日本地球惑星科学連合2019年大会

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[J] 口頭発表

セッション記号 M (領域外・複数領域) » M-IS ジョイント

[M-IS16] 火山噴煙・積乱雲のモデリングと観測

2019年5月30日(木) 09:00 〜 10:30 A05 (東京ベイ幕張ホール)

コンビーナ:佐藤 英一(気象研究所)、前野 深(東京大学地震研究所)、前坂 剛(防災科学技術研究所)、座長:佐藤 英一(気象研究所)

09:00 〜 09:15

[MIS16-01] 異なるタイプの気象レーダによる火山噴煙柱の観測

★招待講演

*真木 雅之1小堀 壮彦1キム ユラ1藤吉 康志2佐藤 英一3徳島 秀彦4井口 正人5 (1.鹿児島大学、2.北海道大学、3.気象研究所、4.FRCコーポレーション株式会社、5.京都大学)

キーワード:Xバンド船舶レーダ、Kuバンド高速スキャンドップラーレーダ、Xバンド偏波レーダ

The present paper describes the results of observational studies of volcanic ash columns using different types of weather radars: X-band marine radar, bi-static Ku-band radar, Ka-band Doppler radar, and operational X-band polarimetric radar. In order to observe eruption columns with extremely fine temporal resolution, an X-band marine radar was set up during three months in 2018 at the Kurokami observatory of Kyoto University located about 4km from the vent of Sakurajima volcano. The marine radar has a slot antenna that has the PPI scanning speed of 48 rpm, with a vertical beam width of 22° and a horizontal beam width of 1.2°, and a range resolution of 8m. We carried out observations by physically changing the rotational axis of the slot antenna from vertical (PPI) to horizontal (RHI) to achieve an elevation angle resolution of 1.2°. The MRI Ku-band radar and Kagoshima University Ku- band radar set up in 2017 in Sakurajima have Luneberg antenna with a horizontal and vertical beam width of 3°. The antenna rotates spirally from an elevation angle of 0° to 90° to obtain hemispherical volume data in one minute. The Ka-band Doppler radar of NIED was operating at the Kurokami observatory during 3 months in 2015 to investigate the inner structure with the RHI antenna scanning. The MLIT operational X-band polarimetric radar located approximately 11km from the vent of the Sakurajima volcano can measure volcanic ash columns three-dimensionally at 5-minute intervals, even though it is an operational radar aiming to measure heavy rainfalls in Sakurajima.

Utilizing these different types of radar data, we perform detailed analysis of eruption columns. The marine radar succeeded in detecting eruptions and at the same time detecting falling pyroclastic particles (Fig. 1). The radar also reveals the fine structure of an ascending eruption column at 1.25-second intervals. While the marine radar observes volcanic ash columns with the wider azimuth angel resolution 22° due to its fan beam antenna, Ka-band Doppler radar can observe the targets with finer azimuthal resolution using RHI scanning of the parabolic antenna. The Ka-band radar RHI observations also reveal the upward speed of the ash echo top at 2-minute intervals. While both the marine radar and the Ku-band Doppler radar measure eruption column vertically at a fixed azimuthal direction, the Ku-band Doppler radar measures all azimuth and elevation angles every 1 minute. Using this scanning strategy, we can clarify the temporal change of the eruption column during its downwind movement: the radar reflectivity factor of the upper part of the eruption column becomes high 5-minute after the eruption, which is probably due to the aggregation process in water clouds (Fig. 2). The operational X-band MP radar collects 20 tilts PPI scan data at 5-minute interval. We can construct three-dimensional data of ash clouds with time and spatial interpolation method. Then we can obtain the wide-area ash fall distributions.

In conclusion, as mentioned above, different types of weather radars are now available for studying volcanic eruption columns and their applications to disaster prevention are promising.