Abstract:Abstract-The sound production from the Morávka fireball has been examined in detail making use of infrasound and seismic data. A detailed analysis of the production and propagation of sonic waves during the atmospheric entry of the Morávka meteoroid demonstrates that the acoustic energy was produced both by the hypersonic flight of the meteoroid (producing a cylindrical blast wave) and by individual fragmentation events of the meteoroid, which acted as small explosions (producing quasispherical shock waves). T… Show more
“…Recently, infrasound records have been combined with satellite data to estimate bolide source energies, luminous efficiencies, and to calibrate influx rates observed by satellite systems (Brown et al 2002b), while multistation recordings have been employed for bolide geolocation (Brown et al 2002c). A recent analysis of the Morávka meteorite fall (BoroviËka et al 2003a;Brown et al 2003) has placed some limits on characteristics of the shock wave source at the fireball from both the ballistic wave and fragmentation events, suggesting that the deviation of the ray normals for the fragmentation events may be as much as 30° beyond that expected from a purely cylindrical line source blast.…”
Section: Infrasonic Recordingsmentioning
confidence: 99%
“…11a and 11b. This numerical model has also been used previously for interpreting infrasonic data measured for the Morávka fireball (see Brown et al [2003] for more details).…”
Section: Acoustic Numerical Ray Modeling (Moving Point Source Model)mentioning
Abstract-We have analyzed several types of data associated with the well-documented fall of the Neuschwanstein meteorites on April 6, 2002 (a total of three meteorites have been recovered). This includes ground-based photographic and radiometer data as well as infrasound and seismic data from this very significant bolide event (Spurn˝ et al. 2002(Spurn˝ et al. , 2003. We have also used these data to model the entry of Neuschwanstein, including the expected dynamics, energetics, panchromatic luminosity, and associated fragmentation effects. In addition, we have calculated the differential efficiency of acoustical waves for Neuschwanstein and used these values to compare against the efficiency calculated using available ground-based infrasound data. This new numerical technique has allowed the source height to be determined independent of ray tracing solutions. We have also carried out theoretical ray tracing for a moving point source (not strictly a cylindrical line emission) and for an infinite speed line source. In addition, we have determined the ray turning heights as a function of the source height for both initially upward and downward propagating rays, independent of the explicit ray tracing (detailed propagation path) programs. These results all agree on the origins of the acoustic emission and explicit source heights for Neuschwanstein for the strongest infrasonic signals. Calculated source energies using more than four different independent approaches agree that Neuschwanstein was certainly <500 kg in initial mass, given the initial velocity of 20.95 km/s, resulting in an initial source energy ≤0.0157-0.0276 kt TNT equivalent (4.185 × 10 12 J). Local source energies at the calculated infrasonic/seismic source altitudes are up to two orders of magnitude smaller than this initial source energy.
“…Recently, infrasound records have been combined with satellite data to estimate bolide source energies, luminous efficiencies, and to calibrate influx rates observed by satellite systems (Brown et al 2002b), while multistation recordings have been employed for bolide geolocation (Brown et al 2002c). A recent analysis of the Morávka meteorite fall (BoroviËka et al 2003a;Brown et al 2003) has placed some limits on characteristics of the shock wave source at the fireball from both the ballistic wave and fragmentation events, suggesting that the deviation of the ray normals for the fragmentation events may be as much as 30° beyond that expected from a purely cylindrical line source blast.…”
Section: Infrasonic Recordingsmentioning
confidence: 99%
“…11a and 11b. This numerical model has also been used previously for interpreting infrasonic data measured for the Morávka fireball (see Brown et al [2003] for more details).…”
Section: Acoustic Numerical Ray Modeling (Moving Point Source Model)mentioning
Abstract-We have analyzed several types of data associated with the well-documented fall of the Neuschwanstein meteorites on April 6, 2002 (a total of three meteorites have been recovered). This includes ground-based photographic and radiometer data as well as infrasound and seismic data from this very significant bolide event (Spurn˝ et al. 2002(Spurn˝ et al. , 2003. We have also used these data to model the entry of Neuschwanstein, including the expected dynamics, energetics, panchromatic luminosity, and associated fragmentation effects. In addition, we have calculated the differential efficiency of acoustical waves for Neuschwanstein and used these values to compare against the efficiency calculated using available ground-based infrasound data. This new numerical technique has allowed the source height to be determined independent of ray tracing solutions. We have also carried out theoretical ray tracing for a moving point source (not strictly a cylindrical line emission) and for an infinite speed line source. In addition, we have determined the ray turning heights as a function of the source height for both initially upward and downward propagating rays, independent of the explicit ray tracing (detailed propagation path) programs. These results all agree on the origins of the acoustic emission and explicit source heights for Neuschwanstein for the strongest infrasonic signals. Calculated source energies using more than four different independent approaches agree that Neuschwanstein was certainly <500 kg in initial mass, given the initial velocity of 20.95 km/s, resulting in an initial source energy ≤0.0157-0.0276 kt TNT equivalent (4.185 × 10 12 J). Local source energies at the calculated infrasonic/seismic source altitudes are up to two orders of magnitude smaller than this initial source energy.
