Yakun Liu
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Yakun Liu has a total of 12 co-authors. Here are the top co-authors by number of shared publications:
- Zhijun Wang
College of Mechanical and Electrical Engineering, North University of China, Taiyuan 030051, China
3 shared publications - Guangjian Bi
Chongqing Hongyu Precision Industry Group Co., Ltd., Chongqing 402760, China
2 shared publications - Jianping Yin
School of Mechanical and Electrical Engineering, North University of China, Taiyuan 030051, China
2 shared publications - Xuepeng Zhang
College of Mechanical and Electrical Engineering, North University of China, Taiyuan 030051, China
2 shared publications - Chengxiang Shi
Key Laboratory for Green Chemical Technology of Ministry of Education, School of Chemical Engineering and Technology Institute of Molecular Plus School of Energy Tianjin University Tianjin China
1 shared publication - Chi Ma
Key Laboratory for Green Chemical Technology of the Ministry of Education, School of Chemical Engineering and Technology, Tianjin University, Tianjin 300072, China
1 shared publication
Latest Publications
- 19 July 2021
- Published by American Chemical Society (ACS) in Industrial & Engineering Chemistry Research
- Vol. 60 (30) , 10978-10987
Synthesis and Performance of Strained Multicyclic Hydrocarbons as Highly Potential High-Energy-Density Fuels
- 19 July 2021
- Published by American Chemical Society (ACS) in Industrial & Engineering Chemistry Research
- Vol. 60 (30) , 10978-10987
Synthesis and Performance of Strained Multicyclic Hydrocarbons as Highly Potential High-Energy-Density Fuels
- Open Access
Correction: Liu et al. The EFP Formation and Penetration Capability of Double-Layer Shaped Charge with Wave Shaper. Materials 2020, 13, 4519
The authors wish to make the following corrections to this paper
Open AccessCorrection: Liu et al. The EFP Formation and Penetration Capability of Double-Layer Shaped Charge with Wave Shaper. Materials 2020, 13, 4519
The authors wish to make the following corrections to this paper
- Open Access
The EFP Formation and Penetration Capability of Double-Layer Shaped Charge with Wave Shaper
Detonation waves will bypass a wave shaper and propagate in the form of a horn wave in shaped charge. Horn waves can reduce the incidence angle of a detonation wave on a liner surface and collide with each other at the charge axis to form overdriven detonation. Detection electronic components of small-caliber terminal sensitive projectile that are limited by space are often placed inside a wave shaper, which will cause the wave shaper to no longer be uniform and dense, and weaken the ability to adjust detonation waves. In this article, we design a double-layer shaped charge (DLSC) with a high-detonation-velocity explosive in the outer layer and low-detonation-velocity explosive in the inner layer. Numerical and experimental simulation are combined to compare and analyze the forming process and penetration performance of explosively formed projectile (EFP) in DLSC and ordinary shaped charge (OSC). The results show that, compared with OSC, DLSC can also adjust and optimize the shape of the detonation wave when the wave shaper performance is poor. DLSC can obtain long rod EFPs with a large length-diameter ratio, which greatly improves the penetration performance of EFP.
Open AccessThe EFP Formation and Penetration Capability of Double-Layer Shaped Charge with Wave Shaper
Detonation waves will bypass a wave shaper and propagate in the form of a horn wave in shaped charge. Horn waves can reduce the incidence angle of a detonation wave on a liner surface and collide with each other at the charge axis to form overdriven detonation. Detection electronic components of small-caliber terminal sensitive projectile that are limited by space are often placed inside a wave shaper, which will cause the wave shaper to no longer be uniform and dense, and weaken the ability to adjust detonation waves. In this article, we design a double-layer shaped charge (DLSC) with a high-detonation-velocity explosive in the outer layer and low-detonation-velocity explosive in the inner layer. Numerical and experimental simulation are combined to compare and analyze the forming process and penetration performance of explosively formed projectile (EFP) in DLSC and ordinary shaped charge (OSC). The results show that, compared with OSC, DLSC can also adjust and optimize the shape of the detonation wave when the wave shaper performance is poor. DLSC can obtain long rod EFPs with a large length-diameter ratio, which greatly improves the penetration performance of EFP.
- Open Access
- 8 November 2019
- Published by Wiley in Propellants, Explosives, Pyrotechnics
- Vol. 44 (11) , 1499
Inside Back Cover: Study on Overdriven Detonation of Double‐Layer Shaped Charge (Prop., Explos., Pyrotech. 11/2019)
- 8 November 2019
- Published by Wiley in Propellants, Explosives, Pyrotechnics
- Vol. 44 (11) , 1499
Open AccessInside Back Cover: Study on Overdriven Detonation of Double‐Layer Shaped Charge (Prop., Explos., Pyrotech. 11/2019)
- Retracted
- 23 July 2019
- Published by Wiley in Propellants, Explosives, Pyrotechnics
- Vol. 44 (11) , 1410-1422
Study on Overdriven Detonation of Double‐Layer Shaped Charge
Overdriven detonation(ODD) means that the detonation process of explosives no longer follows the C−J detonation process and its detonation parameters are larger than the C−J values. ODD is an unstable detonation process. With the increasing of propagation distance, detonation parameters tend to C−J value gradually. The double‐layer shaped charge (DLSC) with high detonation velocity explosive (HE) in the outer layer and low detonation velocity explosive (LE) in the inner layer can keep the axis of shaped charge in the ODD state all the time. The paper derived formulas for calculating the parameters of overdriven detonation when the HE detonates the LE. Based on the conservation of momentum, mass and energy, the functional relationship between the intensity of Mach wave and the incident angle of the detonation wave in the shaped charge is deduced. Study on the propagation law of detonation waves in DLSC with the wave shaper by numerical simulation. The results show that the peak value of Mach wave pressure in DLSC is not increased compared with that in ordinary shaped charge (OSC), but the attenuation speed of Mach wave pressure can be delayed and ultimately in the ODD state. The final parameters of the ODD state are determined by the detonation velocity and the polytropic exponent of the explosive. The results of numerical simulation are consistent with theoretical calculation, which confirms the accuracy of the formulas.
- 23 July 2019
- Published by Wiley in Propellants, Explosives, Pyrotechnics
- Vol. 44 (11) , 1410-1422
RetractedStudy on Overdriven Detonation of Double‐Layer Shaped Charge
Overdriven detonation(ODD) means that the detonation process of explosives no longer follows the C−J detonation process and its detonation parameters are larger than the C−J values. ODD is an unstable detonation process. With the increasing of propagation distance, detonation parameters tend to C−J value gradually. The double‐layer shaped charge (DLSC) with high detonation velocity explosive (HE) in the outer layer and low detonation velocity explosive (LE) in the inner layer can keep the axis of shaped charge in the ODD state all the time. The paper derived formulas for calculating the parameters of overdriven detonation when the HE detonates the LE. Based on the conservation of momentum, mass and energy, the functional relationship between the intensity of Mach wave and the incident angle of the detonation wave in the shaped charge is deduced. Study on the propagation law of detonation waves in DLSC with the wave shaper by numerical simulation. The results show that the peak value of Mach wave pressure in DLSC is not increased compared with that in ordinary shaped charge (OSC), but the attenuation speed of Mach wave pressure can be delayed and ultimately in the ODD state. The final parameters of the ODD state are determined by the detonation velocity and the polytropic exponent of the explosive. The results of numerical simulation are consistent with theoretical calculation, which confirms the accuracy of the formulas.