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Nonflashing mass flux

Nonflashing partial pressure ratio Flashing partial pressure ratio Back pressure ratio Nonflashing mass flux Flashing mass flux Mass flux... [Pg.363]

It should be noted that the derivative is negative, so that at certain conditions the denominator of Eq. (15-51) can be zero, resulting in an infinite pressure gradient. This condition corresponds to the speed of sound, i.e., choked flow. For a nonflashing liquid and an ideal gas mixture, the corresponding maximum (choked) mass flux G follows directly from the definition of the speed of sound ... [Pg.464]


See other pages where Nonflashing mass flux is mentioned: [Pg.326]    [Pg.327]    [Pg.330]    [Pg.364]    [Pg.326]    [Pg.327]    [Pg.330]    [Pg.364]    [Pg.2293]    [Pg.2048]    [Pg.2297]   
See also in sourсe #XX -- [ Pg.326 ]




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