JOURNAL OF GUIDANCE,CONTROL, AND DYNAMICS
Vol. 26, No. 2, March–April 2003
Uncertainty Estimation from Volterra Kernels
for Robust Flutter Analysis
Richard J. Prazenica,
¤
Rick Lind,
†
and Andrew J. Kurdila
‡
University of Florida, Gainesville, Florida 32611-6250
The utterometer is a tool used for predicting the onset of utter during ight testing. This tool uses robust utter
analysis to consider a model with an associated uncertainty description. The utterometer is particularly useful
because the uncertainty description is determined by ight data. However, the standard method of uncertainty
estimation is somewhat suspect because of the effects of nonlinearities in the ight data. A method is introduced
to estimate uncertainties by considering only the linear component of the ight data. The linear component is
extracted by representing the system in terms of Volterra kernels. The rst-order kernel describes the linear
component of the data and, thus, can be used by the utterometer. Flight data from the aerostructures test wing is
used to demonstrate this procedure. The analysis using the rst-order kernel is shown to generate a more accurate
description of the modeling error than standard analysis of the measured ight data.
Nomenclature
A = area of domain
a = scaling function lter
b = wavelet lter
D = length of Volterra kernel
g = function
h = Volterra kernel
K = set of multi-indices
[ P ] = matrix of integral values
T = operator
[ T ] = matrix form of wavelet transform operator
t = time
[U
1
] = matrix of discrete inputs
[U
2
] = matrix of products of discrete inputs
u = input
V = scaling function approximationspace
W = wavelet detail space
y = response
y = vector of discrete output values
® = coefcient of scaling function
® = vector of single-scale kernel coefcients
¯ = coefcient of wavelet
¯ = vector of multiscale kernel coefcients
° = mapping
´, » = time
Á = orthonormal scaling function
’ = scaling function
 = characteristicfunction
à = wavelet
Ä = domain of second-orderkernel
© = summation of vector spaces
ª = subtraction of vector spaces
Received 11 March 2002; presented as Paper 2002-1650 at the AIAA/
ASME/ASCE/AHS/ASC 43rd Structures, Structural Dynamics, and Materi-
als Conference, Denver, CO, 22–25 April 2002;revision received 22 Novem-
ber 2002;accepted for publication25 November 2002.Copyright c ° 2003by
the authors. Published by the American Institute of Aeronautics and Astro-
nautics, Inc., with permission. Copies of this paper may be made for personal
or internal use, on condition that the copier pay the $10.00 per-copy fee to
the Copyright Clearance Center, Inc., 222 Rosewood Drive, Danvers, MA
01923; include the code 0731-5090/03 $10.00 in correspondence with the
CCC.
¤
Graduate Student, Department of Mechanical and Aerospace Engineer-
ing; currently National Research Council Fellow, NASA Dryden Flight Re-
search Center, Edwards, CA, 93523; chad.prazenica@dfrc.nasa.gov.
†
Assistant Professor, Department of Mechanical and Aerospace Engineer-
ing; rick@aero.u.edu. Senior Member AIAA.
‡
Professor, Department of Mechanical and Aerospace Engineering;
ajk@aero.u.edu. Associate Fellow AIAA.
Subscripts and Superscripts
i ; P = counter
j = discretizationlevel
k = value in f0; 1; 2; 3g
r = value in f1; 2; 3g
· = multi-index
Introduction
T
HE analysis of ight data is obviously important for any ight
test. The measurements are usually corrupted by noise and
imperfections; however, these data are often the best indicator of
the true dynamics of the aircraft. The dependencyon data exists for
all types of ight testing, but it is especially prevalent when ight
utter testing for envelope expansion.
A tool called the utterometer has been developed for predicting
the onset of utter during a ight test.
1
This tool is a model-based
utility, but it is directly dependent on ight data. The utterometer
computes a utter speed for an analytical model that is robust with
respect to an uncertainty description.
2
The tool uses ight data to
generate that uncertainty description.Essentially, the uncertainty is
a mathematicaloperatorthat describesdifferencesbetweentransfer
functions of the model and data. The utterometer predicts a utter
speed dependent on characteristics of the uncertainty description
and consequentlydependent on characteristicsof the ight data.
A particularconcernfor testing with the utterometeris the qual-
ity of the uncertainty description. A description that does not con-
sider a sufcient level of modeling error may overpredict the utter
speed. Conversely, a description that considers too much modeling
error may underpredictthe utter speed. Either situation is adverse
to conducting a safe and efcient ight test.
Anaccurateassessmentof modelingerror,usingtheutterometer
approach, can only result from comparing the transfer function of
the modelto a transferfunctionthataccuratelyrepresentsthe aircraft
dynamics.Such an accuratetransferfunctionis difcult to compute.
The ight data used to generate that transfer function often contains
componentsthatviolateassumptions,suchaslinearityandstatistical
properties,associated with standard spectral analysis.
A technique was developed to analyze ight data and assess an
accurate measure of modeling error.
3
This technique actually iden-
tied model parameters and their associated variances simultane-
ously. The approach used wavelets for the signal analysis and a
min–max optimization for the estimation. This method was shown
to generate reasonable results using ight data; however, the results
are somewhat limited in that uncertaintyis only associated with the
observation matrix of the model.
This paper introducesa new techniquefor estimatinguncertainty
descriptions.The techniqueis also a wavelet-basedapproach,but it
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