P or b a b i l i s t ci aD am g e Quna t i f i c ta ino iv ... · sA such, it is cir t i c la for...

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e h t a i v n o i t a c i f i t n a u Q e g a m a D c i t s i l i b a b o r P n o N f o n o i t a r g e t n I - e m i T c i r t e m a r a p - s e i r e S s l e d o M n o i s s e r g e R s s e c o r P n a i s s u a G d n a A M H A S O L U O P O T F A S P O K S I T O F d n a R E M A D R T S B A A T C e n O f o e h t r o j a m s e g n e l l a h c e h t l a r u t c u r t s l a e h h t g n i r o t i n o m ) M H S ( y t i n u m m o c s i g n i c a f y a d o t s i d e t a l e r o t g n i l b a n e e t a r u c c a d n a t s u b o r e g a m a d n o i t c e t e d d n a i f i t n a u q - n o i t a c r e d n u g n i y r a v g n i t a r e p o d n a l a t n e m n o r i v n e s n o i t i d n o c h t i w a d e t i m i l r e b m u n f o g n i s n e s a t a d . s t e s n I , r a l u c i t r a p e t a t s -f o- e h t - t r a e v i t c a - g n i s n e s M H S s e i g o l o n h c e t e c a f t n a c i f i n g i s s e i t l u c i f f i d n i y l e t a r u c c a g n i t c e t e d d n a g n i y f i t n a u q e g a m a d n i h t i w n i a t r e c n u s t n e m n o r i v n e e u d o t e h t k c a l f o e t a i r p o r p p a l a c i t s i t a t s g n i n r a e l d n a e c n e r e f n i . s d o h t e m s A t i , h c u s s i l a c i t i r c r o f e h t y t i n u m m o c o t ha e v v a e l b a l i a s l o o t t a h t y l e t a r u c c a t c e t e d d n a y f i t n a u q e h t g n i s u , e s n e s c i t s i l i b a b o r p a n i , e g a m a d d e t i m i l s e m i t n e t f o r o f n i e l b a l i a v a - o i t a m n. n I s i h t d u t s y, a l e v o n c i t s i l i b a b o r p e g a m a d n o i t c e t e d d n a n o i t a c i f i t n a u q h c a o r p p a s i d e s o p o r p d e s a b n o e h t n o i t a r g e t n i f o n o n - c i r t e m a r a p l a c i t s i t a t s e m i t s e i r e s n e s e r p e r - s n o i t a t d n a n a i s s u a G s s e c o r P n o i s s e r g e R s l e d o M . ) s M R P G ( , y l l a i t i n I n o n - c i r t e m a r a p s l e d o m d e s a b n o t r o h S - e m i T r e i r u o F m r o f s n a r T ) T F T S ( r e w o p l a r t c e p s y t i s n e d ) D S P ( s e t a m i t s e e r a d e s u n i r e d r o o t t c e t e d e g a m a d d n a y l l a c i t s i t a t s e n i m r e t e d l a n g i s ) e v a w ( s h t a p t a h t y r r a c e h t t s o m n o i t a m r o f n i t u o b a e g a m a d . e z i s , t x e N s M R P G e r a d e n i a r t g n i s u e g a m a D x e d n I ) I D ( s e u l a v m o r f d e t c e l e s e v a w n o i t a g a p o r p s h t a p d n a d e s u o t s e- e t a m i t e h t e g a m a d e z i s d e s a b n o e h t t n e r r u c I D . s t e s e h T l a t n e m i r e p x e t n e m s s e s s a s i d e t n e s e r p r o f a t a d d e d r o c e r m o r f a d e h c t o n m u n i m u l a e t a l p . t I s i h so n w , t a h t g n i s u wave n o i t a g a p o r p s h t a p d e t c e l e s y b n o n - c i r t e m a r a p l a c i t s i t a t s , s l e d o m n o i t a m i t s e y c a r u c c a n i- s e s a e r c d n a e g a m a d e z i s t s e n o i t a m i e c n e d i f n o c s l e v e l e m o c e b , r e w o r r a n s u h t g n i d i v o r p a t s u b o r d n a t n e i c i f f e e g a m a d n o i t c e t e d d n a n o i t a c i f i t n a u q . h c a o r p p a N O I T C U D O R T N I h t i W e h t t n e v d a f o w e n g n i s n e s d n a a t a d s i s y l a n a , s d o h t e m e v i t c a - g n i s n e s l a r u t c u r t S h t l a e H g n i r o t i n o M ) M H S ( e t s y s s m e v a h n w o h s l a i t n e t o p n i , g n i t c e t e d g n i z i l a c o l d n a g n i y f i t n a u q e g a m a d . , r e v e w o H e u d o t r i e h t d e s a e r c n i y t i v i t i s n e s o t g n i t a r e p o d n u o b ( - y r a , s n o i t i d n o c , s d a o l ) . c t e d n a l a t n e m n o r i v n e , e r u t a r e p m e t ( , y t i d i m u h ) . c t e i d n o c - , s n o i t e v i t c a - g n i s n e s M H S s d o h t e m l l i t s e c a f t n a c i f i n g i s s e g n e l l a h c n e h w t i s e m o c o t d a m h A , r e m A D h P , t n e d u t S : l i a m E u d e . i p r @ 2 a r e m a . s i t o F , s o l u o p o t f a s p o K t n a t s i s s A , r o s s e f o r P : l i a m E d e . i p r @ f a s p o k u. t n e g i l l e t n I l a r u t c u r t S s m e t s y S b a L , ) L S S I ( t n e m t r a p e D f o , l a c i n a h c e M e c a p s o r e A d n a r a e l c u N N , y o r T , e t u t i t s n I c i n h c e t y l o P r e a l e s s n e R , g n i r e e n i g n E Y, A S U in the Proceedings of the 12th International Workshop on Structural Health Monitoring September 2017, Stanford, CA, USA

