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A linearly-degenerate characteristic curve is a contact wave
Statement
Let be linearly degenerate on a neighborhood and let be its local rarefaction curve. Then the states and are joined by a Rankine–Hugoniot jump of speed , and the corresponding moving discontinuity is a weak solution. The characteristic speed is equal on the two sides; this is a contact wave, not a strict Lax shock.
Facts & Assumptions
Given: A linearly-degenerate eigenpair and its local integral curve.
Strictly hyperbolic conservation systems and characteristic families: and for a linearly-degenerate family.
Rankine–Hugoniot jumps and Lax shocks: the jump condition is .
A moving jump is a weak solution exactly under Rankine–Hugoniot: a moving jump is weak exactly when that equality holds.
Proof
Along the curve, the chain rule gives , so . Also .
Integrating the second identity from to yields , the Rankine–Hugoniot equality [F3]. Applying [F4] gives the weak moving contact wave; equality of the characteristic speed on both sides was proved in step 1.1.
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Used by
Dependency tree · two levels
9 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Alberto Bressan, Hyperbolic Conservation Laws: An Illustrated Tutorial (standard reference, not scraped)
- Randall J. LeVeque, Numerical Methods for Conservation Laws (standard reference, not scraped)