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Stochastic ground motion simulation of the 2016 Meinong, Taiwan earthquake


We applied a stochastic method for the finite-fault modeling of strong ground motions to the 2016 Meinong, Taiwan earthquake. Newly developed attenuation models in Southern Taiwan with the frequency-dependent Q = 86.4f 0.73 and the high-frequency decay factor κ 0 were used in the synthetic model. The horizontal-to-vertical spectral ratios (HVSR) were calculated from weak motions and the Meinong mainshock and used for the site amplification correction of the synthetic waveforms produced by the stochastic ground motion simulation. Simulations incorporating the attenuation models and site correction improved the prediction of the S-wave envelope, duration, and peak ground acceleration (PGA). The nonlinear site response during the Meinong mainshock was identified by the degree of nonlinear site response (DNL), which is a summation of HVSR differences between weak motions and the Meinong mainshock as recorded by the Taiwan Strong Motion Instrument Program. The DNL showed a positive correlation with ground motion intensity. The surface site conditions influenced DNL strength. The percentage of PGA reduction calculated in this study can be an indicator of the spatial distribution of the degree of nonlinear soil effects on the Meinong earthquake in the time domain. Areas that had high levels of PGA reduction overlap with areas that had high liquefaction potential. Based on the residual analysis, forward directivity was identified in a 105° range in the northwestward direction. The amplification of forward rupture directivity was three times greater than the backward rupture directivity.



On February 6, 2016, at 03:57 local time (UTC + 8), an earthquake of magnitude 6.6 on the Richter scale occurred in the Meinong District of Kaohsiung City, Taiwan. According to the Central Weather Bureau (CWB) report, the epicenter was located at 22.92°N 120.54°E and had a focal depth of 14.6 km. The CWB-defined intensity of the Meinong earthquake reached level 7 and the earthquake, which caused widespread damage and 117 deaths, was felt all over the island of Taiwan. The epicenter of the earthquake was located in the Meinong District in Kaohsiung City. However, the worst affected city was Tainan. This may have been due to the strong amplification of surface ground motion by shallow velocity structure and soil liquefaction that occurred during strong shaking, which caused many houses in the areas with soft soil deposits to sink or tip. The shallow velocity structure of the Chianan plain was investigated using the microtremor array analysis (Kuo et al. 2016a). The soil response was simulated (Chen et al. 2016) by considering the shallow structure, and the results revealed that the shallow soft layers influenced the duration of seismic wave shaking and ground motion amplification in the Tainan area.

Darragh and Shakal (1991) analyzed spectral ratios for two rock and soil station pairs and estimated the site response from weak and strong ground motions. They revealed that the amplification factor in the frequency domain from weak motions at the soft soil site was approximately 3–8 times greater than that of the mainshock recording and that this phenomenon is explained by the nonlinear response of the soils. Many nonlinear soil amplification researchers have applied the spectral ratios method for soil-to-rock and for surface-to-downhole station pairs (Wen et al. 1994, 1995; Beresnev et al. 1995a, b). They indicated that, during nonlinear soil behavior, the spectral ratio from strong motions has lower predominant frequency and amplification than the spectral ratio from weak motions. After the earthquakes in 1985 in Michoacan, Mexico, and in 1989 in Loma Prieta, California, several large earthquakes have been recorded by modern digital surface and vertical arrays. Observations around the world established direct evidence of the significance of nonlinear site effects (Beresnev and Wen 1996). Wen et al. (2006) used the horizontal-to-vertical spectral ratio (HVSR) method to analyze the Large-Scale Seismic Test (LSST) array in Lotung, Taiwan, and found that the HVSR method can be used to identify nonlinear site responses. Noguchi and Sasatani (2008, 2011) proposed a new quantitative index to measure the degree of nonlinear site response (DNL). The DNL showed positive correlations with the observed horizontal peak ground acceleration (PGA) on the ground surface and with V S30.