Transcript of P or b a b i l i s t ci aD am g e Quna t i f i c ta ino iv ... · sA such, it is cir t i c la for...

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in the Proceedings of the 12th International Workshop on Structural Health Monitoring September 2017, Stanford, CA, USA

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their operation in dynamic environments and multiple operating conditions under uncer-tainty [1–3]. In addition, even in the case of constant or controlled environments and“hotspot” monitoring, such methods face difficulties in quantifying damage due to theuncertainty in the damage propagation patterns and the variation in the locations of thesensors within nominally identical structural components [1]. When it comes to dam-age quantification, the currently-employed approaches are of deterministic nature, i.e.they do not allow for the extraction of appropriate confidence intervals for damage sizeestimation, and require the collection and analysis of an immense amount of baselinedata from a population of identical structures to account for changing conditions. Thus,active-sensing SHM damage detection and quantification methods are still lacking therequired confidence for large-scale applicability and approaches that are both accurateand robust need to be developed, all without increasing data footprint.

Statistical time series methods have been widely used for vibration-based damagedetection, localization, and quantification within a probabilistic framework [4–6]. How-ever, their use in active-sensing guided-wave SHM has been limited. In a recent study[2], the authors have proposed the use of non-parametric time series models and cor-responding statistical hypotheses tests for probabilistic damage detection via the use ofPower Spectral Density (PSD) estimators of wave propagation signals. Although suchnon-parametric models have the advantage of simplicity, their potential to effectivelytackle the more elaborate task of damage quantification is limited. Therefore, advancedstatistical learning and inference methods are necessary to address the probabilistic quan-tification of damage in the face of uncertainty. In this context, stochastic modeling viaGaussian Process Regression Models (GPRMs) has been used for regression and clas-sification applications within the machine learning community [7, 8], as well as for theidentification of structural dynamics under varying operating conditions [9] and surro-gate modeling of computationally-expensive high-fidelity models [10, 11].

