Research Article  Open Access
Bingrong Miao, Feng Zhou, Chuanying Jiang, Xiangyu Chen, Shuwang Yang, "A Comparative Study of Regularization Method in Structure Load Identification", Shock and Vibration, vol. 2018, Article ID 9204865, 8 pages, 2018. https://doi.org/10.1155/2018/9204865
A Comparative Study of Regularization Method in Structure Load Identification
Abstract
This study aims to correlate the vibration data with quantitative indicators of structural health by comparing and validating the feasibility of identifying unknown excitation forces using output vibration responses. First, numerical analysis was performed to investigate the accuracy, convergence, and robustness of the load identification results for different noise levels, sensors numbers, and initial estimates of structural parameters. Then, the laboratory beam structure experiments were conducted. The results show that using the two identification methods Tikhonov (Lcurve) and TSVD (GCVcurve) can successfully and accurately identify the different excitation forces of the external hammer. The TSVD based on GCV method has more advantages than the Tikhonov based on Lcurve method. The proposed two kinds of load identification procedure based on vibration response can be applied to the safety performance evaluation of the railway track structure in future inverse problems research.
1. Introduction
In the past two decades, a large number of researchers have carried out many effective research studies on inverse problems such as structural load identification and damage identification [1–6], and many of the results have been applied to the structural health monitoring technology of structural integrity and safety assessment [7–10]. Most of the load identification techniques use these regularization methods, such as the Tikhonov method and the truncated singular value decomposition (TSVD) method. However, there are few comparative studies on the accuracy, noise resistance, and robustness of these two methods in the identification of engineering structure loads.
Thite and Thompson considered the influence of regularizing the matrix inversion, which discussed Tikhonov regularization with the ordinary crossvalidation method for selecting the regularization parameter, and they also studied an iterative inversion technique of the method [11]. Jacquelin et al. analyzed the deconvolution problem and utilized general regularization techniques to solve the illposed feature [12]. Choi et al. used the Tikhonov regularization method to improve the stability of the load identification results [13]. Wang et al. proposed an improved iteration regularization method for solving linear inverse problems and chose Morozov’s discrepancy principle to verify the posterior regularization parameter [14]. Similarly, Sun et al. combined a new improved regularization operator with Lcurve method to overcome the ill condition of load reconstruction and obtained the stable and approximate solutions of inverse problems [15]. With the development of techniques, some new regularization methods have been proposed. Aucejo et al. proposed a method able to proceed without defining any regularization parameter beforehand, and the method is called multiplicative regularization method [16]. Gao and Yu presented a new method based on quadratic programming theory to determine the regularization parameter [17]. Considering the sparsity of force in the time domain, Qiao et al. developed a general sparse regularization method based on minimizing l_{1}norm of the coefficient vector of basic functions [18]. Different loads on a mechanical system also have different regularization methods. For random dynamic loads, Jia et al. proposed a weighted regularization approach based on the proper orthogonal decomposition (POD), which the regularization parameter was selected by the GCV method [19]. Then, in order to reconstruct the impact force, Gunawan adopted the Wiener filter method and introduced a regularization technique so that the method can provide an optimum solution which balances the aspects of the minimum noise and the minimum residual [20], and Boukria et al. developed an experimental method to identify the impact force on a reinforced concrete slab [21]. In addition, Qiao et al. imposed a novel impact force reconstruction method based on the primaldual interior point method (PDIPM), which replaced l_{2}norm by l_{1}norm [22]. Gunawan extended the Levenberg–Marquardt (LM) method and a variant of the Gauss–Newton methods, in order to solve the illposed pulsetype impactforce inverse problem in conjunction with a trust region strategy [23]. A novel method was proposed to identify loads with the combination of the Tikhonov regularization and singular value decomposition (SVD) based on the condition [24].
In this paper, the TSVD of regularization parameter selection method based on generalized crossvalidation (GCV) method and Tikhonov regularization based on Lcurve method are compared and analyzed. The identification accuracy and applicability of the two methods have been summarized through the simulation of the singleinput singleoutput model (SISO) and multipleinput multipleoutput model (MIMO), and the identification characteristics of sine wave load and triangle wave load have been demonstrated. Finally, the results of simulation analysis are verified by experiments.
2. Construction of Forward Problem
This paper establishes the forward problem of load identification based on the green kernel function. According to the characteristics of the pulse function, the integral of the product of the pulse function with any other function is equal to the function value of the pulse moment. Therefore, any dynamic load of a structure can be expressed as a superposition of the unit pulse signal in the time domain:where is the external load and is the Dirac function.
