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A Technique to Improve the Empirical Mode Decomposition in the Hilbert-Huang Transform

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A Technique to Improve the Empirical Mode Decomposition in the Hilbert-Huang Transform Vol. 2, No. 1 EARTHQUAKE ENGINEERING AND ENGINEERING VIBRATION June, 2003 Article ID: 1671-3664 ( 2003 ) 01 - 0075-11 A technique to improve the empirical mode decomposition in the Hilbert-Huang transform Yangbo Chen (~)t and Mafia Q. Feng (~(-~)* Civil & Environmental Engineering, University of California, Irvine, CA 92697, USA Abstract: The Hilbert-based time-frequencyanalysis has promising capacity to reveal the time-variant behaviors of a sys- tem. To admit well-behaved Hilbert transforms, component decomposition of signals must be performed beforehand. This was first systematically implemented by the empirical mode decomposition (EMD) in the Hilbert-Huang transform, which can provide a time-frequency representation of the signals. The EMD, however, has limitations in distinguishing different components in narrowband signals commonlyfound in free-decay vibration signals. In this study, a technique for decompo- sing components in narrowband signals based on waves' beating phenomena is proposed to improve the EMD, in which the time scale structure of the signal is unveiled by the Hilbert transform as a result of wave beating, the order of component ex- traction is reversed from that in the EMD and the end effect is confined. The proposed technique is verified by performing the component decomposition of a simulated signal and a free decay signal actually measured in an instrumented bridge structure. In addition, the adaptability of the technique to time-variant dynamic systems is demonstrated with a simulated time-variant MDOF system. Keywords: time-frequency analysis ; Hilbert-Huang transform; component decomposition 1 Introduction provide satisfactory resolution to reveal the changes in the system "s frequencies. The tradeoff is harder to The classical system analysis theory and practice reach when the phenomenon contains multiple time have been overwhelmingly dominated by Fourier scales ( Huang et al. , 1998). transform, which represents system characteristics in Take the structural health monitoring application the frequency domain. However, by computing the as a particular example. The time-variant properties global characteristics of the system averaged over the of the monitored structural system can be attributed to whole period of time, Fourier transform loses the time (1) the non-linearity of the system, such as the track of the sudden events and the gradual variation of structural damages due to extreme loading conditions the system. In reality, many of the signals observed or the structural degradation due to aging or fatigue; are of transient nature; more importantly, there are (2) non-stationary external excitation, for example many applications that concern the time-variant prop- the traffic on the bridges and the earthquakes; (3) erties of the system, such as structural health monito- the time varying boundary conditions and temperature ring. In some cases, one can assume a piecewise lin- stress affected by the environmental temperature chan- ear time-invariant system and apply the Fourier trans- ges; or even (4) the ill-defined system itself, for ex- form within each of the limited time windows, which ample, for bridge monitoring based on traffic-induced is the short time Fourier transform or the spectrogram vibrations, the decrease of the system's natural fre- analysis ( Grtichenig, 2001 ; Mallat, 1999). Howev- quency due to the additional mass of vehicles running er, to represent the time-variant properties of the sys- on the bridge is oftentimes mistakenly interpreted as a tem, the time width of the window is preferably short, decrease in the stiffness of the bridge structure. These but a short-windowed Fourier transform may not time-variant phenomena have different time scales. For example, the structural degradation may have a Correspondence to: Yangbo Chen, Civil & Environmental time scale of years, while the temperature changes Engineering, University of California, Irvine, CA92697, USA. may have a time scale of seasons or days, the non- Tel : 949-824-6359 ; Fax : 949-824-2117 stationary external excitation a scale of hours or mi- E-mail : Yangboc@ uci. edu nutes and the structural damage a scale of several sec- t Ph. D Student; *Professor onds. Received date: 2003-03-17; Accepted date: 2003-06-02 Therefore, an adaptive alternative for analyzing 76 EARTHQUAKE ENGINEERING AND ENGINEERING VIBRATION Vol. 2 the time-variant system is desirable. One of the prom- and the idea of component decomposition contributed ising alternatives is the Hilbert-Huang transform, a by Huang is also reviewed, which is retained and im- time-frequency domain method based on the Hilbert plemented in the proposed technique. transform proposed by Huang and demonstrated to possess the capacity for analyzing the non-linear non- 2 Instantaneous frequency/amplitude stationary data by applying it to the numerical results of some classical nonlinear