In this study, a novel active-sensing probabilistic damage detection and quantifica-tion method is proposed based on the integration of non-parametric time series modelswith stochastic GPRMs. The fundamental premise of the method is that the incorpo-ration of optimized actuator-sensor path information, in the form of properly-selecteddamage indices (DIs), in the GPRM-based statistical learning for damage quantifica-tion can provide accurate and robust damage size estimation with confidence intervals.First, non-parametric Short-Time Fourier Transform (STFT) models are applied in orderto identify the actuator-sensor wave propagation paths that intersect damage, thus lead-ing to the selection of the most damage-sensitive signal paths in order to optimize theamount of information being fed into the GPRM-based statistical learning phase. Next,after the GPRM training phase has been completed via the use of DIs obtained fromthe paths selected in the first step under different damage sizes, GPRMs are used withfresh DI values in order to estimate their corresponding damage size along with statisti-cal confidence intervals, thus fulfilling the damage quantification part of this study. Theuse of GPRMs allows for the accurate prediction of damage size even when a single

sensor-actuator path is used for training. Furthermore, multivariate GPRMs, that utilizethe appropriate number of paths as determined in the first step, are shown to exhibit nar-rower damage confidence intervals when compared to their univariate and multivariatewith randomly selected paths, counterparts. To the authors best of knowledge, this is thefirst time GPRMs are utilized for the quantification of damage in active-sensing SHM.

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GAUSSIAN PROCESS REGRESSION MODELS

The problem of data-based statistical learning for inference and prediction can betackled via stochastic GPRMs that can be used for both regression and classification andtake the form of a full predictive distribution [7, 9]. In the present work, GPRMs areemployed to “learn” the relationship between damage indices and damage size withina Bayesian probabilistic framework. In particular, the model output g(x), i.e. damagesize, is represented via a functional relationship of latent variables f(x) from a Gaussianprocess of the input(s) (scalar or vector; also referred to as covariates or predictors) x,i.e. the DI values of actuator-sensor signal propagation paths, based on a Bayesian linearregression model [7]:

g(x) = f(x) + h(x)T�, where f(x) ⇠ GP(0, k(x,x0)). (1)

In these equations, k(x,x0) designates the covariance function (kernel) of the zero-meanGaussian process f(x). The D-dimensional input vector x is transformed into a p-dimensional feature space using the set of basis functions h(x), that along with thecoefficients (parameters) vector �, to be inferred from the data, represent the mean ofthe model. Incorporating explicit basis functions in the GPRM allows for the completespecification of the Gaussian process mean, thus enabling interpretability of the modeland convenience of expressing prior information.

Fitting such a GPRM includes the joint optimization over the parameters � with thekernel hyperparameters, which are free parameters that the covariance function dependsupon, and are specific to the type of function being used [7]. Thus, given a training dataset {(xi, yi), i = 1, 2, . . . , n}, the output (herein the damage size) can be modeled viathe vector form of the probabilistic GPRM:

P (y|f ,X) ⇠ N(y|f +H�, �2I) (2)

such that

y =

0

BBB@

y1y2...yn

1

CCCA, X =

0

BBB@

xT1

xT2...xTn

1

CCCA, f =

0

BBB@

f(x1)f(x2)

...f(xn)

1

CCCA, H =

0

BBB@

h(xT1 )

h(xT2 )

...h(xT

n )

1

CCCA. (3)

Here, it is assumed that the observed values y differ from the function values g(x)by additive zero-mean Gaussian noise with variance �2. Essentially, the use of GPRMsinstead of regular linear models, entails a joint Gaussian distribution upon the regres-sion parameters, thus providing confidence bounds for the prediction/estimation pro-cess [7, 9]. GPRMs also involve the transformation of a nonlinear problem in the orig-inal input space into a linear one in a high-dimensional feature space using the “kerneltrick” [7,12]. This allows for capturing uncertainties that may stem from operational andenvironmental variability [9].

In this study, the input (predictor) matrix (X) comprises of DI values obtained fromboth single and multiple actuator-sensor wave propagation paths (n is the total numberof observations and D is the number of actuator-sensor paths included in the model)and is used to train univariate and multivariate, respectively, GPRMs for an aluminumnotched plate, which are then utilized to estimate the notch size y.

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Figure 1. The notched Al plate experimental coupon used in this study.

THE EXPERIMENTAL SETUP

A 152.4⇥254 mm (6⇥10 in) 6061 Aluminum coupon (2.36 mm/0.093 in thick) witha 12.7 mm (0.5 in)-diameter hole in the middle was used in this study. Using Hysol EA9394 adhesive, 6 lead zirconate titanate (PZT) piezoelectric sensors (type PZT-5A fromAcellent Technologies, Inc), having a diameter of 3.175 mm (1/8 in) and a thicknessof 0.2 mm (0.0079 in), were attached to the Al plate as shown in Figure 1. A 2 mm(0.079 in) notch was cut extending from the hole of the Al plate using an end mill, thenelongated in 2-mm increments up to 20 mm (0.79 in), for a total of 10 damage cases,using a 0.81 mm (0.032 in) handsaw.

A series of 5-peak tone-burst actuation signals with 90 V amplitude peak-to-peakand various center frequencies were generated in a pitch-catch configuration. A total of20 data sets per structural case (11 cases in total; one healthy and 10 damage cases) werecollected at a sampling rate of 24 MHz using a ScanGenie III data acquisition system(Acellent Technologies, Inc). The data were then exported to MATLAB for analysis1.

RESULTS AND DISCUSSION

In the context of active-sensing using guided waves, there are often multiple sensorsinstalled at the area being monitored, and every actuator-sensor path in the network hasto be examined in order to assess the integrity of the component, which may compromisethe accuracy and robustness of the analysis process. Figure 2 panels a and b show thesignal received at sensor 6 when sensor 2 was actuated (see Figure 1). As shown, becausethis is a damage-intersecting path, a significant change can be observed in the signals asnotch size increases. Exploring actuator-sensor paths that do not intersect damage, suchas path 1-5 (Figure 2 panels c and d) one can observe that the received signals at sensor5 exhibit a significantly smaller change in amplitude with notch size. Thus, informationfrom damage-non-intersecting actuator-sensor paths, such as path 1-5, naturally carry

1Matlab version R2018a.

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Figure 2. Indicative signals for the notched Al plate. (a) Full signal received at sensor 6 whensensor 2 is actuated, and (b) its first-arrival wave packet. (c) Full signal received at sensor 5

when sensor 1 is actuated, and (d) its first-arrival wave packet.

less information when it comes to damage quantification compared to paths that intersectdamage. In order to further support this point, one state-of-the-art DI from the literature[1], was explored to see how damage intersection affects damage quantification usingthe DI approach. Figure 3 panels a and b show the evolution of the selected DI withnotch size for indicative damage-intersecting (path 2-6) and damage-non-intersecting(path 1-5) paths (see Figure 2), respectively. From Figure 3, it becomes apparent that theperformance of damage quantification models may be significantly affected by the typeof information and corresponding data employed to train them.

In this sense, a statistical method was recently developed to assess which actuator-sensor paths intersect damage and which do not, as a preliminary filter for damagequantification models, where only data sets carrying the most important informationare processed [2]. In this method, an STFT-based non-parametric model is used anddamage-intersecting paths are selected according to the PSD change of the path due todamage. Briefly, damaged areas that provide a reduction in guided-wave impedance(reduce wave energy attenuation that would otherwise occur in a healthy component)would allow more signal energy to pass, while less energy would pass if the damagedarea causes the increase in wave impedance. Based on these observations, the developed

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Figure 3. The evolution of the damage index [1] as applied to indicative actuator-sensor paths:(a) damage-intersecting path 2-6 and (b) damage-non-intersecting path 1-5.

method can also identify damage-non-intersecting paths. Figure 4 shows indicative re-sults of applying such a model2 onto the first arrival wave packets of the signals shown inFigure 2. As can be seen in Figure 4a, because the notch is a damage of the second typementioned above, a decrease in the median/mean STFT-based PSD value with increas-ing notch size can be observed for path 2-6. On the other hand, the increase in the PSDwith notch size for the damage-non-intersecting path (see Figure 4b) can be explainedin terms of the energy being scattered off the notch in damage-intersecting paths whensensor 1 is actuated; those scattered waves of energy go to sensors that are not directlyon the path of the notch. Thus, using this approach, it is possible to identify damage-intersecting actuator-sensor signal propagation paths that are expected to contain themost valuable information in terms of damage sensitivity. This feature can be utilizeddirectly in increasing the accuracy and robustness of damage localization and quantifi-cation algorithms. In this study, it is applied to improve the performance of GPRMs fordamage quantification.

Damage Quantification via Univariate GPRMs

For the probabilistic damage quantification task, GPRMs3 for indicative damage-intersecting and non-intersecting paths were trained using 15 DI values for every struc-tural case (healthy case and notch sizes from 0 mm to 20 mm), thus 165 observationswere used to train the model (11 structural cases ⇥ 15 data sets). Next, 5 DI valuesper case were used to estimate the notch size (55 observations) and assess the method.All models presented in this study utilized linear basis functions and exponential kernelfunctions in the estimation process. GPRMs were first implemented for one actuator-sensor path at a time, i.e. GPRMs based on a single input variable which is the DIset of that specific path, in order to assess their ability to quantify damage using a sin-gle path. Figure 5 shows the results of applying univariate GPRMs onto the indicative

2Matlab function spectrogram.m (window size: 400-900; nfft: 960; noverlap: 95%)3Matlab functions fitrgp.m (n: 11 ⇥ 15 data sets for training; basis function: linear; kernel function:

exponential) and predict.m (n: 11 ⇥ 5 data sets for validation/estimation)

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Figure 4. Indicative results of applying the non-parametric model onto actuator-sensor paths.Short Time Fourier Transform (STFT) plots for the signals of (a) damage-intersecting path 2-6

and (b) damage-non-intersecting path 1-5.

damage-intersecting (panel a) and non-intersecting (panel b) paths shown in Figure 2.The estimated damage sizes, using 5 calculated DI sets that were not used in modeltraining, are presented as red stars; the actual damage sizes are depicted in blue circles.An important conclusion from this figure is that the use of a damage-intersecting path inGPRM significantly improves the damage size estimation accuracy compared to usingsignals from actuator-sensor paths that do not directly intersect damage. Thus, usingthe non-parametric model described in the previous section, damage-intersecting pathscan be selected and fed into both univariate and multivariate GPRMs in order to get anaccurate estimation of damage size.

Damage Quantification via Multivariate GPRMs

In this section we investigate the performance of multivariate GPRMs, i.e. using DIsobtained from several wave propagation paths as GPRM inputs, in terms of probabilisticdamage quantification. Indicative GPRMs were trained using 15 data sets, but this timeincorporating DIs from multiple paths, hence multivariate models, where each DI repre-sents an input variable. The aforementioned non-parametric model used for identifyingdamage-intersecting paths was coupled with multivariate GPRMs in order to assess theperformance of quantification when using paths that contain the most accurate infor-mation about damage size. Figure 6 panels a and b show indicative damage estimationresults based on GPRMs trained via two sets of three randomly-selected paths, where thereal notch size, all 5 estimated notch sizes (from 5 DI sets per case), and 95% confidenceintervals for each individual structural case are shown. Figure 6c shows the same plot forthree paths that were marked as damage-intersecting by the STFT model. An apparentdifference between the latter panel and former two is the significantly improved accuracyof the notch size estimation. Hence, prior selection of damage-intersecting paths allowsfor both improved accuracy and narrower confidence intervals.

In order to explore the quantification process using multiple paths, selected bothblindly and based on the STFT model, the standard deviation of the estimated notch

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Figure 5. Indicative univariate GPRM estimation plots trained using 5 DI sets of (a)damage-intersecting path 2-6, and (b) damage-non-intersecting path 1-5.

and the mean estimation errors were used as metrics for assessing the performance ofmultivariate GPRMs. Figure 7a presents the mean of the standard deviation of the es-timated damage sizes as more paths are included in the training phase. The blue barsare for wave paths chosen blindly, i.e. with no regard to the nature of the path in termsof damage intersection. Although there are 30 paths available, the standard deviationmean levels off after 14 paths are used to train the model, so up to 16 paths are shown.Red bars indicate paths marked as damage-intersecting by the non-parametric model,which were 12 in this case. As shown, using as few as 2 selected paths for training themodel, the standard deviation mean decreases by more than 35% compared to the blind(random) path selection. As the number of training signal paths (DI data sets) increases,the models trained via paths selected by the non-parametric method converge to a lowermean standard deviation, even at 12 paths. Using more than 12 paths, the mean standarddeviation decreases until it levels off at 14 paths. Thus, it can be concluded that thedamage size estimation confidence levels become narrower when only selected paths areutilized in training the GPRM, thus leading to more accurate damage quantification.

Figure 7b shows the mean estimation error for all notch sizes versus the numberof incorporated paths when paths, and therefore DI data sets, are chosen blindly or viathe non-parametric model. Again, the estimation error when the model is trained basedon selected paths is significantly smaller compared to the blind selection of paths withno regard to their nature. As expected, the blue and red estimation error percentagesconverge to similar values as the number of training paths increases.

CONCLUDING REMARKS

In this work, an active-sensing probabilistic damage quantification method basedon the integration of non-parametric time-series and GPRMs was introduced. Non-parametric STFT models were used in a notched Al plate to pinpoint damage-intersectingpaths that carry damage-size information. Both uni- and multivariate GPRMs weretrained using single/multiple actuator-sensor paths from 15 data sets, and then used to es-timate damage size for 5 data sets. It was shown that the use of damage-intersecting paths

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Figure 6. Indicative damage size estimation boxplots based on multivariate GPRMs: (a and b) 5DIs used for two sets of three randomly selected paths; (c) 5 DIs used from three paths indicated

by the non-parametric model.

for univariate GPRM training results in increased damage estimation accuracy. Further-more, using paths marked by the non-parametric model as damage-intersecting to trainmultivariate GPRMs, it was observed that damage size estimation confidence intervalsbecome significantly narrower compared to using paths blindly- (randomly-) selected.The reliability of the proposed damage detection and quantification method was assessedusing the mean of the estimation standard deviation, as well as the mean estimation er-ror. It was shown that using as few as two properly-selected actuator-sensor paths fortraining multivariate GPRMs, the estimation standard deviation mean was much lowerthan that for multivariate GPRMs trained using randomly-selected paths. The resultsof this study indicate the potential of coupling non-parametric time-series models withstochastic GPRMs for improved learning towards probabilistic damage quantification.

ACKNOWLEDGEMENTS

This work is carried out at the Rensselaer Polytechnic Institute under the Vertical LiftResearch Center of Excellence (VLRCOE) Program, grant number W911W61120012,with Dr. Mahendra Bhagwat and Dr. William Lewis as Technical Monitors.

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Figure 7. Reliability quantification for the multivariate GPRMs trained using selected and blind(random) paths. (a) Mean of estimation standard deviations for 2-16 paths. (b) Estimation error

percentage for 2-12 paths.

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