NUMERICAL-SIMULATION OF THE PROPAGATION OF SHOCK-WAVES IN COMPRESSIBLE OPEN-CELL POROUS FOAMS

Citation
M. Olim et al., NUMERICAL-SIMULATION OF THE PROPAGATION OF SHOCK-WAVES IN COMPRESSIBLE OPEN-CELL POROUS FOAMS, International journal of multiphase flow, 20(3), 1994, pp. 557-568
Citations number
17
Categorie Soggetti
Mechanics
ISSN journal
03019322
Volume
20
Issue
3
Year of publication
1994
Pages
557 - 568
Database
ISI
SICI code
0301-9322(1994)20:3<557:NOTPOS>2.0.ZU;2-U
Abstract
A numerical model for the simulation of the interaction of weak shock waves with open-cell compressible porous foams is developed. It is ass umed that the foam is infinitely weak and that its volume fraction, wh ich was 0.05 in the cases studied herein, is relevant only when the in teraction between the gaseous and the solid phases is considered. The gas is assumed to be inviscid and thermally nonconductive, except for the viscous drag interaction and the heat transfer between the two pha ses. It is also assumed that the heat transfer between the two phases is extremely efficient, i.e. that the heat transfer coefficient is inf initely large. The range of incident shock wave Mach numbers investiga ted herein is between 1.08 and 1.40, and the range of foam densities i s between 14.8 and 57.4 kg/m3. The numerical results are in very good agreement with experimentally obtained pressure histories and foam par ticle paths when the incident shock wave Mach numbers are between 1.25 and 1.40 (weak shocks). The agreement between experimentally and nume rically obtained pressure histories is poor when the incident shock wa ve Mach numbers are between 1.08 and 1.18 (very weak shocks). The resu lts of the study indicate that when weak shocks interact with open-cel l compressible foam, the transfer of momentum between the gaseous and the solid phases is of paramount importance. On the other hand, if the shocks are very weak, then the elasticity of the foam is an important parameter as well. It is therefore suggested that, while yielding ver y good results for weak shocks, the assumption of infinitely weak foam is inadequate for very weak shocks.