ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu
REMARKS ON REGULARITY CRITERIA FOR THE 3D NAVIER-STOKES EQUATIONS
RUIYING WEI, YIN LI
Abstract. In this article, we study the regularity criteria for the 3D Navier- Stokes equations involving derivatives of the partial components of the velocity.
It is proved that if∇huebelongs to Triebel-Lizorkin space,∇u3 oru3 belongs to Morrey-Campanato space, then the solution remains smooth on [0, T].
1. Introduction
This article is devoted to the Cauchy problem for the following incompressible 3D Navier-Stokes equation:
ut+ (u· ∇)u+∇p=4u, x∈R3, t >0
divu= 0, x∈R3, t >0 (1.1) with initial data
u(x,0) =u0, x∈R3, (1.2)
where u = (u1(x, t), u2(x, t), u3(x, t)) and p = p(x, t) denote the unknown veloc- ity vector and the unknown scalar pressure, respectively. In the last century, Leray [11] and Hopf [8] proved the global existence of a weak solution u(x, t) ∈ L∞(0,∞;L2(R3))∩L2(0,∞;H1(R3)) to (1.1)-(1.3) for any given initial datum u0(x) ∈ L2(R3). However, whether or not such a weak solution is regular and unique is still a challenging open problem. From that time on, different criteria for regularity of the weak solutions has been proposed.
The classical Prodi-Serrin conditions (see [16, 18, 19]) say that if u∈Lt(0, T;Ls(R3)), 2
t +3
s = 1, 3≤s≤ ∞,
then the solution is smooth. Similar results is showed by Beir˜ao da Veiga [1]
involving the velocity gradient growth condition:
∇u∈Lt(0, T;Ls(R3)), 2 t +3
s = 2, 3
2 < s≤ ∞.
Actually, whether the weak solution is smooth when a part of the velocity com- ponents is involved. As for this direction, later on, criteria just for one velocity
2000Mathematics Subject Classification. 35Q35, 76D05.
Key words and phrases. Regularity criteria; Triebel-Lizorkin space; Morrey-Campanato space.
c
2014 Texas State University - San Marcos.
Submitted June 23, 2014. Published October 29, 2014.
1
component appeared. The first result in this direction is due to Neustupa et al [15]
(see also Zhou [21]), where the authors showed that if u3∈Lt(0, T;Ls(R3)), 2
t +3 s =1
2, s∈(6,∞],
then the solution is smooth. A similar result, for the gradient of one velocity component, is independently due to Zhou [22] and Pokorn´y [17]. In [22], Zhou proved that if
∇u3∈Lt(0, T;Ls(R3)), 2 t +3
s = 3
2, 3≤s <∞.
then the solution is smooth on [0, T]. This result is extended by Zhou and Pokorn´y [26]; that is,
∇u3∈Lt(0, T;Ls(R3)), 2 t +3
s = 23
12, 2≤s≤3.
Further criteria, including several components of the velocity gradient, pressure or other quantities, can be found, here we just list some. Zhou and Pokorn´y [25]
proved the regularity condition
u3∈Lt(0, T;Ls(R3)), 2 t +3
s =3 4 + 1
2s, s >10 3 .
And in [10], Jia and Zhou proved that if a weak solution u satisfies one of the following two conditions:
u3∈L∞(0, T;L103(R3)); ∇u3∈L∞(0, T;L30/19(R3)),
then u is regular on [0, T]. Dong and Zhang [5] proved that if the horizontal derivatives of the two velocity components
Z T 0
k∇hu(s)k˜ B˙0∞,∞ds <∞,
then the solution keeps smoothness up to timeT, where ˜u= (u1, u2,0), and∇hu˜= (∂1u, ∂˜ 2u,˜ 0). For other kinds of regularity criteria, see [2, 6, 7, 9, 23, 24, 28, 29, 30]
and the references cited therein.
Throughout this paperCwill denote a generic positive constant which can vary from line to line. For simplicity, we shall useR
f(x)dx to denoteR
R3f(x)dx, use k · kp to denotek · kLp.
The purpose of this article is to improve and extend above known regularity criterion of weak solution for the equations (1.1), (1.2) to the Triebel-Lizorkin space and Morrey-Campanato spaces. The main results of this paper read:
Theorem 1.1. Assume that u0 ∈ H1(R3) with divu0 = 0. u(x,t) is the corre- sponding weak solution to (1.1)and (1.2)on[0, T). If additionally
Z T 0
k∇heu(·, t)kp˙
F0
q,2 3q
dt <∞, with 2 p+3
q = 2, 3
2 < q≤ ∞, (1.3) then the solution remains smooth on[0, T].
