Analysis and Extraction of Temperature Effects on Natural Frequencies of a Footbridge based on Continuous Dynamic Monitoring Wei-Hua Hu, Carlos Moutinho, Filipe Magalhães, Elsa Caetano & Álvaro Cunha Faculty of Engineering of University of Porto (FEUP), Portugal ABSTRACT: The development of efficient vibration based structural health monitoring systems requires distinguishing between abnormal changes in modal parameters caused by structural damage and normal changes due to varying environmental conditions. In this context, this paper is focused on the analysis and extraction of effects of temperature oscillations on natural frequencies of a footbridge, where a long-term dynamic monitoring system was installed by the Laboratory of Vibrations and Monitoring of the Faculty of Engineering of University of Porto. With that purpose, firstly, the temperature influence on the natural frequencies is reported, and correlations between measured temperatures and estimated natural frequencies are analyzed. Then, the Principal Component Analysis (PCA) and the Novelty Detection method are applied to identified natural frequencies: PCA effectively eliminates environmental influence; Novelty analysis on the residual error of PCA predicted model is used as a statistical indication of damage. The proposed procedure is illustrated using continuous dynamic data collected from the footbridge during more than one year. 1 INTRODUCTION Structural Health Monitoring (SHM) has become a major international research topic in recent years in civil engineering. One of the main obstacles in the application of SHM is the environmental and operational variations of structures. The so called ‘damage sensitive’ features are also sensitive to changes in environmental and operational conditions of structures, which often mask subtle structural changes caused by damage (Hoon Sohn 2007). Therefore, important issues in SHM are the analysis of influences of environmental and operational variations, and the achievement of damage indication based on the removal of such effects. In this context, this paper is focused on the analysis and extraction of effects of environmental and operational conditions on natural frequencies of a slender footbridge, where a long-term dynamic monitoring system was installed by the Laboratory of Vibrations and Monitoring (ViBest, www.fe.up.pt/vibest ) of FEUP. Firstly, the temperature influence on natural frequencies is reported, and correlations between measured temperatures and estimated natural frequencies are analyzed. Then, the Principal Component Analysis and the Novelty Detection method are applied to identified natural frequencies. The proposed procedure is illustrated using continuous dynamic data collected from the new Coimbra footbridge. IOMAC' 09 – 3rd International Operational Modal Analysis Conference 56 2 DESCRIPTION OF THE BRIDGE AND DYNAMIC MONITORING SYSTEM The new “Pedro e Inês” footbridge over Mondego River is located in the centre of the City Park of Coimbra, recently developed along the two banks of the river and opened to public in April 2007. This new infrastructure, conceived to become a landmark for the city and to contribute to the quality of a new leisure area, was designed by Adão da Fonseca (Adão da Fonseca et al 2005), leading a team from AFAssociados, in collaboration with Cecil Balmond, leading the architectural team from Ove Arup. The bridge has a total length of 275m and is formed by a parabolic central arch with a span of 110m and two half lateral arches, in steel, supporting with total continuity a composite steel concrete deck (Fig.1). The anti-symmetry of both arch and deck cross-sections along the longitudinal axis of the bridge is a unique feature of this bridge, leading to the creation of a central square with 8m×8m at mid-span. AV1 AV2 AV5 AV3 S3 30.5 0m 64.00 AV6 S2 55.00 m S1 55.00 m 64.00 m west m 6.00 m east AT4 (a) Bridge plan and elevation, deployment of accelerometers and sections (S1-S3) with temperature sensors North North South T2 TA South T1 Section 1 (S1) T3 TC North Section 2 (S2) AT4 AV5 South T4 Section 3 (S3) (b) Sections (S1-S3) and temperature sensors Figure 1. Deployment of accelerometers and temperature sensors Numerical and experimental studies, developed by the Laboratory of Vibration and Monitoring from FEUP, showed that this slender footbridge is prone to excessive vibrations caused by groups or streams of pedestrians. Therefore, six groups of tuned mass dampers (TMDs) were installed (Caetano, Cunha et al 2008). Aiming the permanent characterization of vibration levels after construction, the footbridge