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Three Dimensional System of Globally Modified Navier-Stokes Equations with Infinite Delays

Abstract

Existence and uniqueness of solution for a globally modified version of Navier-Stokes equations containing infinite delay terms are established. Moreover, we also analyze the stationary problem and, under suitable additional conditions, we obtain global exponential decay of the solutions of the evolutionary problem to the stationary solution.

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Three Dimensional System of Globally Modified Navier-Stokes Equations with Infinite Delays

Author: Marín Rubio, Pedro; Márquez Durán, Antonio Miguel; Valero Cuadra, José
Publisher: American Institute of Mathematical Sciences
Year: 2010
DOI: 10.3934/dcdsb.2010.14.655
Source: https://idus.us.es/bitstreams/349812db-82a0-449a-a296-fdba01129701/download
Manusc ip submi ed o Websi e: h p://AIMsciences.o g
AIMS’ Jou nals
Volume 00, Numbe 0, Xxxx XXXX pp. 000–000
THREE DIMENSIONAL SYSTEM OF GLOBALLY MODIFIED
NAVIER-STOKES EQUATIONS WITH INFINITE DELAYS
P. Ma ´
ın-Rubio, A. M. M´
a quez-Du ´
an & J. Real
Depa amen o de Ecuaciones Di e enciales y An´alisis Num´e ico,
Uni e sidad de Se illa,
Apdo. de Co eos 1160,
41080–Se illa, Spain
(Communica ed by Aim Sciences)
Abs ac . Exis ence and uniqueness o solu ion o a globally modi ied e -
sion o Na ie -S okes equa ions con aining in ini e delay e ms a e es ablished.
Mo eo e , we also analyze he s a iona y p oblem and, unde sui able addi-
ional condi ions, we ob ain global exponen ial decay o he solu ions o he
e olu iona y p oblem o he s a iona y solu ion.
Keywo ds: Globally Modi ied Na ie -S okes Equa ions; in ini e delays.
Ma hema ics Subjec Classi ica ions (2000): 35K55, 35Q30, 34D23, 34K20
1. In oduc ion and s a emen o he p oblem. Le Ω ⊂R3be an open
bounded se wi h egula bounda y Γ, and le N∈(0,+∞) be ixed. Le us de ine
FN: [0,+∞)→(0,1] by
FN( ) := min 1,N
, ∈[0,+∞),
and conside he ollowing sys em o globally modi ied Na ie -S okes equa ions on
Ω wi h homogeneous Di ichle bounda y condi ion















∂u
∂ −ν∆u+FN(kuk) [(u· ∇)u] + ∇p= ( ) in (τ, T∗)×Ω,
∇ · u= 0 in (τ, T∗)×Ω,
u= 0 on (τ, T∗)×Γ,
u(τ, x) = u0(x), x ∈Ω,
(1)
whe e ν > 0 is he kinema ic iscosi y, u he eloci y ield o he luid, p he p es-
su e, τ∈Ran ini ial ime, u0 he ini ial eloci y ield, ( ) a gi en ex e nal o ce
ield, and T∗∈(τ, +∞] a gi en inal ime.
The sys em (1) is indeed a globally modi ied e sion o he Na ie -S okes sys-
em – he modi ying ac o FN(kuk) depends on he no m kuk=k∇uk(L2(Ω))3×3,
2000 Ma hema ics Subjec Classi ica ion. P ima y: 35K55; 35Q30; 34D23; 34K20.
Key wo ds and ph ases. Globally Modi ied Na ie -S okes Equa ions; in ini e delays.
Pa ially suppo ed by Minis e io de Ciencia e Inno aci´on (Spain), p ojec MTM2008-00088
and Jun a de Andaluc´ıa, g an P07-FQM-02468.
1
2 P. MAR´
IN-RUBIO, A. M. M´
ARQUEZ-DUR´
AN & J. REAL
which in u n depends on ∇uo e he whole domain Ω and no jus a o nea he
poin x∈Ω unde conside a ion. Essen ially, i p e en s la ge g adien s domina ing
he dynamics and leading o explosions. I iola es he basic laws o mechanics,
bu ma hema ically he sys em (1) is a well de ined sys em o equa ions, jus like
he modi ied e sions o he Na ie -S okes equa ions o Le ay and o he s wi h o he
molli ica ions o he nonlinea e m, see he e iew pape [8]. I is wo h men ioning
ha a global cu o unc ion in ol ing he D(A1/4) no m o he wo dimensional
s ochas ic Na ie -S okes equa ions is used in [9], and a cu -o unc ion simila o
he one we will use he e was conside ed in [23].
