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The Impact of the Chiapas Tsunami of 8 September 2017 on the Coast of Mexico. Part 1: Observations, Statistics, and Energy Partitioning

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Abstract

The major (Mw 8.2) intraplate normal-fault earthquake of 8 September 2017 in the Gulf of Tehuantepec (Chiapas, Mexico) generated a strong tsunami that severely impacted the nearby coasts of Mexico and Central America. Tsunami waves in the near-field area were measured by seventeen high-resolution coastal tide gauges and by three open-ocean DART stations anchored offshore from the affected region. Data from these sites, together with those from four distant DARTs, were used for comprehensive analyses of the 2017 event. De-tided sea level time series were examined to determine the statistical and spectral characteristics of the 2017 tsunami waves along the Mexican and Central American coastline. The characteristics of the recorded waves from this near-field event were compared with those from two great far-field events: the 2010 Chile and the 2011 Tohoku tsunamis. Maximum trough-to-crest wave heights for the 2017 tsunami were recorded at Puerto Chiapas (351 cm), Salina Cruz (209 cm), Acapulco (160 cm), Huatulco (137 cm) and Acajutla, El Salvador (118 cm). While maximum 2010 and 2011 tsunami waves were observed at specific “hot spots” (sites with a high Q-factor and pronounced resonant properties, such as Manzanillo and Acapulco), the “strengths” of the recorded 2017 tsunami waves were mostly determined by distance from the source. Contrary to the maximum wave heights, the general spectral properties of the tsunami signals for all three events were highly similar at a given coastal site and mainly resemble the spectral structure of background oscillations at the same site. This similarity indicates that the frequency properties of the tsunami waveforms for a steady-state tsunami signal are mainly determined by local topographic features rather than by the source parameters. Estimates of the “colour” of an event (i.e., the open-ocean tsunami frequency content) show that the 2017 Chiapas tsunami was mostly “reddish” (long-period), with 68% (DART 43413) to 87% (DART 43412) of the total tsunami energy related to waves with periods > 35 min. In contrast, the 2010 and 2011 tsunamis were “reddish-blue”, with 48–57% associated with long-period waves (> 35 min) and 52–43% with short-period waves (2–35 min). The dominant periods of the tsunami waves were mostly linked to the shape, length, and width of the source region: the larger the source and the shallower its depth, the longer the periods of the generated tsunami waves. The complicated structure of the source explains the saturated and wide frequency-band character of the tsunami spectra. Our analysis also reveals an anisotropic nature to the 2017 tsunami waves; waves that propagated northeastward along the mainland coast of North America and southeastward along the Central American coast were significantly different from those that propagated southwestward, normal to the source orientation. This aspect of the wave field appears to be related to two distinct types of waves; “trapped (edge) waves” retained on the shelf (which plays the role of a “wave guide”), and “leaky waves” that radiate into the open ocean.

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Fig. 1

source coastal region most affected by the earthquake and associated tsunami; “BdC” = Boca del Cielo

Fig. 2
Fig. 3

source area, yellow squares denote three offshore DART stations, red star indicates the epicenter of the 2017 Chiapas earthquake

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Fig. 6

source area; b eight relatively remote tide gauges and c three DARTs. The solid vertical red line labelled “E” denotes the time of the earthquake

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Fig. 11

source and b far-zone groups of coastal stations

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Notes

  1. DART = Deep-ocean Assessment and Reporting of Tsunamis, is an effective network of deep-ocean stations designed for continuous monitoring of tsunami waves in the open ocean and for early tsunami warning (cf. Rabinovich and Eblé 2015).

  2. We could not use the Quepos tide gauge record because it was of poor quality.

  3. We use the common term “spectrum” (S) for brevity for the “Spectral Power Density” (sometimes also shortened to “Power Spectrum”), in which the signal variance is partitioned into frequency bands and has units of amplitude2/frequency (in our study mostly in cm2/cph = “cycles per hour”). Integration of S over the entire frequency band enables us to estimate the total variance of the signal (cf. Thomson and Emery, 2014), which is the same as estimating the total variance directly from the time series (Var in Sect. 3.1).

  4. We do not show the far-field background spectra because they are similar to those for the near-field spectra (Fig. 12 left column).

  5. Unfortunately, for the 2010 and 2011 events, we had to use slightly different DARTs than for the 2017 Chiapas tsunami because the required data for DARTs 32411 and 43412 for 2010 and 2011 were not available.

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Acknowledgements

This work was partially supported by the Mexican National Polytechnic Institute (IPN, project SIP 20181373). Additional support for the first author was provided by SNI (Mexican National System of Investigators). For AR, this study was partly supported by the Russian State Assignment of IORAS #0128-2021-0004. We sincerely thank the Mexican National Mareographic Service of the UNAM and the Laboratory of the Sea Level of the CICESE for providing us the data of coastal sea level gauges, as well as George Mungov (NOAA/NCEI, Boulder, Colorado, USA) for assisting us with the DART data. We gratefully acknowledge the help of Emile Okal (Northwestern University, Evanston, IL, USA), Matias Carvajal (Universidad de Concepción, Chile) and Christopher Moore (NOAA Pacific Marine Environmental Laboratory, Seattle, WA, USA) for their careful editing and valuable suggestions that greatly improved the scientific content of our study.

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Zaytsev, O., Rabinovich, A.B. & Thomson, R.E. The Impact of the Chiapas Tsunami of 8 September 2017 on the Coast of Mexico. Part 1: Observations, Statistics, and Energy Partitioning. Pure Appl. Geophys. 178, 4291–4323 (2021). https://doi.org/10.1007/s00024-021-02893-x

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