Approximate closed solutions for detonation parameters in condensed explosives.

AIAA Journal ◽  
1966 ◽  
Vol 4 (7) ◽  
pp. 1182-1187 ◽  
Author(s):  
MORTON H. FRIEDMAN
Keyword(s):  
Detonation Parameters ◽  
Condensed Explosives

Determination of the detonation parameters of condensed explosives

1965 ◽  
Vol 1 (3) ◽  
pp. 1-5 ◽  
Author(s):  
V. A. Veretennikov ◽  
A. N. Dremin ◽  
K. K. Shvedov
Keyword(s):  
Detonation Parameters ◽  
Condensed Explosives

Shock discontinuity zone effect: the main factor in the explosive decomposition detonation process

1992 ◽  
Vol 339 (1654) ◽  
pp. 355-364 ◽  
Keyword(s):  
Degrees Of Freedom ◽  
Thermal Ionization ◽  
Relaxation Processes ◽  
Explosive Decomposition ◽  
Time Duration ◽  
Active Particles ◽  
Condensed Explosives ◽  
Discontinuity Zone ◽  
Electronically Excited ◽  
Non Equilibrium

A new qualitative conception of the detonation mechanism in condensed explosives has been developed on the basis of experimental and numerical modelling data. According to the conception the mechanism consists of two stages: non-equilibrium and equilibrium. The mechanism regularities are explosive characteristics and they do not depend on explosive charge structure (particle size, nature of filler in the pores, explosive state, liquid or solid, and so on). The tremendous rate of loading inside the detonation wave shock discontinuity zone ( ca. 10 -13 s) is responsible for the origin of the non-equilibrium stage. For this reason, the kinetic part of the shock compression energy is initially absorbed only by the translational degrees of freedom of the explosive molecules. It involves the appearance of extremely high translational temperatures for the polyatomic molecules. In the course of the translational-vibrational relaxation processes (that is, during the first non-equilibrium stage of ca. 10 -10 s time duration) the most rapidly excited vibrational degrees of freedom can accumulate surplus energy, and the corresponding bonds decompose faster than behind the front at the equilibrium stage. In addition to this process, the explosive molecules become electronically excited and thermal ionization becomes possible inside the translational temperature overheat zone. The molecules thermal decomposition as well as their electronic excitation and thermal ionization result in some active particles (radicals, ions) being created. The active particles and excited molecules govern the explosive detonation decomposition process behind the shock front during the second equilibrium stage. The activation energy is usually low, so that during this stage the decomposition proceeds extremely rapidly. Therefore the experimentally observed dependence of the detonation decomposition time for condensed explosives is rather weak.

Titania Nanocrystalline Prepared by Detonation Method and Calculation of Detonation Parameters

2010 ◽  
Vol 36 (1) ◽  
pp. 75-79 ◽  
Author(s):  
Yandong Qu ◽  
Xiaojie Li ◽  
Zheng Zhao ◽  
Guilei Sun
Keyword(s):  
Detonation Parameters ◽  
Detonation Method

scholarly journals Experience in Detonation Nano-Structures Coating Application Technologies using Condensed Explosives and Gas Mixtures

2016 ◽  
Vol 9 (36) ◽  
Author(s):  
Sergei Yurievich Ganigin ◽  
Albert Rafisovich Gallyamov ◽  
Maxim Vladimirovich Nenashev ◽  
Andrey Yurievich Murzin ◽  
Uljanitsky Vladimir Jurevich
Keyword(s):  
Gas Mixtures ◽  
Coating Application ◽  
Nano Structures ◽  
Condensed Explosives
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