The stochastic method has been widely used to simulate high-frequency strong ground motions, and many studies have applied the stochastic method to generate ground motions and investigate site effects in Taiwan. Roumelioti and Beresnev (2003) applied the stochastic finite-fault modeling to simulate the strong ground motions of the 1999 earthquake in Chi-Chi, Taiwan. The nonlinear soil response during the Chi-Chi earthquake was quantified by amplification reduction estimated using the spectral ratio technique. Stochastic simulations for both point source and extended fault ruptures that used region-specific crustal attenuation and source scaling (D’Amico et al. 2012) successfully predicted the strong motions of the Chi-Chi earthquake. The Empirical Transfer Function (ETF) was constructed as the difference in frequency spectra between the observed and synthetic ground motions, using the stochastic point source approach for the Taipei basin (Huang et al. 2017). The ETF well described the site response in Taipei basin and can provide more accurate site correction for future earthquake ground motion simulations. However, they did not consider the nonlinear site effect to construct the ETF. In addition, Kamae et al. (1998) proposed a new hybrid technique that combined the stochastic method generating high-frequency motions with the long-period motions calculated by the 3D finite-difference method to simulate the broadband near-fault ground motions.

In this study, we incorporated a newly developed attenuation model, which contained the frequency-dependent Q (Chang et al. in preparation) and the high-frequency decay factor κ 0 used to generate the Meinong mainshock strong ground motions in the Chianan area, in stochastic finite-fault simulations. We calculated weak and strong motion HVSR as the site amplifications for the simulation of stochastic ground motion and obtained DNL values to identify the degree of nonlinear site response. Areas with high nonlinear site response during the Meinong earthquake were determined using the residuals of the predicted site-corrected PGA between the HVSR of weak motions and the mainshock. The asymmetrical distribution of PGA residuals obtained by our model may also indicate the amplification of the rupture directivity during the Meinong earthquake.


The main goal of this study was to identify the directivity effect and the nonlinear effect during the Meinong earthquake. We simulated the strong ground motion of the Meinong earthquake using the stochastic finite-fault technique and then analyzed the residual of the ground motions between simulated and observed values. The finite-fault simulation utilized the EXSIM code, developed by Boore (2009) and modified from Motazedian and Atkinson (2005). We designed the parameters carefully to include new regional attenuation models to our stochastic modeling and applied site correction processing to the synthetic waveforms using the HVSR of the weak motions and the Meinong earthquake. The synthetic ground motion was applied with the following steps to correct the site response: (1) The Fourier spectrum of the synthetic waveform was calculated. (2) HVSR for individual stations were multiplied by the synthetic Fourier spectrum. (3) An inverse fast Fourier transform was applied to convert the modified synthetic Fourier spectrum back to the synthetic waveform in the time domain. We applied the same steps to site-correct the synthetic waveforms using the HVSR of weak motions and the Meinong mainshock. The nonlinear site effect and source rupture directivity were investigated with residual analysis. We applied the HVSR of earthquakes to correct site amplification in the stochastic modeling because HVSR is readily available. In addition, we analyzed the nonlinear site effect by calculating the DNL values in the frequency domain and the PGA reduction in the time domain. The DNL values can quantify the difference in the Fourier spectrum between strong and weak motions and reveal the de-amplification during strong shaking in the frequency domain. We calculated the PGA reduction during the Meinong mainshock by comparing the simulated PGA that used the HVSR of weak motions and the simulated PGA that used the HVSR of the Meinong mainshock for site correction. The de-amplification site response during strong shaking in the time domain is revealed in the PGA reduction phenomenon. The nonlinear soil effect induced by the Meinong earthquake was identified. In addition, the analysis of the ground motion simulation by two different site corrections using weak and strong motion also indicates the importance of the nonlinear site effect in ground motion prediction especially in regions with soft deposits. We analyzed the residuals of the observed and simulated PGA and compared them with the azimuth to determine the influence of source rupture directivity. The Ground Motion Prediction Equation (GMPE) was applied to verify our results. The amplification of the source forward rupture directivity was estimated, and the forward and backward rupture directivities were determined.

