2012
DOI: 10.1016/j.jmgm.2012.06.013
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New statistical boundary conditions for argon–tungsten interactions

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Cited by 5 publications
(2 citation statements)
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“…The integration of the equation of motion was carried out using a second order velocity Verlet scheme, and the time step in numerical calculation was 10 −16 s. For numerical simulation, a parallel algorithm was developed and software implemented, allowing calculations using NVIDIA general-purpose graphic processors (GPUs) supporting the CUDA (Compute Unified Device Architecture) technology [15][16][17].…”
Section: Methodology and Physical Systemmentioning
confidence: 99%
“…The integration of the equation of motion was carried out using a second order velocity Verlet scheme, and the time step in numerical calculation was 10 −16 s. For numerical simulation, a parallel algorithm was developed and software implemented, allowing calculations using NVIDIA general-purpose graphic processors (GPUs) supporting the CUDA (Compute Unified Device Architecture) technology [15][16][17].…”
Section: Methodology and Physical Systemmentioning
confidence: 99%
“…曹 炳 阳 [22] 将MD方法应用到了微尺度气体的模拟中, 并指 出气体分子在固体表面附近的"俘获-逃逸"行为导 致了氩分子在光滑铂表面上切向动量系数(TMAC) 随温度的变化呈现指数衰减的关系. Finger等 [23] 利用MD方法研究了在气体-表面相互作用过程 中, 气体分子的入射速度、晶体结构、分子间作用 力和吸附层对气体分子散射和切向动量的影响. 此 外, 他们还根据气体分子与壁面的碰撞次数和反射 速度方向对气体分子的散射方式进行了分类, 分析 了不同散射类型对气体分子切向动量变化的影响.…”
Section: Md方法被越来越多的学者应用到稀薄流动和气unclassified