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Earthquake Sound Travel and Pseudo-Dionysius of Tell-Mahre

In the Chronicle of Zuqnin, Pseudo-Dionysius of Tell Mahre reports on the sound of a distant earthquake the night before the earthquake which struck Manbij (aka Mabbug). In an English translation of Part 4 by Harrak (1999:177-178) we can read:
[747-748] The year one thousand and fifty nine:

... A tremor took place during the night, and something like the noise of a roaring bull was heard from a great distance.
While earthquake sound perception depends on a number of factors, it is feasible that a large earthquake, for example from the northern end of the Sea of Galilee, could have been heard ~450 km. away in Manbij (aka Mabbug). Tosi et al (2012) developed a relationship for earthquake perceptibility by examining a survey of ~70,0000 respondents in Italy from smaller magnitude earthquakes (M 5.0-5.5). The input variables are magnitude and distance. In the calculator below, this relationship predicts that ~20% of a population would notice an M 7.0 earthquake at a distance of 450 km. However, it is likely that this relationship underestimates perceptibility for larger magnitude earthquakes (e.g. M 7.0). In this eyewitness account from the 1994 M 6.7 Northridge earthquake, a respondent describes earthquake sounds which woke them up ~115 km. from the epicenter. Because Earthquake sound perception depends on a number of factors, it is difficult to predict so the only conclusion that can be made is that the report by Pseudo-Dionysius of Tell Mahre that a distant earthquake perhaps 450 km. away was heard as a rumble the night before is a credible one. Earthquake researcher Patrizia Tobi contributed the following comments (personal communication, 2021) regarding the perception of earthquake sounds.
In my paper the results are based on many earthquakes and the phenomenon may appear continuous, but in reality the earthquake sound is very variable and does not depend only on the intensity of the ground motion. For example, the study of infrasound showed that waves propagating through the atmosphere are produced by earthquakes through 3 distinct mechanisms: direct generation from seismic waves below the station, propagation of the sound wave produced in the epicenter region by strong ground motion, and radiation from a secondary source such as a high mountain. This implies that the soil composition, rock type, and topography of each site cannot be neglected. These factors, added to others that affect sound propagation in the atmosphere, such as pressure and temperature variations, make the problem very complicated to model.
Calculator - Earthquake perception at distance - Tosi et al (2012)

Source - Tosi et al (2012) - based on a study of earthquakes and fitted for Local Magnitudes between 5.0 and 5.5

The Higher Magnitude Adjustment is a thought experiment to extend the equation of Tosi et al (2012) to higher magnitude (and therefore louder) earthquakes. If, for example, the eyewitness testimony from the 1994 M 6.7 Northridge earthquake indicates an earthquake loud enough to wake someone up at a distance of 115 km. from the epicenter, we can assign a perceptibility of 100% at this distance and create a calibration point. An addition of 51% would need to be added to the result of Tosi et al (2012)'s equation to achieve 100% perceptibility. Adding this 51% to the perceptibility of one of the Sabbatical Year Earthquakes results in a perceptibility of ~72% for an M 7 earthquake where the nearest fault break was at the north end of the Sea of Galilee ~450 km. away. Without the Higher Magnitude Adjustment, perceptibility is ~21%. Thus we can likely constrain perceptibility to between 21% and 72%. In other words, between 21% and 72% of the people in Manbij (aka Mabbug) likely did experience a rumble from the Sabbatical Year earthquake the night before a large earthquake is reported to have collapsed a church in Manbij (aka Mabbug)

Variable Input Units Notes
km.
unitless
unitless
Variable Output Units Notes
% Percentage of people who hear the rumble
  

Experimental Calculator - Earthquake Sound - Tosi et al (2000)

Source - Tosi et al (2000)

Variable Input Units Notes
Moment Magnitude
g/cc Crust Density
km. Source Distance
km./s P wave Velocity in the crust (?) - Typical values are 5-8 km./s
Radiation Pattern of the P-wave
sec. Rise time
Hz. Frequency
? Transmission Coefficient of the compressional wave in the passage ground-air, function of the angle of incidence ϴ - value needed
kg/m3 Air density
m/s Speed of sound in air
Variable Output Units Notes
N-m Seismic Moment
µ? Ground Displacement
µ? Ground Displacement at frequency
µbar Pressure
dB Pressure
  

Notes

Theoretical Model of Earthquake Sound Theoretical Model of Earthquake Sound

Tosi et al (2000)


Units
1 Pa = 1 N/m2
1 dyne is the force required to accelerate 1 gram 1 cm/s2
1 N = 100,000 dynes
1 bar = 10^6 dynes/cm2

References

Articles and Books

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Gold, T., and S. Soter (1979), Brontides: Natural explosive noises, Science, 204, 371-375

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Le Pichon, A., J. Guilbert, A. Vega, M. Games, and N. Brachet (2002), Ground-coupled air waves and diffracted infrasound firm the Arequipa earthquake of June 23, 2001, Geophys. Res. Lett., 29(18), 1886

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Tosi, P., et al. (2000). "Spatial patterns of earthquake sounds and seismic source geometry." Geophysical Research Letters 27(17): 2749-2752.

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