Nozzles and diffusers

The thermal solver computes the flow resistance factor for nozzles and diffusers based on the angles α and β, and various coefficients.

The angles α and β are defined [12]:

where:

  • SE1 is the larger side of the exit
  • SE2 is the larger side of the inlet
  • SI1 is the smaller side of the exit
  • SI2 is the smaller side of the inlet
  • LD is the length of the nozzle or diffuser

α is assumed grater than β. If α < β, the two are reversed. α can take on a maximum value of 40 degrees. If α > 40 degrees, α = 40 degrees is used.

Next, a friction coefficient is defined:

for β > 0.5 degrees, and

for β < 0.5 degrees.

where:

  • A1 is the area at the narrower end.
  • A2 is the area at the larger end.
  • ψFR is the friction coefficient.

For diffusers, a shock and an expansion coefficient are defined at the narrower end:

where:

  • ψEXP is the shock coefficient.
  • ZEXP is the expansion coefficient.

Then the flow resistance factor for a diffuser is:

For nozzles, a length to hydraulic diameter ratio is defined:

where:

  • D1 is the hydraulic diameter at the narrower end.
  • RLD is the length to hydraulic diameter ratio.

Next, an interpolation parameter RINT is computed:

Next, the parameter Z' is defined and the flow expansion coefficient ZEXP is calculated:

Then the flow resistance factor for a nozzle is: