Analysis and Assessment of Ground Motion Characteristics and Similarity Using Dynamic Time Warping Distance

DOI: https://doi.org/10.21203/rs.3.rs-2594272/v1

Abstract

Due to the complex nonstationarity of ground motion in time-frequency domain, the traditional methods of comparing and evaluating earthquake waveforms have not enough ability and accuracy to distinguish the details and changing features of the similar waves, which makes the similarity evaluation of waveform is difficult to be quantified accurately. The similarity degree of different signals can be calculated precisely according to Dynamic time warping (DTW) algorithm, so it can be used for waveform comparison and similarity evaluation. In order to improve the traditional method, a method based on DTW distance is proposed to identify the earthquake waveform and analyze the ground motion characteristics. Based on the statistical analysis of a great quantity of earthquake waves, the changes law of DTW distance considering amplitude, time lag, noise signal ratio, site type and the comprehensive effect is obtained. DTW distance is proved to be used as a compatible evaluation standard for waveform refinement. It is verified that DTW distance and vector norm are essentially equivalent. In the analysis of ground motion, DTW distance is implicated in the equivalent amplitude and energy of earthquake waves. The physical connotation of DTW distance is demonstrated by analyzing the data of the station array, and the results show that the distribution of DTW distance can accurately imply the time-space variation effect of the earthquake in the region. The reasonable reference range of DTW distance is defined by statistical method, and the corresponding evaluation standard of synthetic multi-point ground motion with real characteristics is proposed. In the synthetic accuracy evaluation of artificial ground motion with spatial variation effect, the combination of ground motions with more real characteristics can be obtained by evaluating and optimizing the waveforms according to the variation rule and range of DTW distance.

1. Introduction

The ground motion is a complex time-space stochastic process. Due to the influence of the focal mechanism, propagation path, dispersion effect and site conditions, the frequency distribution and amplitude intensity of a certain earthquake wave have obvious time-varying characteristics and nonstationary characteristics (Faravelli, 1988; Kubo and Penzien, 1979), which result in the structural seismic response are nonstationary both in time domain and frequency domain (Hasgur, 1995). In addition, due to the strong randomness and inhomogeneity of the ground motion in space, the wave characteristics of different measuring position under the same earthquake are variable, which results in the difference in seismic excitation and response at different locations for long-span structures or multipoint support structures (Lin et al., 1997). Many studies have shown that intensity or amplitude, spectrum distribution and duration are three elements of the basic characteristics of ground motion. The current seismic design and structural analysis mainly represent the spectrum characteristics and spectral intensity of the ground motion in terms of the site classification and the amplitude of response spectrum, and this method is relatively macroscopic and rough.

With the development of earthquake engineering (Massa et al, 2006 and Saad et al, 2019), whether accurately describing the seismic time-frequency evolution characteristics and the dissimilarity among different ground motions or evaluating the artificial earthquake wave or the simulated wave generated by shaking table meet the requirements of design specifications and engineering requirements, it is necessary to adopt more accurate quantitative analyses for intensity, frequency distribution and duration. Thus, it is of great research and engineering significance to introduce a comprehensive evaluation index in order to reveal the slight differences in waveform and characteristics of different earthquake waves.

In fact, there are similar demands to discriminate different time-domain signals in other research fields, such as mechanical engineering, clinic diagnosis and signal analysis, the relevant methods can be called waveform similarity evaluation. The index of similarity evaluation for different earthquake waves mainly include peak deviation, wave correlation coefficient and waveform distortion. It is undoubtedly inaccurate to distinguish different waveforms only by the peak deviation. The waveform correlation coefficient method uses the maximum of convolutions of two signal to measure the degree of waveform correlation, which has a large amount of calculation and cannot display the local difference of the signals. The distortion of time domain can be defined as the ratio of the amplitude difference of the contrast wave and the fundamental wave to the amplitude of the fundamental wave. The frequency domain distortion of the signal can be defined as the energy of each subharmonic of the contrast signal and the ratio of the total energy to the fundamental wave. The waveform distortion is generally considered the first choice to measure the similarity of earthquake waves, and the distortion degrees of the displacement waveform and acceleration waveform are mainly used to evaluate the waveform distortion. Although the physical meaning of waveform distortion is clear and easy to calculate, it cannot entirely and accurately reveal the coincidence degree between the contrast waveform and the standard waveform, especially to evaluate the local stochastic characteristics. Therefore, it is necessary to introduce a more accurate method and an index of waveform similarity evaluation.

