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On the Sharpness of a
Superconvergence Estimate in Connection with One-Dimensional
Galerkin Methods
ST. J.GOEBBELS*
LehrstuhlAfor Mathematik,RWTHAachen,Templergraben 55, D-52062 Aachen,Germany
(Received5 November 1997’; Revised 8January 1998)
The present paperstudies someaspects of approximation theoryin the context of one- dimensional Galerkinmethods.Thephenomenonofsuperconvergenceatthe knots is well-known.Indeed, forsmooth solutionstherateofconvergenceat thesepointsisO(h2r)
insteadofO(h+),where isthedegreeofthefinite element space.In ordertoachievea corresponding resultfor less smoothfunctions,weapplyK-functionaltechniquestoa Jackson-type inequality and estimate the relevanterrorby amodulus of continuity.
Furthermore,this error estimaterequiresnoadditionalassumptionsonthesolution,and it turns outthat it issharpin connection withgeneral Lipschitzclasses. Theproofof the sharpnessisbaseduponaquantitativeextensionoftheuniformboundedness principlein connection withsomeideasofDouglasandDupont [Numer.Math.22] (1974)99-109.
Hereit is crucial todesignasequence oftestfunctionssuch thataJackson-Bernstein-type inequalityandaresonance condition are satisfiedsimultaneously.
Keywords." Finiteelements; Superconvergence;Jackson-type inequality;Uniform boundedness principle; Sharpness
AMS1991 SubjectClassification: Primary65L60; 65L70; Secondary41A25
E-mail:[email protected]
1
INTRODUCTION
Weconsiderthetwopoint boundary valueproblem
-(a(x)u’(x))’ + b(x)u(x) --f(x),
xE(0, 1), u(0) u(1)
0.The corresponding weak problemis to find a solution u E
W’2(0, 1)
satisfying
a(u, v) (f, v)L2(o,,
for all v6Wo’2(0, 1), (1.1)
where
a(u, v)’- f[a(x)u’(x)v’(x) + b(x)u(x)v(x)]dx.
HereWS’2(0, 1)
denotes the Sobolev space(cf. [1])
of thosereal-valuedfunctionswhich possess weakderivativesuptothe ordersbelongingtothe HilbertspaceL2(0, 1)
of square integrable functions on(0, 1).
Therefore,WS’2(0, 1)
equippedwiththeinnerproduct(U, V)s,2,(0,1) (U (k), Y(k))L2(0,1
k=0 k=0
u(k)
(x)v
(k)(x)
dxand the norm
Ilulls,=,<0, / I1 < >11 c:/0,]
1/2 is a Hilbert space aswell. Besides, we use the semi-norms Let
Wd’2(0, 1)
be the closure ofC(0, 1)in W’2(0,
1), whereC(0, 1)is
the set of all infinitely often differentiable functions with support in (0,1).
Moreover,similar toW’2(0, 1)
letW’(0, 1)
be the Sobolev space offunctions with weak derivatives up to the orders in the space of essentially boundedfunctionsL(0, 1).
We assume that the function
a(x)
is Lipschitz continuous on [0, 1]and that
b(x) L(0, 1).
Therefore, a(.,.)
is bounded, i.e.,]a(u, v)[ _<
Cllull,
2/0 u,vw ’2(0,
Inordertoensurethata(.,-)isw,2-diirtic,
i.e., there exists a constant c>0 such thata(u,u)>
1,2,(0,1), u W0
(0, 1),
we assumea(x)>
>0 andb(x)>0
a.e.Further, let
f L2(0, 1).
Now the representation theorem ofF. Riesz assurestheunique solvability ofproblem(1.1).
Indeed, the solutionu doesnotonlybelongtoW’2 (0, 1)
buteven toW2’2(0, 1) (cf.
[12, p.200]).
For a discretization via the finite element method we consider the equidistant partitions (h--l/n, hEN; N denotes the set of
natural
numbers)
Th
:={[jh, (j+ 1)hi:
0 <_j< n}.
