1 / 8

ON DETONATION IN ZnS POWDER MIXTURES

XII EPNM Symposium « Explosive Production of New Materials : Science, Technology, Business, and Innovatios ». ON DETONATION IN ZnS POWDER MIXTURES. V.S. Trofimov, E.V. Petrov. Institute of Structural Macrokinetics and Materials Science Russian Academy of Sciences, Chernogolovka. 2.

nessa
Télécharger la présentation

ON DETONATION IN ZnS POWDER MIXTURES

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. XII EPNM Symposium «Explosive Production of New Materials: Science, Technology, Business, and Innovatios» ON DETONATION IN ZnS POWDER MIXTURES V.S. Trofimov, E.V. Petrov Institute of Structural Macrokinetics and Materials Science Russian Academy of Sciences, Chernogolovka

  2. 2 Thermodynamic criterion for detonation ability of reactive mixture N.M. KuznetsovDetonation and gas-dynamic discontinuities in phase transition of metastable substances / Journal of Experimental and Theoretical Physics, 1966, Vol.22,№.5, pp. 1526–1531. A.G. Merzhanov, Yu.A. Gordopolov, V.S. TrofimovOn the possibility of gasless detonation in condensed system / Shock Waves, 1996, Vol.6, №.3, pp. 157-159.

  3. 3 Scheme of experiment Histogram of powder mixtureZnS Zn powder particles size1–11 μm 1 − voltage input 2 − top cover 3 – reactorbody 4 – bottom cap 5 – steel plate S powder particles size11–35 μm

  4. 4 Thermodynamic equation of conservation of energy in the supersonic wave propagation of a chemical reaction in the reactive mixture where: E(P,V) – is the specific internal energy of reaction product (ZnS); P – pressure; V –volume; E0 ,V00 – specific internal energy and volume of starting ZnS mixture, respectively. Characteristics of reaction product (ZnS): ρ = 3950 kg/m3;V0 = 2.532×10-4 m3/kg; Cp = 477 J/kg·K; β = 1.97×10-5 1/K; a = 5000 m/s Gruneisen coefficient calculated for reaction product (ZnS): Г = 1.032 The calculated values ​​for starting ZnS mixture:V00 ≥ 2.602×10-4 m3/kg

  5. 5 Known as functions of Vpressure Pb(V) andspecific internal energy Eb(V) of reaction product (ZnS) ForV > V0 = 2.532×10-4kg/m3andP= 0 Equation of the detonation adiabat of ZnS mixture forV  >  V0 ForV< Vlim, where: ZnS mixture detonating for V00 within the range 2.602×10-4 ≤ V00 < Vlim = 2.759×10-4m3/kg.

  6. 6 Calculated parameters of ZnS mixture at the Jouguet point and measured values for fused TNT. The detonation parameters of ZnS mixture for 2.602×10-4 ≤ V00 < 2.740×10-4m3/kg and TNT are seen to be comparable.

  7. 7 Сonclusions: This implies that, even upon neglect of evaporation, the brisance of porous and bulk ZnS mixtures is comparable with that of common high explosives. A ZnS mixture may find practical application in those processes that require sufficiently strong shock impacts on materials and at the same time it is necessary to avoid explosive action of explosion products on the environment.

  8. Thank you for attention!

More Related