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CD Nozzle Flow Simulator

A converging-diverging nozzle turns pressure into speed. Drag the two sliders to set the inlet and back pressure, then watch the throat choke, a normal shock appear, or the flow leave supersonic.

Inlet Throat A* Exit Aₑ Convergent Divergent Mach number along the nozzle 0 0.2 0.4 0.6 0.8 1.0 Position along nozzle s 0 1.0 2.0 3.0 Mach number Subsonic Supersonic Normal shock
Pressure ratio Pᵦ / P₀
0.375
Flow state
—
Exit Mach number Mₑ
—
What happens, in order Inlet P₀ → Throat A* → Divergent → Normal shock → Exit Mₑ
Display mode

Detailed Explanation

What is a CD nozzle simulator?

A converging-diverging nozzle is a duct that narrows to a throat and then widens again. It is the classic way to turn stored pressure into a fast jet, and it is the shape behind steam turbines, jet exhausts and rocket engines.

This simulator lets you set two numbers: the inlet total pressure P₀ and the back pressure Pᵦ. From those two values it works out whether the throat is choked, where a shock stands, and what Mach number the flow reaches at the exit.

Why look inside?

From the outside it is just a tube. Showing the flow field and the Mach number chart reveals the two features that make the nozzle interesting: the throat reaching Mach 1 and a normal shock standing inside the divergent section.

Two ideas matter most: once the throat chokes the mass flow stops rising, and the exit Mach number is set by the pressure ratio, not by how hard you push.

Components & their role

1. Set the driving pressures

Inlet total pressure P₀ is the energy the air carries as it enters. Back pressure Pᵦ is the pressure the exit sees. Together they set the pressure ratio Pᵦ / P₀ that decides everything downstream.

2. The throat chokes

As the duct narrows, the air speeds up and its static pressure falls. Once the pressure ratio drops below about 0.53 the throat reaches Mach 1, and from then on adding more inlet pressure cannot raise the mass flow any further.

3. The divergent section speeds it up

Past the throat the area grows. In supersonic flow a larger area means faster flow, so the same mass of air keeps accelerating and the Mach number climbs toward the exit.

4. A normal shock can stand inside

If the back pressure is higher than the supersonic exit can match, the nozzle forces a normal shock into the divergent section. Across that thin sheet the flow jumps from supersonic to subsonic and the pressure rises sharply.

5. The exit Mach number settles

With no shock the flow leaves at the fully supersonic Mach number fixed by the nozzle area ratio. With a shock inside, the exit flow is subsonic and the exit Mach number is lower still, exactly as the chart shows.

What does a converging-diverging nozzle do?

It converts pressure into speed. The duct narrows to a throat and then widens, so subsonic air accelerates through the throat and keeps speeding up in the divergent section until it is supersonic.

What does choked mean?

Below a back-to-inlet pressure ratio of about 0.53 the throat reaches Mach 1. Adding more inlet pressure then cannot raise the mass flow any further, so the nozzle is said to be choked.

Why does a shock appear inside the nozzle?

If the back pressure is too high for the supersonic exit to match, the nozzle forces a normal shock into the divergent section. Across the shock the flow drops sharply from supersonic to subsonic.

What sets the exit Mach number?

It is set by the ratio of back pressure to inlet pressure. For a fully supersonic exit the Mach number is fixed by the area ratio; a higher back pressure moves a shock into the duct and lowers the exit Mach number.

What do the shaded colours mean?

Blue marks subsonic flow and orange marks supersonic flow. Watching the two colours shows where the nozzle reaches Mach 1 and where a shock flips the flow back to subsonic.

Why does the chart jump at the shock?

A normal shock is a sudden change, not a gradual one. The Mach number curve drops almost vertically at the shock station and then continues subsonic toward the exit.

Common Misconceptions

A narrower duct always means faster flow. The flow speeds up wherever the duct narrows.
Only subsonic flow does that. In supersonic flow the flow speeds up as the duct widens, which is why the divergent section accelerates it.
Pushing harder keeps raising the flow. Raising the inlet pressure always increases the mass flow.
Once the throat chokes the flow is capped. After the throat reaches Mach 1 the mass flow stops rising no matter how much more pressure you add.
The shock sits at the throat. People expect the sudden change right at the narrowest point.
The shock sits in the divergent section. A normal shock can only stand where the flow is supersonic, so it settles past the throat.
The exit is always supersonic. A CD nozzle always blasts out supersonic flow.
The exit depends on back pressure. A high back pressure forces a shock inside and the flow leaves subsonic.
Disclaimer: Diagrams are heavily simplified for educational demonstration only. Real-world systems contain far more variables and complexity. Not for engineering production use. Not financial, political or professional advice.