<p>The Cauchy problem for non-isentropic compressible Navier-Stokes/Allen-Cahn system with degenerate heat-conductivity <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10255_2025_63_Article_IEq1.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="81" /> </InlineMediaObject> <EquationSource Format="TEX">\(\kappa (\theta) = \tilde \kappa {\theta ^\beta}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>κ</mi> <mo stretchy="false">(</mo> <mi>θ</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mrow> <mover> <mi>κ</mi> <mo stretchy="false">~</mo> </mover> </mrow> <mrow> <msup> <mi>θ</mi> <mi>β</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> in 1-D is discussed in this paper. This system is widely used to describe the motion of immiscible two-phase flow with diffused interface. The well-posedness for strong solution of this problem is established with the <i>H</i><sup>1</sup> initial data for density, temperature, velocity, and the <i>H</i><sup>2</sup> initial data for phase field. The result shows that no discontinuity of the phase field, vacuum, shock wave, mass or heat concentration will be developed at any finite time in the whole space. From the hydrodynamic point of view, this means that no matter how complex the interaction between the hydrodynamic and phase-field effects, phase separation will not occur, but the phase transition is possible.</p>

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The Cauchy Problem for Non-Isentropic Compressible Navier-Stokes/Allen-Cahn system with Degenerate Heat-Conductivity

  • Ya-zhou Chen,
  • Qiao-lin He,
  • Bin Huang,
  • Xiao-ding Shi

摘要

The Cauchy problem for non-isentropic compressible Navier-Stokes/Allen-Cahn system with degenerate heat-conductivity \(\kappa (\theta) = \tilde \kappa {\theta ^\beta}\) κ ( θ ) = κ ~ θ β in 1-D is discussed in this paper. This system is widely used to describe the motion of immiscible two-phase flow with diffused interface. The well-posedness for strong solution of this problem is established with the H1 initial data for density, temperature, velocity, and the H2 initial data for phase field. The result shows that no discontinuity of the phase field, vacuum, shock wave, mass or heat concentration will be developed at any finite time in the whole space. From the hydrodynamic point of view, this means that no matter how complex the interaction between the hydrodynamic and phase-field effects, phase separation will not occur, but the phase transition is possible.