H/V spectral ratio

High-quality strong motion data for the Meinong earthquake were recorded by the Taiwan Strong Motion Instrument Program (TSMIP; Tsai and Lee 2005) and provided by the Geophysical Database Management System (GDMS; Shin et al. 2013) of the CWB. Figure 1 shows the PGA ShakeMap of the Meinong earthquake near the source regions. The maximum PGA reached level 7 and was recorded as 445 and 417 cm/s2 at CHY062 and CHY063, respectively, which were located within 24 km of the epicenter. The anomalously large ground motion was detected in the northern area of the epicenter and formed an asymmetrically distributed PGA ShakeMap. The strong shaking also caused soil liquefaction around the Sinshih and Annan districts, Tainan City. In this study, we analyzed 120 stations within our study domain [between 22.6°–23.6° north (N) and 120°–121° east (E)] that were near the source regions and that recorded the Meinong earthquake. Wen et al. (2006) concluded that the S-wave spectral ratio of horizontal to vertical (S–H/V) can be used to identify the nonlinear site response. Thus, the S–H/V at each station was calculated to investigate the nonlinear site response during the Meinong earthquake. The S–H/V of mainshock and weak events was also applied to the site amplification function for stochastic simulation in the next section. Spectral ratios were calculated as follows (Beresnev and Wen 1996): (1) After baseline correction, the shear wave was identified and selected and the mean value of each trace was obtained; (2) a 5% cosine-tapered window was applied to both sides; (3) the Fourier amplitude spectrum was calculated; (4) the spectrum was smoothed five times using Hanning window averages; (5) the root mean square spectra from the EW and NS horizontal components were calculated; (6) the HVSR was calculated. These values were used to calculate the variation of S–H/V during the Meinong earthquake. The weak events were also calculated with S–H/V used as a reference. Other weak motion earthquake records from TSMIP between 1991 and 2014 with the following criteria were also used in this study: (1) PGA ≥ 10 cm/s2 recorded by one of the three components; (2) PGA ≤ 50 cm/s2; (3) M L < 6. Figure 2 shows the comparison of spectral ratios for the Meinong mainshock and weak events at eight stations. Some of the stations showed significant differences between the S–H/V of strong motion and weak events, whereas others did not. The nonlinear soil response during strong motion events is a possible reason for this discrepancy. The HVSR of weak and strong motion was used to calculate the DNL values and applied to the stochastic simulation as the amplification function.

Fig. 1
figure 1

PGA ShakeMap of the near-source region. The epicenter relocated by the Central Weather Bureau (CWB) is represented by a white star. The PGA distribution is asymmetrical, with the largest PGA (approaching intensity 7) occurring in the area northwestward of the epicenter

Fig. 2
figure 2

HVSR for the Meinong earthquake (red line) and weak events (black line) at eight stations. The thick line represents the mean value, and shadowed areas show the one standard deviation range of weak events. The V S30 and PGA for each station are also shown. The top panels show the cases where there are significant differences in HVSR between strong and weak events. The bottom panels show the cases where the HVSR for strong and weak events are similar

Degree of nonlinear site response

We investigated the nonlinear site response by calculating the index of the DNL to quantify the differences between the ratio for strong motion and the ratio for weak motion. The DNL is defined as follows:

$${\text{DNL}} = \sum\limits_{0.5}^{20} {\left| {\frac{{{\text{HVR}}_{\text{strong}} }}{{{\text{HVR}}_{\text{weak}} }}} \right|} \cdot\Delta f$$

where HVRstrong is the spectral ratio for the strong motion and HVRweak is the spectral ratio for the weak motion. While the strong motion only considered the Meinong mainshock, the spectral ratio of the weak motion was averaged using the historical weak events. In this analysis, the sum of the frequency range was from 0.5 to 20 Hz. The relationship between DNL, the level of ground motion, and site conditions is shown in Fig. 3. The DNLs were categorized into four classes based on the site classification of the stations, which was evaluated from the well logging data by the Engineering Geological Database for TSMIP (EGDT, Kuo et al. 2011, 2012). The DNL values increased slightly as PGA increased (Fig. 3a), and there was a positive correlation although the slope was not steep. The slopes of the trend line for three site classes were similar, but the amplitude of site E was larger than the amplitude of sites C and D. We also examined the relationship of the same DNL with peak ground velocity (PGV) (Fig. 3b) and the ratios of PGV and V S30 (Fig. 3c) and found a stronger correlation between DNL and PGV than with PGA. The trend lines for the three sites had clearly changed; site E showed a steeper slope than site D and site C showed the lowest slope. Nevertheless, there was a correlation between DNL and the ratios of PGV and V S30. The trend lines of the three site classes also showed similar slopes and amplitudes, because the PGV/V S30 ratio already included the site conditions. These results indicate that PGV is a better ground motion parameter that correlates with DNL values. Figure 4 shows the distribution of DNL overlapping with the PGA of the Meinong earthquake, and the analysis indicates that the DNL values are influenced by the level of ground motion and are characteristic of surface geology. However, we cannot ignore the effect of fluctuations on the HVSR technique and the subsequent calculation of DNL.