The sys em (1) was in oduced and s udied in [1] (see also [2,14,15,16,3] and
he e iew pape [13]). Howe e , he e a e si ua ions in which he model is be e
desc ibed i some e ms con aining delays appea in he equa ions. These delays
may appea , o ins ance, when one wan s o con ol he sys em by applying a o ce
which akes in o accoun no only he p esen s a e bu he comple e his o y o he
solu ions. The e o e, in his pape we a e in e es ed in he case in which e ms
con aining in ini e delays appea . We conside he ollowing e sion:













∂u
∂ −ν∆u+FN(kuk) [(u· ∇)u] + ∇p= ( ) + g( , u ) in (τ, T∗)×Ω,
∇ · u= 0 in (τ, T∗)×Ω,
u= 0 on (τ, T∗)×Γ,
u(τ+s, x) = φ(s, x), s ∈(−∞,0], x ∈Ω,
(2)
whe e gis ano he ex e nal o ce con aining some he edi a y cha ac e is ic and φ
is a gi en unc ion de ined in he in e al (−∞,0].
Ou goal is o es ablish he exis ence and uniqueness o solu ion o he abo e
p oblem and o s udy i s asymp o ic beha iou ( o a simila goal in Na ie -S okes
models wi h ini e delay c . [5,6,7], and o ODEs and PDEs wi h unbounded
delay e ms c . [4,18]).
The s uc u e o he pape is he ollowing: in Sec ion 2we ecall some spaces
use ul o he abs ac amewo k and some p ope ies and es ima es ela ed o
he ope a o s in ol ed in he model. In Sec ion 3 he exis ence and uniqueness o
solu ion o he (e olu iona y) p oblem is gi en. The s a iona y p oblem is ea ed
in Sec ion 4, whe e we also p o e ha unde adequa e assump ions, any solu ion o
he e olu iona y p oblem has an exponen ial decay owa d he s a iona y solu ion.
2. P elimina ies. To se ou p oblem in he abs ac amewo k, we conside he
ollowing usual abs ac spaces (see [17] and [21,22]):
V=nu∈(C∞
0(Ω))3: di u= 0o,
H= he closu e o Vin (L2(Ω))3wi h inne p oduc (·,·) and associa e no m |·| ,
whe e o u, ∈(L2(Ω))3,
(u, ) =
3
X
j=1 ZΩ
uj(x) j(x)dx,
3D-GMNS EQUATIONS WITH INFINITE DELAYS 3
V= he closu e o Vin (H1
0(Ω))3wi h scala p oduc ((·,·)) and associa e no m
k·k ,whe e o u, ∈(H1
0(Ω))3,
((u, )) =
3
X
i,j=1 ZΩ
∂uj
∂xi
∂ j
∂xi
dx.
We will use k·k∗ o he no m in V0and h·,·i o he duali y pai ing be ween V0
and V. Finally, we will iden i y e e y u∈Hwi h he elemen u∈V0gi en by
h u, i= (u, )∀ ∈V.
I ollows ha V⊂H⊂V0,whe e he injec ions a e dense and compac .
We conside he linea con inuous ope a o A:V→V0de ined by
hAu, i= ((u, )) ∀u, ∈V. (3)
Deno ing D(A) = {u∈V:Au ∈H},wi h inne p oduc (u, )D(A)= (Au, A ),
hen, by he egula i y o Γ, D(A) = (H2(Ω))3∩V, and Au =−P∆u, ∀u∈D(A),
is he S okes ope a o (Pis he o ho-p ojec o om (L2(Ω))3on o H).
Le us deno e
λ1= in
∈V {0}
k k2
| |2>0,
he i s eigen alue o he S okes ope a o .
Now we de ine he ilinea o m bon V×V×Vby
b(u, , w) =
3
X
i,j=1 ZΩ
ui
∂ j
∂xi
wjdx, ∀u, , w ∈V,
and we deno e
bN(u, , w) = FN(k k)b(u, , w),∀u, , w ∈V.
The o m bNis linea in uand w, bu i is nonlinea in . E iden ly we ha e
bN(u, , ) = 0, o all u, ∈V. We will also make use o he ollowing inequali y
(see [21] and [10])
|b(u, , w)| ≤ 2−1|u|1/4kuk3/4k k|w|1/4kwk3/4,∀u, , w ∈V. (4)
In pa icula , his implies ha he e exis s a cons an C1>0 only dependen on Ω
(namely, C1= (2λ1/4
1)−1) such ha
|b(u, , w)| ≤ C1kukk kkwk,∀u, , w ∈V.
