Nonlinear Analysis, Theory, Printed in Great Britain.
Methods
& Applicalrons,
Vol.
18. No.
I, pp. 9-16,
1992 0
0362-546X192 165.00+ SM 1991 Pergan0n Press plc
ESTIMATES FOR GENERALIZED SUBSOLUTIONS OF FIRST ORDER HAMILTON-JACOBI EQUATIONS AND REARRANGEMENTS ESTERGIARRUSSO Istituto di Matematica, Facolta di Scienze Matematiche, Fisiche e Naturali, UniversiG di Salerno, 84081 Baronissi (SA), Italy (Received
20 September
Key words and phrases:
1990; received
for publication 13 March 1991)
Hamilton-Jacobi
equations, rearrangements.
1. INTRODUCTION THIS WORK
concerns the Dirichlet problem for the first order Hamilton-Jacobi
equation
a.e. in Q; u = 0 on asz
Lu = 1vu1 + c(x)24 = f(x)
(1.1)
where Vu = (uX,, . . . . u,,), and ~2 is an open subset of IR”whose measure is finite. Hamilton-Jacobi equations have been studied by many authors, who investigated the existence, the uniqueness, and the stability of the solutions [7, 8, 191. Herein we employ the properties of the rearrangement of functions and isoperimetric inequalities to get comparison theorems in Lp with p = 1 or 00. In fact, denoted by U(X) a nonnegative generalized subsolution of (1 .l), by C2*the ball of lR” centered at the origin and with the same measure as Q and by (c+), and (cm)* respectively, the spherically symmetric increasing and decreasing rearrangement of the functions c+(x) = max(c(x), 0) and c-(x) = max( -c(x), 01, we consider the symmetrized operator L*w = /VW1 + ((c+)* -
and first we show that
w E wy(a*),
(c-)*)w,
Ibll, 5 I141m*
where w(x) is the decreasing spherically symmetric solution of L*w = g(x)
a.e. in CP,
w = 0 on X2*.
Above g(x) = g( Ix]) is a spherically symmetric rearrangement of f(x), which depends also on the distribution functions of c+(x) and c-(x). In particular cases (e.g. if c(x) L 0), g(x) = f*(x) (see theorem 3.1 and following remarks). Moreover, if c(x) = A = const., we show that and q(x) and o(x) being the decreasing spherically symmetric solutions respectively of L*q = IVql + Aq = f*(x)
a.e. in sZ*,
and L*w = h(x)
a.e. in a*,
w E w;*‘(a*); 9
q E w~J
10
E. GLUWJSSO
here h(x) = h(lx() is a spherically symmetric rearrangement of f(x) which depends on A. In particular cases, h(x) is equal to f*(x), e.g. if 1 I 0 (see theorem 3.2 and following remarks). This paper is understood to be a continuation of the previous ones [14, 151where the case c(x) equal to a nonpositive constant was considered. Schwartz symmetrization has been employed lately to investigate second order linear and nonlinear elliptic and parabolic problems (see for example [l-5, 10, 11, 13, 16, 23-271). 2. KNOWN
FACTS ABOUT THE REARRANGEMENTS
OF A FUNCTION
Let u(x), x E Sz C_R”, be a real valued measurable function and let p(t) = 1(x E Sz : IuI > t)l distribution function. A rearrangement of U(X) is a function g(y), y E IV, equidistributed with u(x), then if U(X)E Lp(sZ), any rearrangement of U(X)has the same LP-norm as u(x). As known, the right-continuous function
be its
U*(s) = suplt 1 0 : p(t) > s], is the decreasing rearrangement
SZO
of u(x), and U*(x) = u*(c,lxl”),
XE rn”
is the spherically symmetric decreasing rearrangement Here and below
of u(x).
n/2 en=
=
r(1 + n/2)
is the measure of the unit n-dimensional ball. Furthermore U*(S) = u*(IQzJ - s) and are the
u*(x) =
~*WnlXl”)
increasing and spherically symmetric increasing rearrangements
of u(x), respectively.