Theorem 1.2. Assume that u0 ∈ H1(R3) with divu0 = 0. u(x, t) is the corre- sponding weak solution to (1.1)and (1.2)on[0, T). If additionally
Z T 0
k∇u3(·, t)k
8 3(2−r)
M˙p,3r
dt <∞, with 0< r≤1, 2≤p≤ 3
r, (1.4)
then the solution remains smooth on[0, T].
Theorem 1.3. Assume that u0 ∈ H1(R3) with divu0 = 0. u(x,t) is the corre- sponding weak solution to (1.1)and (1.2)on[0, T). If additionally
Z T 0
ku3(·, t)k
8 3−4r
M˙p,3r
dt <∞, with 0< r < 3
4, 2≤p≤ 3
r, (1.5)
then the solution remains smooth on[0, T].
Remark 1.4. Noticing that the classical Riesz transformation is bounded in ˙B0∞,∞, if we takeq=∞in Theorem 1.1, then the classical Beal-Kato-Majda criterion for the Navier-Stokes equations is obtained; that is, if
Z T 0
k∇hu(·, t)ke B˙∞,∞0 dt <∞ then the solution remains smooth on [0, T].
Remark 1.5. Since (it is proved in [12, 13])
Lq(R3) = ˙Mq,q(R3)⊂M˙p,q(R3), 1< p≤q <∞, L3r(R3)⊂M˙p,3r(R3)⊂X˙r(R3)⊂M˙2,3r(R3), 2< p≤3
r, 0< r <3 2, the result of Theorem 1.2 is an improved version of [27, Theorem 2]. Also we obtain, if
Z T 0
ku3(·, t)k
8 3−4r
X˙r dt <∞, with 0< r < 3 4, then the solution remains smooth on [0, T].
2. Preliminaries
In this section, we shall introduce the Littlewood-Paley decomposition theory, and then give some definitions of the homogeneous Besov space, homogeneous Triebel-Lizorkin space, Morrey-Campanato space and multiplier space as well as some relate spaces used throughout this paper. Before this, let us first recall the weak solutions of (1.1)-(1.3):
Letu0∈L2(R3) with∇ ·u0= 0, a measurableR3-valued vectoruis said to be a weak solution of (1.1)-(1.3) if the following conditions hold:
(1) u(x, t)∈L∞(0,∞;L2(R3))∩L2(0,∞;H1(R3));
(2) usolves (1.1)-(1.2) in the sense of distributions;
(3) the energy inequality holds; i.e, kuk22+ 2
Z t 0
k4u(·, τ)k22dτ ≤ ku0k22, 0≤t≤T.
Let us choose a nonnegative radial function ϕ ∈ C∞(R3) be supported in the annulus {ξ ∈ R3 : 34 ≤ |ξ| ≤ 83}, such that P∞
l=−∞ϕ(2−lξ) = 1,∀ξ 6= 0. For f ∈S0(R3), the frequency projection operators4lis defined as
4lf =F−1(ϕ(2−j·))∗f,
whereF−1(g) is the inverse Fourier transform ofg. The formal decomposition f =
∞
X
l=−∞
4lf. (2.1)
is called the homogeneous Littlewood-Paley decomposition. Noticing 4lf =
l+1
X
j=l−1
4j(4lf)
and using the Young inequality, we have the following class Bernstein inequality:
Lemma 2.1 ([3]). Let α∈N, then for all 1 ≤p≤q≤ ∞, sup|α|=kk∂α4lfkq ≤ C2lk+3l(1p−1q)k4lfkp. andC is a constant independent off, l.
For s ∈ R and (p, q) ∈ [1,∞]×[1,∞], the homogeneous Besov space ˙Bp,qs is defined by
S˙sp,q={f ∈Z0(R3) :kfkS˙p,qs <∞}, where
kfkB˙p,qs =
P
j∈z2jsqk4jf(·)kqp1/q
, 1≤q <∞, supj∈z2jsk4jf(·)kp, q=∞.
andZ0(R3) denote the dual space of
Z0(R3) ={f ∈S(R3) :Dαfˆ(0) = 0.∀a∈N3}.
