5.7. Approximation of Abstract Differential Equations 325
Then we have
Ilu" - P"uII" <f o"
e-XhIIS,,
(t)Pnv - P S(t)vII"dt
(5.7.43)
and we show that 11u,, - P"ull" - 0 as in the proof of Theorem 5.7.5(a). On
the other hand, Au = Au - v, Au" = Xu" - Pv so that
IIA,,u,, -P"AuII"<XIIu"-P"ull",
(5.7.44)
and it follows that u E D(d) with du = Au, in other words, that A C CT (note
that CT, being densely defined must be single valued by Lemma 5.7.9). We
can then apply (a) to show that d E C'+ and an argument similar to that
ending Lemma 2.3.9 shows that A = 6 as claimed.
5.7.12 Example. The method of lines for a parabolic equation. Let a be a
bounded domain of class C(00) in R',
A = 0 + c(x),
(5.7.45)
where c E C(°°)(S2). As a very particular case of the results in Chapter 4
(Theorem 4.8.11), we know that the operator A with domain consisting of
all u E Cr(S2) such that u E W2' °(E2) for all p < oo and Au E Cr(S2) (F _
boundary of 0) belongs to (2+(1, w) in E = Cr(S2) if
w = maxc(x).
X E 0
(We consider only real spaces and the Dirichlet boundary condition.) The
choice of approximating spaces is essentially that of Example 5.7.3, but the
subdivision of S2 is precisely specified as follows. Assuming 52 is contained in
the hypercube H defined by I x j I < a (1 < j < m ), for each n =1, 2,... we
divide the hypercube into (2n)' hypercubes determined by division of each
side of H into 2n equal segments. These hypercubes will be denoted as
follows: if a = (a1.... ,am) is a multi-index of integers with - n < aj < n - 1,
H" a denotes the hypercube defined by the inequalities
aja/n <x. < (aj + 1)a/n.
(5.7.46)
Also, x",,, denotes the point (a,a/n,...,ama/n) and for each n, J" is the set
of all multi-indices a with x,,,,, E S2, X" the set of all x",,, in 2, r(n) the
number of elements in J". The approximating spaces will be E" = R '(")
whose elements are denoted by ,
a; a E J") or simply each of
these spaces is endowed with the supremum norm
II
II" = Max
n a
l
(5.7.47)
n
The operators P" are defined by
P"u = (u(x",a); a E J"). (5.7.48)
The operators A" will be finite difference approximations to the partial
differential operator A. Obviously there is a great latitude in the choice of