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Vibrations and Acoustic 2017-2018 7. Experimental Modal Analysis
01/08/2017
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Arnaud Deraemaeker ([email protected])
7. Experimental Modal Analysis
Vibrations and acoustics
*Principle of EMA
*Measuring FRFs
*SDOF Identification
*MDOF Identification
Outline of the chapter
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Vibrations and Acoustic 2017-2018 7. Experimental Modal Analysis
01/08/2017
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Principle of EMA
1. Measure FRFs
2. Estimate poles (natural frequencies)
3. Identify mode shapes
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Principle of EMA
Vibrations and Acoustic 2017-2018 7. Experimental Modal Analysis
01/08/2017
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Measuring FRFs
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Measuring FRFs : summary
Vibrations and Acoustic 2017-2018 7. Experimental Modal Analysis
01/08/2017
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Use of windows : summary
No window (synchronisation !)
Exponential window to reduceeffect of noise (output) + force window (input)
Hanning window to reduce leakage
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Measuring FRFs
Shaker excitation
Vibrations and Acoustic 2017-2018 7. Experimental Modal Analysis
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Measuring FRFs
Roving hammer excitation
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Measuring FRFs
Reciprocity
Vibrations and Acoustic 2017-2018 7. Experimental Modal Analysis
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Measuring FRFs in practice
SDOF identification
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Vibrations and Acoustic 2017-2018 7. Experimental Modal Analysis
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The pole-residue model in the frequency domain
The frequency response function of a one dof system is :
The Pole-residue model in the frequency domain is :
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The impulse response function of a one DOF system is :
The Pole-residue model in the time domain is :
The pole-residue model in the time domain
Vibrations and Acoustic 2017-2018 7. Experimental Modal Analysis
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Estimating parameters : Peak-picking method
Natural frequency (ratio k/m)
Damping coefficient (b)
Mass (m)
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Estimating parameters : logarithmic decrement method
Natural frequency (ratio k/m)
Damping coefficient (b)
Mass (m)
Vibrations and Acoustic 2017-2018 7. Experimental Modal Analysis
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Estimating parameters : curve fitting
More equations than unknowns
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Estimating parameters : curve fitting
More equations than unknowns
Moore-Penrose pseudo-inverse : Least-squares solution
Vibrations and Acoustic 2017-2018 7. Experimental Modal Analysis
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MDOF identification
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The pole-residue model in the frequency domain
The FRF matrix of a MDOF system is :
The Pole-residue model in the frequency domain is :
Ri is a matrix
Vibrations and Acoustic 2017-2018 7. Experimental Modal Analysis
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The Pole-residue model in the time domain is :
The pole-residue model in the time domain
Inverse Fourier transform
Ri is a matrix
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Estimating the poles : peak picking method
Natural frequencies and modal damping
Vibrations and Acoustic 2017-2018 7. Experimental Modal Analysis
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Estimating the mode shapes : curve fitting in the frequency domain
For each single FRF :
l=input, k=output
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Estimating the mode shapes
Mode shapes
Keep l fixed, vary k
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Estimating natural frequencies and mode shapes : the complex exponential method
l=input, k=output
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Estimating natural frequencies and mode shapes : the complex exponential method
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01/08/2017
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Estimating natural frequencies and mode shapes : the complex exponential method
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Estimating natural frequencies and mode shapes : the complex exponential method
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Model order and stabilisation diagram
N ?
N
s:stable in both freqand damping
d: stable in damping
f: stable in frequency