On the other hand, for s∈R,(p, q)∈[1,∞)×[1,∞], and for s∈R, p =q=∞, the homogenous Triebel-Lizorkin space is defined as
F˙p,qs ={f ∈Z0(R3) :kfkF˙p,qs <∞}, kfkF˙p,qs =
(k(P
j∈z2jsq|4jf(·)|q)1/qkp, 1≤q <∞, ksupj∈z(2js|4jf(·)|)kp, q=∞.
Notice that by Minkowski inequality, we have the following two imbedding relations:
B˙p,qs ⊂F˙p,qs , q≤p;
F˙p,qs ⊂B˙p,qs , p≤q.
and the following two inclusions:
H˙s= ˙B2,2s = ˙F2,2s , L∞⊂F˙∞,∞0 = ˙B∞,∞0 . We refer to [20] for more properties.
For 1< q ≤p <∞, the homogeneous Morrey-Campanato space inR3 is M˙p,q=
f ∈Lqloc(R3);kfkM˙p,q = sup
x∈R3
sup
R>0
Rp3−3qkfkq(B(x,R))<∞ , For 1≤p0≤q0<∞, we define the homogeneous space
N˙p0,q0 =n
f ∈Lq0|f =X
k∈N
gk, where gk∈Lqcomp0 (R3) and X
k∈N
d3(
1 p0−q10)
k kgkkq0 <∞, where dk = diam(suppgk)<∞o .
For 0< α <3/2, we say that a function belongs to the multiplier spacesM( ˙Hα, L2) if it maps, by pointwise multiplication, ˙Hα toL2:
X˙α:=M( ˙Hα, L2) :=
f ∈S0;kf·gkL2 ≤CkgkH˙α,∀g∈H˙α .
Here, ˙Hα is the homogeneous Sobolev space of orderα, H˙α=
f ∈L1loc;kfkL2 ≡Z
R3
|ξ|2α|ˆu(ξ)|21/2
<∞ . whereLp(1≤p≤ ∞) is the Lebsgue space endowed with normk · kp.
Lemma 2.2([4, 12]). Let1≤p0≤q0<∞, andp, qsuch that 1p+p10 = 1,1q+q10 = 1.
ThenM˙p,q is the dual space ofN˙p0,q0.
Lemma 2.3 ([4, 7, 12]). Let 1 < p0 ≤ q0 < 2, m≥ 2, and 1p +p10 = 1. Denote α=−n2 +np +mn ∈ (0,1] Then there exists a constant C > 0, such that for any u∈Lm(Rn), v∈H˙α(Rn),
ku·vkN˙p0,q0 ≤CkukLmkvkH˙α.
Lemma 2.4 ([13]). For 0 ≤r ≤ 32, let the space M( ˙B2r,1 → L2) be the space of functions which are locally square integrable onR3 and such that pointwise multi- plication with these functions maps boundedly the Besov spaceB˙2r,1(R3)toL2(R3).
The norm inM( ˙Br,12 →L2)is given by the operator norm of pointwise multiplica- tion:
kfkM( ˙Br,1
2 →L2)= sup{kf gk2:kgkB˙r,12 ≤1}.
Then,f belongs toM( ˙B2r,1→L2)if and only iff belongs toM˙2,3r (with equivalence of norms).
3. The proof of main results
Proof of Theorem 1.1. Multiplying (1.1)1 by −4u, integrating by parts, noting that∇ ·u= 0, we have
1 2
d dt
Z
|∇u|2dx+ Z
|4u|2dx= Z
[(u· 5)u]· 4u dx=:I. (3.1) Next we estimate the right-hand side of (3.1), with the help of integration by parts and−∂3u3=∂1u1+∂2u2, one shows that
I=−
3
X
i,j,k=1
Z
∂kui∂iuj∂kujdx
=−
2
X
i,j=1 3
X
k=1
Z
∂kui∂iuj∂kujdx−
2
X
i,k=1
Z
∂kui∂iu3∂ku3dx
−
2
X
j,k=1
Z
∂ku3∂3uj∂kujdx−
3
X
k=1
Z
∂ku3∂3u3∂ku3dx
−
2
X
i=1
Z
∂3ui∂iu3∂3u3dx−
2
X
j=1
Z
∂3u3∂3uj∂3ujdx
≤C Z
|∇heu||∇u|2dx.