Fig. 3
figure 3

Relationship between DNL, ground motion level, and site classification. a The relationship between DNL and PGA, b the relationship between DNL and PGV, c the relationship between DNL and the ratio of PGV to V S30. Black solid triangles represent site class B, blue solid diamonds represent site class C, green solid squares represent site class D, and pink solid circles represent site class E. Inverted gray triangles represent stations without site classification. Linear regression trend lines are plotted for each site class. A steeper trend line slope indicates that the relationship between DNL and the given ground motion parameter is more positively correlated

Fig. 4
figure 4

Distribution of DNL values overlapping with the PGA of the Meinong earthquake. The DNL values are shown by the colored circles. The PGA contour map (background) is shown in grayscale

Results and discussion

Parameters for the stochastic simulation

We used the stochastic method to simulate 120 stations within the study domain (between 22.6°–23.6°N and 120°–121°E), using the fault model and the focal mechanism given by Lee et al. (2016). The rectangular fault was 45 × 25 km with a 281° strike and a 24° dip. Based on the empirical relationship (Beresnev and Atkinson 2002), each subfault was divided into 3 × 2 km; therefore, the fault plane had 15 × 13 subfaults. Figure 5 shows the distribution of the stations and the slip model that we used. Following the EXSIM stochastic finite-fault approach, the source rupture velocity was constant and was calculated as 0.8 × shear-wave velocity. The shear-wave velocity in this study was 3.6 km/s; thus, based on the dimensions of the fault, the rupture process only lasted around 10 s. However, according to Lee et al. (2016; see Fig. 2), asperity II mainly grows after 10 s. Therefore, when we applied the slip model directly to the stochastic finite-fault approach, we found that asperity II contributed to ground motion for about 6 s. Thus, it was unreasonable to use the slip model directly for our stochastic finite-fault approach. Consequently, we slightly reduced the weighting of asperity II in the slip model to obtain the best validation model. The M w value (6.47) of the Meinong earthquake was applied to the stochastic model, and the stress drop was 80 bar, as previously reported by D’Amico et al. (2012).

Fig. 5
figure 5

Slip model that we applied in the stochastic model and the map showing the 120 target stations, represented by black solid diamonds. Red lines show the main faults around the area. The gray circles indicate the aftershocks of the Meinong earthquake. The focal mechanism and slip distribution are given by Lee et al. (2016)

We used a newly developed regional attenuation model to calibrate the stochastic simulation. The frequency-dependent parameter of the regional attenuation model was set to Q = 86.4f 0.73, as estimated from the shear-wave analysis by Chang et al. (in preparation). Geometrical spreading was given by 1/R b, where b = 1.0 for R < 50 km, b = 0 for 50 km R 170 km, and b = 0.5 for 170 km R, for stochastic simulations in Taiwan (Sokolov et al. 2001, 2003, 2006, 2009). Crust amplification (Atkinson and Boore 2006) was determined using a frequency-dependent amplification function for generic rock sites categorized into site A (very hard rock) in Eastern North America (ENA-A). Since Taiwan lacks the site A station, ENA-A was applied to the crust amplification of stochastic modeling in Taiwan. Moreover, amplifications of less than 1.2 on very hard rock sites have a limited influence on our simulation. The κ 0 factor is a distance-dependent parameter that affects the high-frequency attenuation. Larger κ 0 values indicate that the site condition has a large degree of high-frequency attenuation. The combined effect of generic rock amplification and κ 0 diminution was given by Boore and Joyner (1997; see Fig. 8). κ 0 is a key parameter for the description of high-frequency ground motions and varies greatly even at the same site conditions (Atkinson 1996). Therefore, in this study, we applied a newly developed Taiwanese κ 0 model that analyzed from 33,756 TSMIP earthquake records. In this method of κ 0 analysis, κ 0 was calculated using the decay slope of the SH-wave spectrum between the frequency bands f E and f X, where f E is the beginning frequency of the spectral amplitude following an exponential decay and f X is the end frequency of the spectral amplitude following an exponential decay. Diminution is defined as follows:

