ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu
WELL-POSEDNESS OF A POROUS MEDIUM FLOW WITH FRACTIONAL PRESSURE IN SOBOLEV SPACES
XUHUAN ZHOU, WEILIANG XIAO
Abstract. We prove the existence of a non-negative solution for a linear degenerate diffusion transport equation from which we derive the existence and uniqueness of the solution for the fractional porous medium equation in Sobolev spacesHαwith nonnegative initial data,α >d2+ 1. We also correct a mistake in our previous paper [14].
1. Introduction We consider the porous medium type equation
∂tu=∇ ·(u∇p), p= (−∆)−su, 0< s <1, u(x,0)≥0, (1.1) where x ∈ Rn, n ≥ 2, and t > 0 and the fractional Laplacian (−4)s/2 := Λs is given by the psuedo differential operator with symbol|ξ|s, that is:
(−4)s/2f = Λsf =F−1|ξ|sFf.
Using the Riesz potential, one can also define this operator as (−4)s/2f(x) = Λsf(x) =cn,s
Z
Rn
f(x)−f(y)
|y|n+s dy.
This model is based on Darcy’s law with pressure, p, is given by an inverse fractional Laplacian operator. It was first introduced by Caffarelli and V´azquez [4], in which they proved the existence of a weak solution whenu0is a bounded function with exponential decay at infinity. Forα= n+2−2sn , Caffarelli, Soria and V´azquez [3] proved that the bounded nonnegative solutions areCα continuous in a strip of space-time fors6= 1/2. And same conclusion for the indexs= 1/2 was proved by Caffarelli and V´azquez in [5]. [7, 6, 13] give a detailed description of the large-time asymptotic behaviour of the solutions of (1.1). [2, 12] consider degenerate cases and show the existence and properties of self-similar solutions. Allen, Caffarelli and Vasseur [1] study the equation with fractional time derivative, and proved the H¨older continuity for its weak solutions.
In this paper, we study the existence and uniqueness of solutions of (1.1) in Sobolev spaces. Unlike considering the existence of weak solution in L∞ or con- structing approximate solutions of linear transport systems, we solve equation (1.1) by constructing solutions to a linear degenerate diffusion transport systems. The
2010Mathematics Subject Classification. 35K55, 35K65, 76S05.
Key words and phrases. Fractional porous medium equation; Sobolev space;
degenerate diffusion transport equation.
c
2017 Texas State University.
Submitted December 22, 2016. Published October 3, 2017.
1
well-posedness and properties of the linear degenerate diffusion transport are inter- esting results by themselves and lead us to proving that for s∈[12,1), α > d2+ 1, u0∈Hα(Rn) nonnegative, and some T0>0, the equation (1.1) inRn×[0, T0] has a unique solutions. Besides, using the methods and results in this paper, we correct a mistake in our previous paper [14].
2. Preliminaries Defineρ∈Cc∞(Rn) by
ρ(x) =
(c0exp(−1−|x|1 2),|x|<1, 0,|x| ≥1,
wherec0is selected such thatR
ρ(x)dx= 1. LetJ be defined by Ju=ρ∗u=−nρ(·
)∗u.
This operator satisfies the following properties.
Proposition 2.1. (1) ΛsJu=JΛsu,s∈R.
(2) For allu∈Lp(Rn),v∈Hα(Rn), with 1p+1q = 1,R
(Jf)g=R
f(Jg).
(3) For allu∈Hα(Rn),
→0limkJu−ukHα = 0, lim
→0kJu−ukHα−1 ≤CkukHα. (4) For allu∈Hα(Rn),s∈R,k∈Z∪ {0}, then
kJukHα+k≤ Cαk
k kukHα, kJDkukL∞ ≤ Ck
n2+kkukHα
The following propositions can be found in [8, 9].
Proposition 2.2. Suppose that s >0 and1 < p <∞. If f, g ∈ S, the Schwartz class, then we have
kΛs(f g)−fΛsgkLp≤ck∇fkLp1kgkH˙s−1,p2+ckgkLp4kfkH˙s,p3, kΛs(f g)kLp≤ckfkLp1kgkH˙s,p2 +ckgkLp4kfkH˙s,p3
withp2, p3∈(1,+∞)such that 1p =p1
1 +p1
2 = p1
3 +p1
4. Proposition 2.3. If 0≤s≤2,f ∈ S(Rn), then
2f(x)Λsf(x)≥Λsf2(x) for allx∈Rn.
Proposition 2.4. Let α1 and α2 be two real numbers such that α1 < n2,α2< n2 and α1+α2 >0. Then there exists a constant C =Cα1,α2 ≥0 such that for all f ∈H˙α1 andg∈H˙α2,
kf gkH˙α≤CkfkH˙α1kgkH˙α2, whereα=α1+α2−n2.