The dynamic time warping (DTW) algorithm is firstly introduced in speech signal processing and classification (Itakura, 1975). Its core idea is to elongate or shorten the length of the signal until it fits the length of the reference signal. In this process, the time axis of the contrast signal will be distorted or bent, so that its characteristics and standard mode correspond to the contrast and analysis. The DTW can be used to calculate the similarity degree of two signal sequences and provide the point-to-point match, which can minimize the two sequence distances, and the matching and recognition effect is good. The DTW algorithm has been widely used in several fields such as the fault diagnosis of dynamic multivariable industrial processes, biological gene sequencing, and electrocardiogram signal classification (Zhen et al., 2013; Han et al., 2016). Bagnall et al.(2017) have implemented 18 recently proposed algorithms in a common framework and compared them against two standard benchmark classifiers (and each other) by performing 100 resampling experiments on each of the 85 datasets. The results show that the recognition method based on DTW distance has good discrimination capacity.

Currently, researchers attempt to apply the DTW algorithm to seismic analysis and comparison. Joswig and Schultetheis(1993) and Schultetheis and Joswig(1993) take the DTW distance between earthquake waves as the criterion to determine the correlation of weak local earthquakes and use the DTW distance to compare and cluster the locations of induced earthquakes in the Ruhr basin. Orozco-Alzate et al.(2015) proposed a dissimilarity space based on the DTW distance measure to classify seismic volcanic patterns either waveforms or spectrograms as alternative to both the nearest neighbor rule directly applied to the dissimilarities and classification in a dissimilarity space based on the Euclidean distance between pairs of seismic spectra. Li et al.(2010) studied the application of similarity measurement in the similarity analysis of simulated multi-point ground motions, and the analysis results show that the DTW distance method not only can quantitatively represent the similarity of simulated ground motion, but also offers advantages in clustering analysis and singularity recognition of actual multi-point ground motions. However, the variation of DTW distance and the mechanism relationship between DTW distance and ground motion characteristics have not been deeply explored. Hu et al.(2018) proposed a method integrating dynamic time warping and local outlier factor to identify anomalies of time series on various time scales, and a case study is presented focus on the measured foundation uplift beneath the local riverbed blocks of Xixi reservoir dam. Results show that this method can accurately identify abnormal time.

In summary, the above research usually apply DTW distance as the only index of ground motion similarity or convergence, and lack of further excavation of the basic performance and laws of DTW distance, There is also no demonstration of the physical connotation between the non-stationary and distribution characteristics of seismic data in time and space and DTW distance.

In view of this, this paper further studies the application of DTW in the discrepancy of ground motion and introduces an evaluation method of ground motion waveform identification and ground motion characteristics analysis based on the DTW distance. The method considers the change in DTW distance under the effects of the time, amplitude, signal-to-noise ratio and spatial distribution of the factors, and take it as the evaluation standard of artificially generated earthquake wave. The results show that the DTW distance can accurately characterize these factors in detail and identify the stationary and nonstationary characteristics of different waveforms, which becomes an effective basis for the wave similarity evaluation and selection.

2. Dynamic Time Warping (Dtw) Algorithm

When solving the correlation degree of time series data, it can be regarded as the distance between multi-dimensional vectors. Euclidean distance is the most frequently used distance measure in data mining algorithm, but it can only calculate the distance sum of the same sequence position. For two time series with similar shape but staggered in time axis, the distance calculated by Euclidean distance is very large, so the two time series are misjudged as different signals.

