126
V.
Boundedness
of
weak
solutions
In this section we will show that weak solutions
uEL'oc(nT),
r~
I,
are bounded
provided
p > max {
1;
::
r } .
Such integrability condition to insure boundedness is sharp. In § 12
of
Chap. XII
we produce a solution
of
the homogeneous p.d.e. (1.2)
that is unbounded.(I) Thus in the singular range 1 < p < max
{I;
AZ2}'
the
boundedness
of
a weak solutions is not a purely local fact and,
if
at all true, it must
be deduced from some global information. One
of
them is the weak maximum
principle
of
Theorem 3.3 and Remark 3.1. Another is a sufficiently high order
of
integrability.
5-(i). Local estimates
A sharp sufficient condition can be given in terms
of
the numbers
(5.1)
~r
=
N(P-
2)
+rp,
We
assume that u satisfies
(5.2) u E L'oc(nT), for some r
~
1 such that
~r
>
o.
1be global information needed here is
(5.3)
{
u can be constructed as the weak limit in
L,oc
(n
T
)
of
a
sequence
of
non-negative
bounded
subsolutions
of
(2.8).
The notion
of
weak subsolution requires u to be in the class
By the embedding
of
Proposition 3.1
of
Chap. I, we have
N+2
q=p--.
N
Therefore
ifpis
so close to one that
~q
~o,
the orderofintegrability in
(5.1)-(5.2)
is not implicit in the notion
of
subsolution and must be imposed.
(1)
The
notion
of
solutions
that
are not in
the
function class (2.2) is discussed in
Chap. XII