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Illustration of resampling in angle domain after upsampling the time data [6]. 

Illustration of resampling in angle domain after upsampling the time data [6]. 

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In Operational Modal Analysis applications, it is assumed that the structure is excited by white noise. However, in some cases, the operational vibration data are acquired while rotating equipment is active in the background or while it is even the main source of excitation. The structural responses will then consists of a broadband response from w...

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... Operational Modal Analysis applications, it is assumed that the structure is excited by white noise. However, in some cases, the operational vibration data are acquired while rotating equipment is active in the background or while it is even the main source of excitation. The structural responses will then consists of a broadband response from which the structural modes can be determined and additional harmonic response at discrete frequencies, which are disturbing the parameter identification process. Sometimes, the harmonic response is dominating and the Operational Modal Analysis methods only find poles at these harmonic frequencies. Therefore, it is desired to try to remove the disturbing harmonics from the data before applying Operational Modal Analysis. In this paper, a method that serves this purpose will be discussed. If the fundamental frequency of the disturbing harmonics is not known, it will be estimated by applying a “tacho-less rpm extraction” procedure. Using the (possibly fluctuating) rpm, the data can be converted to the angle domain and, then time (or better: angle) synchronous averaging is applied to remove the harmonics. This procedure will be illustrated using simulated data as well as real industrial operational data from an in-flight helicopter test and from a running large diesel engine. Operational Modal Analysis (OMA) is used to derive an experimental dynamics model from vibration measurements on a structure in operational conditions (as opposed to dedicated laboratory testing). Cases exist where it is rather difficult to apply an artificial force and where one has to rely upon available ambient excitation sources. It is practically impossible to measure this ambient excitation and the outputs are the only information that can be passed to the system identification algorithms. In this case one speaks of Operational Modal Analysis. During the last 15 years or so, Operational Modal Analysis developed and reached a mature state with advanced parameter estimation algorithms, commercial software implementations, and very relevant industrial applications. The number of applications is constantly increasing, and recently a considerable interest was raised in the application of OMA in the presence of rotating machinery. Two cases can be distinguished: • The engine is running through its operational rotation speed (rpm) range. In this case the different engine orders (harmonics) are sweeping through a broad frequency band and can be considered as unknown, but useful excitation and there is no need to apply any kind of filtering. In some cases, one has to be careful in the interpretation of certain modes as some of them are so-called “end-of order” effects. More details on this approach can be found in [1]. An example can be found in Figure 1. The engine is running at fixed (or slowly varying) rotation speed. In this case, the best excitation is at the fixed harmonic frequencies. However, these represent only a few spectral lines and do not contain sufficient information to base OMA curve-fitting on. So the modal parameter estimation also relies on the broadband excitation that is supposed to be present next to the harmonics. Unfortunately, the harmonics hamper considerably the identification process since the modal estimators will preferably find harmonics instead of structural modes. Therefore they should be removed from the data. An example can be found in Figure 2. The paper discusses the second case by presenting a method to remove the disturbing harmonics from the data before applying Operational Modal Analysis (Section 2). In Section 3, a simulated example is discussed and in Section 4, some industrial examples are given. Different methods exist in trying to separate discrete harmonic components from broadband random response. In [2] some of these are discussed, including synchroneous averaging [3], adaptive noise cancellation (ANC) [4] and the so-called Discrete-random separator (DRS) [5], which can be used in case of stationary signals (non-varying rpm) and is more efficient and robust than ANC. The difference compared with synchronous averaging is that the discrete frequency components are not required to have harmonic relationships. In [6], a method is discussed to remove order domain content in rotating equipment signals by double resampling. Double resampling refers to the fact that the time signal is first resampled in angle domain, after which the order content can be removed and then a second resampling takes place to convert the signal back to time domain. In [7], such an adaptive resampling procedure is discussed. Figure 3 shows the resampling principle. Figure 4 compares the same signal represented in frequency domain and order domain. In the angle or order domain, it will be possible to remove the disturbing chirping harmonics. Based on the ideas found in the above-cited literature, and after carrying out numerous evaluations [8], the following 4-step method (called “harmonic filter”) was found to be practical and reliable for removing harmonic disturbances in Operational Modal Analysis: 1. Measure (preferred) or estimate the fundamental harmonic / rpm of the rotational phenomenon. 