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AMS 691 Special Topics in Applied Mathematics Lecture 5. James Glimm Department of Applied Mathematics and Statistics, Stony Brook University Brookhaven National Laboratory. Today. Viscosity Ideal gas Gamma law gas Shock Hugoniots for gamma law gas Rarefaction curves fro gamma law gas
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AMS 691Special Topics in Applied MathematicsLecture 5 James Glimm Department of Applied Mathematics and Statistics, Stony Brook University Brookhaven National Laboratory
Today Viscosity Ideal gas Gamma law gas Shock Hugoniots for gamma law gas Rarefaction curves fro gamma law gas Solution of Reimann problems
Two Phase NS Equationsimmiscible, Incompressible • Derive NS equations for variable density • Assume density is constant in each phase with a jump across the interface • Compute derivatives of all discontinuous functions using the laws of distribution derivatives • I.e. multiply by a smooth test function and integrate formally by parts • Leads to jump relations at the interface • Away from the interface, use normal (constant density) NS eq. • At interface use jump relations • New force term at interface • Surface tension causes a jump discontinuity in the pressure proportional to the surface curvature. Proportionality constant is called surface tension
Reference forideal fluid EOS and gamma law EOS @Book{CouFri67, author = "R. Courant and K. Friedrichs", title = "Supersonic Flow and Shock Waves", publisher = "Springer-Verlag", address = "New York", year = "1967", }
Hugoniot curve for gamma law gas Rarefaction waves are isentropic, so to study them we study Isentropic gas dynamics (2x2, no energy equation). is EOS.