Similarity between flashing and nonflashing two‐phase flows

Under certain simplifying assumptions , the generalized solutions developed recently for homogeneous-equilibrium flashing choked flow can be extended to the nonflashing flow case by simply redefining the dimensionless parameter known as ω in the final equations.Based on a theorical approach in deriving a more general dimensionless parameter , a unified treatement is shown to be possible for these compressible flow processes.