U
solves the equa-tion with the
right-hand
sidef (to)
and theboundary
valueuo(to)
so thatwe can define
U(to)
= u. Ifto
= T orthe
proof
iscompleted.
Let andThen there exists a
neighbourhood -~- KR
ofV U(to)~
so that allthe
assumptions
of Theorem 3.1 are satisfied and U is defined on0, to -~- 8),
which is a contradiction with theassumption
on3.5. THEOREM. Let U E
[ W2’ (SZ)]~‘
be the solutionof
theequation (1.2) corresponding
to theright-hand
sidei E [W,2(Q)]"
and theboundary
valueilo
E[ W2’ (S)]’.
Let us suppose that there exists a continuousfunction
c : M -->-
0, -- 00)
so thatfor
all 71 E E M theinequality
holds.
Let F be a continuous
mapping of 0, T)
into Y such thatF(O) = [1, uo].
Then there exists a continuous
mapping
Uof
t¡) c0, T)
into X so thatU(t)
solves theequation (1.2)
with theright-hand
sidef(t)
and theboundary
value
uo(t) (where F(t)
=[ f (t), u,,(t)]) .for
every t E 1).Moreover,
there areonly
twopossibilities of
theshape of
theeither ~ _
0, T)
or there exists a critical valueto
E0, .~’~
so that ~ c0, to)
andThe
proof
isquite analogous
to theproof
of Theorem 3.4.REFERENCES
[1]
J. L.LIONS, Quelques
méthodes de résolution desproblèmes
aux limites non linéai-res,
Dunod,
Paris, 1969(Russian
transl.:Nekotoryje metody reshenija nelinejnych
krajevych
zadac,Mir, Moscow, 1972).
[2]
CH. B. MORREY Jr.,Multiple integrals
in the calculusof
variations,Springer,
Berlin, 1966.[3]
E. GIUSTI - M. MIRANDA, Unesempio
di soluzioni discontinue per unproblema
di minimo relativo ad un
integrale regolare
del calcolo delle variazioni, Boll. Un.Mat. Ital. (4) 2 (1968), pp. 1-8.
[4] J. NE010DAS,
Example of
anirregular
solution to a nonlinearelliptic
system withanalytic coefficients
and conditionsfor regularity,
to appear inBeiträge
Anal. (1977).[5]
V. G. MAZJA,Primery neregularnych reshenij kvazilinejnych ellipticeskich
urav-nenij
s analiticeskimikoeficientami, Funkcional’nyj
Analiz, 2 (1968), vyp. 3.[6]
J. NE010DAS, Les méthodes directes en théorie deséquations elliptiques,
Academia,Prague,
1967.[7] S. AGMON - A. DOUGLIS - J. NIRENBERG, Estimates near