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Module 4 · Rocket Nozzle Lab

Anderson Ch. 10 · convergent–divergent nozzles

One nozzle, six personalities. Lower the back pressure pb and watch the same convergent–divergent nozzle morph: gentle venturi → choked throat → a shock trapped inside → overexpanded (shock diamonds!) → perfectly expanded → underexpanded. The white curve is p/p₀ along the nozzle — the story in one line. 🎯 challenges you to hit design condition like a propulsion engineer.

🔽 Back pressure pb/p₀ 0.90
📏 Exit area Aₑ/A* 2.00
Regime:
Exit Mach:
pₑ/p₀:
Throat:
Quasi-1-D flow (Anderson §10.2–10.3): area decides everything.
Area–Mach relation: (A/A*)² = (1/M²)·[2/(γ+1)·(1 + ½(γ−1)M²)]^{(γ+1)/(γ−1)} — every area ratio has TWO answers, one subsonic and one supersonic. The back pressure picks which one you get.
Isentropic: p/p₀ = (1 + ½(γ−1)M²)^{−γ/(γ−1)}.
Once the throat chokes (M=1), mass flow freezes: ṁ = p₀A*/√T₀ · √(γ/R)·(2/(γ+1))^{(γ+1)/(2(γ−1))} — lowering pb further can't pull more through.
If pb is between the subsonic and shock-at-exit limits, a normal shock stands inside the divergent section exactly where its pressure recovery lets the flow diffuse to pb at the exit.
Slide pb down slowly from 0.90 and name each regime as it appears.