A Riemann problem for a one-dimensional system of conservation laws has two constant initial states, for and for . The data and equation are invariant under . When the physically admissible entropy solution is unique, this invariance makes it a self-similar solution depending on . For ideal-gas compressible flow, the characteristic speeds are . The two acoustic families carry shock waves or rarefaction waves, while the middle family carries a contact discontinuity. Sufficiently strong separating velocities can instead create a vacuum region.
Two positive uniform ideal-gas states can be joined by one nontrivial rarefaction wave precisely when their specific entropy agrees, , and for one they satisfy with . These equations are the constant-entropy and Riemann invariant conditions of the self-similar ideal-gas rarefaction. They are sufficient because its affine profiles match the two states at and , and . The left family has , while the right family has . The inequality alone does not impose the two matching equalities.
A contact discontinuity in one-dimensional gas dynamics moves with the common fluid velocity and has continuous pressure, while mass density and specific entropy can jump. The mass jump condition is automatic with common ; momentum conservation then requires . The energy jump condition is also satisfied. Thus a contact is a material interface, not a compression shock. A smooth self-similar positive-density flow cannot spread this zero-speed-relative-to-the-fluid family into a fan: on an interval would require both and, from continuity, .
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