Aeroelasticity & Structural Dynamics in a Fast Changing World
17 – 21 June 2024, The Hague, The Netherlands
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New Design of Whirl Flutter Aeroelastic Demonstrator


Go-down ifasd2024 Tracking Number 56

Presentation:
Session: Flutter 2
Room: Room 1.6
Session start: 09:40 Wed 19 Jun 2024

Jiri Cecrdle   cecrdle@vzlu.cz
Affifliation: Czech Aerospace Research Centre (VZLU)

Ondrej Vich   ondrej.vich@vzlu.cz
Affifliation: Czech Aerospace Research Centre (VZLU)

Jan Starek   starek@vzlu.cz
Affifliation: Czech Aerospace Research Centre (VZLU)

Jarmil Vlach   vlach@vzlu.cz
Affifliation: Czech Aerospace Research Centre (VZLU)

Martin Kolar   kolar@vzlu.cz
Affifliation: Czech Aerospace Research Centre (VZLU)

Miroslav Smid   smid@vzlu.cz
Affifliation: Czech Aerospace Research Centre (VZLU)


Topics: - Wind Tunnel and Flight Testing (Experimental methods)

Abstract:

The whirl flutter aeroelastic demonstrator (W-WING) represents a half-wing (span 2.56 m) with the nacelle, engine, and propeller (radius 0.35 m). The demonstrator was used for whirl flutter measurements in past. In the frame of the new project, further measurements are planned. Based on the experience, upgrades of the demonstrator were proposed. Submitted paper describes the preparatory activities including the demonstrator design, instrumentation, and aerodynamic and structural analyses. The main change is the installation of the new motor with the sufficient power. Also, additional sensors and equipment were installed. In addition, the system of steady and unsteady flow field measurement was proposed. Finally, the sting-mounted propeller-nacelle variant (W-STING) was proposed for the measurements of aerodynamic derivatives. The wing stiffness is modeled by a duralumin spar. The inertia characteristics are modeled by lead weights. The aileron is actuated by the electromagnetic shaker via a push pull rod. The wing is fixed at the root to the pylon. The nacelle model has two DOFs (pitch and yaw). Stiffness parameters are modeled by means of changeable cross spring pivots. Both pivots are independently movable in the direction of the propeller axis. The gyroscopic effect is simulated by the mass of the propeller blades (two sets are available). The new motor with the sufficient power will enable to operate the propeller in the thrusted mode. The aerodynamic force analytical study using the CFD solver to predict the necessary power and operational margins of the propeller was performed. Based on the results, and on further limitations (mass, dimensions), the motor with the nominal power of 15 kW was selected. The front part of the nacelle was redesigned to accommodate the new motor. The shape of the nacelle remained unchanged. Design also included thrust balance cell, pitch and yaw blocking devices, sliding weight, etc. The appropriate strength checks were performed. System of sensors include strain gauges in two wing sections, 18 accelerometers in the wing and nacelle, servo-amplifier to manage and monitor the propeller rpm, torque, and immediate power, thrust balance cell, independent optical rpm sensor. W-STING include measurement of pitch and yaw moments and deformation angles.