Thus, the above inequality implies 1
2 d
dtk∇uk22+k4uk22≤C Z
|∇hu||∇u|e 2dx. (3.2)
Using the Littlewood-Paley decomposition (2.1),∇huecan be written as
∇hue= X
j<−N
4j(∇heu) +
N
X
j=−N
4j(∇hu) +e X
j>N
4j(∇hu).e
where N is a positive integer to be chosen later. Substituting this into (3.2), one obtains
1 2
d
dtk∇uk22+k4uk22
≤C X
j<−N
Z
|4j(∇hu)||∇u|e 2dx+C
N
X
j=−N
Z
|4j(∇heu)||∇u|2dx +CX
j>N
Z
|4j(∇hu)||∇u|e 2dx
=:K1+K2+K3.
(3.3)
ForKi(i= 1,2,3), we now give the estimates one by one. ForK1, using the H¨older inequality, the Young inequality and Lemma 2.1, it follows that
K1≤C X
j<−N
k4j(∇hu)ke ∞k∇uk22
≤C X
j<−N
23j/2k4j(∇hu)ke 2k∇uk22
≤C X
j<−N
23j1/2 X
j<−N
k4j(∇hu)ke 221/2
k∇uk22
≤C2−3N/2k∇uk32.
(3.4)
Where in the last inequality, we use the fact that for alls∈R, ˙Hs= ˙B2,2s . ForK2, by the H¨older inequality and the Young inequality, one has
K2=C Z N
X
j=−N
|4j(∇hu)||∇u|e 2dx
≤CN2q−32q
Z XN
j=−N
|4j(∇hu)|e 2q/33/(2q)
|∇u|2dx
≤CN2q−32q k∇heukF˙0
q,2q 3
k∇uk22q q−1
≤CN2q−32q k∇heukF˙0
q,2q 3
k∇uk
2q−3 q
2 k4uk3/q2
≤ 1
2k4uk22+CNk∇heuk
2q 2q−3
F˙0
q,2q 3
k∇uk22.
(3.5)
where we used the interpolation inequality
kuks≤Ckuk23s−12kuk32˙−3s
H1 , for 2≤s≤6.
Finally, using H¨older inequality and Lemma 2.1,K3 can be estimated as K3=C X
j>N
Z
|4j(∇heu)||∇u|2dx
≤C X
j>N
k4j(∇heu)k3k∇uk23
≤C X
j>N
2j2k4j(∇heu)k2k∇uk23
≤C(X
j>N
2−j)1/2(X
j>N
22jk4j(∇hu)ke 22)1/2k∇uk2k4uk2
≤C2−N/2k∇uk2k4uk22.
(3.6)
Substituting (3.4), (3.5) and (3.6) in (3.3), we obtain d
dtk∇uk22+k4uk22
≤C2−32Nk∇uk32+CNk∇huke
2q 2q−3
F˙0
q,2q 3
k∇uk22+C2−N/2k∇uk2k4uk22.
(3.7)
Now we chooseN such thatC2−N/2k∇uk2≤ 12; that is N ≥ln(k∇uk22+e) + lnC
ln 2 + 2.
Thus (3.7) implies d
dtk∇uk22≤C+Ck∇huke p˙
F0
q,2q 3
ln(k∇uk22+e)k∇uk22. Taking the Gronwall inequality into consideration, we obtain
ln(k∇uk22+e)≤Ch 1 +
Z T 0
k∇heukp˙
F0
q,2q 3
(τ)dτ ·e
RT 0 k∇huke p˙
F0 q,2q
3
(τ)dτ
i . The proof of Theorem 1.1 is complete under the condition (1.3).
Proof of Theorem 1.2. Multiplying (1.1)1 by −4hu, integrating by parts, noting that∇ ·u= 0, we have
1 2
d dt
Z
|∇hu|2dx+ Z
|∇∇hu|2dx= Z
[(u· 5)u]· 4hu dx=:J. (3.8) Next we estimate the right-hand side of (3.8), with the help of integration by parts and−∂3u3=∂1u1+∂2u2, one shows that
J =−
3
X
i,j=1 2
X
k=1
Z
∂kui∂iuj∂kujdx
=−
2
X
i,j,k=1
Z
∂kui∂iuj∂kujdx−
2
X
i,k=1
Z
∂kui∂iu3∂ku3dx
−
3
X
j=1 2
X
k=1
Z
∂ku3∂3uj∂kujdx
=:J1+J2+J3.
