TY - JOUR
T1 - High dynamic range emission measurements of shocked energetic materials
T2 - Octahydro-1,3,5,7-tetranitro-1,3,5,7-tetrazocine (HMX)
AU - Bassett, Will P.
AU - Dlott, Dana D.
N1 - Funding Information:
The research described in this study is based on the work supported by the U.S. Army Research Office under Award No. W911NF-13-1-0217, the U.S. Air Force Office of Scientific Research under Award Nos. FA9550-14-1-0142 and FA9550-16-1-0042, and the Defense Threat Reduction Agency under Award No. HDTRA1-12-1-0011. Will P. Bassett acknowledges support from the Stewardship Sciences Academic Alliance Program from the Carnegie-DOE Alliance Center, under Grant No. DE-NA20002006. We thank Dr. Dan Hooks of Los Alamos National Laboratory for the HMX powder.
Publisher Copyright:
© 2016 Author(s).
PY - 2016/6/14
Y1 - 2016/6/14
N2 - A new emission apparatus with high time resolution and high dynamic range was used to study shock-induced ignition of octahydro-1,3,5,7-tetranitro-1,3,5,7-tetrazocine in the form of ultrafine powder (4 ± 3 μm particle size), over a range of impact velocities (0.8-4.3 km s-1) and impact durations (2.5-16 ns). A graybody model was used to extract graybody emissivities and time-dependent temperatures from a few ns to 100 μs. The emission transients consisted of three parts: a 6700 K nanosecond burst during the shocks, a 4000-4500 K temperature spike near 0.3 μs followed by a ∼3300 K tail extending out to ∼100 μs. These temperatures varied remarkably little with impact velocity and duration, while the emission intensities and emissivities changed by over an order of magnitude. The emissivity changes were interpreted with a hot spot model, where hot spot temperatures reached a maximum of 6700 K and the hot spot volume fractions increased from 5% to 100% as impact velocity increased from 1 to 3 km s-1. Changing shock durations in the 2.5-16 ns range had noticeable effects on the microsecond emission. The 0.3 μs temperature spike was much smaller or absent with 2.5 ns shocks, but prominent with longer durations. An explanation for these effects was put forth that invoked the formation of carbon-rich clusters during the shock. In this view, cluster formation was minimal with 2.5 ns shocks, but longer-duration shocks produced increasingly larger clusters, and the 0.3 μs temperature spikes represented cluster ignition.
AB - A new emission apparatus with high time resolution and high dynamic range was used to study shock-induced ignition of octahydro-1,3,5,7-tetranitro-1,3,5,7-tetrazocine in the form of ultrafine powder (4 ± 3 μm particle size), over a range of impact velocities (0.8-4.3 km s-1) and impact durations (2.5-16 ns). A graybody model was used to extract graybody emissivities and time-dependent temperatures from a few ns to 100 μs. The emission transients consisted of three parts: a 6700 K nanosecond burst during the shocks, a 4000-4500 K temperature spike near 0.3 μs followed by a ∼3300 K tail extending out to ∼100 μs. These temperatures varied remarkably little with impact velocity and duration, while the emission intensities and emissivities changed by over an order of magnitude. The emissivity changes were interpreted with a hot spot model, where hot spot temperatures reached a maximum of 6700 K and the hot spot volume fractions increased from 5% to 100% as impact velocity increased from 1 to 3 km s-1. Changing shock durations in the 2.5-16 ns range had noticeable effects on the microsecond emission. The 0.3 μs temperature spike was much smaller or absent with 2.5 ns shocks, but prominent with longer durations. An explanation for these effects was put forth that invoked the formation of carbon-rich clusters during the shock. In this view, cluster formation was minimal with 2.5 ns shocks, but longer-duration shocks produced increasingly larger clusters, and the 0.3 μs temperature spikes represented cluster ignition.
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U2 - 10.1063/1.4953353
DO - 10.1063/1.4953353
M3 - Article
AN - SCOPUS:84973925414
SN - 0021-8979
VL - 119
JO - Journal of Applied Physics
JF - Journal of Applied Physics
IS - 22
M1 - 225103
ER -