Thefiniteelement spaces
Vh
of degree rare nowgivenbyVh Vh(r)
:={v
ECo[0, 1]:
vPr[jh,
(j+ 1)hi,
0_<j< n},
whereC[0,
1]
isthe space offunctions continuous on[0,1]
and C0[0,1]
thesubspaceof those functions usatisfying
u(0) u(1)
0.By
79r[c, d]we denote thesetofall algebraic polynomials
v(x) =0
akx
withdegree at most r restricted to [c, d]. Obviously,
Vh c W’2(0, 1).
Thediscretizationof problem
(1.1)
nowreadsa(Uh, V) (f, V)L2(0,1
for all vVh. (1.2)
The theorem ofF. Riesz again guarantees the existence ofa unique solutionuh
Vh.
Furthermore,there still exists auniquesolution if we replace the right hand side of(1.2)
by an arbitrary functional onm’2(0, 1).
The Ritz projectionPh" W01’2(’)
+Vh
is therefore well defined viaa(Phu, v) a(u, v)
for all uwd’2(0, 1),
vCVh. (1.3)
Due to the ellipticity ofa(., .)
the linear operatorPh
is boundedindependently of h whichmeansthat thefiniteelementmethodisstable.
The aim ofthis paper is to discuss the error u-Uh, arising from problem
(1.2),
atthe knots jh of the partitions.Forsmoothsolutionsu one can proveconvergence of orderO(hr)
on thewhole interval [0,1]
whereasinthese special points jhthe rate increases to
O(h 2r) (see [9,10],
cf.[3]).
Butingeneralwe cannotexpect thesolutions tobe sufficiently smoothto ensuretheseJackson-typeinequalities.Section2istherefore concernedwith an errorbound underminimalsmoothnessconditions.Tothisend,weapplyK-functionaltechniques toestimate the errorby a modulus of continuity. It turns out that this error bound is sharp in connection with general Lipschitz classes. This is worked out in Section3 as aconsequenceof a quantitativeextensionofthe uniform boundedness principle. To establish the relevantresonancecondition, weproceedalongsomeideas of Douglasand
Dupont [10].
Letusmention that thearticle of Kfiek andNeittaanmiki
[17]
as wellas the book ofWahlbin[20]
giveadetailed survey of thefield of superconvergence.2
A DIRECT ESTIMATE
Itiswellknown thatCea’slemma yields the inequality
(cf.
[4,p.113]) ]]U- Uh[ll,2,(0,1) --<
CinfIlu- viii,z,(0,1
<_ Cllu- Ilhu[ll,2,/0,/,
where I-[h"C[O,1]--
{vE
C[O,1]:
vE79,.[jh,(j+l)h], 0_<j<n} is the globalLagrange
interpolation operator for the equidistant knots jh+
kh/r, 0<
k<_
r, 0 <j<
n. Thereby, without loss of generality, we assumethe functionuto becontinuous. Using affine transformations in connection with a reference element, one immediately obtains the followingJackson-typeinequality for <j<_
r,0< <
n(cf.
[4,p.125])"
Ilu- IlhUlll,2,(ih,(i+l)h) <_ ChJlu[j+l,2,(ih,(i+l)h),
uwJ+l’2(ih, (i
/1)h).
(2.1)
Thus, in connection with the K-functional
K(6,
u;s) infve
w,.,2(0,1)[llu VilE2(0,1) + SlUls,2,(0,1)]
weconclude theestimate(r > 1)
u
uhlll,2,(0,1) --<
C inf[llu-
v-IIh(u- 1)
1,2,(0,1)wr+,2(o
v ,1)
+
vn vii ,2,0,/]
_<
CvW,+l,2(0,1)inf[hlu- v12,2,(0,1)
/hr[v]r+,2,(o,)]
ChWeWr-inf1’2(0,1
[11 u() -wllL=<0,)/ hr-lwl ,2,(0,)1
ChK(h
r-1 u(2)"r1)
Now, the K-functional
K(h r-l,
u;r-1)
is equivalent to a modulus of continuityoforderr-(see [16])
asdefinedbyr_,(d5,
u,L(0, 1))"-
supwhere
A,-’u(x)’-- y]j=- (-1)r-l-j (r--j)bl(X
--{--jb’). Thus,thereexists a constantC (whichdoesnotdependonhoru)
such that forsolutionsu anduhof(1.1)
and(1.2),
respectively,one obtainsu
Uh[ll,2,(0,1) --< Chcr-l(h,u(2),L2(
O,1)). (2.2)
Since u E
W2’2(0,1),
the right hand side is well defined. Moreover, applyingNitsche’strick,onehasIlu- uh[l2<0,,) Chllu- Uhl]l,2,(0,1)
5 Ch2cOr-l(h,u(2),L2(
O,1)). (2.3)
Thisglobal
L2-estimate
issharpin connection withLipschitz classes(see [11]).
