TY - JOUR
T1 - On decay properties of solutions to the Stokes equations with surface tension and gravity in the half space
AU - Saito, Hirokazu
AU - Shibata, Yoshihiro
N1 - Funding Information:
The first author was partly supported by Grant-in-Aid for JSPS Fellows (No. 25-5259) and by JSPS Japanese-German Graduate Externship at Waseda University. The second author was partly supported by JST CREST, JSPS Grant-in-aid for Scientific Research (S) (No. 24224004), and JSPS Japanese-Germann Graduate Externship at Waseda University.
Publisher Copyright:
©2016 The Mathematical Society of Japan.
PY - 2016
Y1 - 2016
N2 - In this paper, we proved decay properties of solutions to the Stokes equations with surface tension and gravity in the half space R+N = {(x′, xN) | x′ ∈ RN-1, xN > 0} (N ≥ 2). In order to prove the decay properties, we first show that the zero points λ± of Lopatinskii determinant for some resolvent problem associated with the Stokes equations have the asymptotics: λ± = ±icg1/2|ζ′|1/2-2|ζ′|2+O(|ζ′|5/2) as |ζ′| → 0, where cg > 0 is the gravitational acceleration and ζ′ ∈ RN-1 is the tangential variable in the Fourier space. We next shift the integral path in the representation formula of the Stokes semi-group to the complex left half-plane by Cauchy's integral theorem, and then it is decomposed into closed curves enclosing λ± and the remainder part. We finally see, by the residue theorem, that the low frequency part of the solution to the Stokes equations behaves like the convolution of the (N - 1)-dimensional heat kernel and Fζ′-1[e±icg1/2|ζ′|1/2t](x′) formally, where Fζ′-1 is the inverse Fourier transform with respect to ζ′. However, main task in our approach is to show that the remainder part in the above decomposition decay faster than the residue part.
AB - In this paper, we proved decay properties of solutions to the Stokes equations with surface tension and gravity in the half space R+N = {(x′, xN) | x′ ∈ RN-1, xN > 0} (N ≥ 2). In order to prove the decay properties, we first show that the zero points λ± of Lopatinskii determinant for some resolvent problem associated with the Stokes equations have the asymptotics: λ± = ±icg1/2|ζ′|1/2-2|ζ′|2+O(|ζ′|5/2) as |ζ′| → 0, where cg > 0 is the gravitational acceleration and ζ′ ∈ RN-1 is the tangential variable in the Fourier space. We next shift the integral path in the representation formula of the Stokes semi-group to the complex left half-plane by Cauchy's integral theorem, and then it is decomposed into closed curves enclosing λ± and the remainder part. We finally see, by the residue theorem, that the low frequency part of the solution to the Stokes equations behaves like the convolution of the (N - 1)-dimensional heat kernel and Fζ′-1[e±icg1/2|ζ′|1/2t](x′) formally, where Fζ′-1 is the inverse Fourier transform with respect to ζ′. However, main task in our approach is to show that the remainder part in the above decomposition decay faster than the residue part.
KW - Decay properties
KW - Gravity
KW - Half-space problem
KW - Stokes equations
KW - Surface tension
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U2 - 10.2969/jmsj/06841559
DO - 10.2969/jmsj/06841559
M3 - Article
AN - SCOPUS:84992500429
SN - 0025-5645
VL - 68
SP - 1559
EP - 1614
JO - Journal of the Mathematical Society of Japan
JF - Journal of the Mathematical Society of Japan
IS - 4
ER -