was also instrumented with a dynamic monitoring system, formed by signal acquisition, data communication and signal processing modules. The signal acquisition system comprises six uniaxial piezoelectric accelerometers installed in correspondence with the location of TMDs (Fig. 1). Five of them measure vertical accelerations (AV1-AV3, AV5-AV6), whereas another one measures lateral vibrations at mid-span (AT4). All sensors are mounted inside the metallic deck and wired to the corresponding signal conditioners and digital computer incorporating an analogue to digital converter and a UPS system, located in one of the concrete abutments of the structure. An automatic signal acquisition toolkit was developed in LabVIEW environment to record the acceleration signals and generate setup files every 20 minutes. The data communication system sends permanently the most recent collected data to a computer located at FEUP using an ADSL line (Moutinho et al 2008). The signal processing system is a toolkit developed in LabVIEW. It automatically searches the latest data transmitted from the bridge in 57 Coimbra, detects maximum vibration amplitudes and makes statistical treatment of acceleration time series, generates waterfall plots to depict the frequency component distribution and identifies modal parameters using automated EFDD and SSI-COV techniques (Hu et al 2008). Besides the accelerometers, 6 temperature sensors (Fig. 1) were also installed by the Laboratory for Concrete Technology and Structural Behaviour of FEUP to provide environmental data, including the ambient temperature (TA), concrete slab temperature (TC), and temperature in different steel sections (T1-T4), which were well selected by the designer in order to provide an adequate representation of the bridge behaviour (Dimande et al 2008). The set of mentioned components can be considered as a simple dynamic structural health monitoring system that has been operating since the 1st of June 2007 till now, except for a stop from the 1st of September 2007 to the 13th of October 2007. 3 EFFECT OF TEMPERATURE ON NATURAL FREQUENCIES In this study, the temperature data from the 6 temperature sensors exhibit similar trend and therefore the average temperature is used to represent environmental variation. Fig. 2 depicts annual variation of one-hour average temperature during day light time. It is observed that the average temperature at the footbridge ranges from 0.19°C to 34.40°C. Figure 2. Variation of one-hour average temperatures from 1st June 2007 to 31st May 2008 (The monitoring system was not operating from 1st Sep 2007 to 13th Oct 2007) frequency daily average frequency (a) 1st natural frequency identified by EFDD frequency daily average frequency (c) 1st natural frequency identified by SSI-COV frequency daily average frequency (b) 2nd natural frequency identified by EFDD frequency daily average frequency (d) 2nd natural frequency identified by SSI-COV Figure 3. Variation of identified modal frequencies by both EFDD and SSI-COV methods from 1st June 2007 to 31st May 2008 (The monitoring system was not operating from 1st Sep 2007 to 13th Oct 2007) 58 IOMAC' 09 – 3rd International Operational Modal Analysis Conference The structure natural frequencies have been automatically identified by the signal processing system for each hour. Fig. 3 shows the annual variation of the first two natural frequencies estimated by the used methods. To further illustrate the annual tendency, the daily average frequency curve is also displayed. It is observed from Figs. 2-3 that the frequency domain EFDD and the time domain SSI-COV methods produce similar results, and the first two natural frequencies are inversely related to changes in measured temperature. The relation between natural frequencies and temperature may be further clarified by Fig. 4. As shown, the first two natural frequencies identified by different methods both decrease as temperature rises. From a statistical point of view, the relations between temperature and natural frequencies can be assumed as linear. Therefore, a linear regression model was developed to represent the first two natural frequencies as function of the average temperature, which can be mathematically described as fi=a+bti, where a and b are coefficients to be estimated, ti are the samples of average temperature and fi are corresponding natural frequencies. f1=0.843-0.00039t f2=1.402-0.00030t (a) Natural frequencies identified by EFDD versus average temperature f1=0.843-0.00038t f2=1.401-0.00029t (b) Natural frequencies identified by SSI-COV versus average temperature Figure 4. Natural