Concerningasup-normerrorboundonecanproceedinthesame mannerusingaJackson-typeestimatedevelopedin[21].
Butherewe are primarilyinterested intheerror atthe knotsjh, 0<j<
n.From [9,10]we quote that for smoothcoefficientsa(x)
andb(x)
onehas[(u-
uh)(jh)lChrllu- unlit,2,(0,,
), 0 j n.(2.4)
Therefore,oneobtains
(cf. (2.2))
I(u
uh)(jh)l<_
Chr+lOr_(h,
bt(2), L2(0, 1)), (2.5)
where theconstantCisindependent ofj,h,andu.Themain aimofthis paper is to discuss the sharpness of this estimate. For the sake of completeness and since it is neededin our considerations in the next section,wesketchaproofof theerrorbound
(2.4)
restricting ourselves to the casea(x)E Wr’(O, 1)
andb(x)=O.
The Green’s function G:[0,112--
ofproblem(1.1)
isthen given by(cf.
[19, p.265f])
{ f(I/a(t))dtfy(I/a(t))dt
for0<_
x<_
y,G(x,y)
f(I/a(t))dt fx(I/a(t))dtf(I/a(t))dt
fory<
x_< I,
thus
G(., y) W ’2(0, 1)
for eachfixedy [0, 1], andthereholds truea(u, G(.,y)) u(y)
2for alluW ’2(0, 1),
y[0, 1].
Evidently,
G(.,
y)E W +1’2(0,
y)fqW +1,2(y, 1)
andia(. y)lr2+l,2,(O,y)/ ia(. y) Ir+l,2,(y,1)
2Cy(1- y), (2.6)
wheretheconstantCisindependent of y.Therefore,onehas
(cf. (1.3))
lu(jh) Phu(jh)[[a(u-
Phu,G(.,jh))linf
la(u-
Phu,G(.,jh)v)]
v6Vh
<_ C[]u- Phu]ll,2,(o,
vinfVhIIG(.,
jh)vll,2,(o,
<_ Cllu- Phul[,2,(o,1)llG(’,jh) IIhG(.,
jh)111,2,(o,1).
Taking
(2.6)
intoconsideration,wehave(cf. (2.1)) IIG(’,
jh)1-IhG(., Jh)
,2,(o,)< Chr[lG(.
jh)[r+l,e,(0d’h)
2 /[G("
jh)]2r+ 1,2,(/h, 1)]1/2
<_
Chv/jh(1
jh)which establishestheerror bound
(2.5)
inthecaseb-0:](u- Phu)(jh)l <_ Cv/jh(1
-jh)hr[]u-Phull,2,(o,). (2.7)
Onemay furthernotethattheGreen’sfunctionbelongsto
Va
if1/a(x)
isapiecewise polynomialofdegreelessthanr.Then theerrorvanishes in theknots,u(jh) ua(jh)-O,0<_j
<_
n, sinceG(.,
jh) IIhG(.,jh)-O.3
SHARPNESS
We establish the sharpness of
(2.5)
in terms ofcounterexamples for general Lipschitzclasses,determinedbyabstractmoduliof continuity, i.e.,byfunctionsco(e.g.co({5)-
{5with0<
u<
1),continuous on[0,)
suchthat, for0<
j,{52,0
co(O) < co({51) co({5,
/{52) o3({51)
/co({52).
The main propositionof this article isthe following result.