3. Main results
Theorem 3.1. If s ∈ [1/2,1], T > 0, α > n2 + 1, u0 ∈ Hα(Rn), v ≥ 0 and v∈C([0, T];Hα(Rn)), then the linear initial-value problem
∂tu=∇u· ∇(−∆)−sv−v(−∆)1−su,
u(x,0) =u0. (3.1)
has a unique solution u ∈ C1([0, T];Hα(Rn)). If the initial data u0 ≥ 0, then u≥0,(x, t)∈Rn×[0, T].
Proof. For any >0, we consider the linear problem
∂tu=F(u) =J(∇Ju· ∇(−∆)−sv)−J(v(−∆)1−sJu),
u(x,0) =u0. (3.2)
By Propositions 2.1 and 2.2 and bys≥ 12 we can estimate kF(u1)−F(u2)kHα
=kJ(∇J(u1−u2)· ∇(−∆)−sv)−J(v(−∆)1−sJ(u1−u2)kHα
≤C(,kvkHα)ku1−u2kHα.
Using Picard iterations, for any α > n2 + 1, > 0, there exists aT =T(u∗)>0, problem (3.2) has a unique solution u∈C1([0, T);Hα). By Propositions 2.1 and 2.3,
1 2
d
dtkuk2L2 = Z
∇Ju· ∇(−∆)−svJu− Z
v(−∆)1−sJuJu
≤1 2
Z
∇|Ju|2· ∇(−∆)−sv−1 2
Z
v(−∆)1−s|Ju|2
≤1 2
Z
|Ju|2(−∆)1−sv−1 2
Z
|Ju|2(−∆)1−sv= 0.
Moreover, for anyα >0, 1
2 d
dtkΛαuk2L2
= Z
Λα(∇Ju· ∇(−∆)−sv)JΛαu− Z
Λα(v(−∆)1−sJu)ΛαJu
≤Ck[Λα,∇(−∆)−sv]∇JukL2kΛαukL2+ Z
∇(−∆)−svΛα∇JuΛαJu +Ck[Λα, v](−∆)1−sJukL2kΛαukL2−
Z
vΛα(−∆)1−sJuΛαJu. By Proposition 2.2 and Sobolev embeddings,
k[Λα,∇(−∆)−sv]∇JukL2
≤Ck(−∆)1−svkL∞kΛα−1∇JukL2+k∇(−∆)−svkH˙αk∇JukL∞
≤CkvkHαkukHα, k[Λα, v](−∆)1−sJukL2
≤Ck∇vkL∞k(−∆)1−sJukH˙α−1+kvkH˙αk(−∆)1−sJukL∞
≤CkvkHαkukHα.
By Proposition 2.3, Z
∇(−∆)−svΛα∇JuΛαJu− Z
vΛα(−∆)1−sJuΛαJu
≤ 1 2
Z
∇(−∆)−sv∇(ΛαJu)2−1 2
Z
v(−∆)1−s(ΛαJu)2
≤CkvkHαkuk2Hα. Combining the above estimates,
d
dtku(·, t)kHα ≤CkvkHαkukHα. By Gronwall’s inequality,
ku(·, t)kHα≤ ku0kHαexp(C sup
0≤t≤T
kvkHα).
Such the solutionu exists on [0, T]. Similarly, d
dtku(·, t)kHα−1≤CkvkHαkukHα ≤C(kvkHα,ku0kHα, T).
By Aubin compactness theorem [11], there is a subsequence of{un1}n≥1 that con- vergence strongly touin C([0, T];Hα). Ifα > d2+ 1, Hα,→C1, so uis a solution of (3.3).
Ifuand ˜uare two solutions of problem (3.3), thenw=u−˜usatisfies
∂tw=∇w· ∇(−∆)−sv−v(−∆)1−sw, w(x,0) = 0.
Similarly, we get dtdkwkL2 ≤ 0 and dtdkwkH˙α ≤ kvkHαkwkHα, i.e, dtdkwkHα ≤ kvkHαkwkHα. By Gronwall’s inequality,u(x, t) = 0, (x, t)∈Rn×[0, T].
Since u0 ≥ 0 then if there exists a first time t0 where for some point x0 we haveu(x0, t0) = 0, then (x0, t0) will correspond to a minimum point and therefore
∇u(x0, t0) = 0, and
(−∆)1−su(x) =c
Z u(x)−u(y)
|y|n+2−2s dy≤0.
Henceut|(x0,t0)≥0. Sou(x, t)≥0 for all (x, t)∈Rn×[0, T].
