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      KCI등재

      고에너지 물질의 핫 스팟 기반 충격파-폭굉 천이 현상에 대한멀티스케일 해석. Part B: 핫 스팟 기반 멀티스케일 해석 = A Hot Spot Based Shock to Detonation Transition Simulation using Multi-Scale Approach Part B: Hot Spot Based Multi-Scale Simulation

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      https://www.riss.kr/link?id=A105962306

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      다국어 초록 (Multilingual Abstract)

      The hot spot is approximated by the region of high pressure accumulation due to multiple shock reverberations within the polymer binder, surrounded by the bulk of explosive. The meso-scale Smoothed Particle Hydrodynamic (SPH) simulation is adopted to first identify the peak temperatures within the hot spots. These peak temperatures obtained from mesoscale level are then used to initialize the random sites of heat release prior to carrying out the full scale hydrodynamic simulation of shock-to-detonation transition (SDT). For validation of the simulation, a rate stick of 18-mm in radius is experimentally tested. The comparison showed that detonation properties of the explosive are well characterized, and further no-go was witnessed if no mesoscale hot spot model is considered into the hydrodynamic simulation. Thus, the SDT process can be well described by the present model based on the multi-scale hot spot initiation.
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      The hot spot is approximated by the region of high pressure accumulation due to multiple shock reverberations within the polymer binder, surrounded by the bulk of explosive. The meso-scale Smoothed Particle Hydrodynamic (SPH) simulation is adopted to ...

      The hot spot is approximated by the region of high pressure accumulation due to multiple shock reverberations within the polymer binder, surrounded by the bulk of explosive. The meso-scale Smoothed Particle Hydrodynamic (SPH) simulation is adopted to first identify the peak temperatures within the hot spots. These peak temperatures obtained from mesoscale level are then used to initialize the random sites of heat release prior to carrying out the full scale hydrodynamic simulation of shock-to-detonation transition (SDT). For validation of the simulation, a rate stick of 18-mm in radius is experimentally tested. The comparison showed that detonation properties of the explosive are well characterized, and further no-go was witnessed if no mesoscale hot spot model is considered into the hydrodynamic simulation. Thus, the SDT process can be well described by the present model based on the multi-scale hot spot initiation.

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      참고문헌 (Reference)

      1 R. Menikoff, "The SURF Model and the Curvature Effect for PBX 9502, Combust" 16 : 1140-1169, 2012

      2 C.A. Handley, "The CREST Reactive Burn Model" 955 : 373-376, 2007

      3 J.N. Johnson, "Shock-Wave Initiation of Heterogeneous Reactive Solids" 57 : 4323-4334, 1985

      4 E.L. Lee, "Phenomenological Model of Shock Initiation in Heterogeneous Explosives" 23 : 2362-2372, 1980

      5 M. Akiki, "Mechanistic Approach for Simulating of Hot-Spot Formations and Detonation in Polymer-Bonded Explosives" 55 : 585-598, 2017

      6 R. Menikoff, "JWL Equation of Sate" Los Alamos National Laboratory 2015

      7 J. Fang, "Improved SPH Methods for Simulating Free Surface Flows of Viscous Fluids" 59 : 251-271, 2009

      8 A.E.D.M. van der Heijden, "Crystallization and Characterization of RDX, HMX, and CL-20" 4 : 999-1007, 2004

      9 L.E. Fried, "Cheetah 2.0 User’s Manual, Lawrence Livermore National Laboratory"

      10 B. Kim, "Analysis on Shock Attenuation in Gap Test Configuration for Characterizing Energetic Materials" 119 : 145902-, 2016

      1 R. Menikoff, "The SURF Model and the Curvature Effect for PBX 9502, Combust" 16 : 1140-1169, 2012

      2 C.A. Handley, "The CREST Reactive Burn Model" 955 : 373-376, 2007

      3 J.N. Johnson, "Shock-Wave Initiation of Heterogeneous Reactive Solids" 57 : 4323-4334, 1985

      4 E.L. Lee, "Phenomenological Model of Shock Initiation in Heterogeneous Explosives" 23 : 2362-2372, 1980

      5 M. Akiki, "Mechanistic Approach for Simulating of Hot-Spot Formations and Detonation in Polymer-Bonded Explosives" 55 : 585-598, 2017

      6 R. Menikoff, "JWL Equation of Sate" Los Alamos National Laboratory 2015

      7 J. Fang, "Improved SPH Methods for Simulating Free Surface Flows of Viscous Fluids" 59 : 251-271, 2009

      8 A.E.D.M. van der Heijden, "Crystallization and Characterization of RDX, HMX, and CL-20" 4 : 999-1007, 2004

      9 L.E. Fried, "Cheetah 2.0 User’s Manual, Lawrence Livermore National Laboratory"

      10 B. Kim, "Analysis on Shock Attenuation in Gap Test Configuration for Characterizing Energetic Materials" 119 : 145902-, 2016

      11 C.A. Handley, "A Two-Temperature Model for Shocked Porous Explosive" 1793 : 120025-, 2017

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      학술지 이력

      학술지 이력
      연월일 이력구분 이력상세 등재구분
      2022 평가예정 재인증평가 신청대상 (재인증)
      2019-01-01 평가 등재학술지 유지 (계속평가) KCI등재
      2016-01-01 평가 등재학술지 유지 (계속평가) KCI등재
      2012-01-01 평가 등재학술지 유지 (등재유지) KCI등재
      2009-01-01 평가 등재학술지 선정 (등재후보2차) KCI등재
      2008-01-01 평가 등재후보 1차 PASS (등재후보1차) KCI등재후보
      2007-01-01 평가 등재후보 1차 FAIL (등재후보1차) KCI등재후보
      2005-01-01 평가 등재후보학술지 선정 (신규평가) KCI등재후보
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      학술지 인용정보

      학술지 인용정보
      기준연도 WOS-KCI 통합IF(2년) KCIF(2년) KCIF(3년)
      2016 0.31 0.31 0.29
      KCIF(4년) KCIF(5년) 중심성지수(3년) 즉시성지수
      0.27 0.25 0.632 0.05
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