It is assumed that the Green function from the loading point to the responding measurement point is z(t), which is the response of the system under the unit pulse load . According to the principle of superposition, the relation between excitation and response of system can be written as convolution form (Duhamel integral):where denotes the Green kernel function of the structure impulse response, z(t) is the measured responses which can be displacement, velocity, acceleration, strain, and stress. For systems under zero initial conditions, the integral form of Equation (2) in time domain is discretized into linear equations as follows:where is the sampling interval and m is the sampling points.
Then, it is easily to written as
Equation (4) is represented as a linear discrete equation for a SISO system. When a certain number of impact loads are applied to the different locations simultaneously, the total responses of the system can be expressed as the superposition of the dynamic responses at each known measurement point:where is the Green function matrix between the points of application of force and sensor location. Therefore, Equation (5) is transformed into a matrix form as follows:where M and N are the number of points of application and the points of measurement, respectively, and it is needed to ensure that N ≥ M. Equation (6) expresses the linear discrete equation model for MIMO system. In fact, the solution F of the linear system is very sensitive to data errors. And an attempt to solve directly the equation will likely lead to an erroneous solution. Then regularization is used to acquire a meaningful solution.
3. Regularized Method
3.1. Tikhonov Regularization
The Tikhonov regularization method can be expressed as an optimization problem as follows [25]:where is the square of the 2norm for vector is the regularization parameter.
The more exact representation of the objective function in Equation (7) can be expressed as
According to the concept that the gradient of the objective function is equal to zero, the least squares solution of Equation (8) is written as
Deriving from Equation (9), the identified load can be obtained bywhere I is the unit matrix and H indicates Hermitian transpose.
3.2. The TSVD Method
The method for dealing with illconditioned matrices is to derive new problems by using the rank deficient coefficient matrix of rank deficit. The rank deficient matrix H (which can be deduced by SVD) is approximated by k, the nearest matrix of H_{k}, which is extended by the decomposition of the truncated singular value of the rank K in Equation (6). H_{k} can be written aswhere is the singular values of the matrix H, and the vectors are the left and right singular vectors of the matrix H. The truncated singular value decomposition (TSVD) method is used to solve the following equation of the problem [26]:
The solution to Equation (12) can be written as
The solution of is the only solution to the regularization of the numerical zero space in the matrix H without components. In order to avoid excessive amplification of the identified results' disturbance error, the right end of the resulting generalized solution formula is truncated by using the method. In addition, the parts of the previous k corresponding to greater singular values are reserved, and the smaller singular values will be filtered.
4. Methods for Selecting the Tikhonov Regularization Parameter
4.1. LCurve Criterion
and are both functions of regularization parameter . The minimum between the regularization solution and the residual norm has been weighed through the Lcurve method. When the regularization parameter changes, it refers to the change of the demonstration number and the norm of the residual norm. The solution norm and the residual norm are well balanced at the inflection point of the Lcurve (the maximum curvature of the Lcurve), and the regularization parameter is the optimal regularization parameter. Therefore, the reasonable value of the point obtained by the Lcurve criterion is located at the inflection point of the curve. If the relationships are assumed, the curvature of the Lcurve is calculated as follows:
Unfortunately, since optimal regularization parameter value search range is too large, the computational cost will be high or the Lcurve graph is not satisfied.
4.2. Generalized CrossValidation (GCV) Method
The basic idea of generalized crossvalidation (GCV) means if the arbitrary element of the z is ignored, the corresponding regular resolution will be predicted better, and the regularization parameter is chosen as the orthogonal transformation of z. Therefore, choosing the regularization parameter is required to minimize the GCV function.
Equation (14) can also be expressed in discrete form.where denotes the regularized solution produced by multiplied with z (i.e., ) and k is the regularization parameter. A balance between the disturbance error and the regularization error is actually searched by using the GCV method, and the inflection point of the curve is produced.
5. Numerical Example and Test Validation
As shown in Figure 1, the example model is a beam with one end fixed to simulate a steel cantilever beam. The material properties of the beam are as follows: Young’s modulus is 2.1 × 10^{11} Pa, density is 7.8 × 10^{3} Kg/m^{3}, and Poisson’s ratio is 0.3. The size of the beam is 1 × 0.05 × 0.005 m. The beam is divided into ten elements, marked elements 1 to 10. Then, the number of finite element model nodes is expressed from the mark number of one to eleven. Numerical simulation is used to verify the efficiency of two proposed force identification method as well as compared to the identified results. Furthermore, the identified results of different loads applied on the same structure are analyzed.
