1979
DOI: 10.1029/jb084ib09p04592
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Plane shock wave studies of porous geologic media

Abstract: Plane shock wave experiments have been conducted on two highly porous rocks, Mount Helen tuff and Indiana limestone, in both dry and water-saturated states up to stress levels of about 4 GPa. A light-gas gun was used to load the sample in uniaxial strain, and the subsequent wave motion was monitored with particle-velocity gages. All four materials studied show evidence of time-dependent behavior. The timedependent behavior in the highly porous dry rocks is associated with the closing of pores. The strong time … Show more

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Cited by 69 publications
(18 citation statements)
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“…We speculate that this penetration equation will be reasonably accurate for larger scale projectiles, but data from much more expensive field tests must be obtained to confirm our speculation. (Ortiz, 1966;Carnacho and Ortiz, 1997 (Fossum, Senseny, Pfeifle, and Mellegard, 1995), (2) split Hopkinson bar experiments (Green and Perkins, 1968;Lindholm, Yeakley, and Nagy, 1974;and Lipkin, Grady, and Campbell, 1977), (3) plane shock wave studies (Larson and Anderson, 1979), (4) dynamic tensile failure with planar-impact techniques (Grady and Hollenbach, 1979;Ahrens and Rubin, 1993), and (5) compression-shear loading with plate impact experiments (Aidun and Gupta, 1995). Data from other experimental techniques may also be required for a careful target analysis.…”
Section: Introductionmentioning
confidence: 99%
“…We speculate that this penetration equation will be reasonably accurate for larger scale projectiles, but data from much more expensive field tests must be obtained to confirm our speculation. (Ortiz, 1966;Carnacho and Ortiz, 1997 (Fossum, Senseny, Pfeifle, and Mellegard, 1995), (2) split Hopkinson bar experiments (Green and Perkins, 1968;Lindholm, Yeakley, and Nagy, 1974;and Lipkin, Grady, and Campbell, 1977), (3) plane shock wave studies (Larson and Anderson, 1979), (4) dynamic tensile failure with planar-impact techniques (Grady and Hollenbach, 1979;Ahrens and Rubin, 1993), and (5) compression-shear loading with plate impact experiments (Aidun and Gupta, 1995). Data from other experimental techniques may also be required for a careful target analysis.…”
Section: Introductionmentioning
confidence: 99%
“…As a validation test, all of the parameters determined to this point (see Table 1) are used to predict the plate-slap, plane shock-wave experiments of Larson and Anderson [13] on Salem Limestone that provide uniaxial-strain data at extremely high strain rates on the order of 10 5 -10 7 s -1 . Figure 13 shows the results for uniaxial strain simulations made at strain rates of 10 5 , 10 6 , 10 7 , and 10 -5 s -1 (the experimental quasi-static uniaxial-strain results conducted at 10 -5 s -1 are included for comparison).…”
Section: Dynamic Resultsmentioning
confidence: 99%
“…The particle velocity experimental design is similar to those of Grady et al [1974], Larson and Anderson [1979], and Kondo et al [1980] and makes use of electromagnetic particle velocity gauges [Dremin and Shvedov, 1974].…”
Section: Experimental Methodsmentioning
confidence: 99%
“…Similar experiments were conducted on polycrystalline quartz and perthitic feldspar by Grady et al [1975] and Grady and Murri [1976], who used manganin stress gauges to determine Hugoniot sound velocities and found that these rocks lose shear strength when shocked to pressures above 20 GPa. Larson and Anderson [1979] used particle velocity gauges to study limestone and tuff at lower stress levels (4 GPa) and attributed the observed time-dependent behavior to the closing of pores in these rocks.…”
Section: Introductionmentioning
confidence: 99%