Coastal Acoustic Tomography of the Neko-Seto Channel with a Focus on the Generation of Nonlinear Tidal Currents—Revisiting the First Experiment

The first coastal acoustic tomography (CAT) experiment site of the Neko-Seto Channel was revisited to elucidate the propagation and generation characteristics of the M<sub>2</sub> and M<sub>4</sub> tidal currents with a second CAT experiment, which was conducted from 3–6 Apri...

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Bibliographic Details
Published in:Remote Sensing
Main Authors: Minmo Chen, Aruni Dinan Hanifa, Naokazu Taniguchi, Hidemi Mutsuda, Xiaohua Zhu, Zenan Zhu, Chuanzheng Zhang, Ju Lin, Arata Kaneko
Format: Article
Language:English
Published: MDPI AG 2022-03-01
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Online Access:https://www.mdpi.com/2072-4292/14/7/1699
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Summary:The first coastal acoustic tomography (CAT) experiment site of the Neko-Seto Channel was revisited to elucidate the propagation and generation characteristics of the M<sub>2</sub> and M<sub>4</sub> tidal currents with a second CAT experiment, which was conducted from 3–6 April 2018 (local time). Two-dimensional flow fields of the M<sub>2</sub> and M<sub>4</sub> tidal currents and the residual current were reconstructed using a coast-fitting inversion model with the reciprocal travel-time data of five acoustic stations. The M<sub>2</sub> tidal current is a progressive-type wave that propagates eastward at a speed of 0.7 ms<sup>−1</sup>, much slower than expected for free progressive tides in this region (19 ms<sup>−1</sup>). The M<sub>4</sub> nonlinear current constructed an out-of-phase relationship between the western and eastern halves of the tomography domain, implying the generation of standing-type waves. Such nonlinear processes led to flood- and ebb-dominant tidal current asymmetries for the western and eastern halves of the model domain, respectively. The two-day mean residual currents constructed a northeastward current with a maximum speed of 0.3 ms<sup>−1</sup> in the western half of the model domain and a clockwise rotation in the eastern half. The averaged inversion errors were 0.03 ms<sup>−1</sup>, significantly smaller than the amplitude of the aforementioned currents.
ISSN:2072-4292