equation systems and data The cornerstone of time-frequency domain analysis from natural phenomena (Huang et al., 1998; is the concepts of instantaneous frequency and instan- 1999 ). The key part of Huang~ method is the empiri- taneous amplitude of a signal. The well-known Heis- cal mode decomposition (EMD) to decompose the enberg uncertainty theorem (Grschenig, 2001 ) has signal into a finite number of components admitting ruled out the possibility of an exact definition of in- well-behaved Hilbert transforms. The Hilbert-Huang stantaneous frequency based on the Fourier definition transform has found application in different fields, in- of frequency ; that is, if the energy is well localized at cluding earthquake engineering (Zhang and Ma, some special point in time, it is not possible to be lo- 2000), wind engineering (Pan et al., 2003) and calized at any specific value in frequency, and vice structural dynamics ( Yang and Lei, 2000 ; Salvino, versa. Nevertheless, by introducing the Hilbert trans- 2000). form and the notation of the analytic signal, the However, the EMD method has its limitation in unique and physical definitions of the instantaneous distinguishing different components in narrowband sig- frequency and the instantaneous amplitude of a signal nals. In some cases, a narrowband signal is practical- can be obtained, but with a different physical expla- ly considered as only one component; but there are nation of frequency, generalized from the conventional other cases where further decomposition is necessary Fourier definition. to reveal its component structure, especially for the An arbitrary real signal S(t) has its Hilbert trans- purpose of analyzing the system properties based on form Y(t) and its analytic signal Z(t), as the free decay response signals. A narrowband signal may contain either (1) components that have adja- Y(t) = __1 [S(T)dr" " 1) qr J t -T cent frequencies, or (2) components that may not have adjacent frequencies, but one of them has domi- nant energy intensity much higher than the other com- Z(t) = S(t) + iY(t) = a(t)e i~ 2) ponents. In Huang et al. (1998) , the EMD method a(t) = [S2(t) + y2(t)]l/2 3) has been used to analyze narrowband signals of the first category, but extremely stringent criteria have to O(t) = arctan Y(t) (4) be enforced on the EMD so that it can be carried out s(t) to an extreme extent (3000 iterations, as in Huang et al., 1998) to distinguish different components, to(t) = O'(t) (5) which involves significant effort. Narrowband signals of the second category, commonly found in the struc- where, to(t) is denominated as the instantaneous fre- tural vibration measurements, have not yet been ad- quency and a ( t ) the instantaneous amplitude. The dressed. They are hardly distinguishable with the physical explanation (Hahn, 1996) can be achieved EMD method either, as will be shown later with ex- in polar coordinate representation of the analytic sig- amples in section 5. nal Z(t), in which the instantaneous amplitude a(t) In this study, a technique to improve the EMD is the length of the phasor and the instantaneous fre- method for efficiently distinguishing components in quency to (t) is the instantaneous angular speed of the narrowband signals is proposed. The technique is phasor rotation. based on the beating phenomenon of waves, Combi- As can be seen from Eq. (1), the local property ning with Hilbert transform, the technique possesses of S (t) at time t is magnified by Hilbert transform better power to reveal the time-variant properties of when 7 approaches t; indeed, Hilbert transform of a the system embedded in the measured narrowband sig- signal is its best local fit of an amplitude and phase nals. The new technique is demonstrated by applying varying trigonometric function (Huang et al. , 1998). it to the simulated data and the data recorded in the To show the relationship between the Hilbert- real bridge structure under traffic loading. Prior to the based instantaneous frequency/amplitude in Eqs. presentation of the proposed technique, some con- (5) and (3) and the conventional Fourier-based fre- cepts important in time-frequency analysis and an im- quency/ amplitude, it is worthwhile to revisit an im- portant property of Hilbert transform are reviewed, portant property of Hilbert transform. No. 1 YangboChen et al. : A technique to improve the empirical mode decomposition in the Hilbert-Huang transform 77 H[f(t)g(t) ] = f(t)H[g(t) ] (6) 3 EMD and Hilbert-Huang transform provided that f(t) and g (t) are signals of non-over- Only a mono-eomponent signal admits a well-be- lapping spectra and that f(t) has low-pass spectrum haved Hilbert transform (Huang et al. , 1998 ). This while g ( t ) has high-pass spectrum. H [ S ( t ) ] de- can be intuitively demonstrated by a signal with two notes the Hilbert transform of signal S(t). The proof components S( t ) : a~ (t)cos(tolt) + a2 ( t ) cos ( to~t ). of this property can be found in Hahn (1996). After the Hilbert transform, the analytic signal of By inserting a modulated signal S (t) -- A (t) cos (tot) S(t), Z(t) gives only one pair of to(t) and a(t) at into Eqs.
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