EXPLOSION CAMERAS WITH PROTECTIVE FOAMY LINING: DEFORMATION MODES ARISING UPON EXPLOSIVE LOADING EPNM-2012, Strasburg A. G. Kazantsev 2, S. S. Smolyanin.

Slides:



Advertisements
Similar presentations
PH0101 UNIT 1 LECTURE 1 Elasticity and Plasticity Stress and Strain
Advertisements

11 MODIFICATION OF AMORPHOUS Co-BASED METAL ALLOY BY SHOCK-WAVE LOADING A.Z.Bogunov, R.S.Iskhakov, V.I.Kirko, A.A.Kuzovnikov JSC « Pulse technologies »
STATICALLY DETERMINATE STRESS SYSTEMS
Explosive joining of dissimilar metals: experiment and numerical modeling Anan’ev S.Yu., Andreev A.V., Deribas A.A., Yankovskiy B.D. Joint Institute for.
EXPLOSION HAZARD OF HYDROGEN-AIR MIXTURES IN THE LARGE VOLUMES V.A. Petukhov, I.M. Naboko, and V.E. Fortov Joint Institute for High Temperatures of Russian.
1 Thin Walled Pressure Vessels. 2 Consider a cylindrical vessel section of: L = Length D = Internal diameter t = Wall thickness p = fluid pressure inside.
Elasticity by Ibrhim AlMohimeed
Solid Materials.
Particle movement in matter What happens when a particle moves in another matter?
Normal Strain and Stress
Chapter 3 Mechanical Properties of Materials
EXPLOSIVE WELDING OF LARGE BRASS/STEEL SHEETS I.V. Denisov, O.L. Pervukhina, L.B. Pervukhin (Russia) Institute of Structural Macrokinetics and Materials.
The various engineering and true stress-strain properties obtainable from a tension test are summarized by the categorized listing of Table 1.1. Note that.
Fabrication of Mo/Cu Functional Gradient Material by Hot-Explosive Consolidation Pengwan Chen a, *, Xiang Gao a, Weiping Shen b, Zhiming Jiang a, Sanxi.
TRACTOR UNIT MODULE – BREAKABLE CONNECTION DESIGN.
CTC / MTC 222 Strength of Materials
Plate Modeling under Blast Loading By Brian Cabello.
Physics. Properties of Matter Session Session Objectives.
ENGR 225 Section
MECHANICAL PROPERTIES OF MATERIALS
Deforming Solids.
Strength of Material Shear Strain Dr. Attaullah Shah.
EPNM2010 Blast and noise mitigation of open air explosions.
Explosive Production of New Materials (EPNM – 2008) Comparative Tensile Strength and Shear Strength of Detaclad Explosion Clad Products Andy Vargo R&D.
Study on Explosive Forming of Aluminum Alloy
Mechanical Properties
2.2 Materials Materials Breithaupt pages 162 to 171.
Institute of Structural Macrokinetics and Materials Science Russian Academy of Sciences, Chernogolovka XII EPNM Symposium «Explosive Production of New.
FYI: All three types of stress are measured in newtons / meter2 but all have different effects on solids. Materials Solids are often placed under stress.
Msc. eng. Magdalena German Faculty of Civil Engineering Cracow University of Technology Budapest, Simulation of damage due to corrosion in RC.
Detonation Parameters as Inferred from Shock Adiabats of Reaction Products V.S. Trofimov, V.A. Veretennikov Institute of Structural Macrokinetics and Materials.
© 2007 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
One of the most important fields in engineering Mechanics.
L. B. Pervukhin and O. L. Pervukhina
SHOCK-ASSISTED SOLID  SOLID SYNTHESIS: STRUCTURE OF REACTION ZONE S. V. Buravova, Yu. A. Gordopolov, N. A. Denisova, and I. V. Saikov Institute of Structural.
The modeling of the channel deformations in the rivers flowing into permafrost with an increase in ambient temperature E. Debolskaya, E. Zamjatina, I.Gritsuk.
1.Industrial-scale production of clad metals by explosive welding in moscow area:technology and enviroment challenges Sidorov of M.I. 1, Vaginas of A.B.
Analysis of Multi-Material Plates Under Explosive Loading Engineering Project Final Report Presentation By James Danyluk.
Materials PHYA2. MATERIALS DENSITY, SPRINGS, STRESS AND STRAIN Topics 11, pp.162–173.
