Abstract
Mt. Asama, Nagano Prefecture, Japan, erupted at 11:02 UT on September 1st, 2004. Ionospheric disturbances associated with this eruption were detected using TEC data and HF Doppler observations. It has already been reported that the TEC data obtained from GNSS receivers revealed that N-shaped disturbances in TEC with a period of 76 s occurred 12 min after the eruption. In the HF Doppler sounding observations, on the other hand, a spiky variation in the Doppler frequency with a frequency of about 10 mHz was observed 9–11 min after the eruption. Ray tracing calculations of the acoustic waves confirmed that both N-shaped disturbances in TEC and the spiky variations in the Doppler frequency were generated by the acoustic wave due to the eruption of Mt. Asama. Compared to earthquakes, volcanic eruptions are treated as point sources of atmospheric waves. Therefore, the acoustic waves produced by the present eruption were considered to behave as shock waves. In the HF Doppler observation, subsequent to the spiky signature, a longer-period wavy disturbance appeared. The frequency of these long-period disturbances is about 4 mHz, which is almost the same as the coseismic ionospheric disturbances. The cause of these long-period disturbances is considered to be gravity waves due to the partial transformation of the eruption energy or the acoustic resonance between the ground and lower ionosphere. Although both are typical causes of disturbance associated with earthquakes, it was difficult to determine which was the primary cause in the present case. In order to clarify the cause of wavy disturbances in the present event, it is necessary to investigate atmospheric waves associated with volcanic eruptions in detail using additional observation data, such as ground-based infrastructure sound networks.Graphical
Highlights
1 Introduction Recently, it was reported that the extremely strong eruption by the Hunga-Tonga–Hunga Haapai volcano in January 2022 was followed by strong atmospheric waves, which propagated around the entire Earth and excited ionospheric disturbances
Closer look at the Doppler frequency data indicates that two types of disturbances were detected after the eruption: an initial, spiky, short-period disturbance immediately following the arrival of the acoustic wave, and a subsequent, longperiod disturbance
As for coseismic ionospheric disturbances, the period of the coseismic total electron content (TEC) variation is dependent on the magnitude of earthquakes
Summary
1 Introduction Recently, it was reported that the extremely strong eruption by the Hunga-Tonga–Hunga Haapai volcano in January 2022 was followed by strong atmospheric waves, which propagated around the entire Earth and excited ionospheric disturbances. Potential causes for these wavy disturbances include atmospheric gravity waves, such as those reported by De Angelis et al (2011) during the 2008 Okmok eruption Another source of such wavy disturbances in TEC is acoustic resonance between the ground and lower ionosphere, as observed during the 2014 eruption of the Kelud volcano in Indonesia (Nakashima et al 2016). The eruption, with a Volcano Eruption Index (VEI) of 2, introduced ionospheric variations whose characteristics are similar to coseismic disturbances, including N-shaped ionospheric variations beginning approximately 12 min after the eruption and propagating southward with an estimated speed of 1.1 km/s These features imply that the acoustic waves due to the eruption reached the ionosphere and initiated the disturbances. To determine the cause of the different period of the N-shaped disturbances, we have analyzed the ionospheric disturbances associated with this eruption using TEC data and HF Doppler sounding system
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