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Purdue Aeroelasticity
AAE Aeroelasticity Flutter-Lecture 20 Purdue Aeroelasticity
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Quasi-steady flutter with a typical section vibration idealization
Flutter is a self-excited, dynamic, oscillatory instability requiring the of motion and interaction between two different modes an external energy supply Quasi-steady aerodynamic loads capture some dynamic effects of the lift force, but ignore lags between motion and developing forces and moments Assumed harmonic motion Purdue Aeroelasticity
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Flutter and frequency merging
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Purdue Aeroelasticity
What we are looking for Purdue Aeroelasticity
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Free vibration with the air on looking for clumps of parameters
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Purdue Aeroelasticity
The prize Remember what the bars mean. Purdue Aeroelasticity
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Calculate the determinant what do you hope to discover?
2b c.g. shear center aero center Purdue Aeroelasticity
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Quadratic equation for frequency squared
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The A, B terms are airspeed dependent
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Divergence is a special case
set then Purdue Aeroelasticity
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Purdue Aeroelasticity
Divergence Purdue Aeroelasticity
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Solution for natural frequencies
When the airspeed is zero then these eigenvalues are real and distinct. They stay that way as airspeed increases. That means our original assumption of harmonic (sinusoidal) motion is correct. Purdue Aeroelasticity
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Purdue Aeroelasticity
The transition point between stability and instability for this idealization is frequency merging Two solutions with the same frequencies instability Purdue Aeroelasticity
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Frequency depends on airspeed
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Transition to instability
????? Purdue Aeroelasticity
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Purdue Aeroelasticity
Two roots Purdue Aeroelasticity
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Purdue Aeroelasticity
Frequency merging Purdue Aeroelasticity
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Solution for frequency
When the airspeed is zero then these eigenvalues are real and distinct - they also depend on airspeed ... Purdue Aeroelasticity
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Purdue Aeroelasticity
When the frequencies are real and distinct then no energy is input or extracted over one cycle Mode shapes are important Purdue Aeroelasticity
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