By Jeffrey Swab
The Armor Ceramics Symposium presents an annual discussion board for the presentation and dialogue of unclassified info and ideas bearing on the advance and incorporation of ceramic fabrics for armor functions. This selection of articles from the 7th variation of this symposium serious about influence, Penetration and fabric Modeling, fabric innovations, techniques and Characterization, the appliance of NDE, and obvious Armor.
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Extra resources for Advances in Ceramic Armor V (Ceramic Engineering and Science Proceedings) , 1st Edition
Along y and z directions the periodic boundary conditions were imposed. The sample was initially kept at constant temperature T=2 K during 1 ps to eliminate thermal fluctuations in propagation of shock wave. To obtain the shock wave an external force in the x direction was applied to two planes of atoms on one side of the sample. The force was kept constant throughout the simulation. RESULTS A simulation of propagation of shock wave was carried out at the followings intensities of loading: 5, 10, 20, 40, 60, 80, 100, 120, 140, 150, 160, 180, 200, 220, 260, 300, 340 and 380 GPa.
There are several constitutive equations of different complexity for such materials [4-71. We use the following constitutive equations for a material with porosity 8, yield stress of solid phase Y,at uniaxial compression, and porosity functions cp and y [4-71: where T = m l o , - oq/ ;p = (o,+20T)/3. First equation (14) is a condition of plasticity of porous body (in a space of variables lp I - T it defines flow ellipsis), second equation (14) is an associative flow law. Porosity functions cp and y~ are obtained both experimentally and theoretically [4-71.
L. E. J.