“…For example, the Park Forest fireball (March 27, 2004) fragmented three times before reaching the ground ). The Neuschwanstein fireball (April 6, 2002) was also reduced into pieces at the end of its trajectory (Spurný et al 2003;Oberst et al 2004;ReVelle et al 2004), as did the Morávka (May 6, 2000) (Brown et al 2003), the Tagish Lake (January 18, 2000) (Brown et al 2002a), and the Peekskill (October 9, 1992) (Beech et al 1995;Ceplecha et al 1996) events. Such objects usually produce seismic and acoustic signals when they fragment or when the supersonic front shock sweeps the Earth's surface (Brown et al 2003).…”
Abstract-On September 15th, 2007, around 11:45 local time in Peru, near the Bolivian border, the atmospheric entry of a meteoroid produced bright lights in the sky and intense detonations. Soon after, a crater was discovered south of Lake Titicaca. These events have been detected by the Bolivian seismic network and two infrasound arrays operating for the Comprehensive Nuclear-Test-Ban Treaty Organization, situated at about 80 and 1620 km from the crater. The localization and origin time computed with the seismic records are consistent with the reported impact. The entry elevation and azimuthal angles of the trajectory are estimated from the observed signal time sequences and backazimuths. From the crater diameter and the airwave amplitudes, the kinetic energy, mass and explosive energy are calculated. Using the estimated velocity of the meteoroid and similarity criteria between orbital elements, an association with possible parent asteroids is attempted. The favorable setting of this event provides a unique opportunity to evaluate physical and kinematic parameters of the object that generated the first actual terrestrial meteorite impact seismically recorded.
“…Past atmospheric trajectories of reballs have been determined by visual recordings such as photographs and movies (Brown et al, 1994(Brown et al, , 2003, infrasound records (Brown et al, 2002;Le Pichon et al, 2002, and seismic records (e.g., Nagasawa, 1978;Nagasawa and Miura, 1987;Cevolani, 1994;Qamar, 1995;Brown et al, 2002;Cates and Sturtevant, 2002;Le Pichon et al, 2002Ishihara et al, 2003Ishihara et al, , 2004Rydelek and Pujol, 2004;Pujol et al, 2005). An object ying at supersonic velocity produces a sonic boom, and the acoustic-to-seismic coupled signal is often recorded by seismic arrays.…”
The Biwako reball on August 7, 2010, produced a strong sonic boom throughout central Japan around 17:00 JST (UTC+9). There were many visual observations and reports of the sound in the Tokai and Kinki regions at that time. We have estimated the trajectory of this reball and the location of its termination point by analyzing seismograms recorded on a dense local network. The isochrons of the arrival times are close to concentric circles, which suggest that the reball disappeared due to fragmentation during entry. The reball trajectory which explains the arrival times of the signal has a relatively high incident angle (55 degrees relative to the horizon) and the source is thought to disappear at a height of 26-km east of Lake Biwa. The azimuthal angle and velocity of the reball are dif cult to determine uniquely from this dataset. We identi ed an event thought to be due to fragmentation, with a location 3-km ENE and 9-km higher than the termination point. This location is consistent with the trajectory determined from the signal arrival. Based on this trajectory model, the source of the signal spans a horizontal range of 26 to 70 km, and the altitude of the source producing the sonic boom is about 30 to 50 km.
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