2. Resample the data in angle domain (after upsampling) 3. Apply sliding window (angle) synchroneous averaging for separating discrete (harmonic) and random (broadband response) components (see also Figure 5). 4. Restore the signal in time domain Note that after the procedure, a time signal is obtained with the same length and sampling frequency as the original signal. Therefore it is possible to apply also time-domain OMA methods. It is also worth noting that in [9] an alternative approach was developed consisting in the reformulation of some classical modal parameter estimation algorithms to account for the presence of undamped harmonics, i.e. the modal equations were complemented by harmonics with fixed and known frequencies, but amplitudes and phases which are estimated together with the modal parameters. A 6 Degree-of-Freedom (DOF) system was excited by white noise. A disturbing harmonic was added to the excitation. In order to make it challenging, the frequency did not remain constant, but was constructed as an FM-modulated 12 Hz component of which the frequency could vary with about ± 4 %. Moreover, the carrier frequency (12 Hz) of the disturbance coincides with a mode of the system. Figure 6 shows the simulation results. When the disturbing component is not removed from the data, the modes could be identified, but in addition, much more modes around 12 Hz showed up in the stabilization diagram. Also the mode shape estimation is seriously compromised by the disturbing high-amplitude peaks in the spectra. When removing the disturbance using the 4- step approach outlined in Section 2, the PolyMAX modal parameter estimation results correspond very well to the true values. In this section, the procedure outlined in Section 2 will be applied to real industrial operational data from an in-flight helicopter test and from a running large diesel engine (Figure 7). Key to the method is the knowledge of the fundamental frequency of the disturbing harmonics. It is always a good idea to measure it during the operational test using a tacho probe. However, when it is not available, the “tacho-less rpm extraction” procedure developed in [10] can be applied to a response signal which is “close” to the harmonic excitation source. Also the Hilbert transform is useful to verify the stationarity and phase of these signals: Figure 8 shows the envelope of two helicopter roof acceleration signals which were band-pass filtered around the blade-pass frequency. It is clear that in this 30s recording, the harmonic amplitude is not constant (non-stationary signal). Figure 9 shows the phase of the Hilbert transform from which the instantaneous pulsation can be obtained by derivation (Figure 10). In this way, also an estimate of the rpm can be obtained. The 2 signals seem to agree well, except for some spikes in the signal, which indicate a bad estimate of the instantaneous pulsation in the signal due to low amplitudes (spikes in Figure 10 correspond to low envelope values in Figure 8. Using the measured or estimated (possibly fluctuating) rpm, the data can be converted to the angle domain and, then time (or better: angle) synchronous averaging is applied to remove the harmonics. Such a filtered spectrum is shown in Figure 11. A typical in- flight helicopter mode shape is shown in Figure 7. mode was found (Figure 12 – Top). After filtering the harmonics from the time series, OMA could be successfully applied (Figure 12 – Bottom). Moreover, it was found that the OMA modal parameters were in good agreement with the modal parameters identified using impact test and classical modal analysis (the engine was not running during impact testing). This paper introduced the “harmonic filter”, a method which is able to filter disturbing harmonics from broadband time data. The envisaged application is Operational Modal Analysis, where it was observed that the applicability to certain industrial problems was hampered by the presence of these harmonics. It was shown that the harmonic filter successfully filters the measured time signals so that the, originally hidden, structural modes can be identified using e.g. Operational PolyMAX. This work was carried out in the frame of the EUREKA project E! 3341 FLITE2. The financial support of the Institute for the Promotion of Innovation by Science and Technology in Flanders (IWT) is gratefully ...

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... The presence of harmonics in the vibration measurements can lead to th e failure of typical OMA techniques in numerous ways. If the harmonic response is dominant , it can mask and suppress the true modal content of the structure [9], or it can be wrongfully identified as a lightly damped structural resonance [10]. When structural and periodic modes are close, further errors in parameter estimation can arise as the identification methods usually result in poor convergence of the parameters [11]. ...