frequency versus average temperature According to Fig. 4, it may be concluded that the frequencies identified by both EFDD and SSI-COV methods can reflect similar global effect of temperature, despite the better performance of SSI-COV, which allows a better frequency resolution of the estimates. Although other environmental and operational factors such as wind, humidity and traffic loading may also affect the natural frequencies, from the viewpoint of long term monitoring, temperature may be considered the main environmental factor. Statistical analysis of these two natural frequencies shows that the normal temperature change produces variations of 1.7% and 1.4%, which may mask the change of natural frequency caused by structural damage. To establish a baseline for long term structural health monitoring, such effect induced by temperature should be eliminated effectively, and features which are sensitive to damage yet insensitive to environmental change are necessary. 59 4 ELIMINATION OF THE TEMPERATURE EFFECT 4.1 Theory of Principal Component Analysis and Novelty Detection technique Principle component analysis (PCA) is a multi-variate statistical method. Under the assumption that the environmental conditions have a linear effect on the identified parameters, PCA methodology can eliminate such effect. In the current study, PCA analysis is used to remove temperature effect. Subsequently, novelty detection technique may be used to detect possible damage. The basic idea of novelty detection is first to build an internal representation of the structure’s baseline in normal condition, and then examine subsequent data to see if they significant depart from a normal condition. Let us consider the matrix Y ∈ R n× N whose column vectors y k are the identified n-order natural frequencies at time tk,(k=1,2,…..,N, N is the number of samples). A singular value decomposition of the covariance matrix of Y is YY T = UΣU T (3) Σ1 0 (4) Σ= 0 Σ2 where U is an orthonormal matrix ( UU T = I ), whose columns define the principal components and form a subspace spanning the data, Σ is the singular value matrix representing the active energy of the associated principal components. Matrix Σ can be split in two parts: Σ1 = diag (σ 12 , σ 22 ...σ m2 ) is a diagonal matrix with the square of the first m singular values on the diagonal, ranked by decreasing order, and Σ 2 = diag (σ m2 +1 , σ m2 + 2 ...σ n2 ) . Define the indicator: m i =1 I= σ i2 n i =1 σ i2 (5) and determine m as the lowest integer such that I > e(%) , where e is a threshold value (i.e. 95%). The meaning of this threshold is as following: m unobserved factors contribute to e% of the variance in the observed data (Deraemaeker et al 2007). The first m columns of U are the principal components, which are associated with the most influencing unobserved factors and constitute a transformation matrix T (loading matrix). T can project the frequency matrix Y into the environmental-factor characterized space X (scores matrix) X=TTY (6) The new data can be re-mapped into original space Yˆ = TX (7) The residual error E due to the loss of information while performing the two-way projection can be calculated as E = Y − Yˆ (8) The new feature vector is given by E, it corresponding to the dynamic features from which the environmental effects have been removed. Applying the novelty detection technique to the residual error E, the Novelty Index (NI) can be defined using the Mahalanobis norm NI k = E kT R −1 E k (9) T where R=(YY )/N is the covariance matrix of frequency matrix Y. To detect possible damage, an X-bar control chart (Yan et al 2005; Diego et al 2005) is constructed by drawing two lines: a centre line (CL) and an additional horizontal line corresponding to an upper limit (UCL), these are: C L = NI (10) IOMAC' 09 – 3rd International Operational Modal Analysis Conference 60 UCL = NI + ασ (11) where NI and σ is the mean value and standard deviation of NI in the reference healthy state. α is taken as 3, which corresponding to 99.7% confidence. Two criteria can be employed as damage warning (Deraemaeker et al 2007; Yan et al 2005; Diego et al 2005): (1) outlier analysis, counting for the percentage of the NI lying outside the UCL and (2) ratio of NI between healthy and damage state. In the healthy state, the new vibration features should stay in the hyperplane spanned by the features in reference state. Percentage of the NI overpassing UCL is rather small and ratio of NI → 1 . On the contrary, with the emergence of damage, the new vibration features will depart from hyperplane in the reference healthy state, which will cause a significant increase of outliers and relatively large ratio of NI . 