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Exploring Compressible Flow Dynamics

Nov 13, 2024

Lesson 15b: Compressible Flow and Choking in Converging Ducts

Key Topics

  • Compressible flow in a converging duct
  • Calculating critical conditions
  • Mass flow rate
  • Definition and examples of choking

Compressible Flow in a Converging Duct

  • Flow starts at zero speed and accelerates into the converging duct.
  • Subsonic flow:
    • Speed increases
    • Mach number increases
    • Pressure decreases
    • Temperature decreases
  • Mach number approaches 1 but cannot exceed 1 in a converging duct.

Supersonic Flow

  • If Mach number > 1, the behavior is opposite (not valid in a converging duct):
    • Speed decreases
    • Mach number decreases
    • Pressure increases
    • Temperature increases

Choking in Converging Ducts

  • Choking: Occurs when Mach number equals 1 at the exit plane.
  • Flow cannot go supersonic in a converging duct.
  • Conditions at choke point denoted with an asterisk (), e.g., T, P*, ρ*.

Back Pressure (Pb)

  • Determines whether flow is subsonic or choked.
  • Three cases:
    • Pb > P*: Flow is subsonic, Mach number < 1.
    • Pb = P*: Flow is choked, Mach number = 1.
    • Pb < P*: Flow remains choked, Pe = P*.
  • Choked flow continues unchanged despite further decreases in Pb.

Example Problem

  • Scenario: Air flows from pressurized tank through a converging nozzle.
  • Given: P0, T0, Pb, exit area.
  • Need to determine if flow is subsonic, sonic, or supersonic.
  • Calculate Mach number and temperature at the exit plane.

Assumptions

  • 1D flow, ideal gas, steady, nearly isentropic, adiabatic conditions.
  • Large tank with constant conditions.

Findings

  • Part A: Flow is subsonic when Pb > P*.
  • Part B: Flow becomes sonic at Pb = P* (83.47 kPa).
  • Part C: Mach number at exit plane MaE = 0.823, Temperature TE = 458 K.

Mass Flow Rate in Converging Duct

[ \dot{m} = \rho VA ]

  • Derived using the ideal gas law and Mach number relations.

  • General equation for mass flow rate:

    [ \dot{m} = P_0 A M_A \sqrt{\frac{k}{R}} \left(1 + \frac{k-1}{2}M_A^2\right)^{-\frac{k+1}{2(k-1)}} ]

  • For choked flow, simplifies when Ma = 1.

Example Calculation

  • Mass flow rate for given conditions: 3.54 kg/s
  • Maximum mass flow rate (m_dot_max) for choked flow: 3.64 kg/s

Conclusion

  • Understanding the relationship between back pressure and flow conditions is crucial in compressible flow.
  • Choked flow is significant as it determines limits of flow rate changes.