@InProceedings{FigueiredoVaBeBoTaWr:2022:SeGrWa,
author = "Figueiredo, Cosme Alexandre Oliveira Barros and Vadas, Sharon and
Becker, Erich and Bossert, Katrina and Takahashi, Hisao and
Wrasse, Cristiano Max",
affiliation = "{Instituto Nacional de Pesquisas Espaciais (INPE)} and {NorthWest
Research Associates} and {NorthWest Research Associates} and
{Arizona State University} and {Instituto Nacional de Pesquisas
Espaciais (INPE)} and {Instituto Nacional de Pesquisas Espaciais
(INPE)}",
title = "Secondary Gravity Waves Generated by the Tonga Volcano Explosion
and Its Effect on the New Zealand, Australia, and South America
Ionosphere",
year = "2022",
organization = "AGU Fall Meeting",
publisher = "AGU",
abstract = "In this presentation, we discuss the Traveling ionospheric
disturbances observed over New Zealand, Australia, and South
America that were caused by the multiple explosions of the Tonga
volcano (20° S; 175° W) on January 15, 2015, the first one of
which occurred at ~4:15 UT. To observe the ionospheric effects at
these locations, approximately 1000 GNSS receivers were used to
calculate the detrended total electronic content (dTEC).
Approximately 1.0 - 1.5 hour after the first explosion, traveling
ionospheric disturbances (TIDs) were observed over New Zealand
with a horizontal wavelength (\λ_H) of 1300-1525 km,
horizontal phase velocity (C_H) of 551-635 m/s, period (\τ)
of 39-40 min, and azimuth (?) (\α) of 210-215°. On the other
hand, in Australia, TIDs were observed 3 hours after the explosion
with \λ_H, C_H, \τ, and \α of 861 km, 478 m/s,
30 min, and 266°, respectively. Finally, in South America, 8 hours
after the explosion, we observed TIDs with the following
characteristics: \λ_H between 348 and 1174 km, C_H of 294 -
515 m/s, \τ of 19 - 36 min., and \α of 32°. Between
18:00 UT and 19:00 UT, we also observed TIDs over South America
with \λ_H of 330-505 km, C_H of 275 - 350 m/s, \τ of
20 - 24 min., and \α of 32-139°. We then discuss using the
Model for gravity wavE SOurce, Ray trAcing and reConstruction
(MESORAC) to calculate the primary GWs and the HIAMCM (HI Altitude
Mechanistic general Circulation Model) model to determine the
secondary GWs in the thermosphere created by these explosions. Via
comparison with these model results, we show that it is the
secondary GWs which propagate over New Zealand, Australia, and
South America.",
conference-location = "Chicago, IL",
conference-year = "12-16 Dec. 2022",
urlaccessdate = "11 maio 2024"
}