THEOREM 2.1 (cf. [17]). If u(x) and v(x) are measurable, then
s THEOREM
2.2 (cf. [22], Polya-Szego
principle). If u E Wd*p(CQand p 2 1, then
This theorem implies the absolute continuity of u*(s) in [a, Ial], with (I > 0, when U E w;*“(n), p 2 1. More details and proofs on this topic can be found in [4, 6, 18, 20, 21, 24, 261. Now let (B,], 0 5 t < ao, be a family of measurable subsets of iR, such that I&( = T and B,, c B,* if r1 < r,, then set d(a) = u*(r)
where r = inf {r 2 0 : CTE B,),
(2.1)
First order Hamilton-Jacobi
equations
11
we have (cf. [21, lemma 12, p. 511) (a)* = u* (i.e. C(a) is a rearrangement
of u(x)) and (fi > t) G B, c (ti 2 t)
if p(t) = I@: U*(s) > t)I I t I I@: U*(s) I t]J = p(t-) and u*(s) is continuous in T. Now let U(X) and Q(s), 0 I s 5 IQ/, be measurable functions and let (B,J, T 2 0, be an increasing family of subsets of IT? such that IB,I = ‘5 and B, = (s I 0 : IQ(s)] > t) if r = I@: I@(s)/ > t)J. Then denoted by G&s) the rearrangement of U(X) related to such (B,) according to (2.1) it results ([21, theorem 2, p. 521) @*(s)@(s))* = (a,)*@*(s) = U*(s)@*(s) hence
InI k.(s)
s0
IQ(4I d.s=
1621
u*(s)@*(s) ds.
(2.2)
i0
Now consider the family ID,), s E [0, IQ/], of subsets of IF? such that ID,/ = s, Ds, c Ds2 if s, < s, and D, = (x: IuJ > t) if s = p(t). Then (see [3]), if f(x) 2 0 belongs to P(Q), p 2 1, there exists a function f(it) E P(0, Isz() such that
and the following lemma holds. LEMMA
2.1 [3]. There exists a sequence of functions (f&))
that lim
Ifll fk(M~)
d.s =
s0
Idl AM@
50
all equidistributed
withf(x)
such
d.9
where g(s) E Lp”p-l’(O, l&2()if p > 1 and g(s) is a function of bounded variation on [0, JsZl]if p = 1. 3. COMPARISON
THEOREMS
Suppose U(X)E W~9’(a) verifies the inequality Lu = (VUJ + c(x)24 5 f(x),
U(X) 2 0,
a.e. in M
(3.1)
where c(x) E L”(Q)
and
f(x) EL’(Q).
(3.2)
Set c+(x) = max(c(x), 0),
c-(x) = max(-c(x),
and L*w = lvwl + ((c+)*(x) - (c-)*(x)]w the following theorems hold.
0)
E. GIARRUSSO
12
THEOREM3.1. Let c(x) and f(x) be in P(sZ), p > n, then
where w(x) is the decreasing spherically symmetric solution of the problem L*w = &,(C,[x\“)
here./&)
is the rearrangement
a.e. in a*,
W E w;*‘(n*),
of f(x) according to the function [see (2.1) and (2.2)]
Q(t) = s
exp( 1’ [-(c+),(r)
+ (c-)*(r)] g
0 tE
(3.3)
n
dr)
1% Dll.
Suppose now c(x) = A E R and consider the problems L*q = (Vql + Iq = f*(x)
a.e.
q E Wy(n*>
in Q*,
(3.4)
and L*o
=
(Vwl + A0 = &(C,lx(“)
& being the rearrangement
a.e.
in 0,
w E Woi”(Q2*),
(3.5)
of f(x) according to the function [see (2.1) and (2.2)]
then we have the following theorem. THEOREM 3.2.
If there exists a decreasing spherically symmetric solution q(x)[o(x)l [(3.5)] it results that IIAl1 5 llc?ll1
of (3.4)
[llu*(x) e-xix’ll, 5 (lo(x) e-X’x’\ll]. To prove theorem comparison lemma.
3.1 and theorem
3.2 we have first to show the following pointwise
LEMMA 3.1. Let y(s), E+(s), and c”-(s) be the functions respectively, according to lemma 2.1, then set
related to If(x)\,
c+(x),
and c-(x),
IQI
Y(s) = exp
s it results that
for a.e. s E 10, \!A(].
