<p>In this paper, we consider a two-phase problem of inhomogeneous incompressible viscous fluids in the <i>N</i>-dimensional Euclidean space <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\textbf{R}^N\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi mathvariant="bold">R</mi> <mi>N</mi> </msup> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(N\ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>. One fluid occupies an upper half-space-like domain <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\Omega _+(t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Ω</mi> <mo>+</mo> </msub> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, while another fluid occupies <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\Omega _-(t)=\textbf{R}^N\setminus \overline{\Omega _+(t)}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Ω</mi> <mo>-</mo> </msub> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msup> <mi mathvariant="bold">R</mi> <mi>N</mi> </msup> <mo lspace="0.15em" rspace="0.15em" stretchy="false">\</mo> <mover> <mrow> <msub> <mi mathvariant="normal">Ω</mi> <mo>+</mo> </msub> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </mrow> <mo>¯</mo> </mover> </mrow> </math></EquationSource> </InlineEquation> for time <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(t\ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. The two fluids are thus separated from one another by a sharp interface for <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(t\ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, and the time-dependent domains <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\Omega _\pm (t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Ω</mi> <mo>±</mo> </msub> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> need to be determined as part of the problem. In this situation, it is known that local existence theorems hold for several two-phase flows such as homogeneous or inhomogeneous incompressible two-phase flows, compressible two-phase flows, and compressible-incompressible two-phase flows. On the other hand, our aim of this paper is to construct global-in-time solutions for small initial data and to show large time decay of solutions. Furthermore, this paper provides a new tool to prove global existence theorems for two-phase problems in unbounded domains on the basis of maximal regularity and time decay estimates of the two-phase Stokes semigroup in an <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(L_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>-in-time and <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(L_q\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mi>q</mi> </msub> </math></EquationSource> </InlineEquation>-in-space setting.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Global solvability for a two-phase problem of inhomogeneous incompressible viscous fluids

  • Kenta Oishi,
  • Hirokazu Saito

摘要

In this paper, we consider a two-phase problem of inhomogeneous incompressible viscous fluids in the N-dimensional Euclidean space \(\textbf{R}^N\) R N for \(N\ge 3\) N 3 . One fluid occupies an upper half-space-like domain \(\Omega _+(t)\) Ω + ( t ) , while another fluid occupies \(\Omega _-(t)=\textbf{R}^N\setminus \overline{\Omega _+(t)}\) Ω - ( t ) = R N \ Ω + ( t ) ¯ for time \(t\ge 0\) t 0 . The two fluids are thus separated from one another by a sharp interface for \(t\ge 0\) t 0 , and the time-dependent domains \(\Omega _\pm (t)\) Ω ± ( t ) need to be determined as part of the problem. In this situation, it is known that local existence theorems hold for several two-phase flows such as homogeneous or inhomogeneous incompressible two-phase flows, compressible two-phase flows, and compressible-incompressible two-phase flows. On the other hand, our aim of this paper is to construct global-in-time solutions for small initial data and to show large time decay of solutions. Furthermore, this paper provides a new tool to prove global existence theorems for two-phase problems in unbounded domains on the basis of maximal regularity and time decay estimates of the two-phase Stokes semigroup in an \(L_p\) L p -in-time and \(L_q\) L q -in-space setting.