Thus by he de ini ion o FN,i we deno e
hBN(u, ), wi=bN(u, , w),∀u, , w ∈V,
we ha e
kBN(u, )k∗≤NC1kuk,∀u, ∈V. (5)
We ecall (see [21]) ha he e exis s a cons an C2>0 depending only on Ω
such ha
|b(u, , w)| ≤ C2kuk1/2|Au|1/2k k|w|,(6)
o all u∈D(A), ∈V, w ∈H, and
|b(u, , w)| ≤ C2kukk k|w|1/2kwk1/2,(7)
o all u, , w ∈V. (See [20] o he p oo o (7)).
4 P. MAR´
IN-RUBIO, A. M. M´
ARQUEZ-DUR´
AN & J. REAL
Le Xbe a Banach space. The no a ion BX(a, ) will be used o deno e he open
ball o cen e aand adius in he space X. Gi en a unc ion u: (−∞, T∗)→X,
o each <T∗we deno e by u he unc ion de ined on (−∞,0) by he ela ion
u (s) = u( +s), s ∈(−∞,0).
One possibili y o deal wi h in ini e delays, and which we will use he e (c .
[18,11,12]), is o conside , o any γ > 0, he space :
Cγ(H) = ϕ∈C((−∞,0]; H) : ∃lim
s→−∞ eγsϕ(s)∈H,
which is a Banach space wi h he no m
kϕkγ:= sup
s∈(−∞,0]
eγs|ϕ(s)|.
In o de o s a e he p oblem in he co ec amewo k, le us i s es ablish some
ini ial assump ions on some e ms in he equa ion:
We will assume ha ∈L2(τ, T; (L2(Ω))3) o all T∈(τ, T∗]∩R.
Fo he e m g, in which he delay is p esen , we assume ha g: (τ, T∗)×
Cγ(H)→(L2(Ω))3sa is ies
(g1) Fo any ξ∈Cγ(H) he mapping (τ, T∗)3 7→ g( , ξ) is measu able,
(g2) g( , 0) = 0 o all ∈(τ, T∗),
(g3) he e exis s a cons an Lg>0 such ha o any ∈(τ, T∗) and all ξ, η ∈
Cγ(H),
|g( , ξ)−g( , η)| ≤ Lgkξ−ηkγ.
Rema k 1. (i) Condi ion (g2) is no eally a es ic ion, since o he wise, i |g(·,0)| ∈
L2(τ, T ) o all T∈(τ, T∗]∩R,we could ede ine ˆ
( ) = ( ) + g( , 0) and ˆg( , ·) =
g( , ·)−g( , 0).In his way he p oblem is exac ly he same and ˆ
and ˆgsa is y he
equi ed assump ions.
(ii) Condi ions (g2) and (g3) imply ha
|g( , ξ)| ≤ Lgkξkγ,
so ha |g(·, ξ)| ∈ L∞(τ, T∗).
We will deno e Pm he o hogonal p ojec o o Hon o he ec o space gene a ed
by he i s meigen unc ions o he S okes p oblem in Ω wi h homogeneous Di ichle
bounda y condi ions.
An example o ope a o sa is ying assump ions (g1)-(g3) is gi en he e.
Example 1. We conside he ope a o g: (τ, T∗)×Cγ(H)→(L2(Ω))3de ined as
ollows:
g( , ξ) := Z0
−∞
G( , s, ξ(s))ds ∀ ∈(τ, T∗),∀ξ∈Cγ(H),
whe e he unc ion G: (τ, T∗)×(−∞,0) ×R3→R3sa is ies he ollowing assump-
ions:
(a) G( , s, 0) = 0 o all ( , s)∈(τ, T∗)×(−∞,0).
(b) The e exis s a unc ion κ: (−∞,0) →(0,+∞) such ha
kG( , s, u)−G( , s, )kR3≤κ(s)ku− kR3
∀u, ∈R3,∀( , s)∈(τ, T∗),×(−∞,0),
3D-GMNS EQUATIONS WITH INFINITE DELAYS 5
(c) and he unc ion κsa is ies ha κ(·)e−(γ+)·∈L2((−∞,0)) o some  > 0.
Namely, he ope a o gde ines an elemen o (L2(Ω))3in he ollowing way:
g( , ξ)(x) = Z0
−∞
G( , s, ξ(s)(x))ds ∀x∈Ω.