For the purpose of studying the effect of noise on identified results, the noise is added to the response data.where z is the response of load identification and represents the response obtained by simulation. denotes the standard deviation of the computed response. and are the noise level and white noise sequence with the same length as , which is a mean value of 0 and a variance of 1. And the relative error between the real load and the identified load is defined as follows:
5.1. Load Identification of SingleInput SingleOutput System (SISO System)
A sinusoidal load is applied at node 11. The direction of the load is perpendicular to the Z axis of the beam, and a sampling period is . The identified load is obtained by using the response of node 10. At the noise levels 1%, 2%, and 5%, the two identification methods mentioned above are used to identify the loads. Figure 2 shows the results of the two methods when the noise level is 1%. The overall relative error of the two methods are shown in Table 1 at 0%,1%, 2%, and 5% noise levels. Among them, the noise level is 0%, which means no noise.
(a)
(b)

As shown in Figure 2, the two methods can accurately identify the load applied to the system. Obviously, it can be found clearly that the identification accuracy of Figure 2(a) is less than that of Figure 2(b) in the initial period of time. It refers that the two methods of the identified results show the analogous situation in the absence of noise in Table 2. It can be found that the identification error of Tikhonov based on the Lcurve method is greater than the TSVD method based on GCV in the case of noise. In addition, the latter method also has weak sensitivity to noise and has better adaptability. In fact, periodic synthetic signal gives naturally better results than the ones obtained from nonperiodic signal for inverse analysis, because SVD (TSVD) is based on Fourier series.

5.2. Load Identification of MultipleInput MultipleOutput System (MIMO System)
To study the differences between the two methods, a sinusoidal load in the Z direction and a triangular load in the Y direction are applied at the nodes 11 and 7, respectively, and the responses of the nodes 10 and 6 are measured. Among them, the sinusoidal load and the triangular load are described as follows:where is a period of sinusoidal load and is a quarter period of triangle load. In this case, the sampling time interval is 0.001 s, 0.0005 s, and 0.00025 s, respectively. Clearly, Figures 3 and 4 show the identification result of the above two kinds of loads in the different sampling time. Due to the great influence of high levels of noise on load identification results of MIMO system, the main features of the load to the maximum amplitude are concerned. And at the noise level 1%, the identified results of the two methods are shown in Figures 5 and 6.
According to Figures 3 and 4, it can be found that the sampling time interval has a great influence on the identification of triangle wave load, while the sine wave load is not. It means that the sampling time required for the triangular wave load is shorter than the sinusoidal load. In addition, the TSVD method has a more accurate effect than the Tikhonov method, and the former method is not sensitive to noise shown in Figures 5 and 6. Simultaneously, it can be found that the actual noise has a great influence on the identification results.
6. Experimental Validation
The cantilever beam structure applied for force identification is set up as shown in Figure 7. The material is structural steel, the length is 1.196 m, the width is 0.06 m, and the thickness is 0.0055 m. In this experimental study, the beam is clamped at one end and the excitation point is selected to be near the end of the beam. For the material properties of the steel beam, modulus of elasticity is 2.1 × 10^{11} N/m^{2}, density is 7.8 × 10^{3} Kg/m^{3}, and Poisson ratio is 0.3. Four points of the beam are attached by four accelerometers, which are IEPE voltage output piezoelectric acceleration sensor. A shaker is used to generate the sinusoidal force. The measured signals containing the force and acceleration are synchronously recorded by DH9522 data acquisition system. For the purpose of modal frequency, the finite element model of the structure is established and calculated according to the actual information of the geometry, material, and boundary conditions. A modal impact hammer is used to impose impact forces acting on the cantilever beam. The natural frequencies of simulation and experiment are compared as shown in Table 2, and the finite element model is modified according to the experimental model. And the mentioned methods of identification are verified by experiments.
(a)
(b)
From the natural frequency of Table 2, the relative error of the natural frequency of the test and simulation is relatively small and is less than 5%. It means that the established finite element model is more reliable and can be used for the identification of sinusoidal loads directly.
