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103Topologicalderivativeforsemilinearproblemsin3D
21
Inviewof(1.13),thefirsttermsontheleftandtherightarecancelledand,more-
over,wsatisfiestheproblem(1.12)withu(O)=v(O),
{ęw(ę)=0,
w(ę)=v(O),ę,
ęR3\ω,
whiletheboundarydatumcomesfromtherelation:
v(x)+w(E1x)+Ev(x)=v(O)+w(E1x)+O(E),xE.
Wehave:
w(ę)=v(O)P(ę)
(1.26)
(1.27)
wherePisthecapacitypotential[14,31],e.g.,aharmonicfunctioninR3\ωsuch
thatP(ę)=1onand:
P(ę)=|ę|1cap(ω)+O(|ę|2),
wherecap(ω)isthecapacityofthesetω.Since:
w(E1x)=−|x|1Ev(O)cap(ω)+O(E2|x|2),
wecollectcoefficientsonEin(1.25)andobtain:
{xv
(x)v(x)F
v(x,v(x))=ao(x)F
v(x)=ao(x),
v(x,v(x)),x,
xaΩ,
(1.28)
(1.29)
(1.30)
wherea=4πv(O)cap(w)ando(x)=(4π|x|)1isthefundamentalsolutionof
theLaplaceequationinR3.
SinceadirectcalculationyieldsF(·,v)oΛ0,α
γ
()withanyγ>1+α,we
obtainthesolutionvΛ2,α
β()ofproblem(1.30)suchthatvv(O)Λ2,α
γ
()
whereβα(2,3)andγα(1,2)canbetakenarbitrarilyintheprescribed
intervals.
Wereferthereaderto[9]forjustificationofasymptotic.
10302Theformalasymptoticoftheshapefunctional
Wehave:
J(uE;(E))=
(E)
J(x,v(x))dx+
(w(E1x)+Ev(x))J
v(x,v(x))dx+···
(E)
=
J(x,v(x))dx+E
(v(x)ao(x))J
v(x,v(x))dx+...(1.31)