We check now ha gsa is ies he assump ion (g3), and using (a) abo e, we
ob ain ha i is well de ined as a map wi h alues in (L2(Ω))3:
ZΩZ0
−∞
κ(s)kξ(s)(x)−η(s)(x)kR3ds2
dx
=ZΩZ0
−∞
κ(s)e−(γ+)se(γ+)skξ(s)(x)−η(s)(x)kR3ds2
dx
≤ZΩZ0
−∞
κ2(s)e−2(γ+)sdsZ0
−∞
e2(γ+)skξ(s)(x)−η(s)(x)k2
R3dsdx
=Z0
−∞
κ2(s)e−2(γ+)sdsZΩZ0
−∞
e2(γ+)skξ(s)(x)−η(s)(x)k2
R3dsdx
=CκZ0
−∞ ZΩ
e2(γ+)skξ(s)(x)−η(s)(x)k2
R3dxds
≤Cκ"sup
s∈(−∞,0]
e2γs ZΩ
kξ(s)(x)−η(s)(x)k2
R3dx#Z0
−∞
e2sds
=Cκkξ−ηk2
γ
1
2
=Lgkξ−ηk2
γ,
whe e we ha e deno ed Cκ=kκ(·)e−(γ+)·k2
L2(−∞,0) and Lg=Cκ/(2).
3. Exis ence o solu ions. In his sec ion we es ablish exis ence o solu ion o
(2) by a compac ness me hod using a Faedo-Gale kin scheme.
De ini ion 1. A weak solu ion o (2) is a unc ion u∈C((−∞, T]; H)∩L2(τ, T ;V)
o all T∈(τ, T ∗]∩R, wi h uτ=φand such ha o all ∈V,
d
d (u( ), ) + ν((u( ), )) + bN(u( ), u( ), )=( ( ), )+(g( , u ), ),
in he sense o D0(τ, T ∗).
Rema k 2. I uis a solu ion o (2) in he sense gi en abo e, hen usa is ies an
ene gy equali y, namely:
|u( )|2+ 2νZ
s
ku( )k2d
=|u(s)|2+ 2 Z
s
[( ( ), u( )) + (g( , u ), u( ))] d ∀s, ∈[τ, T∗]∩R.
Fi s , we will p o e he uniqueness o weak solu ions o ou model in a simila
way as done in [20] o he model wi hou delay. We will only include he de ailed
es ima es which in ol e he delay e m.

6 P. MAR´
IN-RUBIO, A. M. M´
ARQUEZ-DUR´
AN & J. REAL
Theo em 1. Unde he abo e assump ions, he e exis s a mos a weak solu ion u
o (2).
The p oo is simila o, bu a bi mo e complica ed han o he 2D-Na ie -S okes
equa ions and depends on he ollowing
Lemma 1. ([20]) Fo e e y u, ∈V, and each N > 0,
1. 0 ≤ kukFN(kuk)≤N,
2. |FN(kuk)−FN(k k)| ≤ 1
NFN(kuk)FN(k k)ku− k.
P oo o Theo em 1:Le u, be wo weak solu ions wi h he same ini ial condi ions
and se w= −u. Then, using he ene gy equali y, we ob ain
1
2
d
d |w|2+νkwk2+hNL(u, ), wi= (g( , )−g( , u ), w), ∈(τ, T∗),
whe e we ha e se hNL(u, ), wi=FN(kuk)b(u, u, w)−FN(k k)b( , , w).F om he
p ope ies o he ilinea o m bi easily ollows ha
hNL(u, ), wi=FN(kuk)b(w, u, w)+(FN(kuk)−FN(k k))b( , u, w)
+FN(k k)b( , w, w).
Now using Lemma 1, o mula (7) and Young’s inequali y (see [20] o he de ails)
he e exis s a cons an C3>0,which depends on C2and ν, such ha ,
| hNL(u, ), wi | ≤ νkwk2+C3N4|w|2.
Consequen ly, aking (g3) in o accoun , we ob ain
d
d |w( )|2≤2C3N4|w( )|2+ 2Lgkw kγ|w( )|, ∈(τ, T∗).
Obse e ha w(s) = 0 i s≤τ. The e o e, o ∈(τ, T∗) :
kw kγ= sup
θ≤0
eγθ|w( +θ)| ≤ sup
θ∈[τ− ,0]
|w( +θ)|.
