Sondipon Adhikari
http://engweb.swan.ac.uk/~adhikaris/ Twitter: @ProfAdhikari
Research directions in Engineering Dynamics COPPE/UFRJ and Swansea - - PowerPoint PPT Presentation
Research directions in Engineering Dynamics COPPE/UFRJ and Swansea Workshop November 2014 Sondipon Adhikari http://engweb.swan.ac.uk/~adhikaris/ Twitter: @ProfAdhikari Engineering Dynamics Principal investigators: Prof Friswell, Prof
http://engweb.swan.ac.uk/~adhikaris/ Twitter: @ProfAdhikari
Automatic Rotor Balancing
Energy Harvesting
Model Updating and Inverse Problems Nonlinear Structural and Rotor Dynamics Morphing Aircraft
MORPHLET – Morphing Winglet FishBAC Active Camber FE Model Identification Corrugated Skins Bistable Plates
2 4 6 10–6 10–4 10–2 100
Rotating Machine Diagnostics
Comparison of non-probabilistic and probabilistic stochastic model updating using the DLR AIRMOD test structure
Simplified AIRcraft MODel- AIRMOD (DLR-Germany)
Surrogate modelling (Kriging and Polynomial Chaos Expansion) Development of non-probabilistic Stochastic Model Updating techniques
Variations in the fuel load and its effect on the aeroelastic behavior of the Semi-Span Super-Sonic Transport wind-tunnel model (S4T)
Uncertainty Quantification
Probabilistic Non-probabilistic-Fuzzy Rapid perdition of worst case gust loads
5 10 15 20 25 30 5 10 15 20 25 30 1 2 3 4 5 6 7 8 9
Fitted coefficient matrix Ckj
Damping identification from experimental measurements
Nonlinear vibration energy harvesting
under random ambient excitations
Stochastic Structural Dynamics Vibration Energy Harvesting
Nonlocal continuum method of vibration based nanosensors
Dynamics of Nanoscale Structures
Atomistic finite element method for dynamics of general nano scale structures like DNA, Graphene sheets, Boron Nitride Experimental methods for uncertainty quantification in structural dynamics Novel computational methods for transient dynamic response of dynamical systems with uncertainty
L
x y
ρA
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0.1 0.2 1 2 3 4 1 2 3 4 5
α ζ Normalized mean power
Base Piezo- ceramic Proof Mass x xb + v Rl
The average harvested power due to white-noise base acceleration with a circuit without an inductor can be obtained as The optimal condition is
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Uncertainty modeling Parametric uncertainty: mean matrices + random field/variable information Random field discretization Nonparametric uncertainty: mean matrices + a single dispersion parameter for each matrices Random matrix model
100 200 300 400 500 10
−8
10
−7
10
−6
10
−5
10
−4
10
−3
Frequency (Hz) Mean of deflection (m) deterministic direct MCS 2nd order spectral 3rd order spectral 4th order spectral 100 200 300 400 500 10
−8
10
−7
10
−6
10
−5
10
−4
10
−3
Frequency (Hz) Standard deviation of deflection (m) direct MCS 2nd order spectral 3rd order spectral 4th order spectral
500 1000 1500 2000 2500 3000 3500 4000 −40 −30 −20 −10 10 20 30 40 50 60 Frequency (Hz) Mean of amplitude (dB) Reduced diagonal Wishart Experiment
500 1000 1500 2000 2500 3000 3500 4000 10
−2
10
−1
10 10
1
Relative standard deviation Frequency (Hz) Reduced diagonal Wishart Experiment
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1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30
Natural Frequency Damping Modal Mass
Correlation of visible in scatter diagram Monte Carlo Simulation (MCS) Mode 12 Mode 13
1 2 n
…Young’s modulus … joint stiffness … density
frequency 4n wing bend. in-plane bend.
Finite Element representation
Scatter Diagram
Randomise Parameters (Latin Hypercube Sampling)
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