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Rankine-Hugoniot jump equations

The term energy per unit area is referred to as the energy fluence (Ref 8). Recalling the Rankin-Hugoniot jump conditions, specifically the mass and momentum equations for a shock, we had derived that... [Pg.311]

These equations can be combined to eliminate the velocities, yielding the Rankine Hugoniot equation for internal energy jump in terms of pressures and specific volumes (V s 1/p)... [Pg.11]

Conservation equations Expressions that equate the mass, momentum, and energy across a steady wave or shock discontinuity ((2.1)-(2.3)). Also known as the jump conditions or the Rankine-Hugoniot relations. [Pg.40]

The downstream fluid is considered to be an equilibrium state, which could be either liquid, a liquid-vapor mixture, or pure vapor depending on the solution branch and fluid type. For single-phase downstream states, the jump equations (1-3) must be solved numerically by an iterative procedure. This is most conveniently performed by combining equations 1-3 to obtain the Rankine-Hugoniot equation. [Pg.8]


See other pages where Rankine-Hugoniot jump equations is mentioned: [Pg.179]    [Pg.180]    [Pg.181]    [Pg.183]    [Pg.474]    [Pg.179]    [Pg.180]    [Pg.181]    [Pg.183]    [Pg.474]    [Pg.232]    [Pg.15]    [Pg.942]    [Pg.943]   
See also in sourсe #XX -- [ Pg.179 ]




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