The dynamic response of the structure is measured by experiment, and the Green kernel function between the loading point and the measuring point is calculated by the finite element method. Therefore, the load identification equation based on the Green kernel function has been established. As shown in Figure 8, the identified results of the TSVD based on the GCV method and the Tikhonov based the on Lcurve method are compared and analyzed. The conclusion of the identified result shows that the identification load reconstructed by the TSVD based on the GCV method has higher accuracy than the Tikhonov based on the Lcurve method, and it is in suitable agreement with the actual load. And using the Tikhonov regularization method leads to obtain worse correlation error of identification near the initial moment.
7. Conclusions
This study proposes a comparative research method for the inverse problem of load identification including the TSVD (GCV) method and Tikhonov based on the Lcurve method. At the same time, numerical methods and experiments are used to verify the recognition effectiveness and robustness of these two approaches based on vibration response to identify the external excitation force. For these two kinds of regularization methods under different noise levels, the equations based on the established inputoutput relations for unknown external excitation forces are iteratively estimated. Some detailed conclusions are briefly listed below:(1)In the absence of noise, both the two mentioned methods of the above identification methods can accurately identify the load imposed on the system.(2)By virtue of the proposed method, the noise should be considered to the simulation and experiment. The results of numerical simulations and experimental are indicated that the identification accuracy of the TSVD based on the GCV method is much higher than that of the Tikhonov based on the Lcurve method. In other words, the former method is less sensitive to noise.(3)The difference between the two methods is mainly due to the fact that the Lcurve generated by the experiment is unobservable, and the optimal point on the Lcurve is difficult to localize with accuracy.(4)The results of different loads in different sampling time can get the conclusion that the identified effect of triangle wave load changes obviously with the change of sampling time. Therefore, the sampling time of linear load such as triangle wave is short; in other words, the sampling frequency could be large.
Data Availability
The data used to support the findings of this study are included within the article. The data are published on figshare website. (https://figshare.com/s/5edc2999caa536c9ef42).
Conflicts of Interest
The authors declare that they have no conflicts of interest.
Acknowledgments
The authors thank the National Natural Science Foundation of China (51375405 and 51775456) and the SelfDeveloped Research Project of the State Key Laboratory of Traction Power (2016TPL T10).
References
 H. Xue, K. Lin, Y. Luo, and H. Liu, “Timevarying wind load identification based on minimumvariance unbiased estimation,” Shock and Vibration, vol. 2017, Article ID 9301876, 15 pages, 2017. View at: Publisher Site  Google Scholar
 F. Naets, J. Cuadrado, and W. Desmet, “Stable force identification in structural dynamics using Kalman filtering and dummymeasurements,” Mechanical Systems and Signal Processing, vol. 5051, pp. 235–248, 2015. View at: Publisher Site  Google Scholar
 P. Ghaderi, A. J. Dick, J. R. Foley, and G. Falbo, “Practical highfidelity frequencydomain force and location identification,” Computers and Structures, vol. 158, pp. 30–41, 2015. View at: Publisher Site  Google Scholar
 W. Y. He, Y. Wang, and S. Zhu, “Adaptive reconstruction of a dynamic force using multiscale wavelet shape functions,” Shock and Vibration, vol. 2018, Article ID 8213105, 11 pages, 2018. View at: Publisher Site  Google Scholar
 I. Duvnjak, M. Rak, and D. Damjanović, “A new method for structural damage detection and localization based on modal shapes,” International Symposium on LifeCycle Civil Engineering, vol. 5, no. 2016, 2016. View at: Google Scholar
 P. Cao, S. Qi, and J. Tang, “Structural damage identification using piezoelectric impedance measurement with sparse inverse analysis,” Smart Materials and Structures, vol. 27, no. 3, Article ID 035020, 2018. View at: Publisher Site  Google Scholar
 C. P. Fritzen and M. Klinkov, Load Identification for Structural Health Prognosis: Structural Health Monitoring of Military Vehicles Lecture Series, vol. 2, North Atlantic Treaty Organization, Brussels, Belgium, 2014.
