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: