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Detonation is a process of combustion in which a supersonic shock wave propagates through a body of detonable material, such as an oxygen-methane mixture or a high explosive. In a detonation, the supersonic shock wave (also known as a detonation wave) originating at the point of ignition compresses the surrounding material, thus increasing its temperature to the point of ignition. The previously-ignited material burns behind the shock wave, releasing heat energy and a high-pressure volume of gas that supports the shock wave's propagation, creating a self-sustaining reaction. Combustion is different from a deflagration, the other of the two general classes of combustion, which propagates at a subsonic rate through heat conduction. Because detonations generate high pressures, they are usually much more destructive than deflagrations.

Detonations can be produced by explosives, reactive gaseous mixtures, certain dusts and aerosols.

[edit] Etymology

Look up detonation in Wiktionary, the free dictionary.

French détoner, to explode; from Latin detonare, to expend thunder; from de-, ~off + tonare, to thunder

[edit] Theories

The simplest theory to predict the behavior of detonations in gases is known as Chapman-Jouguet (CJ) theory, developed around the turn of the 20th century. This theory, described by a relatively simple set of algebraic equations, models the detonation as a propagating shock wave accompanied by exothermic heat release. Such a theory confines the chemistry and diffusive transport processes to an infinitely thin zone.

A more complex theory was advanced during World War II independently by Zel'dovich, von Neumann, and Doering. This theory, now known as ZND theory, admits finite-rate chemical reactions and thus describes a detonation as an infinitely thin shock wave followed by a zone of exothermic chemical reaction. In the reference frame in which the shock is stationary, the flow following the shock is subsonic. Because of this, energy release behind the shock is able to be transported acoustically to the shock for its support. For a self-propagating detonation, the shock relaxes to a speed given by the Chapman-Jouguet condition, which induces the material at the end of the reaction zone to have a locally sonic speed in the reference frame in which the shock is stationary. In effect, all of the chemical energy is harnessed to propagate the shock wave forward.

Both CJ and ZND theories are one-dimensional and steady. However, in the 1960s experiments revealed that gas-phase detonations were most often characterized by unsteady, three-dimensional structures, which can only in an averaged sense be predicted by one-dimensional steady theories. Modern computations are presently making progress in predicting these complex flow fields. Many features can be qualitatively predicted, but the multi-scale nature of the problem makes detailed quantitative predictions very difficult.

[edit] Applications

Detonations are hard to control and are used primarily for demolition and in warfare. A great deal of research is conducted on achieving or preventing detonation in various materials to improve the performance of explosives and engines. An experimental form of jet propulsion, the pulse detonation engine, uses a series of well-timed detonations to generate thrust.

[edit] References

For a good layman's introduction to the theory of detonation, see:

Davis, William C., "The detonation of explosives," Scientific American, vol. 256, pages 106-112, 128 (May 1987).

[edit] See also

• Detonation section of Explosive, Detonator.
• Nuclear testing
• Detonation diamond
• Predetonation of nuclear weapons
• Chapman-Jouguet condition
• Engine knocking