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Aeroelasticity Flutter With Unsteady Aero Darin Haudrich [email protected] 4/8/2015

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Vibration

AeroelasticityFlutter With Unsteady Aero

Darin Haudrich

[email protected]

4/8/2015

Background

We previously went through a 2-DOF rigid airfoil example and home with steady aerodynamics. We will now look at the use of unsteady aerodynamics in the flutter equations.

2DOF Airfoil

Rigid Airfoil

P reference point

C Center of Mass

Q Aerodynamic center

T chord point

b chord

e and a go from -1 to 1

X = e-a

EOM

EOMs:

Assume harmonic motion:

Substituting into EOMs above:

Where lift and moment are:

Substituting lift and moment in:

Flutter Formulation

Since the EOM are linear and homogenous the determinant must be zero for a nontrivial solution.

How to solve

1)Specify an altitude to fix

2)Specify M

3)Specify K values, start with 0.001 to 1.0

4)At each k, M calculate lh, l, mh, m

Flutter Formulation

How to Solve continued

5)Solve the flutter determinant which is a quadratic equation with complex values for (/)2 that correspond to each of the selected values of k.

6)Interpolate to find the value of k at which the imaginary part of the one of the roots becomes zero. This can be done graphically as well

7)Determine U = b/k and M=U/c

Repeat 3-7 with the value of M obtained in step 7 until Min =Mout and then that is the correct flutter speed.

Repeat process at different values of to determine flutter as a function of altitude.

K-method

EOMs:

Where D=

Nondimensionalizing:

g is equivalent structural damping

Z the unknown is formulated as:

K-Method

Flutter determinant:

Frequency and Damping from the solution comes from eigenvalue of Z:

Where g = 0 is flutter.

The damping value g is an artificial value of structural damping to achieve simple harmonic motion at a frequency i

The k-method is easy to implement but inherently is a mathematically improper formulation. The only place this method is valid is g=0.

P-k method

The p-k method tries to overcome some the mathematical issues that the k-method introduces.

We start by creating a dimensionless time

EOM becomes:

M and are diagonal matrices and:

For a given speed and altitude the flutter determinant is solve for n+1 p values

where k is the reduced frequency and is log dec dam

P-k method

If the aerodynamics are a function of k:

The results have to be iterated on such the k value for the aero is adjusted to match the value from the system eigenvalue for each eigenvalue for each velocity chosen.

Comparison plots

Summary

g=0 results are the same for each method.

At the same velocity, a mode can have two frequencies???

the instability can become more unstable as speed decreases???

NASTRAN K-Method

NASTRAN K-Method

NASTRAN K-Method