TY - JOUR
T1 - Nonlinear stability of Ekman boundary layers in rotating stratified fluids
AU - Koba, Hajime
PY - 2014/3
Y1 - 2014/3
N2 - A stationary solution of the rotating Navier-Stokes equations with a boundary condition is called an Ekman boundary layer. This booklet constructs stationary solutions of the rotating Navier-Stokes-Boussinesq equations with stratification effects in the case when the rotating axis is not necessarily perpendicular to the horizon. We call such stationary solutions Ekman layers. This booklet shows the existence of a weak solution to an Ekman perturbed system, which satisfies the strong energy inequality. Moreover, we discuss the uniqueness of weak solutions and compute the decay rate of weak solutions with respect to time under some assumptions on the Ekman layers and the physical parameters. It is also shown that there exists a unique global-in-time strong solution of the perturbed system when the initial datum is sufficiently small. Comparing a weak solution satisfying the strong energy inequality with the strong solution implies that the weak solution is smooth with respect to time when time is sufficiently large.
AB - A stationary solution of the rotating Navier-Stokes equations with a boundary condition is called an Ekman boundary layer. This booklet constructs stationary solutions of the rotating Navier-Stokes-Boussinesq equations with stratification effects in the case when the rotating axis is not necessarily perpendicular to the horizon. We call such stationary solutions Ekman layers. This booklet shows the existence of a weak solution to an Ekman perturbed system, which satisfies the strong energy inequality. Moreover, we discuss the uniqueness of weak solutions and compute the decay rate of weak solutions with respect to time under some assumptions on the Ekman layers and the physical parameters. It is also shown that there exists a unique global-in-time strong solution of the perturbed system when the initial datum is sufficiently small. Comparing a weak solution satisfying the strong energy inequality with the strong solution implies that the weak solution is smooth with respect to time when time is sufficiently large.
KW - Asymptotic stability
KW - Boussinesq system
KW - Coriolis force
KW - Ekman spiral
KW - Maximal Lp-regularity
KW - Perturbation theory
KW - Real interpolation theory
KW - Smoothness and regularity
KW - Stability of Ekman boundary layers
KW - Stratification effect
KW - Strong energy equality
KW - Strong energy inequality
KW - Strong solutions
KW - Uniqueness of weak solutions
KW - Weak solutions
UR - http://www.scopus.com/inward/record.url?scp=84891958891&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84891958891&partnerID=8YFLogxK
U2 - 10.1090/memo/1073
DO - 10.1090/memo/1073
M3 - Article
AN - SCOPUS:84891958891
SN - 0065-9266
VL - 228
SP - 1
EP - 127
JO - Memoirs of the American Mathematical Society
JF - Memoirs of the American Mathematical Society
IS - 1073
ER -