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The safety of dams is of extreme importance, considering the high economic value and cost of failure. To assess the performance of these structures over their lifetime, vibration monitoring can be a useful tool. However, in hydroelectric generating power plants, rotating machinery can introduce harmonics into the measurements and make current methods of modal parameter estimation invalid, necessitating harmonic removal. While recent research has focused on harmonic removal in rotating mechanical machinery like wind turbines and large generators, there is a gap in understanding of monitoring gravity dams in environments with significant harmonic contamination. Most ambient vibration tests of dams have been conducted on arch and buttress-type structures, which have experienced relatively low harmonic contamination. To address this gap, a study was performed on the Mactaquac Generating Station, the largest hydroelectric power plant in the Maritime provinces, using full-scale monitoring data as part of the Mactaquac Life Achievement Project (MLAP). The study found that under low operation demand, it was possible to successfully estimate the benchmark modal parameters of the structure. However, during high operational demand, the measured signals were dominated by harmonic content, which caused several errors in the modal estimation results compared to periods of low demand. However , by reducing the harmonics in the signal, the first four mode shapes of the dam structure were successfully identified. This demonstrates that harmonics can significantly impact the accuracy of mode estimation, but their effects can be mitigated through harmonic reduction techniques.
... The oldest reported methods belong to the techniques denoted broadly as Time Synchronous Averaging (TSA), which are intuitively sound and easy to implement, at least in their most basic form. TSA was proposed for wind turbines in Peeters et al. [12] and has been more recently used in Manzato et al. [10]. The idea is to average consecutive cycles of the signal to eliminate its stochastic part and retain the deterministic (periodic) one; this is to say, TSA is an implementation of a so called comb filter, as shown in Braun [13]. ...
... Finally, the modified DFT is transformed back in the angular domain and the resulting signal is resampled in the time domain. To improve the accuracy, the process relies on large oversampling factors (10)(11)(12)(13)(14)(15)(16)(17)(18)(19)(20). ...
... The figures have the same internal inlet structure, as explained next. (12) corresponding to 1P, 3P, 6P and 9P. The analysis frame duration used was 10 s (CS1), 11 s (CS2) and 14 s (CS3) according to the criterion from Section 2.3. ...
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... It was applied to near healthy gears, and used mainly to extract the time varying mesh stiffness (TVMS), and separate it from the geometric transmission error (GTE). In [42], the signals were pre-processed by the time synchronous averaging (TSA) method [43] to remove the deterministic components, which may cause disturbances in the OMA process. The transfer functions were identified from the extracted random part of the signals by the cepstrum-based OMA, and were then removed from the original TE measurements to reconstruct the forcing functions. ...
... Secondly, the random excitation of the system needs to be frequentially smooth and flat (on a log scale). For gear signals, it is reasonable to assume that the system has broadband excitation after removing the deterministic components by the time synchronous averaging (TSA) method [43] or the cepstral editing technique [17]. Detailed justifications of these two assumptions were provided in [42]. ...
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... To some extent, the drawbacks of harmonic filtering can be alleviated by using time synchronous averaging (TSA) (Peeters et al., 2007), where harmonics can be removed by isolating them from the measurement data. In this method, given the known rotor speed, the response data are resampled into the "angle" domain using constant angular speed increments. ...
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... The first, that the excitation is a broadband stochastic process, has been extensively studied, with techniques put forward for both strongly harmonic or cyclic loading and mitigating the impact of non-stochastic loading (e.g. [2], [3], [4], [5]). The second, that the systems behaviour is linear; for a given input force the response of the system is constant, has seen growing interest in recent years due to increased adoption of long-term monitoring of structures. ...
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... The well-established methods, namely stochastic subspace identification (SSI), a parametric time-domain technique, and enhanced frequency domain decomposition (EFDD), a non-parametric frequency-domain technique, are known to have imprecise identification when dealing with random loads combined with a steady-state signal. In frequency analysis, the harmonics are known to hide or bias the estimation of physical mode [18], while in the SSI algorithm, the harmonics are usually identified as very lightly damped stable poles [19]. ...
