Abstract

We studied the collapse of individual helium gas bubbles in the homogeneous explosive nitromethane (NM) to investigate effects of hot-spot formation on the detonation process. A bubble was injected into a NM sample, and a shock wave from an explosive detonator compressed the bubble, creating a localized hot spot. We measured shock and detonation wave speeds with optical velocimetry, and we used a high-speed camera to image the shock propagation and the pre- and post-bubble collapse processes. An infrared camera image showed the residual radiance temperature distribution after the bubble collapse, and an optical fiber pyrometer measured the time-resolved thermal radiance. We measured the optical spectra of light emitted from detonating NM without a bubble and from a collapsing bubble in shocked, undetonated NM. We estimated temperatures of the detonation fronts and of the hot spots formed by bubble collapse. To study the incipient detonation process, we performed all bubble collapse experiments at pressures below the threshold for creating a sustained detonation. Where the bubble collapsed, we observed an opaque, thermally emissive region believed to be chemical reaction products. Chemical reactions in NM can be produced with lower shock pressures (∼1 GPa) when a helium bubble is present than without a bubble (∼10 GPa). We used hydrodynamic modeling to predict shock wave propagation, extent of chemical reaction, and subsequent temperature rise from the collapsing bubble. Simulations using a temperature-dependent Arrhenius burn model gave much better results than reactive burn models that depend only on pressure and density.

Highlights

  • In the shock initiation of high explosives (HE) to detonation, chemical reactions are initiated following shock compression of the unreacted explosive

  • We studied the collapse of individual helium gas bubbles in the homogeneous explosive nitromethane (NM) to investigate effects of hotspot formation on the detonation process

  • In homogeneous HE, initiation occurs via a thermal explosion mechanism that arises from bulk shock heating due to shock wave compression

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Summary

INTRODUCTION

In the shock initiation of high explosives (HE) to detonation, chemical reactions are initiated following shock compression of the unreacted explosive. Experiments involving adding inhomogeneities to study the effects of small impurities and voids[9–11] were quantified in the more recent work of Dattelbaum et al.[6] They loaded solid and hollow glass microspheres into gelled liquid explosive nitromethane (NM) and shocked the samples with impactors from a two-stage, large-bore gas gun. The bulk properties such as pressure, density, and run-to-detonation distance demonstrated an increase in explosive sensitivity with hollow spheres vs solid microspheres and illustrated a switch-over from a hot-spot-driven mechanism to a thermal explosion mechanism with subcritical hot-spot seed densities. In addition to determining these signatures, we expect the experimental findings in this study will assist the modeling community in refining their simulations of void collapse and help guide future experimental studies of void collapse in explosives

EXPERIMENTAL SETUP AND OPERATION
EXPERIMENTAL RESULTS
Shock wave with no bubble
Detonations with no bubble
Bubble collapse experiments without detonations
Time sequence of images of NM detonation
Images of bubble collapse in shock-compressed NM
Bubble collapse imaging with varying input shock pressures
IR camera results
Spectral emission
Shocked NM
Detonation from shock
Bubble collapse experiments
MODELING
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