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High-energy-density materials (HEDMs) are widely used in explosives and propellants, but their sensitivity to shock, temperature, and defects remains a critical limitation for both safety and combustion performance. Although previous studies have identified decomposition pathways and developed macroscopic ignition models, the direct link between microscopic-scale defects and reaction kinetics under shock loading remains insufficiently understood. In this work, we develop a multiscale computational framework to determine how molecular vacancies influence the decomposition mechanisms and shock response of 1,3,5-trinitro-1,3,5-triazine (RDX). By combining ab initio molecular dynamics (AIMD) with large-scale reactive molecular dynamics (RMD), we quantitatively assess how molecular vacancies, located in the unit cells surrounding nanoscale void, influence chemical reaction kinetics, hotspot formation, and the coupled thermomechanical response over a broad range of temperatures and shock velocities. AIMD results reveal that vacancy-containing cells undergo significantly accelerated reactions, exhibiting lower activation energies than vacancy-free cells (47.23 kcal·mol -1 vs. 51.14 kcal·mol -1 ). At 1100 K, the characteristic reaction time decreases from 196 ns in vacancy-free cells to 65 ns in vacancy-containing cells. RMD shock simulations reveal a pressure-dependent, dual-mechanism behavior: at lower particle velocities (2.0∼2.5 km·s -1 ) vacancies enhance local thermalization and accelerate hotspot growth, whereas above a critical velocity (3.0 km·s -1 ) shock pressure and pressure-volume ( p - V ) work from void collapse dominate hotspot evolution and mask vacancy effects. Overall, these results provide a quantitative, physics-based framework for predicting ignition thresholds associated with void defects and establish a microscopic foundation for next-generation detonation models. A multiscale AIMD-RMD framework was developed to study how molecular vacancies affect the decomposition and shock response of RDX. Vacancies lower the activation energy from 51.14 to 47.23 kcal·mol -1 and shorten the characteristic reaction time at 1100 K from 196 to 65 ns. Shock simulations show a dual mechanism: at 2.0-2.5 km·s -1 , hotspot growth is dominated by vacancies, while at 3.0-4.0 km·s -1 , shock compression and void-collapse P - V work dominate and mask vacancy effects. These results link defect chemistry with shock-induced hotspot evolution. • A multiscale AIMD-RMD framework is developed for defective RDX under shock. • Vacancies lower the activation energy and strongly accelerate RDX decomposition. • Vacancies dominate hotspots at low velocity, while shock compression dominates at high velocity.
Wei et al. (Fri,) studied this question.