$$d\left( f \right) = \exp \left( { - \pi \kappa \left( {f - f_{\text{E}} } \right)} \right).$$

Based on the definition of κ 0, we utilized κ 0 diminution in the stochastic method, with individual κ 0 and f E parameters for each station. The difference between our κ 0 diminution and the default treatment in EXSIM is shown in Fig. 6. Our κ 0 diminution showed less attenuation than that of the default and the f E parameters dominated the shape and amplification of diminution, even for the stations with similar κ 0 values. Table 1 summarizes all the parameters used in the synthetic model.

Fig. 6
figure 6

Schematic of κ 0 diminution applied in this study. Dashed lines are the default κ 0 diminution in EXSIM, and solid lines are the κ 0 diminution with the f E parameter. For κ 0 with 0.0518 or 0.0582 s, the f E parameters result in diminution with far less attenuation than the default. In default κ 0 diminution, similar κ 0 values result in comparable diminution. However, diminution in this study is dominated by f E

Table 1 Modeling parameters

Site correction of the stochastic simulation

After EXSIM stochastic modeling, we adopted the HVSR of the Meinong mainshock and weak events for the site correction of each station. The synthetic waveform was converted to a Fourier spectrum using the fast Fourier transform (FFT) algorithm and then multiplied by the amplification function of the HVSR of each station. The Fourier spectrum that was amplified with the HVSR was inverse-fast-Fourier-transformed to obtain the synthetic waveform after site correction. The schematic procedure of site correction is shown in Fig. 7. The site-corrected synthetic ground motion showed significant improvement in the waveform pattern and PGA in the time domain. The Fourier spectrum also had a substantial improvement in the frequency domain. Thus, we achieved satisfactory results in the use of HVSR for site correction to improve the ground motion simulation using the stochastic method.

Fig. 7
figure 7

Comparison of the synthetic waveform with the site-corrected waveform. a The observed waveform is shown in black, the synthetic waveform without site correction is shown in blue, the synthetic waveform after site correction with the HVSR of weak events is shown in green, and the synthetic waveform after site correction with the HVSR of the mainshock is shown in red. b The comparison as a Fourier amplitude spectrum. The observed horizontal Fourier amplitude spectrum Hori-OBS is obtained from the root mean square of the EW and NS components

Model validation

There were insufficient rock stations located near the seismogenic fault of the Meinong earthquake. Moreover, the Meinong earthquake showed an asymmetrical intensity distribution, which may be caused by rupture directivity and site amplification (Lee et al. 2016). Hence, we used all 120 stations within the study domain to validate the stochastic models. The model bias, calculated as the logarithm (base 10) of the ratio of the observed to the simulated Fourier spectra and averaged over 120 sites, is shown in Fig. 8. We compared the model bias calculated with and without site correction using the HVSR of the mainshock and the weak events. The bias model A (Fig. 8a) is the synthetic model with default κ 0 diminution in EXSIM stochastic modeling, and the bias model B (Fig. 8b) is the newly developed κ 0 diminution with f E parameters. While bias model A showed underestimation in the high frequency band, model B showed calibration with flat bias. The application of f E parameters in this study is novel and resulted in a better bias model than the default.

