11. Young measures and fuzzy functions 85
(11.77) @
t
.u
"
/ C @
x
q.u
"
/ precompact in H
1
loc
./;
which is hypothesis (11.59) of Proposition 11.5. Therefore, we have the following:
Proposition 11.7. Given solutions u
"
;0<" 1 to (11.66), satisfying (11.67)–
(11.69), a weak
limit u in L
1
./,as" D "
j
! 0, satisfies
(11.78) @
t
u C @
x
F.u/ D 0:
The approach to the solvability of (11.78) used above is given in [Tar].
In Chap.16, 6, we will obtain global existence results containing that of
Proposition 11.7, using different methods, involving uniform estimates of
k@
x
u
"
.t/k
L
1
.R/
. On the other hand, in 9 of Chap. 16 we will make use of
techniques involving fuzzy functions and the div-curl lemma to establish some
global solvability results for certain 2 2 hyperbolic systems of conservation
laws, following work of R. DiPerna [DiP].
The notion of fuzzy function suggests the following notion of a “fuzzy solu-
tion” to a PDE, of the form
(11.79)
X
j
@
@x
j
F
j
.u/ D 0:
Namely, .u;/2 Y
1
./ is a fuzzy solution to (11.79)if
(11.80)
X
j
@
@x
j
F
j
D 0 in D
0
./; F
j
.x/ D
Z
F
j
.y/ d
x
.y/:
This notion was introduced in [DiP], where .u;/ is called a “measure-valued
solution” to (11.79). Given jF
j
.y/jC hyi
p
, we can also consider the concept
of a fuzzy solution .u;/ 2 Y
p
./. Contrast the following simple result with
Proposition 11.5:
Proposition 11.8. Assume .u
j
;
j
/ 2 Y
1
./; ku
j
k
L
1
M , and .u
j
;
j
/ !
.u;/in Y
1
./.If
(11.81)
X
k
@
k
F
k
.u
j
/ ! 0 in D
0
./;
as j !1, then u is a fuzzy solution to (11.79).
Proof. By Proposition 11.1, F
k
.u
j
/ ! F
k
weak
in L
1
./. The result follows
immediately from this.
In [DiP] there are some results on when one can say that, when .u;/ 2
Y
1
./ is a fuzzy solution to (11.79), then u 2 L
1
./ is a weak solution to
(11.79), results that in particular lead to another proof of Proposition 11.7.