2016
DOI: 10.1016/j.jde.2016.09.010
|View full text |Cite
|
Sign up to set email alerts
|

Global strong L well-posedness of the 3D primitive equations with heat and salinity diffusion

Abstract: Consider the full primitive equations, i.e. the three dimensional primitive equations coupled to the equation for temperature and salinity, and subject to outer forces. It is shown that this set of equations is globally strongly well-posed for arbitrary large initial data lying in certain interpolation spaces, which are explicitly characterized as subspaces of H 2/p,p , 1 < p < ∞, satisfying certain boundary conditions. In particular, global well-posedeness of the full primitive equations is obtained for initi… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
35
0

Year Published

2016
2016
2020
2020

Publication Types

Select...
4
2

Relationship

1
5

Authors

Journals

citations
Cited by 38 publications
(35 citation statements)
references
References 34 publications
0
35
0
Order By: Relevance
“…The additional assumption on the time regularity of Ppf in Theorem assures that this solution is also an L 2 solution, and by Proposition vH1(δ,T;D(A2))C(false[δ,Tfalse];D(A2)) for δ(0,T). (c)Concerning analyticity of solutions, for solutions u to the Navier–Stokes equations in Rn with initial values in u0Ln(double-struckRn)n estimates on DβuLq(double-struckRn), βdouble-struckN0n, have been established in using heat kernel estimates. However, the method used there is not applicable in the presence of boundaries. (d)The surface pressure πs can be reconstructed from v , compare [, Equation (6.2)]. This gives πsLμq(0,T;Hper,01,pfalse(Gfalse)), where Hper,01,pfalse(Gfalse)=πsHper1,p(G):Gπs=0.…”
Section: Resultsmentioning
confidence: 99%
See 3 more Smart Citations
“…The additional assumption on the time regularity of Ppf in Theorem assures that this solution is also an L 2 solution, and by Proposition vH1(δ,T;D(A2))C(false[δ,Tfalse];D(A2)) for δ(0,T). (c)Concerning analyticity of solutions, for solutions u to the Navier–Stokes equations in Rn with initial values in u0Ln(double-struckRn)n estimates on DβuLq(double-struckRn), βdouble-struckN0n, have been established in using heat kernel estimates. However, the method used there is not applicable in the presence of boundaries. (d)The surface pressure πs can be reconstructed from v , compare [, Equation (6.2)]. This gives πsLμq(0,T;Hper,01,pfalse(Gfalse)), where Hper,01,pfalse(Gfalse)=πsHper1,p(G):Gπs=0.…”
Section: Resultsmentioning
confidence: 99%
“…The regularizing effect plays an important role when extending local solutions to global ones by means of certain a priori bounds. So far, in order to control the existence time in Lp‐spaces, H 2 ‐a priori bounds have been used in . In the following, we show that a priori bounds in the maximal regularity space L2(0,T;H2)H1(0,T;L2) are already sufficient to prove the global existence of a solution in LqLp‐spaces.…”
Section: Introductionmentioning
confidence: 82%
See 2 more Smart Citations
“…Remarkably, different from the three-dimensional Navier-Stokes equations, global existence and uniqueness of strong solutions to the three-dimensional primitive equations has already been known since the breakthrough work by Cao-Titi [16]. This global existence of strong solutions to the primitive equations were also proved later by Kobelkov [23] and Kukavica-Ziane [25], by using some different approaches, see also Hieber-Kashiwabara [22] and Hieber-Hussien-Kashiwabara [21] for some generalizations in the L p settings.…”
mentioning
confidence: 98%