Fig. 8
figure 8

Bias models showing the logarithm (base 10) of the ratio of the observed to the simulated Fourier spectra, averaged over 120 sites. The blue line shows the simulated Fourier spectra without site correction, the green line shows the site-corrected simulated Fourier spectra with the HVSR of weak events, and the red line shows the site-corrected simulated Fourier spectra with the HVSR of the mainshock. a The bias model using default κ 0 diminution and b the bias model using κ 0 diminution with f E. Bias model B outperforms bias model A

Site-corrected simulations using the HVSR of the mainshock and weak events both fit well with the observed data. The differences in HVSR between the mainshock and the weak events could be due to nonlinear soil effects during strong ground motions.

In Fig. 9, we compared site-corrected synthetic waveforms using mainshock HVSR with observed waveforms at twelve stations uniformly distributed around the northern and southern areas of the seismogenic fault. The whole waveform trace lasted 40 s, and in most cases, the envelop, duration, and PGA of synthetic ground motions matched the observed waveforms well.

Fig. 9
figure 9

Comparison of observed and synthetic horizontal acceleration waveforms at 12 selected stations. Each trace has duration of 40 s and is drawn at the same scale

We quantified the ability of using EXSIM stochastic modeling to predict PGA. The misfit (σ ln Err) for PGA residuals is defined as follows:

$$\sigma_{{\ln {\text{Err}}}} = \sqrt {\frac{1}{N}\sum\limits_{i = 1}^{N} {\left( {\ln {\text{PGA}}_{{{\text{S}}i}} - \ln {\text{PGA}}_{{{\text{O}}i}} } \right)^{2} } } ,$$

where N is the number of stations, PGAO is the observed PGA, which is the root mean square of the peak north–south (NS) and east–west (EW) component values (i.e., \({\text{PGA}} = \sqrt {\left( {{\text{PGA}}_{\text{NS}}^{2} + {\text{PGA}}_{\text{EW}}^{2} } \right)/2}\)), and PGAS is the simulated PGA.

Figure 10 shows the comparison of the observed and predicted PGA and the residuals for the Meinong earthquake; the site-corrected synthetic PGA showed significant improvement. Without site correction, the misfit was 1.031; the site correction using the HVSR of weak events reduced the misfit to 0.716. The site-corrected synthetic PGA generated using the HVSR of the mainshock had the best misfit of 0.585. The results indicate that the stochastic model can be used as a reputable simulator for the Meinong earthquake.

Fig. 10
figure 10

Comparison of observed and predicted PGA and residuals for the Meinong earthquake. The top panel shows the observed and predicted PGA, along with the hypocenter distance. The bottom panel shows the residuals calculated using Eq. 3. Misfit is quantified by averaging the residuals and is reduced from 1.031 to 0.716 and 0.585 by applying the site correction

Effects of source rupture directivity

The EXSIM stochastic model that utilizes HVSR for site correction could satisfactorily predict ground motions of the Meinong earthquake. However, the PGA residuals showed a symmetrical spatial distribution where high residual values were usually located on the northern and southern azimuth of the seismogenic fault. The residuals showed similar patterns only when the values had different amplitudes (Fig. 11a–c). Kuo et al. (2016b) analyzed the Meinong earthquake records from free-field and borehole arrays and indicated that asymmetrical PGA distribution is mainly caused by rupture directivity. The forward directivity effect was identified from 270° to 15° of the azimuth, with a total range of 105°. Forward rupture directivity effects that occur when the rupture front propagates toward the site cause larger ground motion amplitudes and shorter durations than average directivity conditions. Backward directivity effects that occur when the rupture propagates away from the site cause long duration motions and low amplitudes at long periods (Somerville et al. 1997). In this study, we attempted to correlate the residuals of predicted PGA with the azimuth and the results showed a high correlation (Fig. 12). Most of the positive residuals were located on the backward range, while negative residuals were located on the forward range; our model showed that the simulation overestimated PGA in the backward direction, but underestimated PGA in the forward direction. We could not calibrate the residuals during the validation step by revising the potential parameters; therefore, the strong source rupture directivity should be the primary cause of the symmetrically distributed residuals. In order to verify this argument, we also used GMPE (Jean et al. 2006; Chang et al. 2010) with site correction to predict the PGA of the Meinong earthquake. The distribution of the residuals is shown in Fig. 11d and the misfit of the GMPE model is 1.225. Even the GMPE failed to predict the PGA of the Meinong earthquake, the pattern of the residual distribution was similar to that of our stochastic model, where the northern and southern areas were under and overestimated, respectively. This result indicates that the source rupture directivity plays an important role in controlling the characteristics of strong ground motions. Using the average residual from the forward (σ ln Errf  = −0.2) and backward (σ ln Errb  = 0.9) directions, we estimated the amplification of the forward rupture directivity compared with the backward rupture directivity. The amplification of the rupture directivity effect A d can be calculated using the following equation:

