AE 315 · Experimental Aerodynamics · Spring 2025 · ERAU
Before any aerodynamic test can be trusted, the wind tunnel itself must be understood. This lab established how the ERAU open-circuit wind tunnel behaves — mapping how fan speed translates to airflow velocity and how that airflow varies across the test section height. These baseline measurements are the foundation every subsequent experiment in the course depends on.
A traverse pitot-static probe was held at a fixed height while the fan swept from 0 to 25 Hz in 5 Hz steps. Airspeed was computed from the measured differential pressure q using:
V = √(2q / ρ)
where air density ρ was derived from ambient temperature and pressure via the ideal gas law. In a second experiment, the fan was fixed at 15 Hz while the probe traversed 1–40 inches in height. At each position, turbulence intensity I = 100 × σV / V̄ was computed to assess flow quality near the tunnel walls. Reynolds number per unit length Re/l = ρV/μ was also recorded at each fan speed, using viscosity from Sutherland’s formula.
Differential pressures were loaded from CSV, converted from inches of water to Pascals (×248.84), and used to compute speed and turbulence intensity across both experiments.
% Convert inH2O ? Pa and compute airspeed
Hz_15 = (data(:,4) - data(:,1)) * 248.84;
rho = 1.213; % kg/m³, ideal gas
V_15 = sqrt(2 * Hz_15 / rho);
% Turbulence intensity across probe heights
v_avg = mean(v, 2);
intensity = (std(v_avg) ./ v_avg) * 100;
% Velocity uncertainty (standard error, %)
UC_V = (std(V_15) / sqrt(length(V_15))) * 100;