Airburst of a small cosmic body. When and how does it begin?
Turning asteroids into stardust
by Luigi Foschini

Not always a cosmic body heading toward a planet does actually hit the ground. It must be of certain size or composition, to get throughout the atmosphere and collide. How does this work? How big must an asteroid or a comet be to pass the atmosphere layer by layer and hit? Some put the limit of strength dominated regime at 150 m. Below this limit, the presence of the atmosphere plays an important role in defining the impact hazard. Indeed, in this case, the fragmentation begins before the impact and, after the break up, the small asteroid/comet begins to expand, increasing its cross section to the air flow, which in turn results in increasing the drag and deceleration.
This process is like an explosion. For this reason, the atmospheric fragmentation is often called "explosion" or "airburst" in the scientific literature, even though they are not related to TNT or nuclear explosions.

Fallen trees in the Tunguska area (1928). Tunguska Page of Bologna University
The best known event of this type is the Tunguska event of 30 June 1908, when a 10-20 Mton explosion at 5-10 kilometres height, destroyed 2150 square kilometres of siberian taigà and more than 80 million of trees. The nature of the cosmic body which caused this event is still under discussion and on July 1999 (Tunguska99) an expedition went to Siberia to collect data and samples, hoping to find the decisive argument.
The key problem in the study of airburst is to understand when the cosmic body begins to break up. First models put this condition when the dynamical pressure in the front of the asteroid/comet is equal to the mechanical strength of the material. However, during nineties Zdenek Ceplecha showed that this is not true. He studied airburst from tiny asteroids , that is, meters-sized bodies: for some of these bodies there are available photographic and video records, that made it possible to calculate with great precision the height of fragmentation and the corresponding dynamical pressures.

It resulted that the pressure is systematically lower (more than one order of magnitude) than the mechanical strength. Some authors invoked special features of the incoming body: non-homogeneity, additional flaws and cracks, internal voids. But all of them could give explanations for some episodes, not a general theory.
One possible solution to this conundrum -the one I have proposed to the discussion - is based on the study of unsteady flow around the small asteroid/comet. In this case, the distortion of the schock wave created during the passage in the atmosphere, interacts with the turbulence, which results in sudden outburst of the dynamical pressure, up to twelve times its nominal value. Therefore, even though the dynamical pressure cannot reach the mechanical strength, the amplification of turbulence can produce the required effect. This could also explain why meteorites reaching the ground are cold: the break up occurs after a simple mechanical process and not because of thermo-mechanical stress.
It is worth noting that the condition for the existence of this mechanism is that the Mach number (i.e., the ratio between the speed of the cosmic body and the local sound speed) is changing. If it is constant, the interaction between shock wave and turbulence does not occurs, and the fragmentation occurs because of thermo-mechanical stress.
This solution is developed only from a conceptual point of view and numerical modelling is necessary to fully develop and test the theory. However, for the moment, it is the only available.

 

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