THEOREM 3.1 There exists a
function a(x)E Wr’(O, 1)
witha(x) >
r;
>
O,such thatif
onediscussesproblems(1.1),(1.2)
in connectionwiththe innerproducta(u, v)- f a(x)u’(x)v’(x)dx,
then there holds true the following assertionfor finite
element spacesof
degree r>
1:for
each0
< 60 < 1/2
and every modulus satisfying(3.1)
andlim
((5)/(5 (3.2)
there exists a counterexample
u W’2(O, 1)V W2,2(0, 1)
which is asolution
of
problem(1.1)
with a suitable inhomogenityf L2(O, 1),
determinedby u, such thatontheonehand
(5
--+0+, h1/n 0+) COr_l((5, u),L2(O, 1))
butonthe other hand
(cf. (2.5))
]U(/)- (U)h(/)l # o(hr+lo3(hr-1))
for
each ue
:={j/2n: <_j< 2n,
ne 1} N(6o, 1-60).
Inparticular,u
isa
(common)
counterexample independentof
thepointsu.
The proof of Theorem 3.1 is much more sophisticated than a discussion of the sharpness of
(2.3)
because we have to establish a lowerestimateforamuch smallererror.The restofthis sectiondeals with thisproof. Inthecontextof approximation theory such negative resultsareoftenobtained onthebasisof quantitativeextensions ofthe uniformboundedness principledeveloped byDickmeis, Nessel andvan Wickeren(cf. [5]-[8]).
Fora
(real)
Banach space Xwithnorm[[.[Ixlet
X~ bethesetofnon-negative-valued sublinearboundedfunctionals Ton X,i.e., Tmaps X into
I,
thesetofrealnumbers, suchthat for allf,gEX,u 1Tf>_ O,
T(f + g) <_ Tf +
Tg,T(uf) T[Ix
:=sup{ Tf
THEOREM 3.2 Suppose that
for
afamilyof
remainders{ Tn,:
nI,
u
}
CX-, where()n
risasequenceof
non-empty indexsets,andfor
a measureof
smoothness {$6:(5> 0}
c X~there are test elementssuch that the following inequalities holdtrue
(6 >
0, ncx)"
IIgll c1
S’gn
<- C2 min{1, n )
I[Zn,utlx~ <_ C3,n
Tn,,gj<_ C4,u C5 T,,,,gn >_ C6, >
0for
alln lI,(3.3)
for
alln ENI,
6>
0,(3.4)
for
allu ]n, n ll,(3.5)
for
all <_j<_
n-1, Un,
n Ell,(3.6)
for
alluI,. (3.7)
Here
a(6)
isafunction,strictlypositiveon(0, cx), and(P,)n
NCIRis a strictlydecreasingsequencewithlimno
q, 0. Thenfor
eachmoduluscosatisfying
(3.1)
and(3.2)
there existsa(strictly increasing) subsequence(nk)k
rC1tandacounterexamplefo
Xsuchthat(6
s6L o(((6))),
Zn,ufw
for
eachu :=limsuPk_]nk
:---Nk%l Uj--k nj.
Fora proof,further comments, and applications to approximation theorysee[5,13,14] and theliterature citedthere.
Proof of
Theorem 3.1 To applyTheorem 3.2,wespecify the quantities accordingto(h
2-",n1)
X-
W’(0, 1) W2’2(0, 1), I1" IIx- 112,2,/0,/,
(/gn hr_
2(r_l)n
0"(6)- r-1,
s _(6,u(:),L:(O, 1)),
Itn’-
-"
l_<j_< -1(60,1-60)
Zn,,U- 2(+)nl(u- ehU)()l h-(r+’)l(u- ehu)(u)l, . .
Indeed, $6,
T,,E
X~(cf. (2.2), (2.7)),
and we note that, c n+l
CC ]
Un=l
]]n. The crucialpointis to find a suitablesequence of test elementsandtoshowtheresonance condition(3.7). At
first,wewillconstruct asequence
(n)nEN
which isindeed suitable inconnectionwith(3.7).
Butthesefunctions arenotsmoothenoughtosatisfy the Jackson- Bernstein-type inequality(3.4).