The dynamic time warping (DTW) algorithm is a nonlinear regularity algorithm that combines time warping and distance measurement. Its core idea is to find a valid path through the search to accurately calculate and measure the distance between two waves at each time and determine the similarity based on the distance. A smaller DTW distance corresponds to a higher similarity degree (Gollmer and Posten 1996; Forestier et al., 2012). Suppose there are two earthquake waves T and R with N and M data points, respectively, and N ≠ M. n and m are the data point number corresponding to each wave. As shown in Fig. 1, data points T and R along the horizontal and vertical coordinates are listed, the relation between each data point can form a grid, any cross point in the grid (n, m) means an intersection of T(n) and R(m), and the distortion degree of the intersection point is d[T(n), R(m)], i.e., the Euclidean distance between T(n) and R(m). Based on DTW algorithm, the best path from the starting point to the termination point through each intersection point can be found and the total degree of distortion of all intersection points on the path is minimum.

The selection of the DTW path is not arbitrary. First, considering the time sequence of the ground motion waveform, the order of every part cannot be reversed, so the choice of the route must start from the lower left corner and terminate at the upper right corner. Second, to make the path not excessively lean, the maximum and minimum of the average slope of each path must be limited, so that with the symmetrical distribution of slope on both sides of the diagonal, the maximum and minimum of the slope can be constrained in the range of 0.5 ~ 2. Then, the path selection must consider all data points and cannot skip any point. Finally, the former point when one arrives at any point (ni, mi) can only be a point among three points (ni−1, mi), (ni−1, mi−1), and (ni, mi−1). At this point, the DTW distance is D(n, m) and it can be expressed as a recursive formula as follows:

$$D({n_i},{m_i})=d[(T({n_i}),R({m_i}))]+\hbox{min} [D({n_{i+1}},{m_i})+D({n_{i+1}},{m_{i+1}})+D({n_i},{m_{i+1}})]$$
1

With the above recursive formula, the best path from the starting point to the end point and the DTW distance between the two waveforms can be obtained. The above analysis shows that it is feasible to use the DTW distance to test the similarity degree of the ground motion and evaluate the characteristics of the waveform. To test the accuracy of the DTW algorithm, two typical earthquake waves are selected, the time interval is 0.02 s and the first 10 seconds are mainly analyzed. Figure 2 shows the dynamic warping path graph of the two waves, where the white curve indicates the selection process of the best path in the calculation, and the DTW distance is 12.97, so the algorithm eliminates the adverse effects of the bending phenomenon on the distance measure, can effectively handle the local time displacement, and finally the reasonable matching results are obtained. If the local amplitude values of one earthquake wave are shifted, as shown in Fig. 3, the distance of the DTW path is 7.15, which is relatively small. When the local waveforms of the two waves coincide, the DTW path is a straight line, whereas the path of the alignment part becomes a curve. The result shows the calculation process of the DTW algorithm is dynamic when selecting the best path, and the DTW distance and path are sensitive to the change in waveform. The above research shows that DTW distance is relatively accurate and objective as an index for evaluating the similarity of ground motion waves.

3. Characteristic Evaluation Of The Earthquake Wave Based On Dtw

The characteristics of ground motion can generally be indicated by the three basic elements: amplitude, spectrum and time history. For different ground motions, it is relatively easy to identify and evaluate the characteristics when the three elements are only different on the extreme or overall boundary. However, when all three elements changes or only local subtle differences occur, the difficulty of the similarity evaluation dramatically increases. For natural ground motion, the earthquake waves acquired under analogous site conditions contain similar mechanisms and change regulation, but their randomness and nonstationary often obscure the inherent similarity, so we must analyze the data in detail. On the other hand, for the synthesis of artificial ground motion, because the algorithm cannot fully represent the real vibration characteristics, besides the introduced random noise, it is necessary to introduce a precise and stable method to evaluate the accuracy of different synthesis methods or the similarity of different waves generated by the same synthesis method. In addition, when one uses the shaking table structural dynamic test, the error control system causes an output wave with different amplitudes of the original wave and a mix of noise and output time-lag, the determination of whether the wave generated by the shaking table satisfies the accuracy requirements needs an accurate waveform similarity evaluation method (Shortreed et al., 2002; Phillips et al., 2014).

