Printer Friendly

Research of mine imitator interaction with deformable surface/Minos imitatoriaus saveikos su besideformuojanciu pavirsiumi tyrimas.

1. Introduction

The purpose of the mine imitator system is training of artillery specialists. The trainer consists of a body whose external surface, in principle, repeats the contour of a combat mine, and its inside is installed with a barrel with an infixed charge. To imitate an explosion, "the warhead" is filled with smoke powder, and while falling into the ground it should explode in this way imitating the explosion of a mine. The trainer has four charges, consisting of a "warhead" and muzzle with respective amounts of powder, which ensure firing ranges to the scale of 1/10 [1, 2]. Where "the warhead" hits the surface of the ground, the detonator goes off and it initiates the explosion of the imitative smoke powder charge [1].

The trainer is used at different soil surface conditions and should ensure the reliable performance of the mine imitator. This is predefined by sufficient displacement of the detonator's stud with respect to the capsule during interaction process of the detonator's cap and the soil. The numerical modeling of mine imitator interaction with deformable surfaces and results of the performed experiments are presented in the paper.

The strength of coarse soil-materials due to dynamic impacts highly depends upon the microstructure of the soil, the grain size of the soil, and the void between particles or grains. The same soil can behave quite differently for dynamic impacts depending on the moisture content. The pores between the grains can be filled with either highly compressible air or with water. Sand has no tensile strength when dry, but wet sand does have some tensile strength due to cohesion. Therefore some of the inputs for material model of the soil were adjusted according to the experimental data. The modeling of the air and moisture pore pressure was not attempted in this work.

A finite element model of the mine imitator was developed and executed by LS-DYNA. The numerical results and predictions were correlated with experimental test data. The level of agreement is dependent on modeling accuracy of the behavior of the soil.

2. Simulation of mine imitator interaction with soil material

Simulations of the of the mine imitator impact into deformable soil surfaces were performer using explicit code LS-Dyna v.971. [4] Simulations were conducted for a period of 20 ms.

If the interaction with the soft soil will ensure the detonating, then the mine imitator will be treated as reliable. Therefore for the interaction analysis we choose dry loose sand which is as soft soil. The soil was modeled using robust soil material model *MAT _ SOIL _ AND _ FOAM FAILURE (Mat 14) by LS-DYNA [3]. The Mat 14 model was chosen for the analysis because of its simpli-city. As the Mat 14 model is more fluid-like under many conditions, it is ideal for a soft soil. In the Mat 14 material model, the yield surface, i.e. strength of the soil, increases with larger confining pressures. In addition, the Mat 14 model has a shear failure surface that is pressure dependent, which is a basic property of geo-materials, and allows for a separate unloading bulk modulus. The shear failure criteria in Mat 14 has a pressure dependent failure strength of the form [a.sub.0] + [a.sub.1]p + [a.sub.2][p.sup.2] where the a's are coefficients determined from the experimental test and "p" is the mean stress. If the yield is low, the Mat 14 model gives fluid-like behavior. The behavior and post impact velocity of the mine imitator highly depends on soil material model constants [6]. Initial data for Mat 14 was taken from the series of uniaxial compression tests of dry loose sand material in the laboratory. The tests were conducted using the universal hydraulic 50 t tension-compression testing machine, which applied the axial load through the flat end plate. The soil in the tube of 200 mm diameter was compressed with the flat circular plate without any radial strain. From the uniaxial compression tests we obtained pressure versus natural (logarithmic) volumetric strain (Fig. 1) for input into the Mat 14 model.

[FIGURE 1 OMITTED]

Some of the material constants were adjusted comparing simulations results with the experimental data from the polygon. Simplified FE model of the rigid mine imitator impacting into the soft soil material with the initial velocities (35, 45, 52 and 57 m/s) was created for fast simulation of the interaction process (Fig. 2, a).

