<p>This is the first in a series of papers connecting the boundary conditions for the compressible Navier-Stokes system from the Boltzmann equations with the Maxwell reflection boundary. The slip boundary conditions are formally derived from the Boltzmann equation with both specular and almost specular reflection boundary conditions. That is, the accommodation coefficient <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\alpha _\varepsilon =O(\varepsilon ^\beta )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>α</mi> <mi>ε</mi> </msub> <mo>=</mo> <mi>O</mi> <mrow> <mo stretchy="false">(</mo> <msup> <mi>ε</mi> <mi>β</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\beta &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> or <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\alpha _\varepsilon =0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>α</mi> <mi>ε</mi> </msub> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. Here, the small number <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\varepsilon &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ε</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> denotes the Knudsen number. The systematic formal analysis is based on the Chapman-Enskog expansion and the analysis of the Knudsen layer. In particular, for the first time, we employ the appropriate ansatz for the general <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\beta &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>β</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. This completes the program started in [<CitationRef CitationID="CR2">2</CitationRef>]. In the second part, the compressible Navier-Stokes-Fourier approximation for the Boltzmann equation with specular reflection in general bounded domains is rigorously justified. The uniform regularity for the compressible Navier-Stokes system with the derived boundary conditions is investigated. For the remainder equation, the <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(L^2\text{- }L^6\text{- }L^\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mtext>-</mtext> <mspace width="0.333333em" /> <msup> <mi>L</mi> <mn>6</mn> </msup> <mtext>-</mtext> <mspace width="0.333333em" /> <msup> <mi>L</mi> <mi>∞</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> framework is employed to obtain uniform estimates in <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ε</mi> </math></EquationSource> </InlineEquation>.</p>

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Compressible Navier-Stokes System with Slip Boundary from the Boltzmann Equation with Reflection Boundary: Derivations and Justifications

  • Ning Jiang,
  • Yulong Wu

摘要

This is the first in a series of papers connecting the boundary conditions for the compressible Navier-Stokes system from the Boltzmann equations with the Maxwell reflection boundary. The slip boundary conditions are formally derived from the Boltzmann equation with both specular and almost specular reflection boundary conditions. That is, the accommodation coefficient \(\alpha _\varepsilon =O(\varepsilon ^\beta )\) α ε = O ( ε β ) with \(\beta >0\) β > 0 or \(\alpha _\varepsilon =0\) α ε = 0 . Here, the small number \(\varepsilon >0\) ε > 0 denotes the Knudsen number. The systematic formal analysis is based on the Chapman-Enskog expansion and the analysis of the Knudsen layer. In particular, for the first time, we employ the appropriate ansatz for the general \(\beta >0\) β > 0 . This completes the program started in [2]. In the second part, the compressible Navier-Stokes-Fourier approximation for the Boltzmann equation with specular reflection in general bounded domains is rigorously justified. The uniform regularity for the compressible Navier-Stokes system with the derived boundary conditions is investigated. For the remainder equation, the \(L^2\text{- }L^6\text{- }L^\infty \) L 2 - L 6 - L framework is employed to obtain uniform estimates in \(\varepsilon \) ε .