As previously mentioned, the waveform similarity evaluation based on DTW has promising prospects, and it can comprehensively compare the amplitude ratio, traveling wave effect (time lag), noise level and local variation in detail, and it is the ideal waveform similarity identification index. Hence, it is necessary to explore the effect of these factors on the characteristics of ground motion based on the DTW distance. To obtain the relevant mechanism, the DTW statistical analysis of natural ground motion data is conducted in this study. First, the variation rule of the DTW distance under the influence of each factor is studied; then, the ground motion waveform similarity evaluation and feature recognition standard considering the comprehensive effectiveness are proposed. In the specific analysis, 40 typical acceleration waves are selected from the PEER ground motion database (Harichandran and Vanmarcke, 1986) as samples. Ten earthquake waves are collected in four site types, and all the time intervals are 0.02 s. The variation rule of the DTW distance under various factors is statistically analyzed.

3.1 Relationship between amplitude and the DTW distance

To study the effect of different peak acceleration for DTW distance, we randomly selected two earthquake wave data w1 and w2 from the above 40 waves. First, the two earthquake waves are normalized, and the amplitude of the wave w2 is multiplied by different amplification coefficients to generate various waves; then, we calculated the DTW distance between the waves and w1, respectively. The typical results are shown in Fig. 4. There is a strict linear relationship between the dynamic amplitude of the earthquake and the distance of the DTW, and the effect of the amplitude on the distance of the DTW is significant. Therefore, the DTW distance of different amplitude magnification coefficients can be directly calculated for the same ground motion according to the linear relationship. In addition, the results indicate that when the effect of the factors excluding the amplitude on the earthquake waves is required, the maximum amplitude of the waves should be adjusted to the same value.

3.2 Statistical analysis of the DTW distance considering the traveling wave effect

To obtain the statistical rule of the DTW distance under the traveling wave effect (time lag), we firstly normalized 40 earthquake waves to eliminate the effect of the amplitude on the DTW distance. Then, the zero-value sequence was added to the data starting point to increase the time difference. The DTW distances under the traveling wave effect of four site types are obtained, as shown in Fig. 5, where, the mean value is µ, and the mean square is σ. The variation curve of the mean DTW distance of all earthquake waves with the time difference is shown in Fig. 6. The effect of the time difference on the DTW distance of waves is random, approximately linear, and the degree of influence is weak.

3.3 Statistical analysis of the DTW distance considering the signal-to-noise ratio

Although the noise does not change the overall variation trend of earthquake wave, the noise can cause the wave local mutation and result in the difference of DTW distance of two identical earthquake waves. To obtain the change rule of the DTW distance under the effect of the noise-signal ratio (ratio of the noise amplitude to the signal amplitude and the signal-to-noise ratio as its reciprocal), we normalized 40 selected waves and generated equal-standard normal white noise. The noise-signal ratio is the ratio of the maximum amplitude of white noise to the maximum amplitude of the normalized wave, and white noise with different intensities is added to the normalized earthquake wave to form earthquake waves with different signal-to-noise ratios. For different earthquake waves, the DTW distance of the new wave and the original wave with different signal-to-noise ratio is calculated, and all results are shown in Fig. 7.

The DTW distance is approximately linearly related to the signal-to-noise ratio, and the effect of the noise-signal ratio on the DTW distance is obvious. Figure 8 shows a statistical distribution map of the DTW distance to the signal-to-noise ratio, which further determines the reasonable range of the DTW distance considering different noise-signal ratios.