(3.9)
ForJ2 andJ3, we obtain
|J2+J3| ≤C Z
|∇u3||∇hu||∇u|dx. (3.10) J1 is a sum of eight terms, using the fact−∂3u3=∂1u1+∂2u2, we can estimate it as
J1=− Z
(∂1u1+∂2u2)[(∂1u1)2−∂1u1∂2u2+ (∂2u2)2]dx
− Z
(∂1u1+∂2u2)[(∂2u1)2+∂1u2∂2u1+ (∂1u2)2]dx
= Z
∂3u3[(∂1u1)2−∂1u1∂2u2+ (∂2u2)2+ (∂2u1)2+∂1u2∂2u1+ (∂1u2)2]dx
≤C Z
|∇u3||∇hu||∇u|dx.
(3.11) Substituting the estimates (3.9)-(3.11) in (3.8), we obtain
1 2
d
dtk∇huk22+k∇∇huk22≤C Z
|∇u3||∇hu||∇u|dx=:L. (3.12) when 2< p≤ 3r, using Lemmas 2.2 and 2.3, and the Young inequality, we obtain
L≤Ck∇u3k ˙
Mp,3rk|∇u| · |∇hu|k
N˙p0,3−r3
≤Ck∇u3k ˙
Mp,3rk∇hukH˙rk∇uk2
≤Ck∇u3k ˙
Mp,3rk∇ukL2k∇huk1−r2 k∇∇hukr2
≤1
2k∇∇huk22+Ck∇u3k
2 2−r
M˙p,r3
k∇uk22.
(3.13)
where we used the inequality kfkH˙r =k|ξ|rfkˆ 2= (
Z
|ξ|2r|fˆ|2r|fˆ|2−2rdξ)1/2≤ kfk1−r2 k∇fkr2, with 0< r≤1.
In the casep= 2, using H¨olders inequality, Lemma 2.4, and the Young inequality, we can estimateLas
L≤Ck|∇u3| · |∇hu|k2k∇uk2
≤Ck∇u3k ˙
M2,3rk∇hukB˙2r,1k∇uk2
≤Ck∇u3k ˙
M2,3rk∇huk1−r2 k∇∇hukr2k∇uk2
≤ 1
2k∇∇huk22+Ck∇u3k
2 2−r
M˙2,3r
k∇uk22.
(3.14)
where we used the following interpolation inequality [14]: for 0≤r≤1,kfkB˙r,12 ≤ kfk1−r2 k∇fkr2.
Now, gathering (3.13) and (3.14) together and substituting into (3.12), we obtain d
dtk∇huk22+k∇∇huk22≤Ck∇u3k
2 2−r
M˙p,3r
k∇uk22. (3.15)
Multiplying (1.1)1 by−4u, integrating by parts, noting that∇ ·u= 0, we have (see [25])
1 2
d
dtk∇uk22+k4uk22= Z
[(u· 5)u]· 4u dx
≤C Z
|∇hu||∇u|2dx
≤Ck∇huk2k∇uk24
≤Ck∇huk2k∇uk1/22 k∇uk632
≤Ck∇huk2k∇uk1/22 k∇∇huk2k4uk1/22 . Integrating, with respect tot, yields
1
2k∇u(t)k22+ Z t
0
k4u(τ)k22dτ
≤1
2k∇u0k22+C sup
0≤τ≤t
k∇hu(τ)k2( Z t
0
k∇u(τ)k22dτ)1/4
×Z t 0
k∇∇hu(τ)k22dτ1/2Z t 0
k4u(τ)k22dτ1/4 .
(3.16)
Substituting (3.15) in (3.16), using H¨olders inequality and the Young inequality, we obtain
1
2k∇u(t)k22+ Z t
0
k4u(τ)k22dτ
≤1
2k∇u0k22+ (C+C Z t
0
k∇u3k
2 2−r
M˙p,3r
k∇u(τ)k22dτ)Z t 0
k4u(τ)k22dτ1/4
≤C+CZ t 0
k∇u3k
2 2−r
M˙p,3r
k∇u(τ)k232k∇u(τ)k1/22 dτ4/3 +1
2 Z t
0
k4u(τ)k22dτ
≤C+CZ t 0
k∇u3k
8 3(2−r)
M˙p,3r
k∇u(τ)k22dτZ t 0
k∇u(τ)k22dτ1/3
+1 2
Z t 0
k4u(τ)k22dτ
≤C+C Z t
0
k∇u3k
8 3(2−r)
M˙p,3r k∇u(τ)k22dτ +1 2
Z t 0
k4u(τ)k22dτ.
(3.17)
Absorbing the last term into the left hand side, applying the Gronwall inequality and combining with the standard continuation argument, we conclude that the solu- tionsucan be extended beyondt=Tprovided that∇u3∈L3(2−r)8 (0, T; ˙Mp,3r(R3)).
