First-order flow screening
- ṁ
- 0.010 kg/s
- pref
- 101325 Pa
- Tref
- 300 K
- ri
- 20 mm
- R
- 287 J/(kg K)
- γ
- 1.4
Scope and authority
\text{case inputs} \rightarrow \text{analytical expectations} \neq \text{solver output}Every value below is established before solving from the declared reference state and inlet geometry. It is a screening calculation, not validation and not a reconstruction of CFD output.
Inlet reference area
A_i = \pi r_i^2The deterministic nozzle definition supplies the 20 mm inlet radius. The full circular area is used for this independent reference-scale calculation.
Reference density
\rho_{ref} = \frac{p_{ref}}{R T_{ref}}Perfect-gas air at the declared reference pressure and temperature provides a pre-solve density scale. This is not the solved density field.
Continuity velocity scale
V_i = \frac{\dot{m}}{\rho_{ref} A_i}Steady mass continuity converts the commanded mass flow into an inlet mean-velocity scale using only case inputs.
Compressibility screen
a_{ref}=\sqrt{\gamma R T_{ref}},\qquad M_i=\frac{V_i}{a_{ref}}The reference Mach number screens the inlet regime before choosing and running the numerical model.
Dynamic-pressure scale
q_i = \frac{1}{2}\rho_{ref}V_i^2This establishes an order-of-magnitude pressure scale and the expected quadratic response to mass flow. It is not a nozzle pressure-drop prediction.
What is not established
\Delta p_{analytical}=\text{NOT YET ESTABLISHED}The available inputs do not justify an independent loss model for this converging-diverging turbulent nozzle. Aero therefore does not fabricate an analytical pressure drop or reuse the CFD result as its own prediction.