By R. A. Graham (auth.), Lee Davison, Y. Horie, Mohsen Shahinpoor (eds.)
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Extra info for High-Pressure Shock Compression of Solids IV: Response of Highly Porous Solids to Shock Loading
Setchell, in Shock Compression of Condensed Matter-1991 (eds. C. Schmidt, RD. W. G. Tasker), North-Holland, Amsterdam, pp. 883-886 (1992). M. Baer, private communication (1995). U. Anderson, RA. T. Holman, in High-Pressure Science and Technology-1993 (eds. C. W. A. Samara, and M. Ross), American Institute of Physics, New York, pp. 1111-1114 (1994). H. Holt, W. U. T. A. Graham, in Shock Waves in Condensed Matter-1995, (eds. C. C. Tao), American Institute of Physics, New York (1996). A. Sheffield, RL.
1. A. L. D. , fluids-and stresses apply to materials with strength. Since porous REs have some strength, it would be more appropriate to use stress rather than pressure, particularly at the low input stresses where strength effects are important. The energy deposited by a wave passing through a material is determined by the area, E = P I!. V / 2, below the Rayleigh line. ) Compared with a solid, the energy deposited in a distended material is larger simply because the initial specific volume is larger and, thus, the volume change is greater.
Then the number of particles contained in a wave may turn out to be the same whether the particles are large or small. We are studying this at the present time. In order to decouple the effect of reaction on the rise times, sugar (sucrose) was chosen as a simulant for the HMX. As indicated earlier, the coarse HMX has the appearance of sugar, so it seemed natural to pick this material to simulate it. In fact, granulated sugar was used to simulate the coarse HMX and powdered or confectioners' sugar (known to have about 3 % corn starch in it to keep it from agglomerating) was used to simulate the fine HMX.