| OCR Text |
Show 26 attenuated until the intensity plastic flow of plexiglas, free surface the terminal shock as a but sufficient The purpose qf the steel 0 pressure as shown in Figure 15 reles,e a are plexiglas adjacentl plate 'which covered reflect the inttia1. to was one;""half contrasted to the free surface reflecting as wave produce spalling of the to plexiglas block surface of the the initial shock The reduced below that necessary for was tension or The results also wave!' in qualitative 'Agreement with e.quati.on' (8b) to the free surface while the high spalled, I 0 impedance plate prevented spalling. ';rhe reflected graphs while the re1Fase front appear s dark corresponding than the background which r ef'Lec red causes it to the on original photo pressure front is aPl>ear lighter ahead of the be to ... release front. The effec t of the nar-row air gap at the solid solid interface ... - 'ox Figure '14 prompted a transmitting medium It intima,te1y sandwiched between study was to observe the effect of thickness of decided that pl.exf g Las oQse,rv'ation of the shock behavior j, A a highly mismatched impe4anc blocks would allow diagram of a photographic typical "sandwich" chage is shown .in ,Figure 16.1' 3" x'l" plexiglas (sq) Brass Figure 16: a plate 3" (sq) U' (d) X X 2" plexiglas 2" pentolite of components to observe shock behavior v thi,ckness of mismatched impedance, Arrangement p; |