$$A_{d} = {\text{e}}^{{\left( {\left| {\sigma_{{\ln {\text{Err}}f}} } \right| + \left| {\sigma_{{\ln {\text{Err}}b}} } \right|} \right)}}$$
Fig. 11
figure 11

Distribution of residuals for each station of four models. Warm tones indicate overestimation of PGA, while cool tones indicate underestimation of PGA. a The stochastic model without site correction, b the site-corrected stochastic model using the weak events HVSR, c the site-corrected stochastic model using the mainshock HVSR, demonstrating the northwestward rupture directivity and the division of forward and backward rupture directivity, d the GMPE model by Jean et al. (2006) and Chang et al. (2010)

Fig. 12
figure 12

Correlation between the residuals of predicted PGA and the azimuth. Red squares represent positive residuals that indicate overestimation by the simulation and blue circles represent negative residuals that indicate underestimation by the simulation. The pink and green backgrounds highlight the backward and forward areas, respectively

Thus, the amplification of the forward rupture directivity effect obtained was three times the backward rupture directivity.

PGA reduction during the Meinong earthquake

We calculated DNL to investigate the nonlinear soil effect of the Meinong earthquake in the frequency domain. Large DNL values indicated de-amplification and a variety of dominant frequencies during strong ground shaking. In this study, we simulated the PGA of the Meinong earthquake using a stochastic method that utilizes the HVSR of the mainshock and the weak events. Hence, we could identify the areas with high nonlinear soil effects by calculating the reduction in synthetic PGA using the mainshock HVSR compared to the PGA calculated using the HVSR of weak events. The PGA reduction can be expressed as follows:

$${\text{PGA}}\;{\text{reduction}} = \frac{{{\text{PGA}}_{\text{strong}} - {\text{PGA}}_{\text{weak}} }}{{{\text{PGA}}_{\text{strong}} }} \times 100\% .$$

Ideally, PGA will be reduced due to de-amplification (Boore et al. 1989) occurring during nonlinear soil effects. Hence, the reduction in PGA could reveal the degree of nonlinear soil effects during strong shaking. The contour map of the percent PGA reduction is shown in Fig. 13. The solid diamonds represent the stations that show moderate PGA reduction, and red solid circles represent the stations that show a significant PGA reduction (i.e., more than −30%). The high color intensity in the PGA reduction contour map demonstrates that a high degree of nonlinear soil effects mainly occurred in the area around Tainan City, which is near the mouth of the Zengwun River and the Pingtung Plain. The Meinong earthquake induced major liquefactions around the Sinshih and Annan districts in Tainan City and caused lateral spreading damage of the Rixin embankments at the Danei Bridge of the Zengwun River in the Tainan District (NCREE 2016). The locations that experienced major liquefaction are located in areas with high PGA reduction. The contour map of a high percentage of PGA reduction also overlaps with the areas of high liquefaction potential, as shown by a liquefaction potential map published by the Central Geological Survey (, Accessed 25 Dec 2016).

Fig. 13
figure 13

Contour map of the percentage of PGA reduction calculated by Eq. 4. Red solid circles show stations that have significant PGA reduction (i.e., over −30%). Different color shades indicate the degree of de-amplification during the Meinong earthquake. Deep colors show the areas that may have experienced a high degree of nonlinear effects during the Meinong earthquake


High-frequency ground motion prediction is important for seismic hazard analysis. Greater accuracy of ground motion prediction could improve seismic hazard assessment performance and therefore reduce losses in the event of an earthquake. In this study, we calculated the DNL values and applied the stochastic finite-fault method to model the ground motion of the 2016 Meinong earthquake. The directivity and nonlinear effects were investigated in this study.

