2007
DOI: 10.1016/j.jastp.2006.10.011
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Acoustic analysis of shock production by very high-altitude meteors—I: infrasonic observations, dynamics and luminosity

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Cited by 30 publications
(28 citation statements)
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“…For the IS27 composite plot, the elevation angle and back azimuth suggests that ~35km is the source height though these are not strongly constrained solutions. This height is also consistent with the ballistic angle closest to 90, consistent within uncertainty to a true ballistic arrival assuming some non-linear shock behaviour near the source (Brown et al, 2007). This is the most internally consistent height for a true cylindrical shock for this station.…”
Section: Antarctica Fireball -September 3 2004supporting
confidence: 77%
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“…For the IS27 composite plot, the elevation angle and back azimuth suggests that ~35km is the source height though these are not strongly constrained solutions. This height is also consistent with the ballistic angle closest to 90, consistent within uncertainty to a true ballistic arrival assuming some non-linear shock behaviour near the source (Brown et al, 2007). This is the most internally consistent height for a true cylindrical shock for this station.…”
Section: Antarctica Fireball -September 3 2004supporting
confidence: 77%
“…However, bolides produce cylindrical line source shock along their entire trail (ReVelle, 1976), thus the period measured at each station can be different simply because returns correspond to the size of the cylindrical blast cavity at that particular segment of the trail having an acoustical path to each station. The actual length of segment of the trail that contributes to the signal is unclear since the length depends on non-linear bending near trail (Brown et al, 2007). So one possibility for this large variation is that signals are coming from different part of the bolide trail.…”
Section: Period-yield Relationmentioning
confidence: 99%
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“…Moreover, the seasonal winds in the upper stratosphere (at ~ 50 km altitude) can create a favorable propagation duct when the energy is moving in the directions of those winds (e.g., Tolstoy, 1973;Georges et al, 1977;Drob et al, 2003;Kulichkov, 2010). Because meteoroids can produce shock waves at any altitude up to ~ 100 km and in rare cases even higher (depending on the parameters described in preceding sections, such as Kn) (Zinn et al, 2004;Brown et al, 2007;Silber and Brown, 2014), the resulting infrasound signals may take multiple paths through the atmosphere, and even reach altitudes of 120 km before being refracted back to the surface. Thus, the full atmospheric state from the ground to those altitudes is needed for source characterization, although this in itself is a challenging task (e.g., see de Groot-Hedlin et al, 2010).…”
Section: Infrasoundmentioning
confidence: 99%
“…A further indicator explaining detections and nondetections at numerous stations is the local time of day and the associated ambient noise conditions at the stations during this time [Bowman et al, 2005;Matoza et al, 2013]. At most stations, clear detections of the Chelyabinsk meteorite event predominantly took place during nighttime.…”
Section: Introductionmentioning
confidence: 99%