Download presentation
Presentation is loading. Please wait.
1
AAE 556 Aeroelasticity Lecture 18
Resonance, Mode shapes Purdue Aeroelasticity
2
Purdue Aeroelasticity
Summary MDOF systems with n degrees of freedom have n possible “modes of motion” Mode of motion means a (natural, resonant) frequency with a well-defined mode shape Eigenvectors – another word for mode shapes – provide information about node lines or node points Experiments provide node lines and frequencies to compare with analysis Purdue Aeroelasticity
3
Typical section equations of motion - 2 dof
measured from static equilibrium position Purdue Aeroelasticity
4
Review - Equations of motion for free vibration
Trial solution assume harmonic motion result Purdue Aeroelasticity
5
Harmonic forcing at or near the natural frequencies
Trial solution harmonic motion result Purdue Aeroelasticity
6
Harmonic forcing at or near the natural frequencies
At or near resonance, the amplitude of the response is large (here it is infinite because we have no damping) Purdue Aeroelasticity
7
Purdue Aeroelasticity
Defining mode shapes what will the vibrations look like if we force the system at natural frequencies? (1) (2) eigenvalues & eigenvectors Purdue Aeroelasticity
8
A different expression
Purdue Aeroelasticity
9
Purdue Aeroelasticity
System mode shapes If q is 1 then how much is h? Purdue Aeroelasticity
10
Purdue Aeroelasticity
example Purdue Aeroelasticity
11
Purdue Aeroelasticity
example reference bending actual reference torsion actual Purdue Aeroelasticity
12
Purdue Aeroelasticity
Mode shape When we let h/b=1 then we are asking about the amount of q in the plunge mode 1 unit Purdue Aeroelasticity
13
Shake testing identifies modes and frequencies
Purdue Aeroelasticity
14
Torsional frequency and mode shape
1 radian node point Purdue Aeroelasticity
15
Purdue Aeroelasticity
Node point definition A point in space where there is no displacement, velocity or acceleration when the structure is vibrating at a natural frequency x Purdue Aeroelasticity
16
Node point depends on eigenvector
x divide by b first mode Purdue Aeroelasticity
17
Node point for second frequency
Purdue Aeroelasticity
18
Purdue Aeroelasticity
Summary MDOF systems have n modes of motion Mode of motion means a (natural, resonant) frequency with a mode shape Eigenvectors – mode shapes – provide node lines or node points Experiment provides node lines and frequencies Purdue Aeroelasticity
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.