Thereforewehavetosmooth them.This willbe done usingapartition of unity. The stability of thefiniteelement methodassuresthat for the smoothedfunctions(gn)n rtheresonance condition still remains valid.Thuslet us start withthe sequence
(n)ner
which is definedby,n(X) "--hr_l fn(t)
dt,where
(0
_<j<
2n-1)
0 x=0,
n(X)
:= (x-jh)r XE (jh, (j+ 1)h]
forj_<
2n-1 1,I,-((j
+ 1)h x)
x (jh, (j+ 1)hi
forj>_
2n-l,
i.e.,jh>_1/2.
The
functionL
isodd withrespectto thepoint1/2,i.e.,L(x) -jn (1 x)
a.e. Obviously, is piecewise polynomial ofdegree r
+
and satisfies(0) (1)
0such thatW01’2 (0, 1).
Moreover,h
(3.8)
where
II,llL0,
) denotes the essential supremum. The next stepis to smoothf,
with a suitable partition of unity. To this end, given an arbitrary 0<e_<
1/4, there exists an infinitely often differentiable function with(cf.
[15, p.35])1: x
<_ 1/2-
q(x)=
O:x> 1/2+ s(x) e(1 x),
xR,
and 0
<
p(x)_<
1.Withtheaidofthisfunctionwedefinef,
asfollows:(a)
forx [(j+ 1/2)h,
(j+ 3/2)h],
0_<j_<
2"-
2"+ (1 e -fh))(x-(j+ 1)h) r,
(b)
forxE[(j+
1/2)h,(j+
3/2)h1,2n-1_<j<_ 2n-2 fn,s(X)
:=e
((j+ 1)h x)
-(1 e (\x ;h) )
((j+ 2)
hx)r.,
(c)
forxE[(2’-l-1/2)h,(2
n-1+
1/2)h]-[(j+ 1/2)h,(j+3/2)h]
withj_2--l_l
(1
(#e(x ;h) )
((j..l._2)h x)r;
(d)
forx [0, hi2]u [l-h/2, 1]"
Notethat
f.,
isinfinitely oftendifferentiableandIlfn,llfto,l
supIfn,(x)l <_
hxe[0,]
(3.9)
Furthermore,duetothedefinitionsoff.
and thefunctionf.,
isoddwithrespectto
1/2.
Therefore,the resonanceelementsg.(x) g.,(x)
h- f.,(t)
dtsatisfy the boundary condition
gn,(0) g.,(1)
0, and they are infinitely oftendifferentiable. Inparticular,(g.,).
erc
X. The param- eter c will be fixed later. Straightforward calculations yield (l_<k_<r+ 1)Ign,l,2,<0,/ Ilfn,-/ll/0,/
<_ hr_fllf,-llllc[o,l] <_ Ceh
2-k(3.10)
where the constant
C
is independent of h. Furthermore, Poincar6’s inequality(cf.
[1, p.159])
yieldsIIg,,,[12,2,/o,) < Ilgn,ll,2,/0,/ + Ign,el2,2,(0,1)
<_ C(Ign,e [1,2,(0,1) -- [gn,e 12,2,(0,1))
Therefore, condition
(3.3)
is established. Concerning(3.4)
we have(el. (3. o))
COr_l(6,
g(2)Z2(O, 1)) < Clgn’]2’2’(’) <-
Ce,n,e,
(c6r_llgn,elr+l,2,(o,1) ce6r_lh2_(r+l)__Ceff(6)/n.
Concerning the crucial resonance condition(3.7),we firstinvestigate how much the functiongn,differs from
oan.
One observes thatjTn(x) =f,,(x)
outside the balls S(2eh,jh)={x: ]x-jh
<
2eh}. OnceagainbyPoincar6’s inequalityI[n gn,e [11,2,(0,1) finn gn,e 11,2,(0,1)
C
hr_
[ln fn,e[IL-(O,1)
hr-1 In(X) fn,(x)l
2dxkj=0 d(j+l)h-2eh
c /11.
hr_-
([(
2n1)4eh]
2Cx/
hr_
(I]LIILoo(o,1)+
Togetherwith
(3.8)
and(3.9)
this yieldsIIn- gn,e]]l,2,(0,1)--< Chx/.
Itisimportantto notethat theconstantCdoes notdependon candh.