3.4 Three-dimensional statistical analysis of the DTW distance considering the time difference and noise-signal ratio

The difference in actual ground motion is determined by many factors. Therefore, whether comparing the differences of different actual ground motions or evaluating the accuracy of simulated ground motions, the effect of a single factor cannot be considered alone. Because the effect of the amplitude on the DTW distance is the most significant, its relationship is clear, and the effect can be directly identified. Consequently, researchers are more concerned about the waveform variation and detail difference. Thus, the influence of time difference and noise-signal ratio are both considered in this study. We obtain the DTW distances among 40 different normalized earthquake waves according to different time differences and noise-signal ratios, and the 3D surface map of DTW mean values is shown in Fig. 9. The results show that the distribution of DTW distance, which considers the time difference and noise-signal ratio, is basically on the oblique plane and has obvious regularity.

For artificial synthetic waves or earthquake waves generated by the shaking table, when we evaluate whether it is consistent with the characteristics of natural earthquake wave, we generally only consider whether it satisfies the accuracy requirements of the response spectrum and power spectrum. In fact, because the amplitude of earthquake waves has been determined by engineering requirements, researchers are more concerned about the characteristics and variation rules of the waves, but there has been no effective evaluation index until now. The result of Fig. 9 is the statistical mean value which is obtained from many real ground motion data points, and its numerical value and range is stable. Therefore, the DTW distance can be used as the standard for a refined evaluation of waveforms. In the evaluation, we can compare the DTW distance between the generated ground motion and the typical normalized real earthquakes and determine whether the accuracy of the waveform satisfies the requirements with Fig. 9. If the calculated DTW distance exceeds the reference value under the allowable time difference and SNR range, the generated wave should not be used, and one must generate or select a better one. When evaluating the accuracy of synthetic ground motion, the effect of the noise-signal ratio can be considered alone, so the result of Fig. 8 can be directly used as the reference value of the evaluation. When evaluating the accuracy of the earthquake waves generated by the shaking table, additional noise and time delay may occur. Therefore, the results of Fig. 9 should be strictly considered the evaluation criteria, and the waveform detail comparison can be combined with the DTW path.

4. Spatial Variation Effect Of Ground Motion Based On The Dtw Distance

In the above studies, each earthquake wave is independently selected from different earthquake records, and the calculated DTW distance is not directly correlative. The corresponding results are applicable to the evaluation of the usual earthquake waveform. For a certain earthquake, the ground motion in a small-scale area has similar propagation paths, site conditions, and attenuation characteristics. Therefore, there is both the relation and different between the waveforms recorded by different points on the surface, which reveals the effect of the time-space variation. This effect has great influence on long-span structures and bridges. Therefore, the time-space evolutionary characteristics and laws of ground motions must be revealed in real time for the seismic analysis of long-span structures and bridges. To verify whether the DTW distance can represent the time-space variation characteristics of ground motion and its capability as the evaluation index of the multipoint ground motion and the variation regularity of earthquake motion field, we must analyze the strong motion observation data of the actual array.

China's Taiwan SMART-1 (Strong Motion Array in Taiwan-1) array is a high-density array established in 1979, which includes a central station measuring point (C-00) and 36 stations which are evenly distributed at the station survey point and the extension line at three radii of 200 m, 1000 m and 2000 m on concentric circles (Forestier et al., 2012; Shortreed et al., 2002). The distribution of the SMART-1 array points is shown in Fig. 10. Except two stations on the extension line, all stations are located on alluvial soil. Thus, all the points except the two extension points are selected as the effective points.

In this study, the representative earthquake data (north-south direction) in the Event40 of the array records are selected. The point O07, which is the nearest point to the focus is set as the reference point, and the distance between the measuring point and the reference point of the DTW distance are calculated. The DTW of acceleration signals from the outer ring (the initial is O), the central ring (the initial is M) and the inner ring (the initial is I) are plot in the polar plot, respectively, and the results are shown in Fig. 11. According to the similar method, the DTW distance of the corresponding displacement is drawn in the polar coordinate Fig. 12.