This completes the proof of Theorem 1.2.
Proof of Theorem 1.3. We start from (3.9), we can estimateJ2 andJ3 as
|J2+J3| ≤C Z
|u3||∇u||∇∇hu|dx. (3.18)
From (3.11), we find that
J1≤C Z
|u3||∇u||∇∇hu|dx. (3.19) Combining (3.9),(3.17), (3.18) with (3.8), we obtain
1 2
d
dtk∇huk22+k∇∇huk22≤C Z
|u3||∇u||∇∇hu|dx=:V. (3.20) When 2< p≤3r, similarly as in the proof ofLin (3.13), we obtain
V ≤Cku3k ˙
Mp,3rk|∇u| · |∇∇hu|k˙
Np0,3−r3
≤Cku3k ˙
Mp,3rk∇ukH˙rk∇∇huk2
≤Cku3k ˙
Mp,3rk∇∇hukL2k∇uk1−r2 k4ukr2
≤ 1
2k∇∇huk22+Cku3k2
M˙p,3rk∇uk2(1−r)2 k4uk2r2 .
(3.21)
Whenp= 2, similarly as in the proof ofL in (3.14), we have V ≤Ck|u3| · |∇u|k2k∇∇huk2
≤Cku3k ˙
M2,3rk∇ukB˙2r,1k∇∇huk2
≤Cku3k ˙
M2,3rk∇uk1−r2 k4ukr2k∇∇huk2
≤ 1
2k∇∇huk22+Cku3k2˙
M2,3rk∇uk2(1−r)2 k4uk2r2 .
(3.22)
Substituting (3.21) and (3.22) in (3.20), we find that d
dtk∇huk22+k∇∇huk22≤Cku3k2
M˙2,3rk∇uk2(1−r)2 k4uk2r2 . (3.23) Substituting (3.23) in (3.16), we obtain
1
2k∇u(t)k22+ Z t
0
k4u(τ)k22dτ
≤ 1
2k∇u0k22+ C+C
Z t 0
ku3k2˙
Mp,3rk∇u(τ)k2(1−r)2 k4u(τ)k2r2 dτ
×Z t 0
k4u(τ)k22dτ1/4
≤C+1 4
Z t 0
k4u(τ)k22dτ +CZ t 0
ku3k2˙
Mp,3rk∇u(τ)k2(1−r)2 k4u(τ)k2r2 dτ4/3
≤C+1 4
Z t 0
k4u(τ)k22dτ +CZ t 0
k4u(τ)k22dτ4r/3
×Z t 0
ku3k
2 1−r
M˙p,3r
k∇u(τ)k22dτ4(1−r)3
≤C+1 2
Z t 0
k4u(τ)k22dτ +CZ t 0
ku3k
2 1−r
M˙p,3r
k∇u(τ)k
3−4r 2(1−r)
2 k∇u(τ)k
1 2(1−r)
2 dτ
4(1−r) 3−4r
≤C+1 2
Z t 0
k4u(τ)k22dτ +CZ t 0
ku3k
8 3−4r
M˙p,3r
k∇u(τ)k22dτZ t 0
k∇u(τ)k22dτ3−4r1
≤C+1 2
Z t 0
k4u(τ)k22dτ +C Z t
0
ku3k
8 3−4r
M˙p,3r
k∇u(τ)k22dτ.
By a similar argument as in the proof of Theorem 1.2, provided that u3 ∈ L3−4r8 (0, T; ˙Mp,3r(R3)), we complete the proof of Theorem 1.3.
Acknowledgements. Ruiying Wei and Yin Li would like to express sincere grat- itude to Professor Zheng-an Yao of Sun Yat-sen University for enthusiastic guid- ance and constant encouragement. This work is partially supported by Guang- dong Provincial culture of seedling of China (no. 2013LYM0081), and Guangdong Provincial NSF of China (no. S2012010010069), the Shaoguan Science and Technol- ogy Foundation (no. 313140546), and Science Foundation of Shaoguan University.
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Ruiying Wei
School of Mathematics and Information Science, Shaoguan University, Shaoguan, Guangdong 512005, China.
Department of Mathematics, Sun Yat-sen University , Guangzhou, Guangdong 510275, China
E-mail address:weiruiying521@163.com
Yin Li
School of Mathematics and Information Science, Shaoguan University, Shaoguan, Guangdong 512005, China.
Department of Mathematics, Sun Yat-sen University , Guangzhou, Guangdong 510275, China
E-mail address:liyin2009521@163.com