Thus we ob ain
|w( )|2≤2C3N4Z
τ
|w(s)|2ds + 2LgZ
τ
sup
∈[τ,s]
|w( )||w(s)|ds
≤(2C3N4+ 2Lg)Z
τ
sup
∈[τ,s]
|w( )|2ds,
o any ∈[τ, T∗).
Now we deduce ha
sup
∈[τ, ]
|w( )|2≤(2C3N4+ 2Lg)Z
τ
sup
∈[τ,s]
|w( )|2ds,
o any ∈[τ, T∗),whence he G onwall lemma inishes he p oo .
Ou main esul is he ollowing
Theo em 2. Suppose ha ∈L2(τ, T; (L2(Ω))3) o all T∈(τ, T∗]∩R, g :
(τ, T∗)×Cγ(H)→(L2(Ω))3sa is ying he assump ions (g1)–(g3), and φ∈Cγ(H)
a e gi en, and ha 2γ > νλ1.Then, he e exis s a unique weak solu ion uo (2),
which in ac is a s ong solu ion in he sense ha
u∈C((τ, T ]; V)∩L2(τ+ε, T;D(A)),
3D-GMNS EQUATIONS WITH INFINITE DELAYS 7
o all 0< ε < T∗−τand any T∈(τ+ε, T∗]∩R.
Mo eo e , i φ(0) ∈V, hen usa is ies
u∈C([τ, T ]; V)∩L2(τ, T;D(A)),
o all T∈(τ, T∗]∩R.
P oo . We spli he p oo in se e al s eps.
S ep 1: A Gale kin scheme. Le us conside { j} ⊂ V, he o hono mal basis
o Ho all he eigen unc ions o he S okes ope a o . Deno e Vm= span[ 1, . . . , m]
and conside he p ojec o Pmu=Pm
j=1(u, j) j.
De ine also
um( ) =
m
X
j=1
αm,j( ) j
whe e he uppe sc ip mwill be used ins ead o (m) o sho since no con usion
is possible wi h powe s o u, and whe e he coe icien s αm,j a e equi ed o sa is y
he ollowing sys em:
d
d (um( ), j) + ν((um( ), j)) + bN(um( ), um( ), j)
= ( ( ), j)+(g( , um
), j),1≤j≤m, (8)
whe e he equa ions a e unde s ood in he sense o D0(τ, T∗),and he ini ial condi-
ions is um(τ+s) = Pmφ(s) o s∈(−∞,0].
The abo e sys em o o dina y unc ional di e en ial equa ions wi h in ini e delay
ul ills he condi ions o exis ence and uniqueness o local solu ion o [12, Th.1.1,
p.36].
Nex , we will deduce a p io i es ima es ha assu e ha he solu ions do exis
o all ime ∈[τ, T∗]∩R.
S ep 2: A p io i es ima es. Mul iplying (8) by umwe ob ain
1
2
d
d |um( )|2+νλ1
2|um( )|2+ν
2kum( )k2≤( ( ), um( )) + (g( , um
), um( ))
≤ | ( )||um( )|+Lgkum
kγ|um( )|
≤ν
4kum( )k2+| ( )|2
νλ1
+Lgkum
k2
γ.
Hence
|um( )|2+ν
2Z
τ
e−νλ1( −s)kum(s)k2ds
≤e−νλ1( −τ)|u(τ)|2+ 2 Z
τ
e−νλ1( −s)| (s)|2
νλ1
+Lgkum
sk2
γds. (9)
Fu he
kum
k2
γ≤max (sup
θ∈(−∞,τ− ]
e2γθ|φ(θ+ −τ)|2,sup
θ∈[τ− ,0] e2γθ−νλ1( −τ+θ)|u(τ)|2
+2e2γθ Z +θ
τ
e−νλ1( +θ−s)| (s)|2
νλ1
+Lgkum
sk2
γds).
8 P. MAR´
IN-RUBIO, A. M. M´
ARQUEZ-DUR´
AN & J. REAL
On he one hand
sup
θ∈(−∞,τ− ]
eγθ|φ(θ+ −τ)|= sup
θ≤0
eγ(θ−( −τ))|φ(θ)|
=e−γ( −τ)kφkγ.
On he o he hand, as we a e assuming ha 2γ > νλ1,
sup
θ∈[τ− ,0]
e2γθ−νλ1( −τ+θ)|u(τ)|2≤e−νλ1( −τ)|u(τ)|2
and
sup
θ∈[τ− ,0]
e2γθ Z +θ
τ
e−νλ1( +θ−s)| (s)|2
νλ1
+Lgkum
sk2
γds
≤Z
τ
e−νλ1( −s)| (s)|2
νλ1
+Lgkum
sk2
γds.
