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Snapshots of atmospheric disturbances at 12:00, 18:00, and 20:00 KST on March 4, 2018. (a) Predicted air pressure (E -09 h). The dashed circles enclose the area with air pressure disturbances. (b) Calculated air pressure disturbance using the LDAPS prediction (E -09 h). The black empty squares indicate the tide gauges where strong meteotsunamis were detected. The dashed box encloses the shared area between the LDAPS domain and radar coverage along the west coast of the Korean Peninsula. (c) Observed rain rate in radar images. (For interpretation of the references to color in this figure legend, the reader is referred to the Web version of this article.)

Snapshots of atmospheric disturbances at 12:00, 18:00, and 20:00 KST on March 4, 2018. (a) Predicted air pressure (E -09 h). The dashed circles enclose the area with air pressure disturbances. (b) Calculated air pressure disturbance using the LDAPS prediction (E -09 h). The black empty squares indicate the tide gauges where strong meteotsunamis were detected. The dashed box encloses the shared area between the LDAPS domain and radar coverage along the west coast of the Korean Peninsula. (c) Observed rain rate in radar images. (For interpretation of the references to color in this figure legend, the reader is referred to the Web version of this article.)

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A traveling air pressure disturbance of several hPa over a short period (5–10 min) can generate tsunami-like waves in coastal areas owing to a multi-resonant mechanism. Pressure-forced meteotsunamis have been reported over the Korean Peninsula on a regular basis in recent years. However, the Korean meteotsunami early warning system does not always...

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... be estimated by following the traveling air pressure disturbances for an early warning of the meteotsunamis ( ˇ Sepi´cSepi´c and Vilibi´cVilibi´c, 2011;Vilibi´cVilibi´c et al., 2016). We analyzed the horizontal distribution of the surface pressure field of a recent prediction (E -09 h) to examine LDAPS performance based on simulated propagation (Fig. 4a). In the surface pressure field, a low-pressure system (1,000-1,005 hPa at the center) with a discontinuous pattern located at its edge (dashed circles in Fig. 4a) landed on the west coast of the Korean Peninsula from China across the Yellow Sea. Eq. (1) was used for each grid to filter out the spatial and temporal evolution of air ...
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... et al., 2016). We analyzed the horizontal distribution of the surface pressure field of a recent prediction (E -09 h) to examine LDAPS performance based on simulated propagation (Fig. 4a). In the surface pressure field, a low-pressure system (1,000-1,005 hPa at the center) with a discontinuous pattern located at its edge (dashed circles in Fig. 4a) landed on the west coast of the Korean Peninsula from China across the Yellow Sea. Eq. (1) was used for each grid to filter out the spatial and temporal evolution of air pressure disturbances (i.e., discontinuous patterns) before and after the onset of the event (E). Consequently, the low-pressure system was removed from the simulated ...
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... temporal evolution of air pressure disturbances (i.e., discontinuous patterns) before and after the onset of the event (E). Consequently, the low-pressure system was removed from the simulated pressure field. A cluster of air pressure jumps propagated in the same order as the observed order of meteotsunamis at the DH, WD, YG, and GS tide gauges (Fig. 4b). In addition, we found similar spatial scales and propagation patterns between the clusters of air pressure jumps (Fig. 4b) and rain rates above 5 mm/h (Fig. 4c) based on the correlation between the intensity of rain and air pressure anomalies, as mentioned above. Overall, the cluster of air pressure jumps from the LDAPS prediction ...
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... Consequently, the low-pressure system was removed from the simulated pressure field. A cluster of air pressure jumps propagated in the same order as the observed order of meteotsunamis at the DH, WD, YG, and GS tide gauges (Fig. 4b). In addition, we found similar spatial scales and propagation patterns between the clusters of air pressure jumps (Fig. 4b) and rain rates above 5 mm/h (Fig. 4c) based on the correlation between the intensity of rain and air pressure anomalies, as mentioned above. Overall, the cluster of air pressure jumps from the LDAPS prediction arrived more slowly than the observed rain rate on the radar; nevertheless, the simulated spatiotemporal propagation pattern ...
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... was removed from the simulated pressure field. A cluster of air pressure jumps propagated in the same order as the observed order of meteotsunamis at the DH, WD, YG, and GS tide gauges (Fig. 4b). In addition, we found similar spatial scales and propagation patterns between the clusters of air pressure jumps (Fig. 4b) and rain rates above 5 mm/h (Fig. 4c) based on the correlation between the intensity of rain and air pressure anomalies, as mentioned above. Overall, the cluster of air pressure jumps from the LDAPS prediction arrived more slowly than the observed rain rate on the radar; nevertheless, the simulated spatiotemporal propagation pattern was ...
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... that increased up to several hPa in a few minutes. The long-term trends of the predicted air pressures were overestimated with deviations of 1-4 hPa. The peaks of the shorter-lasting disturbances (i.e., air pressure disturbances) were underestimated and had a time lag of approximately 1-2 h (Fig. 5a), similar to the previous propagation pattern (Fig. 4). In addition, we found that the time resolution (output time interval of 10 min) was insufficient to reproduce the disturbance details. These details play an essential role in the final magnitude of the meteotsunamis. For meteotsunami simulations, atmospheric forcing should be applied every minute to capture the intensity of ...
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... warning by tracking the propagation pattern (propagation path and speed range) of the simulated air pressure jumps beyond the observation coverage (Fig. 8). From noon on March 4, 2018, clusters of air pressure disturbances below the limit of the air pressure jump propagated toward the open Yellow Sea from the source location in eastern China (Fig. 4b). The evolution of the air pressure jump that developed in a y-shaped structure from 15:00 to 20:00 KST was tracked based on hourly monitoring (red scatters in Fig. 8). The meteotsunami hazard area derived from the simulated propagation path was consistent with that determined by observation points where air pressure jumps, and ...
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... atmospheric model should capture wavelength of box-like air pressure oscillations (Fig. 2a) to predict pressure-forced meteotsunamis. As the LDAPS domain (inner grid) covers most of the Yellow Sea area with a horizontal resolution of 1.5 km, the cluster of air pressure disturbances can be found in the simulated surface pressure field ( Fig. 4a and b). To examine the number of LDAPS grid points included within the wavelength of the air pressure oscillations more quantitatively, we roughly estimated the wavelength. The estimation of the wavelength was based on the wave period (30 min), assumed as the time difference between the two air pressure jumps at the DH (15) AWS (red circles ...

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... 10-min meteorological data around Japan were available from JMA (https:// www.data.jma.go.jp/stats/etrn/index.php) since 2009. Radar reflectivity images from South Korea and Japan during the time span of maximum events were obtained from four articles (Kim et al., 2019;Kim et al., 2021a;Kim et al., 2021b;Kim et al., 2022) and the Research Institute for Sustainable Humanosphere of Kyoto University (https:// d a t a b a s e . r i s h . ...
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