[F+(t) - F-(t)] g
n
,,> ,
Ial 1 u*(s) 5 u(s) = f”(t)‘I’(t) s ‘y(s) s s
0 < s I IQj,
dt
(3.6)
First order
Hamilton-Jacobi
Proof. To get (3.6) we prove that U*(S) verifies the following -1+1/n
s&l*= -u*‘(s)
+ {E+(s)-
13
equations
differential
inequality
-1+1/n
e(s))u*(s)~n
I
f_(S)Sc._ncy”
a.e. s E IO, IQ(].
’
(3.7)
a.e. s E 10, [al].) (Note that iv = J$)(s- l+“n/nC~‘n) For this purpose integrate both sides of (3.1) over the set (x: t < u I t + hJ, h > 0; t L 0, to obtain 1 ’
1
lvul dx + ;
h ,t
C+UdXIt
h
1
c-u&u + h
t
*
Then let h + 0 to get for a.e. t 2 0 --
d
because
Above P is the perimeter Moreover t
5 --
u>t
ll>t
On the other hand, formula [ 121
i
c+udx
lvu] dx - $
dt
c+(x) dx
d dt i u>t
of the De Giorgi isoperimetric
in the sense of De Giorgi
.i t
t
theorem
d dt
by definition
= I(-;
c+(x)Uti
c+(x) dx .it
ju>tc+o~)
U>f
of E+(x). Analogously, --
by definition
of c-(x)
and f(x)
d dt 1 U>f
c-W
dx = u*(P(t))e-(P(t))(-Pu’(t)),
as well as --
d dt .r
Combining
the above
15
formulas
u>t If(x)1 d-x = “mt))(-p’(t)).
we derive from (3.8)
(p(t))-‘“‘”
~[-~‘WO) + c”-(P(t))lu*wo) + _fMWJ
nCl,”
(3.8)
[9] and a Fleming-Rishel
and so --
d.Y.
(see 19, 241).
t+h c+(x)24dx 5 h
5 ;
d - tl>t If( dt .i
c-udx
(-P’(O)
n
for a.e. t E [0, ess. sup u[,
(h > 0)
E. GIARRUSSO
14
which integrated between t, and tz, with 0 I t, < t2 < ess. sup u, gives r-1+1/n P(tl) tz -
{(-E+(T)
tl 5
+
5PU2)
c"-(T))u*(T) + f(it)j___ nC;/”
dT*
From the above, by the definition of u*(s) we obtain, with h > 0, u*(s) - u*(s + h) h
5-
1 h
s
*-1+1/n
s+h
((-C+(T)
+
c”-(T))u*(T)
+ f(7)]
-iKdty G
S
which implies (3.7). Now multiply both sides of (3.7) by Y(s) to obtain (3.6), since u*(s)Y(s) is an absolutely continuous function in [a, (Szl], with a > 0. Proof of theorem 3.1. Let s -+ O+ in (3.6) to get f-l+l/n
(-E+(r) + c”-(r))---
___ ncy
dt.
Then by lemma 2.1 and theorem 2.1, lOI y(t)@(t) dt 5
JIUJJ,= u*(o+) 5
s0
InI .&(t)@(t) dt,
(3.9)
0
again by lemma 2.1 and theorem 2.1, and by (2.2). Now set w(x)
=
c’ ,X,n (-d(r) ”
+
(c-)*(r))
routine calculations show that w(x) decreases with respect to 1x1. In fact, denoted by E = (x E S2 : c(x) < 01, and by 0, , the ball of R” centered at the origin and with radius w(x) is the product of two positive and decreasing spherically symmetric functions (]E ]KJ”“, in Szg and, in a* - n*,, w(x) decreases with respect to (xl, since f*(t) is decreasing in [IEI, (&?I],because Q(t) is. [Note that if (El s t I IQl,&(t) = f*(v*(@(t))), v* being the distribution function of Q(t).] Hence w(x) verifies (3.3) and so (3.9) implies the thesis. Remark 3.1. If sup(c_)*s””
_i (n - I)Ci’”
E
(in particular if c(x) 1 0) Q(s) decreases in IO, IQ]] and so.&,(s) = f*(s), (cp. with [14, 151 for the case c(x) = const. 5 0). Remark 3.2. If n = 1 Q(t) = + exp 3 (i
t (-(c+),(r) 0
+ (c-)*(r)) dr
, >
thus j&s) increases in [0, (El] and decreases in []SJj - ]G(, IQ]], where G = (x:c(x) > 0). Hence in particular if c(x) I 0, &s) = f*(s) and if c(x) L 0, _&(s) = f*(s) (see [14, 151).