Collec ing hese inequali ies we deduce
kum
k2
γ≤e−νλ1( −τ)kφk2
γ+ 2 Z
τ
e−νλ1( −s)| ( )|2
νλ1
+Lgkum
sk2
γds.
By he G onwall lemma we ha e
kum
k2
γ≤e−(νλ1−2Lg)( −τ)kφk2
γ+2
νλ1Z
τ
e−(λ1ν−2Lg)( −s)| (s)|2ds.
Then we ob ain he ollowing es ima es: o any R > 0 and T∈(τ, T∗]∩R, he e
exis s a cons an C=C(τ, T, R),depending on some cons an s o he p oblem
(namely, λ1, ν, Lgand ), and on τ, T and R, such ha
kum
k2
γ≤C(τ, T, R)∀ ∈[τ, T],∀ kφkγ≤R, ∀m≥1.(10)
In pa icula , his implies ha
{um}is bounded in L∞(τ, T;H)∀T∈(τ, T∗]∩R.(11)
Now, i ollows om (9) and (10) ha
ν
2e−νλ1(T−τ)ZT
τ
kum(s)k2ds
≤ν
2ZT
τ
e−νλ1(T−s)kum(s)k2ds
≤ |u(τ)|2+ 2 ZT
τ
e−νλ1(T−s)| (s)|2
νλ1
+Lgkum
sk2
γds
≤R2+ 2 ZT
τ
e−νλ1(T−s)| (s)|2
νλ1
+LgC(τ, T, R)ds,
so ha we conclude he exis ence o ano he cons an ( elabelled he same) C(τ, T, R)
such ha
kumk2
L2(τ,T ;V)≤C(τ, T, R)∀ kφkγ≤R∀m≥1,∀T∈(τ, T∗]∩R.(12)
Now, obse e ha (8) is equi alen o
dum
d =−νAum−PmBN(um, um) + Pm ( ) + Pmg( , um
).(13)
3D-GMNS EQUATIONS WITH INFINITE DELAYS 9
F om (5), (11), (12) and (13), by he choice o he basis one also deduces ha
k(um)0k2
L2(τ,T ;V0)≤C(τ, T, R)∀ kφkγ≤R∀m≥1,∀T∈(τ, T∗]∩R.(14)
So, his implies he exis ence o a
u∈L∞(τ, T ;H)∩L2(τ, T;V) wi h u0∈L2(τ, T;V0),∀T∈(τ, T∗]∩R,
and a subsequence o {um}which con e ges weak-s a o uin L∞(τ, T;H),weakly
o uin L2(τ, T ;V),wi h {(um)0}con e ging weakly o u0in L2(τ, T;V0) o all
T∈(τ, T∗]∩R.
Obse e in pa icula ha u∈C([τ, T]; H) o all T∈(τ, T∗]∩R.
By a compac ness esul (c . [17, Ch.1,Th.5.1]), one can hen deduce ha a
subsequence in ac con e ges s ongly o uin L2(τ, T;H) and a.e. in (τ, T) wi h
alues in Hand a.e. in (τ, T)×Ω o all T∈(τ, T∗]∩R.
S ep 3: Some mo e a p io i es ima es. The es ima es ob ained abo e a e
no enough o pass o he limi and deduce ha uis a solu ion o (2). Namely, we
ha e wo main di icul ies. On he one hand, we need o pass o he limi in g(um),
his will be done in S ep 4, p o ing ha ac ually um
→u in Cγ(H).On o he
hand, he weak con e gence in L2(τ, T;V) is no enough o ensu e ha
kum( )k→ku( )k
o a leas
FN(kum( )k)→FN(ku( )k) o a.a. ,
which is needed o manage he nonlinea e m BN(um, um).
In o de o so ou his las ouble, we need o ind a s onge es ima e. We
p oceed now wi h ha . Take he inne p oduc o he Gale kin ODE (8) wi h Aum
and ob ain
1
2
d
d kum( )k2+ν|Aum( )|2+bN(um( ), um( ), Aum( ))
= ( ( ), Aum( )) + (g( , um
), Aum( )).(15)
Ob iously,
( ( ), Aum( )) ≤ | ( )||Aum( )| ≤ ν
8|Aum( )|+2
ν| ( )|2
and
|(g( , um
), Aum( ))| ≤ ν
8|Aum( )|2+2
ν|g( , um
)|2.