(1) – Russian Federal Nucler Center, Sarov, Nizhni Novgorod region, Russia (2) – Institute of Structural Mycrokinetics of Russian Academy of Sciences,
Design of Concrete Structure I Dr. Ali Tayeh First Semester 2009 Dr. Ali Tayeh First Semester 2009.
Institute of Structural Macrokinetics and Materials Science, Russian Academy of Sciences, Chernogolovka, Moscow, Russia
1 Confidential Proprietary Application of layers with internal stress for silicon wafer shaping J. Šik 1, R. Lenhard 1, D. Lysáček 1, M. Lorenc 1, V. Maršíková.
Behavior of bubble pulse in food processing using underwater shock wave Hideki Hamashima*, Manabu Shibuta**, Yosuke Nishimura**, Shigeru Itoh** *Kumamoto.
Relationship between the bands of localized deformation and the state of deformed material Institute of Structural Macrokinetics and Materials Science,
DISSIPATION OF EXPLOSIVE ENERGY BY SOLID CELLULAR MATERIALS: EXPERIMENTAL EVALUATION R. D. Kapustin 1, L. B. Pervukhin. 1, P. A. Nikolaenko 1, A. D. Chudnovskii.
BOMBARDING OF MATERIALS WITH EXPLOSION-ACCELERATED PARTICLES: EVALUATION OF DEVELOPED PRESSURES E.V. Petrov 1, R.G. Kirsanov 2, and A.L. Krivchenko 3 1.
CONSTRUCTION MATERIALS
Lecture Outline Chapter 9 College Physics, 7 th Edition Wilson / Buffa / Lou © 2010 Pearson Education, Inc.
Mechanical Designs of The Central Detector Jinyu Fu
1.To understand the keywords associated with the deformation of different types of solids 2.To be able to calculate stress, strain and hence Young’s modulus.
1.To understand the keywords associated with the deformation of different types of solids 2.To be able to calculate stress, strain and hence Young’s modulus.
-Elastic Properties of Solids AP Physics C Mrs. Coyle.
4. Properties of Materials Sediment (size) Physical States of Soil Concepts of Stress and Strain Normal and Shear Stress Additional Resistance Components.
PROTECTION AGAINST DYNAMIC DAMAGE A.F. Belikova, S.N. Buravova, Yu.A. Gordopolov Institute of Structural Macrokinetics and Materials Science, Russian.
Finite elements simulations of surface protrusion evolution due to spherical voids in the metals 2013 University of Tartu: V. Zadin A. Aabloo University.
SOLID-STATE DETONATION SYNTHESIS Yu.A. Gordopolov, D.L. Gur’ev, S.M. Gavrilkin and S.S. Batsanov Institute of Structural Macrokinetics and Materials Science.
Department of Physics & Astronomy Institute for Gravitational Research Scottish Universities Physics Alliance Brownian thermal noise associated with attachments.
The Innovative Design of Piezoelectric Heat Pipe Generator Professor: David. T. W. Lin J.C. Hsieh Student: Cheng-Feng Shen 1.
1. Two rods, one of nylon and one of steel, are rigidly connected as shown in Fig. P.1.2. Determine the stresses and axial deformations when an axial load.
Northwestern Polytechnical University
Mechanics of Solids (M2H321546)
Bulk properties of solids
Acoustic field modulation in a regenerator
Day Topic: Snaky and Slinky Lab
Mechanical Properties: 1
Shear in Rubber Apparatus
ON DETONATION IN ZnS POWDER MIXTURES
Describing deformation
Tutorial.
Presentation transcript:

EXPLOSION CAMERAS WITH PROTECTIVE FOAMY LINING: DEFORMATION MODES ARISING UPON EXPLOSIVE LOADING EPNM-2012, Strasburg A. G. Kazantsev 2, S. S. Smolyanin 2, L. B. Pervukhin 1, P. A. Nikolaenko 1, and R. D. Kapustin 1 1 Institute of Structural Macrokinetics and Materials Science RAS, Chernogolovka, Moscow, Russia 2 Central Research Institute for Machinery Industry (TsNIITMash), Moscow, Russia

As is known, from the published data, gas-liquid foams most effectively use for effective dissipation of shock energy. But gas-liquid foams exhibit a restricted service life. In this work, we explored the applicability of solid refractory foams for the above purpose.