The DTW distance near each focal point can exhibit the decay characteristics of different earthquake waves. The acceleration DTW distance distribution on each ring is irregular. In addition to the attenuation in the northwest direction, the randomness in other directions is more obvious. Furthermore, the distribution of DTW distance of displacement on each ring is more regular.

Next, we further discuss the physical connotation of the DTW distance. According to the principle of the DTW algorithm, we know that the DTW distance is the cumulative sum of the best path distance from the starting point to the termination point, and the norm in mathematics is a length measure of the current vector in space. Therefore, we can assume that the DTW distance has a similar mathematical meaning to the vector norm. Moreover, the DTW distance is equal or greater than 0 and linearly related to the dynamic amplitude of the earthquake, so it can be considered positive definite and homogeneous in the perspective of the vector norm. The sum of the absolute value of the signal is the 1-norm, and the square root of the sum of the signal energy is the 2-norm. Thus, according to the norm equivalence principle, the DTW distance should be closely related to these two norms, i.e., the equivalent amplitude and energy of the signal. To verify this assumption, the sums of the absolute values of the displacement wave, velocity wave and acceleration wave are calculated and compared. The results of the outer ring, middle ring and inner ring are shown in Fig. 13-Fig. 15.

By comparing the results of Fig. 11-Fig. 15, we find that the distribution characteristics of the acceleration DTW distance of each measuring point are very similar to the sum of the absolute values of the acceleration of earthquake waves at each measuring point, and it also has some characteristics of the sum of the absolute value of displacement or velocity. The distribution of the displacement DTW distance of each measurement point is also very similar to the sum distribution of the absolute value of the displacement history at each test point.

Hence, the DTW distance of each physical quantity can represent the equivalent amplitude and energy of the corresponding time domain signal of the corresponding physical quantity. In addition, it can show the comprehensive effect of different earthquake wave propagation characteristics and time difference, and the distribution of DTW distance can generally represent the time-space characteristics of ground motion. Therefore, it is reasonable to take the DTW distance as an effective evaluation index of the time-space evolutions of the multi-point ground motion and seismic dynamic field.

5. Spatial Variation Effect And Accuracy Evaluation Of Artificial Ground Motion Based On Dtw Distance

In the field of ground motion synthesis, the researchers have conducted numerous studies and proposed synthetic methods (Harichandran and Vanmarcke, 1986; Hao et al., 1989; Abrahamson et al., 1991; Yang and Chen, 2000; Bogdanoff et al., 1961). Because the main purpose of ground motion synthesis is to provide basic data for structural seismic design and analysis, most of the current methods attempt to synthesize the earthquake waves that match both the design response spectra and the power spectra (Shinozuka, 1972; Jennings et al., 1968; Saragoni and Hart, 1973). In addition, the original waveform is multiplied by the envelope function in time domain to ensure the nonstationarity of earthquake waves. Recent studies have shown that the stochastic characteristics of ground motion are jointly determined by the amplitude spectra and phase difference spectra. The synthetic ground motion based on the phase difference spectrum can more realistically represent the nonstationarity of ground motion (Niu, 1991; Clough and Penzien, 1975). In addition, considering the spatial variation effects of the seismic field (including effect of traveling wave, partial coherence, and local field), synthesizing the ground motion at multiple locations based on a theoretical model of the coherence function is necessary. Synthesized ground motion derived from stochastic simulation is usually unable to fully and accurately reveal the nonstationarity of real earthquakes in time-frequency domain. When considered with the inherent characteristics and limitations of various theories and methods, this leads to different accuracy in various ground motion synthesis methods. Therefore, whether the accuracy of different methods or the similarity of different waveforms randomly generated by the same method is evaluated, the accurate and stable evaluation criteria are required to select the most realistic and reliable synthesized ground motion. Waveform evaluation based on DTW distance provides a relatively good solution for the aforementioned problems.