By (6), Lemma 1and Young’s inequali y, i ollows
|bN(um( ), um( ), Aum( ))| ≤ N
kum( )kC2kum( )k3/2|Aum( )|3/2
=NC2kum( )k1/2|Aum( )|3/2
≤ν
4|Aum( )|2+CNkum( )k2,
wi h CN=27(NC2)4
4ν3.
Thus (15) simpli ies o
d
d kum( )k2+ν|Aum( )|2≤4
ν| ( )|2+4
ν|g( , um
)|2+ 2CNkum( )k2.(16)
16 P. MAR´
IN-RUBIO, A. M. M´
ARQUEZ-DUR´
AN & J. REAL
Thus, i we ake
β=λ−1/2
1| |
ν−Lgλ−1
1
,
we ob ain ((Rmu, u)) ≥0∀u∈Vmsuch ha kuk=β.
Consequen ly by a co olla y o he B ouwe ’s ixed poin heo em (see [17, p.53]),
o each m≥1 he e exis um∈Vmsuch ha Rm(um)=0,wi h kumk ≤ β.
Obse e mo eo e ha Aum∈Vm,and he e o e
ν|Aum|2=−hBN(um, um), Aumi+ ( , Aum)+(g(um), Aum) (40)
≤ν
2|Aum|2− hBN(um, um), Aumi+| |2
ν+L2
gβ2
νλ1
.
Mo eo e , by (6) and Young’s inequali y,
|hBN(um, um), Aumi| ≤ ν
4|Aum|2+CNkumk2(41)
≤ν
4|Aum|2+CNβ2,
wi h CN=27(NC2)4
4ν3.
F om (40) and (41), we deduce ha he sequence {um}is bounded in D(A), and
consequen ly, by he compac injec ion o D(A) in V, we can ex ac a subsequence
{um0} ⊂ {um}, ha con e ges weakly in D(A) and s ongly in V o an elemen
u∗∈D(A). I is now s anda d o ake limi s in (38) and o ob ain ha u∗is an
s a iona y solu ion.
In o de o p o e he inal egula i y ema k, i is enough o ake in o accoun
ha e e y s a iona y solu ion u∗ o (34) is also a solu ion o (2), bu wi h ini ial
da a φ( ) = u∗ o ∈(−∞,0], and o cing e m +g(u∗). Thus, we can apply
Theo em 2.
Uniqueness Le us suppose ha u∗and eu∗a e wo s a iona y solu ions o (34).
Then,
νhAu∗−Aeu∗, i+hBN(u∗, u∗)−BN(eu∗,eu∗), i
= (g(u∗)−g(eu∗), ),∀ ∈V. (42)
Taking =u∗−eu∗and p oceeding as in (39) we ob ain om (42)
νku∗−eu∗k2≤ |FN(ku∗k)b(u∗−eu∗, u∗, u∗−eu∗)|
+|(FN(ku∗k)−FN(keu∗k))b(eu∗, u∗, u∗−eu∗)|
+λ−1
1Lgku∗−eu∗k2.(43)
F om his inequali y, aking in o accoun (4), ha b(eu∗, u∗, u∗−eu∗) = 0,and
he ac ha FN(ku∗k)≤1,we ob ain
νku∗−eu∗k2≤λ−1/4
1ku∗k ku∗−eu∗k2+λ−1
1Lgku∗−eu∗k2,
and he e o e, by he es ima e (36),
νku∗−eu∗k2≤ λ−1/4
1
λ−1/2
1| |
ν−λ−1
1Lg
+λ−1
1Lg!ku∗−eu∗k2.(44)

3D-GMNS EQUATIONS WITH INFINITE DELAYS 17
On he o he hand, i in (43) we use (4), and Lemma 1, i.e. ku∗kFN(ku∗k)≤N
and keu∗kFN(keu∗k)≤N, we ob ain
νku∗−eu∗k2≤Nλ−1/4
1ku∗−eu∗k2+λ−1
1Lgku∗−eu∗k2.(45)
F om (44) and (45) we deduce ha i (37) holds, hen u∗=eu∗.
Theo em 4. Assume ha he assump ions in Theo em 2wi h and gindependen
o ime and (37) hold. Then he e exis s a alue 0< λ < 2γsuch ha o he
solu ion u(·,0, φ)o (2) wi h τ= 0,T∗= +∞and φ∈Cγ(H), he ollowing
es ima es hold o all ≥0:
|u( , 0, φ)−u∗|2≤e−λ |φ(0) −u∗|2+Lg
2γ−λkφ−u∗k2
γ,(46)
ku (·,0, φ)−u∗k2
γ
≤max e−2γ kφ−u∗k2
γ, e−λ |φ(0) −u∗|2+Lg
2γ−λkφ−u∗k2
γ,(47)
whe e u∗is he unique s a iona y solu ion o (34) gi en by Theo em 3.
