Ideal systems like MHD and Euler flow may develop singularities in vorticity
(w = curl v). Viscosity and resistivity are dissipative regularizations. We
propose a minimal, local, conservative, nonlinear, dispersive regularization of
compressible flow and ideal MHD, in analogy with the KdV regularization of the
1D Hopf equation. This work significantly extends earlier work on
incompressible Euler and ideal MHD. It involves a cut-off lambda inversely
proportional to square-root of density rho, which is like a position-dependent
mean free path. In MHD, lambda can be taken of order the electron collisionless
skin depth. The regularizing twirl' term is - lambda w x curl w. Such a term could be important in high speed flows with vorticity and arise in an expansion of kinetic equations in Knudsen number. A magnetic analogue of the twirl term - (B x curl B)/(rho mu_0), arises as the Lorentz force in ideal MHD. Our regularization preserves symmetries of the ideal systems, and with appropriate boundary conditions, implies associated conservation laws. Energy and enstrophy are subject to a priori bounds determined by initial data. A Hamiltonian and Poisson bracket formulation is developed and used to generalize the constitutive relation to bound higher moments of w and curl w. A swirl’
velocity field is shown to transport w/rho and B/rho, generalizing the
Kelvin-Helmholtz and Alfv'en theorems. The steady regularized equations are
used to model a rotating vortex, MHD pinch, plane vortex sheet, channel flow,
plane flow and propagating spherical and cylindrical vortices; solutions are
more regular than corresponding Eulerian ones. The proposed regularization
could facilitate simulations of fluid/MHD equations and provide a consistent
statistical mechanics of vortices/current filaments in 3D, without blowup of
enstrophy. Implications for detailed analyses of fluid and plasma systems are
discussed.

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