5.1 Artificial ground motion accuracy evaluation based on DTW distance

For the schemes evaluation of the synthetic ground motion, we can determine whether the DTW distance accuracy of different synthetic schemes satisfies the requirements, so we must determine the DTW distance accuracy evaluation standard. This paper selects 40 earthquake waves calculated by the DTW distance, obtains 780 different results from the DTW. The statistics of the mean and standard deviation are used to determine the standard DTW distance accuracy evaluation. The standard deviation of ± 0.5 times of the mean value is taken as the reasonable DTW range of the synthetic seismic wave, and the standard deviation of ± 1 times of the mean value is taken as the acceptable DTW range. Through statistical calculation and analysis, the reasonable range of DTW distance of synthetic earthquake waves is [134.9, 287.1], and the corresponding range of DTW distance is [58.9, 363.2].

After the accuracy evaluation standard is determined, multiple earthquake waves are generated through the various synthetic methods randomly, and the DTW distance between the seismic waves obtained by each synthesis method is obtained, and its mean value and variance are calculated. Compared with the above DTW distance range standard, the rationality and accuracy of each synthesis method are evaluated.

In this paper, various theoretical models and synthetic methods in the ground motion simulation are used to produce artificial ground motion, and the relevant references are marked in Table 1.

Table 1

Relation between each method or model and acronym symbol for nonstationary wave generation

 

A

B

C

D

E

N

Synthesis method

Based on envelope function and power spectrum

Based on phase difference spectrum model

Based on known seismic records

Fitting based on response spectrum with envelope function

Fitting based on phase difference spectrum

-

Coherence function model

Harichandran[19]

Hao[20]

Abrahamson [21]

Yang[22]

-

-

Envelope function model

Bogdanoff[23]

Shinozuk[24]

Jennings[25]

Saragoni[26]

-

-

Power spectrum model

Kanai-Tajimi[27]

Markov[28]

Clough-Pizen[29]

 

-

-

The synthetic earthquake wave is the corresponding seismic acceleration for different field sites. Four different methods or models such as the synthesis method, coherence function, envelope function and power spectrum are represented by letters A, B, C, D, E respectively to form different combinations to represent various earthquake generation schemes. N means no corresponding method is adopted. Table 1 shows the relationship among the methods or models and the letters. For example, ABBC indicates the method that synthesize spatially correlated nonstationary seismic waves generated by the envelope function and power spectrum. Specifically, Hao model is considered a coherent function model, the envelope function is selected as Shinozuk model, and the power spectrum model is Clough-Pizen model (Hao et al., 1989; Shinozuk, 1972; Clough and Penzien, 1975).

In the synthetic process of artificial ground motion, the site type is assumed as class C, and the spatial variation effect of ground motion is considered. Ten earthquake waves are synthesized by each generation scheme, the DTW distance between 10 earthquake waves in each scheme is calculated, and the statistical mean is calculated. The results are shown in Table 2. The analysis of the result table shows that the correlation function between types of artificial earthquake waves from the DTW effect is similar and negligible. Therefore, we only need to analyze the last column in Table 2 of the data integration scheme and compare the results in Fig. 16 with the above statistical earthquake wave DTW obtained from the mean DTW, the reasonable range is set as [µ + 0.5σ, µ-0.5σ], and the acceptable range is set as [µ + σ, µ-σ].