Theorem 3.2. Let n≥2,s∈[12,1),α >d2+ 1,u0∈Hα(Rn), andu0≥0. Then there the linear initial value problem
∂tu=∇ ·(u∇(−∆)−su), u(x,0) =u0.
has a unique solution u ∈ C1([0, T0], Hα(Rn)). If the initial data u0 ≥ 0, then u≥0,(x, t)∈Rn×[0, T0].
Proof. Set u1 = u0. Note that ∂tu = ∇ ·(u∇(−∆)−su) = ∇u· ∇(−∆)−su− u(−∆)1−su, and let{un} be the sequence defined by
∂tun+1=∇un+1· ∇(−∆)−sun−un(−∆)1−su(n+1),
un+1(x,0) =u0. (3.3)
By Theorem 3.1,u2∈C([0, T);Hα), for allT <∞, satisfiesu2≥0 and sup
0≤t≤T
ku2kHα ≤ ku0kHαexp(Cku1kHαT).
If exp(2Cku1kHαT0)≤2, for exampleT0=2C(1+kuln 2
0kHα), we have sup
0≤t≤T0
ku2kHα ≤2ku0kHα.
By the standard induction argument, ifun∈C([0, T0];Hα),un≥0 is a solution of (3.3) withkunkHα ≤2ku0kHα. By Theorem 3.1 un+1∈C([0, T0];Hα) , un+1≥0 and
sup
0≤t≤T0
kun+1kHα≤ ku0kHαexp(CkunkHαT0)≤2ku0kHα, d
dtkun+1kHα−1 ≤CkunkHαkun+1kHα≤Cku0k2Hα.
By Aubin compactness theorem [11], there is a subsequence ofun that convergence strongly touin C([0, T];Hα). Ifu≥0,u˜≥0 are two solutions of problem (3.3), thenw=u−u˜satisfies
∂tw=∇ ·(w∇(−∆)−su) +∇ ·(˜u∇(−∆)−sw), w(x,0) = 0.
By Proposition 2.2, 1
2 d
dtkwk2L2= Z
w∇ ·(w∇(−∆)−su) + Z
w∇˜u· ∇(−∆)−sw− Z
w˜u(−∆)1−sw
=:I1+I2+I3. Note that
I1= Z
w∇w· ∇(−∆)−su= 1 2
Z
∇w2· ∇(−∆)−su
= 1 2
Z
w2(−∆)1−su≤CkukHαkwk2L2, I3≤ −1
2 Z
u(−∆)˜ 1−sw2= Z
−1
2(−∆)1−su˜·w2≤CkukHαkwk2L2. Whens >1/2,
I2≤CkwkL2k∇u· ∇(−∆)−swkL2
≤CkwkL2k∇ukH˙n2+1−2sk∇(−∆)−swkH˙2s−1 ≤CkukHαkwk2L2.
When s = 1/2, the above estimates are still valid. Combining the above esti- mates we have dtdkwkL2 ≤CkwkL2kukHα. By Gronwall’s inequality we can deduce
w(x, t) = 0 on [0, T0].
4. Correction
In [14], trying to establish the well-posedness of (1.1) in Besov spaces the authors incurred in a mistake in page 9 when estimating the termJ40 in equation [14, (4.5)].
To correct the mistake, we modify our proof the following way.
[14, Theorem 1.1] Let n ≥ 2, s ∈ [12,1], α > n+ 1. If the initial data u0 ∈ B1,∞α , then there existsT =T(ku0kBα1,∞) such that (1.1) has a unique solution in
[0, T]×Rn. Such a solution belongs toC1([0, T];B1,∞α+2s−2)∩L∞([0, T];B1,∞β ), with β∈[α+ 2s−2, α].
Proof. First we construct the approximate equation
u(n+1)t =∇u(n+1)· ∇(−4)−su(n) −u(n) (−4)1−su(n+1); u(n+1)(0) =σ∗u0, u(1) =σ∗u0.
(4.1) By the argument in section 2, there exists a sequence u(n) that solves the linear systems (4.1). Assuming thatu0 ≥0, we prove thatu(n+1) ≥0. Inspired by [4], we assume thatx0 is a point of minimum of u(n+1) at timet=t0. This indicates that∇u(n+1)(x0) = 0, and
(−4)1−su(n+1)(x0) =c
Z u(x0)−u(y)
|y|n+2(1−s) dy≤0.
Thus we deduce that ∂t∂u(n+1) t=t
0 ≥ 0, and by induction we have u(n+1) ≥ 0.
