Flight Envelope Protection Using Flap Hinge Moment Measurement
By: Phillip J. Ansell
Adviser: Dr. Michael B. Bragg
M.S., University of Illinois at Urbana-Champaign, 2010
ABSTRACT
An experimental investigation of the sensitivity of flap hinge moment to airfoil surface
contamination was conducted at the University of Illinois at Urbana-Champaign Aerodynamics
Research Lab. Tests were conducted on two airfoil models, an NACA 3415 and an NACA
23012, at Reynolds numbers of 1.8 × 106 and 1.0 × 106. The effects of six different simulated
contamination configurations on the performance characteristics of both airfoils were tested.
These configurations consisted of glaze ice, rime ice, two severities of distributed leading-edge
roughness, three-dimensional leading-edge damage, and three-dimensional upper-surface
damage. Additionally, the effects of flap deflection and trim tab deflection on the unsteady
hinge moment were studied.
Results from this study found that large increases in Ch,StDev often occurred at the same
angle of attack as Cl,max. By correlating regions of separated flow observed in Cp distributions
and fluorescent-oil flow visualizations to Ch,StDev at discrete angles of attack, it was determined
that regions of boundary-layer separation were the primary driver for large increases in
unsteadiness in the hinge moment. It was also found that the unsteady hinge moment had
negligible dependence on trim tab deflection. The response of Ch,StDev was dependent on the
stalling characteristics of the airfoil model.
Of all of the contamination configurations tested, the two simulated ice cases had the
largest effect on the performance of the airfoils. For the distributed leading-edge roughness
cases, the larger roughness elements had a larger effect on the performance than the smaller
roughness elements, but the Ch,StDev response of both roughness cases were comparable. While
the 3D simulated damage cases did not significantly affect the lifting characteristics of either
model, the magnitude of the Ch,StDev response of the 3D simulated damage case was comparable
to the 2D contamination cases. Additionally, the large increase in Ch,StDev occurred prior to stall
due to localized regions of separated flow that resulted from the simulated damage.