Table 2

Mean value of the DTW distance for each generation scheme

Scheme 1

Scheme 2

Scheme 3

Mean of integration scheme

ABBC = 129.1

AABC = 109.5

ADBC = 106.9

A-BC = 115.2

ABCC = 275.1

AACC = 275.4

ADCC = 250.3

A-CC = 275.3

BBNC = 482.9

BANC = 425.7

BDNC = 527.8

B-NC = 482.4

DBBC = 216.3

DABC = 246.3

DDBC = 259.0

D-BC = 246.5

DBCC = 378.3

DACC = 371.8

DDCC = 297.8

D-CC = 378.2

EBNC = 463.8

EANC = 434.3

EDNC = 443.1

E-NC = 443.3

Figure 16 shows that schemes D-BC and A-CC are in the reasonable DTW range of [µ + 0.5σ, µ-0.5σ], and A-BC is in the acceptable DTW range of [µ + σ, µ-σ], whereas the D-CC, B-NC and E-NC data significantly deviate in an unreasonable range. In summary, the simulation precision of ground motions are generally required to choose Clough-Pizen model as the power spectrum model generation program, including the following methods: (1) Using envelope function and power spectrum to generate spatially correlated nonstationary seismic field, and Jennings model is selected for envelope function model; (2) The response spectrum fitting based on envelope function is selected for the spatial correlation non-stationary seismic field, and Shinozuk model is selected for the envelope function model. The acceptable generation scheme include that the envelope function and power spectrum are used to generate the spatial correlation non-stationary seismic field, and the Shinozuk model is selected as the envelope function model. The other ground motion schemes may be unstable and should be carefully chosen.

5.2 Evaluation of spatial variation effect of synthetic ground motion

After determining the reasonable generation scheme, we must further evaluate different waveform characteristics generated by the same plan to select more typical ground motion. When multiple ground motions are required, it is necessary to ensure that the ground motions contain the basic rules of the spatial variation effect. Considering the effect of spatial variation, it is generally assumed that if two earthquake waves are relatively close to each other, the difference between them is smaller, and the corresponding DTW distance is smaller. If the two waves are far away from each other, the difference between them and the corresponding DTW distance are larger. According to the previous study, especially the results of Fig. 11 and Fig. 12, we can think that when the multipoint ground motion is generated, with the increase in distance of each point, the DTW distance also gradually increases, which can represent the general rule of the time and space effect of ground motion. Therefore, when selecting earthquake waves from the results of several multipoint synthetic earthquake waves, we should at least ensure that one set of seismic accelerations, DTW distance and displacement DTW distance can satisfy the above conditions.

The requirements are further illustrated by an example. Five points that must generate ground motion on the same line have the coordinates of (0, 0), (500, 0), (1000, 0), (1500, 0) and (2000, 0), and the unit is m. The selected site type is class C considering the spatial variation effect, and the apparent wave velocity is 1000 m/s. Three sets of earthquake wave data are synthesized using a reasonable DTW distance generation scheme 2 with 5 random earthquake waves in each group. The DTW distance between the points and the origin is calculated, and the corresponding results are shown in subgraphs (a), (b) and (c) of Fig. 17 and Fig. 18.

It is obvious that the DTW distance of the 3 sets of earthquake waves does not always increase with increasing distance, so it cannot completely represent the basic law of the spatial variation effect. To solve this problem, we combine the earthquake waves and calculate the DTW distance among 5 new earthquake waves. After the adjustment, the results satisfy the requirements, as shown in Fig. 17 (d) and Fig. 18 (d). The acceleration time history and displacement time history of corresponding earthquake waves are shown in Fig. 19 and Fig. 20, respectively.

For this group of earthquake waves, with the increase in distance among the points, the displacement DTW distance and acceleration DTW distance increase, so they can better represent the spatial variation effect of ground motion. Hence, the synthetic accuracy evaluation and selection of artificial ground motion based on the DTW distance are more accurate and effective, which can select more authentic and effective ground motion, and provide more reliable excitation source data for the structural dynamic analysis.

6. Conclusion

Declarations

Acknowledgments

We thank the Editor and anonymous reviewers.

Author contribution

Haoxiang He carried out the whole essay idea and article writing. Haoding Sun carried out part of the partial article and picture writing. Yifei Chen carried out the table and part of the photo production project. All the authors contributed equally in writing the manuscript. All authors reviewed the manuscript.

Funding information

This work is partially supported by the National Key R&D Program of China under Grant No. 2017YFC1500604 and 2017YFC1500603 and the National Natural Science Foundation of China under Grant No. 51878017.

Competing interests The authors declare no completing interests.

Ethics approval and consent to participate Not applicable.

Consent for publication Not applicable.

Conflict of interest The authors declare no competing interests.

ORCID iD

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