[FIGURE 2 OMITTED]

The material model of the dry loose sand was validated comparing the depth of resulting penetration of the mine imitator. The final material constants of the soil material for further analysis of the interaction between the cap of mine imitator and dry loose sand are given in Table [5]. A picture of the finite element model of the mine imitator with deformable cap impacting into the soft soil is shown in Fig. 2, b. Two contact keywords *CONTACT _ _AUTOMATIC _ NODES _ TO _ SURFACE and *CONTACT _ ERODING _ NODES _ TO _ SURFACE were used to perform impact simulations of interaction between the body of mine imitator and the shell and between the shell and soil material. Initially, nominal values of contact friction coefficient [mu] = 0.15 and [mu] = 0.4 respectively were assigned to these contact pairs. The sand was modeled using solid elements with material model Mat 14 which has the input data presented in Table. Body of the mine imitator and stud was modeled using rigid undeformable solid elements with the densities of steel to evaluate inertia properties of real imitator. Function of the stud is to initiate blast at its contact with the detonator's capsule. Therefore the main measured parameters are displacement and velocity of the contact surface of the stud and the capsule. To obtain the sufficient displacements of the stud, the cap should deform plastically. Geometrical model of the cap is divided into 3 parts of different thickness and shell elements are used for its modeling. The cap is made from aluminum alloy and the material model *MAT_PLASTIC_KINEMATIC is used to describe the material properties.[[sigma].sub.y] = 240 MPa, [E.sub.t] = 1050 MPa.

The changes of contact axial forces and absorbed energy by the cap according to the sand penetration depth are presented in Figs. 3 and 4. For the analysis data the contact axial forces was run through an SAE class 300 low-pass filter.

[FIGURE 3 OMITTED]

[FIGURE 4 OMITTED]

The contact force acting the cap reaches the maximum value at the beginning of the penetration in to the soil material. The FE simulations show that in case of soft sand soil and impact velocity v = 35 m/s, the reliability of mine imitator is on the limit to initiate explosion or not. The curve of absorbed energy (Fig. 4) shows that the cap deforms just in the first 2.0--2.5 mm of penetration. This is also seen from the cap deformations presented in Fig. 5, b comparing to the initial form (Fig. 5, a). Residual impact energy (about 99% at v = 45 m/s) is absorbed only by deformations of the soil material (Fig. 6, b).

Using explicit FE code the calculation time increases to infinity when velocity of the system decreases to zero. Therefore the calculations were stopped at the velocity of about 2.5 m/s.

[FIGURE 5 OMITTED]

[FIGURE 6 OMITTED]

Comparing the structural behaviors of mine imitator it was estimated that the deformations of the caps at all analyzed velocities were similar. In all cases the cap deforms similarly and different just final penetration depth of the soil.

3. Deformation of the soil and the cap at different firing angles

The soil deforms under the effect of load due to mine imitator or different factors of mechanical and physical nature deforms; the imitator penetrates the soil much and unevenly thus creating specific conditions for penetration into the soil. As such very weak compression soils, light sands and bulk soils are considered.

The main factors effecting structure of the soil, causing their significant deformations and reduction of strength, may be different. This is the load of mine imitator, mechanical factors--the destruction of natural structure, various dynamic effects on the mine imitator and physical factors--soil moisture and dryness. You can see penetration depth into the soil at different firing angles (45[degrees], 60[degrees], 80[degrees]) of the mine imitator and soil deformation different firing angles of the mine imitator in Fig. 7.

[FIGURE 7 OMITTED]

4. Experimental tests

The detonator should initiate the mine imitator's explosion when it hits any type of the soil. For this purpose the investigation of the detonator's cap of the mine imitator interaction with the two types of soil (dry loose sand and grass) were performed (Fig. 8).

Experimental results of the compression test of detonator cap into the soil material are presented in Fig. 8.

During tests it was revealed that for reliable initiation of the detonator its cap structure should be weakened by increasing depth of the cuts. (Fig. 9, b).

Experimental field tests of the developed training facilities were performed. For this purpose a batch of 100 test imitators was manufactured. Imitators of the batch were tested simulating all firing charges and all firing angles -45[degrees], 60[degrees], 80[degrees]. There were at all no non performance cases during the tests.

[FIGURE 8 OMITTED]

[FIGURE 9 OMITTED]

For test simulation the cap views of the mine imitator after initiation when firing with initial speed v = 45 m/s at 45[degrees], 60[degrees], 80[degrees] firing angles are shown (Fig. 10).

[FIGURE 10 OMITTED]

In Fig. 11 it is seen how experimental results differ from the theoretical results. Experimental studies have been performed at polygon, and the theoretical using LS-DYNA software.