Purpose of the work - to determine the effectiveness of the dissipation of explosive energy by solid porous materials (solid foams). In the represented work is investigated the possibility of application for the dissipation of the shock waves of the solid aluminosilicate porous materials VBF of the production Privately held company NPKF “MaVR”. Purpose of the work

Experimental model finite-element model Metall shell Cellular material VBF explosive charge (TNT); air

Strains in metall shell TNT m=600 gramm Model without solid aluminosilicate porous material VBF TNT m=900 gramm Model with solid aluminosilicate porous material VBF

Pressure upon a container wall TNT m=600 gramm Model without solid aluminosilicate porous material VBF TNT m=900 gramm Model with solid aluminosilicate porous material VBF

Plastic deformations in metall shell A) TNT m=600 gramm Model without solid aluminosilicate porous material VBF В) TNT m=900 gramm Model with solid aluminosilicate porous material VBF

Experimental model 1 – Cellular material VBF ; 2 – the strain gauge; 3 – explosive charge (TNT); 4 – the electric detonator; 5 – camera for the electric detonator and opening for wires or detonation cord; 6 – metall shell of the experimental model;

Strains in metall shell of experimental models, MPa TNT mass, gramm Model without solid aluminosilicate porous material VBF Model with solid aluminosilicate porous material VBF the upper surfaceThe sidethe upper surfaceThe side 20072,28831,842, ,72431, ,3397,2137,8194, ,9423,4

The calculation of the efficiency of shock energy dissipation Q V = 1,4/0,14 = 10 MJ/m3 = 10 J/sm3 Q V – volumetric energy-absorption of material VBF; Q П – the quantity of energy, absorbed by material VBF according to the results of the tests of experimental models; V – the volume of material VBF in the experimental models

Calculation of the stress-strain state Material of metall shell – steel 9MnSi5; Diameter-1,2 m, Thickness of a wall-12 mm Mass without VBF 700±20 kg Cellular material VBF, thickness of a layer of 300 mm ρ = 0,7 gramm/sm3 При R≤αr 0 TNT, kgr, mσ н, МПа 0,250, ,50, ,750, , ,250, ,50, ,750, , ,250, ,50, ,750, , ,250, ,50,08762 где: σ н – Strains in metall shell caused by influence on it of a shock wave, R об – radius of metall shell, δ – thickness of metall shell, r 0 –TNT radius, α = 10 – the factor considering limiting expansion of products of a detonation, Q – specific energy allocation of TNT, Е – material,s elasticity module of shell, ρ 0 – TNT density, ρ в – air density, μ – Poisson's ratio

The results of the experiment m TNT,kgL sircle, mm of metall shell before explosion L sircle, mm of metall shell after explosion relative lengthening Notes 3, ,5Plastic deformation is negligible or no 4, ,3Plastic deformation 7, ,2tensile strength exceeding

Main conclusions 1) Is developed the procedure of the experimental determination of the energy-dissipate ability of the solid cellular materials by the method of their accomodation into closed metal shell from a change in the deformation of this of shell. 2) Used the method of calculation, based on the method of finite elements and the combined Lagrangian-Eulerian formulation of the equations of motion of a continuous medium. It allows to adequately describe the impact of a shock wave on the wall of the pilot sample, as with VBF, so without it. Experimental results were found to reasonably agree with calculated ones. 3) The foamy materials under investigation showed good results: the efficiency of shock energy dissipation was found to attain a value of about 10 J/cm3. Material VBF with the volume of 1 m3 absorbs the energy, isolated with explosion of the charge of TNT by the mass of 2,4 kg. 4) The scale factor in the case of a proportional increase in sample sizes and thickness of energy absorbing layer does not affect the ability of the VBF dissipation of shock energy

THANK YOU FOR ATTENTION!