1D flow and nozzle Flashcards
Describe the underlying assumptions of a one-dimensional isentropic flow in a nozzle or a duct.
Write down basic relation for a one-dimensional isentropic flow in a nozzle or a duct.
Applying the integral form of mass conservation laws for a compressible gas to a one-dimensional steady-
state flow in a pipe, show that the mass flow rate is the same in every cross-section of the pipe.
Applying the integral form of energy conservation laws for a compressible gas to a one-dimensional
adiabatic steady-state flow in a pipe, show that the stagnation enthalpy is constant in the pipe
Explain why the momentum equation for a compressible flow in a constant cross-section pipe 𝑝+𝜌𝑣^2=𝑐𝑜𝑛𝑠𝑡 and the Bernoulli equation 𝑝+(1/2)𝜌𝑣^2=𝑐𝑜𝑛𝑠𝑡 do not contradict each other.
Derive formula for the sound speed in an ideal gas
Derive area/velocity variation in a 1D isentropic flow of compressible gas
Derive area/Mach number variation in a 1D isentropic flow of compressible gas
Explain the term stagnation properties of the gas flow
Derive relation between static and stagnation temperatures for an adiabatic flow of a perfect gas
Derive relation between static and stagnation pressure for an isentropic flow of a perfect gas
For which model of gas and which type of flow (adiabatic, isentropic) the following relation between static
and stagnation temperature is valid
𝑇0=𝑇(1+(𝛾−1/2)𝑀^2)
For which model of gas and which type of flow (adiabatic, isentropic) the following relation between static
and stagnation pressure is valid 𝑝0=𝑝(1+((𝛾−1)/2)𝑀^2)^(𝛾/(𝛾−1))
What does it mean for the flow if the static pressure is below the critical pressure?
Describe the regimes of adiabatic flow in the converging nozzle for various values of background pressure.
Sketch the pressure and Mach number variation along the nozzle.