[FIGURE 11 OMITTED]

Comparing the experimental results with the theoretical ones, the depths of penetration of the mine imitator into the soil practically coincide. This shows that the reliable construction of the detonator cap was chosen, which ensures the imitator's initiation at different soils.

5. Conclusions

The FEA shows that with all impact velocities the cap deforms similarly and differs just final penetration depth.

Changes of the cap absorbed energy versus penetration depth shows that the cap deforms just in the first 2.0 mm of the penetration. Residual impact energy (about 99% at v = 35 m/s) is absorbed only by deformations of the soil material.

The contact force acting the cap reaches the maximum value at the beginning of the penetration into the soil material. Comparing the acting forces obtained from FEA and experiments we see that in case of soft sand and impact velocity v = 35 m/s, the reliability of mine imitator is on the limit to initiate explosion or not.

Received February 03, 2009

Accepted April 03, 2009

References

[1.] Fedaravicius, A., Jonevicius, V., Ragulskis, M. Development of mortar training equipment with shell-in-shell system. -75th Shock and Vibration Symposium. SAVIAC, Abstracts. October 17-22, 2004, Virginia Beach, Virginia, p.70-71.

[2.] Fedaravicius, A., Ragulskis, M. K., Klimavicius, Z. Computational support of the development of a mortar Simulator with resuable shells. -WIT Transactions on Modelling and Simulation: Computational Ballistics II. Southampton: WIT Press. ISBN 1-84564-015-2. p.381-389.

[3.] Isenberg, J., Vaughan, D.K, Sandler, I.S. Nonlinear Soil-Structure Interaction. Electric Power Research Institute report EPRI NP-945.-Weidlinger Associates, 1978.-189p.

[4.] Hallquist, John O. LS-DYNA Theory Manual. Liver more Software Technology Corp., March 2006.

[5.] Ravikiran Chikatamarla, Stephan Gruber Optimisation of Cushion Materials for Rockfall Protection Galleries, "vdf Hochschulverlag AG", 2007.-267p.

[6.] Tretjekovas, J., Kacianauskas, R., Simkevicius, C. FE simulation of rupture of diaphragm with initiated defect. -Mechanika. -Kaunas: Technologija, 2006, Nr.6(62), p.5-10.

A. Fedaravicius *, P. Saulys **, P. Griskevicius ***

* Kaunas University of Technology, Kestucio 27, 44312 Kaunas, Lithuania, E-mail: algimantas.fedaravicius@ktu.lt

** Kaunas University of Technology, Kestucio 27, 44312 Kaunas, Lithuania, E-mail: povilas.saulys@stud.ktu.lt

*** Kaunas University of Technology, Kestucio 27, 44312 Kaunas, Lithuania, E-mail: paulius.griskevicius@ktu.lt
Table

Mat 14 Input for Soft Soil in LS-DYNA

Density               Shear     Bulk Unloading
                      Modulus   Modulus

[rho], kg/[m.sup.3]   G, MPa    K, MPa
1700                  1.84      69.0

Density               Yield Surface
                      coeff.

[rho], kg/[m.sup.3]   [[alpha].sub.0], [Mpa.sup.2]
1700                  0

Density               Yield Surface          Yield Surface
                      coeff.                 coeff.

[rho], kg/[m.sup.3]   [[alpha].sub.1], MPa   [[alpha].sub.2]], -
1700                  0                      0.3

Density               Pressure   Crushing      Reference
                      Cutoff     option        Geometry

[rho], kg/[m.sup.3]   MPa        VCR           REF
1700                  -50        0 (default)   0 (default)
COPYRIGHT 2009 Kauno Technologijos Universitetas
No portion of this article can be reproduced without the express written permission from the copyright holder.
Copyright 2009 Gale, Cengage Learning. All rights reserved.

Article Details
Printer friendly Cite/link Email Feedback
Author:Fedaravicius, A.; Saulys, P.; Griskevicius, P.
Publication:Mechanika
Article Type:Report
Geographic Code:4EXLT
Date:Mar 1, 2009
Words:2079
Previous Article:Mechanics of initial dot contact/Pirminio taskinio kontakto mechanika.
Next Article:The effects of water aging on the mechanical properties of glass-fiber and kevlar-fiber epoxy composite materials/Sendinimo vandenyje itaka stiklo ir...
Topics:

Terms of use | Copyright © 2018 Farlex, Inc. | Feedback | For webmasters