Because of the uniformboundedness of the operator
Ph
we concludeTaking thedirect estimate
(2.7)
intoconsideration,oneobtains(u I(n-ehn)(U)l
I(gn, ehgn,)(u)l + I(gn, --n)(U) eh(g,, -n)(U)l
< I(gn,e Phg,,,)(u)l + Chrllgn,e ,n Ph(gn,e n)lll,2,(0,1)
-< I(g, ehgn,)(u)l + Ch[[IPh(gn, -n)ll,2,/0,/+ Ilgn, --nll,2,/0,/]
<_ I(gn, Phgn,)(u)l + Chr+lv/-
and therefore
Tn,,gn, h-(r+l)l(gn, Phgn,)(u)l
>-- h-(r+l)l(n Phn)(U)l CV/- Zn,.n Cx/-.
In what follows wewillprove the crucialinequality
T,,, >_ cmin{u, u} (3.11)
for uE
,
and n 1. Then accordingto the definition of one has min{u,u} > 60 >
0 such thatT,,,g,, >_ C6o- C6o/2- C6o/2
for eache
<_
min{1/4,[Co/(2C)]2}.
Summarizing, we then have found a reso- nance sequence which satisfies(3.3), (3.4), (3.7).
Since the conditions(3.5)
and(3.6)
follow from thedirect estimates(2.2)
and(2.7),
i.e.,IlZn,llx Ch-(r+l)hr+l-C,
Tn,,gj,e
< CWr_l(h,
"-’(2)L2(0, 1))
<- Chr-l lgj,elr+l,2,(o,1) CJ,e
n,Theorem 3.2 yieldsacounterexample
u
which satisfies the assertions of Theorem 3.1. Indeed, this counterexampleis a solutionofproblem(1.1),
where the inhomogenityf
is determined by partial integration.It remains toprove
(3.11).
In[10]
Douglas andDupont
investigate the sharpness ofanestimate(2.4)
in connection withthecase()=
which is excluded here.They are able topresent explicitly an elemen- tarycounterexample forwhichthe superconvergenceerrorisexactly of order
(Q(hzr).
Thereby, thecrucialpointisasuitablerepresentationfor theerrorwhich we willapplyaswell.At
thispointitbecomes necessaryto fixthe function
a(x)
and therefore to determine the innerproducta(., .).
Leta(x)E Wr’(O, 1)
be even with respect to1/2,
i.e.,a(x)=
a(1 x)
a.e., such that the followingconditionsholdtrue(a(x)
>> 0):
a(x)
E
"]’)r[0, 1/2]
fq79r(1/2, 1]
witha(x)
(a()
(r){?", --r!,
XX[0, (1/2,1] 1/2]
e’Dr[O, 1]
with(a)(r)-r!
ifriseven,ifris odd.
Onemaynotethatadiscussionofcasesisnecessaryto assurethat
1/a(x)
anda(x)
are even. Forexample, we canchoosea(x) (x (1/2)) + (r even),
a(x) (x (1/2)
4-1’
x{0, 1/2]
(1/2, 1]
(x- (1/2))
r’ X(r odd).
Evidently,
1/a(x)
is a piecewise polynomial of degree r and not of degree r- 1. This is important because otherwise the error vanishes(cf.
Section2).
Duetotheir constructionboth thefunctions
a(x)
andoan
areevenwithrespecttothe point
1/2.
Therefore,theRitzprojectionPhoan
iseven,too.This iseasytoprove because thepartitions
Th
areequidistant.Inother words, the erroren(x)’-ao,(x)--Phn(X)
is even ande’
is odd. Thisisnecessarytoestablishtheerrorrepresentation
(cf. [1 0])
e,(u) a(x)e’,,(x) z(x)
dx(3.12)
a(x)e’n(X z(x)
dxfor allz E
79r_,h,
u, (3.13)
where
"Dr,h
:--{z: [0, l]
---+ ]l: z "]’)r(jh, (j4-1)h],
0 <_j_<
n1}.
Weprove
(3.12) (3.13)
follows inthesame way). Tothis end, given a function z E79r_l,h
we definev(x) f z(t)
dt xfd z(t)
dr. Thenv E
79r,
hfqC[0,1] and the construction assuresv(0) v(1)
0 such that vVh(r). By
virtue off a(x)en (x)
0weobtain(cf. 1.3))
( )
(aen z)L2(0,1 (aen
V)L2(0,1) -+- aen, z(t)
dtL2(0,1)
(aen,
v)L2(0,1) + (ae
n,1)L2(0,1) z(t) at (aen, V’)L2(0,1 a(en, v)
O.Now let z
"]")r-l,h
and un.
