397 - 407 |
Reactive not Proactive: Explosive Identification Taggant History and Introduction of the Nuclear Barcode Taggant Model Seman J, Giraldo CHC, Johnson CE |
408 - 412 |
The Detonation Properties Research on TKX-50 in High Explosives Xing XL, Zhao SX, Wang XF, Zhang WP, Diao XQ, Fang W, Li WX |
413 - 422 |
Effect of Sodium Alginate on the Morphology and Properties of High Energy Insensitive Explosive TKX-50 Dong WB, Chen SS, Jin SH, Chen ML, Yan B, Chen Y |
423 - 428 |
Initiation and Overdriven Detonation of High Explosives Using Multipoint Initiation Guo JF, Zeng QX, Qin GS, Li MY |
429 - 437 |
The Effect of HMX Impurity and Irganox Antioxidant on Thermal Decomposition Kinetics of RDX by TG/DSC Non-Isothermal Method Sinapour H, Damiri S, Ravanbod M, Pouretedal HR |
438 - 446 |
Thermal Decomposition Enhancement of HMX by Bonding with TiO2 Nanoparticles Zhu Q, Xiao C, Xie X, Zheng BH, Li SB, Luo G |
447 - 454 |
X-ray Phase Contrast Imaging of the Impact of a Single HMX Particle in a Polymeric Matrix Kerschen NE, Sorensen CJ, Guo ZR, Mares JO, Fezzaa K, Sun T, Son SF, Chen WNW |
455 - 463 |
Sensitivity Prediction of Exploding Foil Initiator Chen QC, Ma T, Li Y |
464 - 471 |
Hydroxide-Based Nanoenergetic Materials Yolchinyan SA, Eads RW, Hobosyan MA, Martirosyan KS |
472 - 483 |
Non-Isothermal Solid Phase Diffusion in Activated Powder Mixtures. Thermal Regimes and Critical Conditions Filimonov VY, Koshelev KB |
484 - 492 |
Vapor Pressure of Linear Nitrate Esters Determined by Transpiration Method in Combination with VO-GC/MS Hartel MAC, Klapotke TM, Stierstorfer J, Zehetner L |
493 - 504 |
Numerical Simulation and Unsteady Combustion Model of AP/HTPB Propellant under Depressurization by Rotation Ye ZW, Yu YG |
505 - 512 |
Barium Titanate: A Novel Perovskite Oxide Burning Rate Modifier for HTPB/AP/Al Based Composite Propellant Formulations Jain S, Khire VH, Kandasubramanian B |
513 - 518 |
Oxidation of Catocene in AP/Catocene Mixture at Low Temperature Jiang BZ, Wang TP |