 Z. Boukria, P. Perrotin, A. Bennani, F. Dupray, and A. Limam, “Structural monitoring: identification and location of an impact on a structurally dissipating rockshed structure using the inverse method,” European Journal of Environmental and Civil Engineering, vol. 16, no. 1, pp. 20–42, 2012. View at: Publisher Site  Google Scholar
 D. Baroudi and E. Thibert, “An instrumented structure to measure avalanche impact pressure: error analysis from Monte Carlo simulations,” Cold Regions Science and Technology, vol. 59, no. 23, pp. 242–250, 2009. View at: Publisher Site  Google Scholar
 D. Baroudi, B. Sovilla, and E. Thibert, “Effects of flow regime and sensor geometry on snow avalanche impactpressure measurements,” Journal of Glaciology, vol. 57, no. 202, pp. 277–288, 2011. View at: Publisher Site  Google Scholar
 A. N. Thite and D. J. Thompson, “The quantification of structureborne transmission paths by inverse methods. Part 2: use of regularization techniques,” Journal of Sound and Vibration, vol. 264, no. 2, pp. 433–451, 2003. View at: Publisher Site  Google Scholar
 E. Jacquelin, A. Bennani, and P. Hamelin, “Force reconstruction: analysis and regularization of a deconvolution problem,” Journal of Sound and Vibration, vol. 265, no. 1, pp. 81–107, 2003. View at: Publisher Site  Google Scholar
 H. G. Choi, A. N. Thite, and D. J. Thompson, “A threshold for the use of Tikhonov regularization in inverse force determination,” Applied Acoustics, vol. 67, no. 7, pp. 700–719, 2006. View at: Publisher Site  Google Scholar
 L. Wang, X. Han, J. Liu, and J. Chen, “An improved iteration regularization method and application to reconstruction of dynamic loads on a plate,” Journal of computational and applied mathematics, vol. 235, no. 14, pp. 4083–4094, 2011. View at: Publisher Site  Google Scholar
 X. Sun, J. Liu, X. Han, C. Jiang, and R. Chen, “A new improved regularization method for dynamic load identification,” Inverse Problems in Science and Engineering, vol. 22, no. 7, pp. 1062–1076, 2014. View at: Publisher Site  Google Scholar
 M. Aucejo and O. De Smet, “A multiplicative regularization for force reconstruction,” Mechanical Systems and Signal Processing, vol. 85, pp. 730–745, 2017. View at: Publisher Site  Google Scholar
 W. Gao and K. Yu, “A new method for determining the Tikhonov regularization parameter of load identification,” in Proceedings of International Symposium on Precision Engineering Measurement and Instrumentation, p. 944619, International Society for Optics and Photonics, 2015. View at: Google Scholar
 B. Qiao, X. Zhang, C. Wang, H. Zhang, and X. Chen, “Sparse regularization for force identification using dictionaries,” Journal of Sound and Vibration, vol. 368, pp. 71–86, 2016. View at: Publisher Site  Google Scholar
 Y. Jia, Z. Yang, and Q. Song, “Experimental study of random dynamic loads identification based on weighted regularization method,” Journal of Sound and Vibration, vol. 342, pp. 113–123, 2015. View at: Publisher Site  Google Scholar
 F. E. Gunawan, “Impact force reconstruction using the regularized Wiener filter method,” Inverse Problems in Science and Engineering, vol. 24, no. 7, pp. 1107–1132, 2016. View at: Publisher Site  Google Scholar
 Z. Boukria, P. Perrotin, and A. Limam, “Experimental impact force location and identification using inverse problems: application for a circular plate,” International Journal of Mechanical Sciences, vol. 5, pp. 48–55, 2011. View at: Google Scholar
 B. Qiao, X. Zhang, J. Gao, R. Liu, and X. Chen, “Sparse deconvolution for the largescale illposed inverse problem of impact force reconstruction,” Mechanical Systems and Signal Processing, vol. 83, pp. 93–115, 2017. View at: Publisher Site  Google Scholar
 F. E. Gunawan, “Levenberg–Marquardt iterative regularization for the pulsetype impactforce reconstruction,” Journal of Sound and Vibration, vol. 331, no. 25, pp. 5424–5434, 2012. View at: Publisher Site  Google Scholar
 R. Guo, H.q Fang, S. Qiu et al., “Novel load identification method based on the combination of Tikhonov regularization and singular value decomposition,” Journal of Vibration and Shock, vol. 33, no. 6, pp. 53–58, 2014. View at: Google Scholar
 A. N. Tikhonov, VI. A. Arsenin, and F. John, Solutions of IllPosed Problems, Winston, Washington, DC, USA, 1977.
 P. C. Hansen, “Truncated singular value decomposition solutions to discrete illposed problems with illdetermined numerical rank,” SIAM Journal on Scientific and Statistical Computing, vol. 11, no. 3, pp. 503–518, 1990. View at: Publisher Site  Google Scholar
Copyright
Copyright © 2018 Bingrong Miao et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.