First, we calculated the S–H/V of the Meinong earthquake and weak events to investigate the nonlinear site response using DNL, which is a quantitative index that reveals the difference in S–H/V between strong and weak motions. The DNL of S–H/V showed a positive correlation with the measures of ground motion intensity, such as PGA and PGV, particularly PGV. Site conditions influenced the DNL strength; for example, stations belonging to site class E with strong motion PGA above 100 cm/s2 usually had larger DNL values than sites C or D.

Second, we calibrated the stochastic model for all 120 stations, which provided dense spatial coverage around the source. The source slip model of the Meinong earthquake provided by Lee et al. (2016) was adopted for the finite-fault model. However, the EXSIM program for stochastic simulation could not handle complex rupture processes, as exhibited by the Meinong earthquake. Asperity II of the slip model was revised to be less severe so that the simulated and observed waveforms and PGA were well matched. Since the contribution of asperity II occurs 10 s after the beginning (Lee et al. 2016), the whole rupture process in the stochastic finite-fault model theoretically lasts only about 10 s. The results suggested that the stochastic finite-fault technique should be considered when managing the complex rupture behavior. The new attenuation models in Taiwan include frequency-dependent Q (Chang et al. in preparation) and high-frequency decay factor κ 0, the use of which is novel in stochastic finite-fault modeling. The performance of our calibrated model was satisfactory when these new attenuation parameters were applied.

Third, the area influenced by the rupture directivity was identified with the residual analysis. We determined the forward directivity in the northwest within a 105° range (Fig. 11c), which was consistent with the results of Kuo et al. (2016b) who analyzed the surface and borehole records. Wu et al. (2016) analyzed the records of the Meinong earthquake using a P-alert network and also concluded that the fault plane may be in the NW–SE direction and that the source may have ruptured northwestwardly. We calculated the amplification of forward rupture directivity, which was three times larger than the backward rupture directivity. The amplification of rupture directivity was difficult to apply to the earthquake simulation because the fault rupture was unpredictable and unique; nevertheless, our results provided a description of the amplification of rupture directivity and revealed future challenges for ground motion prediction.

Fourth, we calculated the percentage of PGA reduction that could be an indicator of the spatial distribution of the degree of nonlinear soil effects of the Meinong earthquake in the time domain. Although the results indicated that S–H/V is useful for site correction in the stochastic method and that the nonlinear effect should be considered essential in ground motion prediction, the strong motion S–H/V is unavailable in earthquake simulations. Hence, creating empirical strong motion S–H/V records for stations that may exhibit nonlinear behavior could likely contribute to the site correction for stochastic earthquake ground motion simulations.

Investigating the characteristics of the site effects is important because the site condition has a complex influence over the amplification of seismic waves or the reduction in PGA. The effect of rupture directivity cannot be ignored; in some cases, rupture directivity may strongly affect the PGA shake distribution. These factors should be considered in ground motion simulations in future studies to improve prediction accuracy.


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Authors’ contributions

CTC analyzed the strong ground motion data, including the observations and simulations, and drafted the manuscript. SCC performed the modeling; KLW and SCC calibrated and improved the synthetic results. All authors participated in the discussion and the interpretation of the data. All authors read and approved the final manuscript.


The authors would like to thank the Central Weather Bureau and the National Center for Research on Earthquake Engineering for providing the strong motion data. This work was funded by the Ministry of Science and Technology (MOST105-2811-M-001-058, MOST103-2625-M-008-017-MY3) and Taiwan Earthquake Research Center (TEC). The TEC contribution number for this article is (00135). We also thank two anonymous reviewers for their valuable comments and suggestions.

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The authors declare that they have no competing interests.

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Correspondence to Chun-Te Chen.

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Chen, CT., Chang, SC. & Wen, KL. Stochastic ground motion simulation of the 2016 Meinong, Taiwan earthquake. Earth Planets Space 69, 62 (2017).

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  • Stochastic method
  • HVSR
  • Nonlinear site response
  • Rupture directivity