The function(x)’-z(x)
for x<_
u,(x)
"-0 for x>
u, belongs to7)r_l,h
as well, and therefore 0-fd a(x)e (x)(x)
dxf a(x)e (x)z(x)
dxsuch that(a(x) > > O)
en(u) en(X
dxa(x)en(X) z(x
dx.Finally, we use the representation
(3.12), (3.13)
to establish the isthesame as resonancecondition(3.11).
The leadingcoefficient ofen
of
hl-@n
and the leading coefficient of1/a
has been fixed by theconditions on
a(x)"
reven rodd
Leadingcoefficientof
1/a(x)
Leadingcoefficientofe(x)
+1 +1
-1
+
h1-r ifx_<1/2
-h1-r ifx>
1/2
if
x< 1/2
ifx>
1/2
+
h1-rFor that reason, one can choose
z
("Dr-l,h
such that forx (jh, (j
+
1)h] thereholdstrueen(X)[a ] { +hr-l[en(x)]2 frx<-l/2’
(3.14) Zn(X)
-h
r-l[en(x)]
2 forx> 1/2.
Inconnection with
(3.12)
oneobtainsforu_< 1/2
Tn,,n h-- len()l -> a(x)en(X) Zn(X)
dxhr+l a(x)e.(x) Zn(X X
ajh
hr-1 (_-[(j+)h
hr+ a(x)[en(X)]
2dxj=0 aJh
[en (x)]
2dx.\e[0,1]
5
i=0 ai
In view of the positivity of
[eP,(x)]
2 the rest of theproofis a routine argument. Indeed, sincePhn
EI?r(jh, (j+1)hi,
one hasl?r_(jh, (j
+ 1)hi
and(j+l)h
inf
[’ (x) v(x)]
dxvTVr_ (jh,(j+1)hiJjh
[ I]
2---
h2 .= VEPr-l(jh,(j+l)h]inf djhv(x
dx(/h)-I
h2 inf xr-
v(x)
dxvePr-(jh,(j+1)hi,Ijh
h2h2(r 1)
(u/h)-I
[(j+l)h
inf
Ix v(x)]
2dxvPr- (jh,(j+l)h]
j=O djh
(u/h)-I
Z )r
dtinf h
[(ht
+jhv(ht +jh)]
2h2h2(r 1) vpr_(jh,(j+1)hi
"_
(u/h)-l
h2r+l Z
inff0
h2hz(r-1)
j=0 V6Pr_[0,1]
It
r-v(t)]
2dt> ch/h
=cu>0.
By virtue of
(3.13)
(cf.(3.14))
one analogously obtains thatT,,,n > c(1 u)
in the caseu> 1/2.
This finishestheproofof(3.11).
Thoughspecific, the present resultsarebyno meansrestricted tothe particular superconvergence phenomenon under consideration.
As
a second example letusbrieflymentionsuperconvergenceatGaussand Lobatto points. Using well-known Jackson-type inequalities(cf.
[2,18]), one can establish intermediate error bounds analogously to(2.5)
interms ofmoduli of smoothness which are sharp in connection with general Lipschitz classes. Againthis canbeprovedusing theresonance principle of Theorem 3.2
(cf. [11]).
Hereit seems tobenaturaltobuild up a resonancesequence byLegendre polynomials because theGauss and Lobatto pointsare zerosofthese polynomials andtheirderivatives.Then the resonance condition follows from the fact that the zeros of Legendre polynomials
Pk
andPz:
+ aredifferent.Acknowledgement
The results ofthis paper are part of the author’s doctoral thesis
[11]
whichhas beenwrittenunder supervision of ProfessorR.J. Nessel. The authorisverygratefulforhisvaluableadviceand interestingcomments.
The author would also like to thank Professor H. Esser for his constructive suggestions and the Graduiertenf6rderung von Nord- rhein-Westfalenforfinancialsupport.
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