Skip to main navigation Skip to search Skip to main content

WELL-POSEDNESS FOR MOVING INTERFACES WITH SURFACE TENSION IN IDEAL COMPRESSIBLE MHD

  • Yuri TRAKHININ
  • , Tao WANG*
  • *Corresponding author for this work

Research output: Journal Publications and ReviewsRGC 21 - Publication in refereed journalpeer-review

62 Downloads (CityUHK Scholars)

Abstract

We study the local well-posedness for an interface with surface tension that separates a perfectly conducting inviscid fluid from a vacuum. The fluid flow is governed by the equations of three-dimensional ideal compressible magnetohydrodynamics (MHD), while the vacuum magnetic and electric fields are supposed to satisfy the pre-Maxwell equations. The fluid and vacuum magnetic fields are tangential to the interface. This renders a nonlinear hyperbolic-elliptic coupled problem with a characteristic free boundary. We introduce some suitable regularization to establish the solvability and tame estimates for the linearized problem. Combining the linear well-posedness result with a modified Nash-Moser iteration scheme, we prove the local existence and uniqueness of solutions of the nonlinear problem. The non-collinearity condition required by Secchi and Trakhinin [Nonlinearity, 27 (2014), pp. 105-169] for the case of zero surface tension becomes unnecessary in our result, which verifies the stabilizing effect of surface tension on the evolution of moving vacuum interfaces in ideal compressible MHD.
Original languageEnglish
Pages (from-to)5888-5921
JournalSIAM Journal on Mathematical Analysis
Volume54
Issue number6
Online published9 Nov 2022
DOIs
Publication statusPublished - Dec 2022

Research Keywords

  • ideal compressible MHD
  • moving interface
  • pre-Maxwell equations
  • surface tension
  • well-posedness

Publisher's Copyright Statement

  • COPYRIGHT TERMS OF DEPOSITED FINAL PUBLISHED VERSION FILE: © 2022, Society for Industrial and Applied Mathematics.

Fingerprint

Dive into the research topics of 'WELL-POSEDNESS FOR MOVING INTERFACES WITH SURFACE TENSION IN IDEAL COMPRESSIBLE MHD'. Together they form a unique fingerprint.

Cite this