Consider a one-dimensional simple small-amplitude solution
to the
isentropic compressible Euler equations which has smooth initial data, coincides with
a constant state outside a compact set, and forms a shock in finite time. Viewing
as a
plane-symmetric solution to the full compressible Euler equations in three
dimensions, we prove that the shock-formation mechanism for the solution
is
stable against all sufficiently small and compactly supported perturbations. In
particular, these perturbations are allowed to break the symmetry and have
nontrivial vorticity and variable entropy.
Our approach reveals the full structure of the set of blowup-points at the first
singular time: within the constant-time hypersurface of first blowup, the solution’s
first-order Cartesian coordinate partial derivatives blow up precisely on the zero level
set of a function that measures the inverse foliation density of a family of
characteristic hypersurfaces. Moreover, relative to a set of geometric coordinates
constructed out of an acoustic eikonal function, the fluid solution and the inverse
foliation density function remain smooth up to the shock; the blowup of the
solution’s Cartesian coordinate partial derivatives is caused by a degeneracy
between the geometric and Cartesian coordinates, signified by the vanishing of
the inverse foliation density (i.e., the intersection of the characteristics).