P oo . Fo sho deno e u( ) = u(·,0, φ).Le us also deno e w( ) = u( )−u∗.
Conside ing equa ions (34) o u( ) and (35) o u∗,one has
d
d (w( ), ) + ν((w( ), )) + bN(u( ), u( ), )−bN(u∗, u∗, )=(g(u )−g(u∗), ),
o > 0, o any ∈V.
F om ene gy equali y and he Lipschi z condi ion on g, and in oducing an ex-
ponen ial e m eλ wi h a posi i e alue λ o be ixed la e on, we ob ain
d
d (eλ |w( )|2)≤eλ λ|w( )|2−2νkw( )k2
+2|bN(u( ), u( ), w( ))−bN(u∗, u∗, w( ))|+ 2Lgkw kγ|w( )|),
o > 0.
Reasoning as o (44) and (45), we ha e
|bN(u( ), u( ), w)−bN(u∗, u∗, w)| ≤ µku( )−u∗k2,
whe e
µ:= min (Nλ−1/4
1,λ−3/4
1| |
ν−λ−1
1Lg).
Hence, using a Young inequali y wi h δ > 0 o be ixed la e on, we conclude
ha
d
d (eλ |w( )|2)≤eλ (−2ν+λλ−1
1+ 2µ+δλ−1
1Lg)kw( )k2+Lg
δeλ kw k2
γ.
The e o e, in eg a ing om 0 o , we ha e
eλ |w( )|2≤ |w(0)|2+Lg
δZ
0
eλskwsk2
γds
+(−2ν+λλ−1
1+ 2µ+δλ−1
1Lg)Z
0
eλskw(s)k2ds. (48)
18 P. MAR´
IN-RUBIO, A. M. M´
ARQUEZ-DUR´
AN & J. REAL
In o de o con ol he e m R
0eλskwsk2
γds, we p oceed as ollows.
Z
0
eλs sup
θ≤0
e2γθ|w(s+θ)|2ds
=Z
0
eλs max{sup
θ≤−s
e2γθ|w(s+θ)|2,sup
θ∈[−s,0]
e2γθ|w(s+θ)|2}ds
=Z
0
max{e−(2γ−λ)skφ−u∗k2
γ,sup
θ∈[−s,0]
e(2γ−λ)θeλ(s+θ)|w(s+θ)|2}ds.
So, i λ≤2γ, using he abo e equali y in (48), we ob ain
eλ |w( )|2≤ |w(0)|2+Lg
δkφ−u∗k2
γZ
0
e(λ−2γ)sds
+−2ν+λλ−1
1+2µ+δλ−1
1Lg+Lg(λ1δ)−1Z
0
max
∈[0,s]eλ kw( )k2ds.
Obse e ha he (op imal) choice o δ= 1 makes ha δλ−1
1Lg+Lg(λ1δ)−1is
minimal and he coe icien o he las in eg al is nega i e wi h a sui able choice o
λ∈(0,2γ) by (37). So, we can omi his e m and deduce ha
eλ |w( )|2≤ |w(0)|2+Lg
2γ−λ(1 −e(λ−2γ) )kφ−u∗k2
γ,
whence (46) ollows.
Finally, (47) can be deduced in he ollowing way:
kw k2
γ= sup
θ≤0
e2γθ|w( +θ)|2
= max{sup
θ∈(−∞,− ]
e2γθ|φ( +θ)−u∗|2,max
θ∈[− ,0] e2γθ|w( +θ)|2}
= max{e−2γ kφ−u∗k2
γ,max
θ∈[− ,0] e2γθ|w( +θ)|2},
and he second e m can be es ima ed using (46) and ha e(2γ−λ)θ≤1.
Acknowledgemen s. The au ho s would like o hank he e e ees o hei in e -
es ing sugges ions and commen s.
This wo k was pa ially suppo ed by Spanish Minis e io de Ciencia e Inno aci´on,
P ojec MTM2008-00088, and he Conseje ´ıa de Inno aci´on, Ciencia y Emp esa
(Jun a de Andaluc´ıa), P oyec o de Excelencia P07-FQM-02468.
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E-mail add ess, P. Ma ´ın-Rubio: [email p o ec ed]
E-mail add ess, A. M. M´a quez-Du ´an: [email p o ec ed]
E-mail add ess, J. Real: [email p o ec ed]