Arguing as in [14], taking4j on (4.1), we obtain
∂t4ju(n+1)=X
[4j, ∂i(−4)−su(n) ]∂iun+1+X
∂i(−4)−su(n) 4j(∂iu(n+1))
−[4j, u(n) ](−4)1−su(n+1)−u(n) 4j(−4)1−su(n+1). Multiplying both sides by 4ju(n+1)
|4ju(n+1)|, and integrating over Rd, then denote the corresponding part in the right side by J10, J20, J30, J40, respectively. We obtain the estimates,
J10 ≤C2−jαku(n+1)kB1,∞α ku(n)kBα+1−2s
1,∞
J20 ≤C2−jαku(n+1)kB1,∞α ku(n)kBα+1−2s
1,∞
J30 ≤C2−jαku(n)kBα
1,∞ku(n+1)kBα+1−2s
1,∞ .
The estimate for the termJ40 is now replaced by J40 =−
Z
u(n)4j(−4)1−su(n+1) 4ju(n+1)
|4ju(n+1)|
≤ − Z
u(n)(−4)1−s|4ju(n+1)|
≤ − Z
(−4)1−su(n)|4u(n+1)|
≤2−jαkunkBr+2−2s
1,∞ ku(n+1)kBα1,∞.
Here r > d is any real number. The first inequality uses the following pointwise estimate.
Proposition 4.1 ([10]). If0≤α≤2,p≥1, then
p|f(x)|p−2f(x)Λαf(x)≥Λα|f(x)|p. for any f ∈ S(Rd)
Takingrsuch thatr+ 2−2s < α, e.g. setr=α−1, we conclude d
dtku(n+1)kBα1,,∞ ≤ ku(n)kB1,,∞α ku(n+1)kB1,,∞α .
The other parts of the proof need no modification.
Acknowledgement. We are very grateful to Ph. D. Mitia Duerinckx for point- ing out our mistake and share some good views on this problem. This paper is supported by the NNSF of China under grants No. 11601223 and No.11626213.
References
[1] M. Allen, L. Caffarelli, A. Vasseur; Porous medium flow with both a fractional potential pressure and fractional time derivative.arXiv preprint arXiv:1509.06325, 2015.
[2] P. Biler, C. Imbert, G. Karch;The nonlocal porous medium equation: Barenblatt profiles and other weak solutions.Archive for Rational Mechanics and Analysis, 2015, 215(2): 497-529.
[3] L. Caffarelli, F. Soria, J. L. V´azquez;Regularity of solutions of the fractional porous medium flow.arXiv preprint arXiv:1201.6048, 2012.
[4] L. Caffarelli, J. L. V´azquez;Nonlinear porous medium flow with fractional potential pressure.
Archive for rational mechanics and analysis, 2011, 202(2): 537-565.
[5] L. Caffarelli, J. L. V´azquez;Regularity of solutions of the fractional porous medium flow with exponent1/2.arXiv preprint arXiv:1409.8190, 2014.
[6] L. Caffarelli, J. L. V´azquez;Asymptotic behaviour of a porous medium equation with frac- tional diffusion.arXiv preprint arXiv:1004.1096, 2010.
[7] J. A. Carrillo, Y. Huang, M. C. Santos, J. L. V´azquez; Exponential convergence towards stationary states for the 1D porous medium equation with fractional pressure. Journal of Differential Equations, 2015, 258(3): 736-763.
[8] A. C´ordoba, D. C´ordoba;A maximum principle applied to quasi-geostrophic equations.Com- munications in mathematical physics, 2004, 249(3): 511-528.
[9] N. Ju;Existence and uniqueness of the solution to the dissipative 2D quasi-geostrophic equa- tions in the Sobolev space.Communications in Mathematical Physics, 2004, 251(2): 365-376.
[10] C. Miao, J. Wu, Z. Zhang; Littlewood-Paley Theory and Applications to Fluid Dynamics Equations.Monographson Modern Pure Mathematics, No. 142 (Science Press, Beijing, 2012).
[11] J. Simon.Compact sets in the spaceLp(0, T;B) Ann. Mat. Pura. Appl., (4) 146, 1987, 65-96.
[12] D. Stan, F. del Teso, J. L. V´azquez; Transformations of self-similar solutions for porous medium equations of fractional type. Nonlinear Analysis: Theory, Methods Applications, 2015, 119: 62-73.
[13] J. L. V´azquez; Nonlinear diffusion with fractional Laplacian operators.Nonlinear Partial Differential Equations. Springer Berlin Heidelberg, 2012: 271-298.
[14] X. Zhou, W. Xiao, J. Chen; Fractional porous medium and mean field equations in Besov spaces, Electron. J. Differential Equations, 2014 (2014), no. 199, 1-14.
Xuhuan Zhou
Department of Information Technology, Nanjing Forest Police College, 210023 Nan- jing, China
E-mail address:[email protected]
Weiliang Xiao
School of Applied Mathematics, Nanjing University of Finance and Economics, 210023 Nanjing, China
E-mail address:[email protected]