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The paper investigates the use of operational modal analysis (OMA) techniques applied directly into a rotating machinery with hydrodynamic journal bearings. OMA has proven to be a strong tool for analyzing the dynamics of large structures, especially to its capabilities in civil engineering; however, its application in rotordynamics is still very incipient. The objective here is to make a broader analysis of how this technique can be used in the universe of rotating machines and how the results become reliable. The application of this technique in rotating machines implies some care due to the inherent operating conditions of the system, especially regarding the presence of harmonic forces. The study emphasizes resonance problems with the early natural modes of the structure and its damping. The main novelty of the paper is to present a simple procedure, tapping throughout the rotor, which made possible the application of OMA to extract the modal parameters with satisfactory results in a system in which the classical EMA steeped sine technique was insufficient to provide a good analysis of the rotor. In this type of system, the hydrodynamic bearings and misalignments caused by the coupling of shaft and motor (something quite common in real systems) may cause difficulty in extracting modal parameters depending on the technique used. However, when applying traditional OMA methods, using both the frequency domain (enhanced frequency domain decomposition) and the time domain (stochastic subspace identification), it was possible to make a good identification of the modal parameters of the rotor, with promising results to encourage a broader modal identification of rotating machinery in operating conditions.
... An analysis of simulated vibration data by the pLSCF method showed that a harmonic frequency, coinciding with a structural mode, led to spurious stable poles around this frequency [11]. The authors also analyzed operational data of a large diesel engine. ...
... Although different studies report successful utilization of SSI [6,12] and pLSCF [4,10,11] methods for OMA of rotating machinery, it is believed that no direct performance comparison of these methods has been conducted yet. ...
... In a 6 DOF simulation [11], the method was able to remove the disturbing influence of harmonics on the subsequent modal estimation with the pLSCF method despite a harmonic coinciding with a structural mode. Results from a real operational inflight helicopter and a running diesel engine showed that TSA resulted in much cleaner stabilization diagrams and thus facilitated the estimation of structural modes. ...
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... For example, time-synchronous-averaging (TSA) is a method extracting periodic waveforms from signals by averaging their blocks synchronized in the angular domain. For OMA, this averaged signal is subtracted from the raw measurements, which results in the removal of the periodic frequencies selected to synchronize the blocks [4]. Angle matching is often achieved with tachometer measurements, which is not practical in real-life applications and was attempted to be overcome in the context of TSA in [5]. ...
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The modes of linear time invariant mechanical systems can be estimated from output-only vibration measurements under ambient excitation conditions with subspace-based system identification methods. In the presence of additional unmeasured periodic excitation, for example due to rotating machinery, the measurements can be described by a state-space model where the periodic input dynamics appear as a subsystem in addition to the structural system of interest. While subspace identification is still consistent in this case, the periodic input may render the modal parameter estimation difficult, and periodic modes often disturb the estimation of close structural modes. The aim of this work is to develop a subspace identification method for the estimation of the structural parameters while rejecting the influence of the periodic input. In the proposed approach, the periodic information is estimated from the data with a non-steady state Kalman filter, and then removed from the original output signal by an orthogonal projection. Consequently, the parameters of the periodic subsystem are rejected from the estimates, and it is shown that the modes of the structural system are consistently estimated. Furthermore, standard data analysis procedures, like the stabilization diagram, are easier to interpret. The proposed method is validated on Monte Carlo simulations and applied to both a laboratory example and a full-scale structure in operation.
... Stable milling operations consist of both periodic content and random background noise [14,15]. In addition, application of OMA in fields outside manufacturing, such as in vibrating civil structures [16], in-flight helicopters [17], and wind turbines [18], have shown that forces containing both types of signals can generate broadband excitation of the structures, which enables estimation of FRFs. Because 6-dof industrial robots are significantly more compliant than their CNC machine tool counterparts, the background random noise can excite the robot's natural modes of vibration to measureable levels suitable for OMA. ...
Article
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Impact hammer experiments are typically used for identifying the Frequency Response Function (FRF) of six-degree-of-freedom (6-dof) industrial robots for machining applications. However, the modal properties of 6-dof industrial robots change as a function of robot arm configuration. Hence, describing the robot’s modal parameters within its workspace requires off-line impact hammer experiments performed at discrete robot end effector positions, which are costly and time consuming. Instead, it is more efficient to calculate the robot FRF using Operational Modal Analysis (OMA), a method that utilizes data acquired during the actual machining process. This paper presents an OMA approach to identify the robot FRF from measured milling forces and robot tool tip vibrations. Analysis of the milling process data reveal that periodic forces produced in the milling process are accompanied by background white noise that induce broadband excitation across the robot structure’s frequency spectrum. Hence, the tool tip vibration signal contains the signature of the structure’s free response that enables the use of OMA to estimate the robot’s FRF. The FRF calculated using OMA is shown to be in good agreement with results obtained from impact hammer experiments.