4.2 Application of Principal Component Analysis and Novelty Detection Methodology PCA and novelty detection have been already applied in numerical and laboratory models (Deraemaeker et al 2007; Yan et al 2005; Diego et al 2005). In this paper, this method is used for the long term monitoring results of Coimbra footbridge. According to Fig. 4, it can be assumed that temperature has a linear effect on the first two natural frequencies. Temperature linear effect on frequencies can be also reflected by linear relation between different frequencies, as shown in Fig. 5. These two natural frequencies identified by EFDD method constitute matrix Y= [y1, y2]. Substituting Y into Eqs. (3-5), one obtains the singular values 2.654 and 3.751E-6 with I > 99.9% , which indicates that only one environmental factor markedly affects the variation of natural frequencies. In the following part, two sets of frequencies identified by EFDD method both in winter time and in summer time are investigated to illustrate the potential of removing the temperature effect. (a) EFDD results (b) SSI-COV results Figure 5. Correlation between the first two natural frequencies from 1st, June 2007 to 31st, May 2008 Fig. 6 shows two sets of consecutive samples both in summer and winter. The corresponding average temperature varies from 18.17 ºC to 34.40 ºC in summer, whereas changes from 0.19 ºC to 16.46ºC in winter. It is clear that most of the two natural frequencies estimates in winter time are higher than those in summer time because of temperature effect. PCA and Novelty Detection are applied to these data and results are shown in Fig. 7. It can be observed that NI in both two sets stay in the same level, the results of outlier analysis are similar and the ratio of NI → 1 . The effect of temperature is efficiently removed. This footbridge is new and no damage is reported from 1st June, 2007 to 31st May, 2008. A baseline healthy state of this footbridge has been constructed based on the monitoring results during this period. The successive monitored data from 1st June 2008 to 1st December 2008 is used to compare with baseline state. The corresponding results of NI are displayed in Fig. 8. Compared with baseline healthy state, the NI during the period 1st June 2008 to 1st December 2008 still remain small, outlier analysis exhibits similar results and ratio NI are still close to 1, which means that the footbridge is still in a healthy stage and no damage occurred, as expected. 61 winter summer winter summer (a) 1st frequency (b) 2nd frequency Figure 6. Comparison of the first two natural frequencies both in summer (18.17 ºC -34.40 ºC) and winter (0.19 ºC -16.46ºC) winter outlier analysis: 1 % summer outlier analysis: 1% NIw/NIs=0.977 Figure 7. Residual error of data in summer (18.17 ºC -34.40 ºC) and winter (0.19 ºC -16.46ºC) Set I Set II outlier analysis: 0.8 % outlier analysis: 1.3% NI I / NI II =0.991 Figure 8. Comparison of residual error of data in Set I:1st June, 2007-31st May, 2008 and Set II: 1st June, 2008- 1st December, 2008 5 CONCLUSION This paper mainly discusses the effect of temperature on natural frequencies of a new footbridge based on long term dynamic monitoring data. Firstly, results from appropriate data processing confirm that temperature is an important environmental factor that originates a linear effect on identified natural frequencies. To remove this effect, PCA and Novelty Detection techniques were introduced. The potential of this methodology is illustrated by two sets of data in winter and summer time. Finally, long term monitoring data collected during the first year is used to construct a baseline healthy state. The remaining data is processed and compared with this baseline state to detect possible damages. As this footbridge is quite new, the ratios between averaged NI remained close to one, as expected. In the future, possible damage will be 62 IOMAC' 09 – 3rd International Operational Modal Analysis Conference numerically simulated and the potential of PCA and Novelty Detection techniques will be further investigated. ACKNOWLEDGMENTS The authors acknowledge the financial support provided by the Portuguese Foundation for Science and Technology (FCT) in terms of Basic Funding of CEC / FEUP, as well as the Ph.D. Scholarship provided to the first author. REFERENCE Hoon Sohn. 2007. Effects of environmental and operational variability on structural health monitoring. Phil.Trans.R.Soc.A (365), p.539-560 Adão da Fonseca.A and Balmond.C. 2005. 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