First order Hamilton-Jacobi
equations
15
Proof of theorem 3.2. By lemma 3.1 we derive
(3.10) On the other hand the function a(t) = e
-X(t/C,)““f-l+l/n
f ex(s/c,)“”
&
i 0
strictly increases in [0, +a~). This is obvious for A = 0. For 2 # 0, computing d(t) check that v t E IO, +oo[ u’(t) > 0 iff -n
1
+
k(a) = ____ n --a
cl@”
I‘
ex(s/c”)“”
it is easy to
&
0
s C”d
A
ev”/w”
n
&
+
Cna”
,h
>
0,
va
E
IO,
+a[.
(3.11)
o
Now,
1
C,O"
k’(a) = C,,an-’ ehn - n
ex(s/c,)“” &
9
90 hence, if n = 1 or if L < 0 and n E IV, k(a) strictly increases in [0, +oo) and this implies (3.1 I), since k(0) = 0. If,I>Oandn>l,wehave k”(a) = C,(n - l)P2eX”, and this implies that k’(a) > k’(0) = 0 V a > 0, so, as before, k(a) strictly increases in [0, +co). Thus, (3.11) holds v Iz E R. Hence, by (3.10), lemma 2.1, theorem 2.1 and (2.2) we obtain llnllr 5 ~"lfto4r)dt = 11~11~. 0
Analogously,
by (3.6),
11 u*(x) e-xixi 11 1
=
IRI
i0
f&MWdt
[by lemma 2.1, theorem 2.1, and by (2.2)]
Ilw(x) e-xixill, .
Remark 3.3. Of course, existence assumption
A”jQj I C, and&(t)
of theorem 3.2 is verified if L 5 0 or if ,I. > 0, e-x(t’cn)“” decreases in [0, la/].
E. GIARRUSSO
16
Remark
3.4. If I I 0 of course f^a(s) = f,(s). (In [15] it was proved also that if (n - l)/(A[ < (IQj/C,)““, then u*(x) I w(x) in Q* - Szz, L-2:being the ball centered at the origin with radius (n - l)/lA(.) If A > 0, P(t) strictly increases in [0, C,/A”] and strictly decreases in [C,/A”, (Szl] and so the vp being the distribution function of P(t). same is true for &p(t) = f*(v@(t))), Of course, j&s) = f,(s) if [sZ( 5 C,/A”. REFERENCES LIONS P. L. & TROMBETTI G.. On ontimization problems with prescribed rearrangement, Nonlinear _ (1989). results for elliptic and parabolic equations via Schwartz 2. ALVINO A., LIONS P. L. & TROMBETTI G., Comparison symmetrization, Ann. Zst. Henri Poincare 7, 37-66 (1990). per una classe di equazioni ellittiche degeneri, 3. ALVINO A. & TROMBETTI G., Sulle migliori costanti di maggiorazione 1. ALVINO A..
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Math. 28, l-177 (1971). 7. CRANDALL M. G., EVANS L. C. & LIONS P. L., Some properties of viscosity solutions of Hamilton-Jacobi equations, Trans. Am. math. Sot. 282, 487-502 (1984). equations, Trans. Am. math. Sot. 277, 8. CRANDALL M. G. & LIONS P. L., Viscosity solutions of Hamilton-Jacobi l-42 (1983). 9. DE GIOROI E., Su una teoria generale della misura (r - 1) dimensionale in uno spazio ad r dimensioni, Annali Mat. pura appl. 36, 191-213 (1954). 10. FERONE V., Symmetrization results in electrostatic problems. Rc. Mat. 37, 359-370 (1988). results for elliptic equations with lower-order terms, Afti Semin. 11. FERONE V. & POSTERARO M. R., Symmetrization mat. fis. Univ. Modena (to appear). 12. FLEMING W. & RISHEL R., An integral formula for total gradient variation, Arch. Math. 11, 218-222 (1960). 13. GIARRUSSO E., Su una classe di equazioni nonlineari ellittiche, Rc. Mat. 31, 245-257 (1982). in a class of first-order Hamilton-Jacobi equations, Nonlinear 14. GIARRUSSO E. & NUNZWNTE D., Syrhmetrization
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