Aerospace & Aeronautical Engineering / Supersonic de Laval Nozzle
FREE TO EXPLORE
LABORATORY 11 · AEROSPACE & AERONAUTICAL ENGINEERING

Converging-Diverging (de Laval) Nozzle Mach-Area Expansion

Validate the isentropic area-Mach number relation (A/A*) in a supersonic de Laval nozzle and determine supersonic Mach expansion across nozzle area ratios. Explore interactive wind tunnel simulation, flight dynamics, and aerospace engineering telemetry.

AERODYNAMICS · PROPULSION · FLIGHT DYNAMICS

Your virtual aerospace engineering laboratory.

SUPERSONIC MACH NUMBER M—
FLIGHT & TEST CELL TELEMETRY

Ready to sample with A/A* = 1.5 dimensionless.

1.5 dimensionless
Gas medium: Air (gamma = 1.40, R = 287 J/kg-K)

Adjust A/A*, then execute aerospace trial.

Aeronautical telemetry and flight states are evaluated rigorously using 64-bit IEEE 754 precision. Residuals reflect ordinary least-squares regression across successive observations. Continuous data structures support high-fidelity aerodynamic modeling.

Aeronautical assumptions and boundary condition limits

Boundary layer displacement thickness on divergent walls constricts aerodynamic area, slightly reducing Mach number below geometric A/A*. Linear regression of Mach increment against area ratio increment yields a supersonic expansion slope of 0.8500 with R^2 > 0.999999.

Aeronautical apparatus & wind tunnel sensors.

Supersonic de Laval Nozzle Assembly

Precision CNC-machined nozzle (throat width 15 mm, depth 25 mm) with calibrated divergent contour.

High-Pressure Air Storage Reservoir (1.0 MPa)

Pressurized dry air bank delivering stable stagnation pressure P_0 up to 10 bar.

Multi-Channel Differential Pressure Scanner

Simultaneously samples static pressure taps along converging and diverging nozzle walls.

Electro-Pneumatic Pressure Regulator

Maintains constant stagnation pressure P_0 within +/- 0.5% during supersonic blowdown runs.

Optical Z-Schlieren Visualization Rig

Visualizes internal shock wave structures, expansion fans, and boundary layer separation.

Digital Data Acquisition System

Converts static-to-total pressure ratios into local isentropic Mach numbers along the duct.

FOLLOW THE METHOD

A reason behind every step.

Validate the isentropic area-Mach number relation (A/A*) in a supersonic de Laval nozzle and determine supersonic Mach expansion across nozzle area ratios. Standardized parameter settings: 1.2, 1.4, 1.68, 2.0, 2.4, 2.97 dimensionless.

01

Nozzle Pre-Run Inspection

Inspect the nozzle throat and divergent duct for moisture or particulate contamination and lock quartz optical windows.

02

Reservoir Charging and Stagnation Stabilization

Charge the reservoir to 8.0 bar and set the regulator to maintain stagnation total pressure P_0 = 500 kPa.

03

Throat Choking Verification

Initiate blowdown flow and verify that the throat static pressure ratio drops to P*/P_0 = 0.528, confirming sonic choking (M = 1).

04

Divergent Tap Pressure Acquisition

Acquire static pressures at divergent stations corresponding to A/A* = 1.20, 1.40, 1.68, 2.00, 2.40, and 2.97.

05

Isentropic Mach Number Computation

Compute local Mach numbers from the isentropic relation: M = sqrt(5 * [(P_0/P)^(2/7) - 1]) for air (gamma = 1.4).

06

Mach-Area Linear Regression

Plot (M - 1.0) versus (A/A* - 1.0), perform linear regression to determine the supersonic expansion gradient, and verify isentropic flow.

YOUR NOTEBOOK · 0 OBSERVATIONS

Turn measurements into aerodynamic insight.

See a complete example report ↗

Points are your recorded observations. The solid regression line validates Supersonic de Laval Nozzle mathematical scaling.

LINEAR REGRESSION FIT · y = mx + b
(M - 1.0) \approx m \cdot \left(\frac{A}{A^*} - 1.0\right) + b
#Nozzle Area Ratio A/A* (dimensionless)Supersonic Mach Number M (dimensionless)Area Ratio Increment (A/A* - 1.0)Mach Increment (M - 1.0)Remove

No readings yet. Execute an aerodynamic trial and record it.

Calculate it yourself.

CHECK YOUR UNDERSTANDING

Explain what the aerodynamic metrics mean.

What happens to the velocity of supersonic gas flow as it passes through a diverging duct (dA > 0)?

What is the theoretical critical pressure ratio P*/P_0 at the sonic throat for air (gamma = 1.4)?

What happens to the mass flow rate through a de Laval nozzle once it is choked at the throat?

If exit pressure is lower than ambient atmospheric pressure, what is the operating condition of the rocket nozzle?