新型纳米材料对氢同位素的吸附

Suheyl Polat, Aaron Stinebaugh, Jungkyu Park
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引用次数: 0

摘要

通过分子动力学研究氢同位素的吸附、反射和渗透,探讨了利用各种新型纳米碳控制氢同位素的可能性。纳米碳的纳米尺寸同素异形体彻底改变了碳材料的研究趋势,在许多应用领域开辟了许多令人兴奋的可能性。1985年富勒烯C60被发现后,研究人员开始关注碳纳米材料。1991年碳纳米管的发现和2004年单层石墨烯首次从石墨中分离出来,鼓励了研究人员通过计算和实验来测量这些碳纳米材料的热学、电学和机械性能。在本研究中,我们研究了具有随机结构的石墨烯层和纳米结构碳。REBO和airbo电位与lamps一起用于模拟氚与石墨烯片的相互作用。使用定制的MATLAB代码来创建石墨烯结构,并沿着石墨烯片上方平行的平面随机分布100个氚原子。氚原子被固定在原位,而石墨烯薄片经历了多个阶段的平衡。选择氚原子的速度,以便在一次模拟中入射能量可以为0.1、0.2、0.5、1、2、5、10、20、50、100、200或500 eV。在低入射能量下,反射是主要的相互作用。吸附速率随入射能量的增加而增加,直到能量达到5 eV。5 eV后,吸附速率随入射能量的增加而降低。当入射能量大于5 eV时,吸附速率随石墨烯层数的增加而增加。在低入射能量(< 1 eV)下,由于主要的相互作用来源于π电子的力,因此没有观察到同位素对相互作用的影响。对不同入射角的氚进行了模拟。当氚原子垂直向石墨烯移动(θ = 0°)时,吸附率最高,而当角度最大(θ = 60°)时,吸附率最低,只有少数例外(5 eV和10 eV)。石墨烯对氚的吸附与REBO电位有显著差异。与REBO电位相比,AIREBO电位始终表现出较低的吸附率和较高的反射率。本研究的结果将用于开发新型纳米材料,用于控制氚。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Adsorption of Hydrogen Isotopes on Novel Nanomaterials
We investigated the possibility of using various novel nanostructured carbon for control of hydrogen isotopes by exploring the adsorption, reflection, and penetration of hydrogen isotopes using molecular dynamics. Nanometer sized allotropes of nano-carbons have completely changed the research trend in carbon materials, and opened numerous exciting possibilities in many applications. Researchers started to pay attention to carbon nanomaterials when Fullerene C60 was discovered in 1985. The discovery of carbon nanotubes in 1991 and the first isolation of single layer of graphene from graphite in 2004 have encouraged researchers to measure the exciting thermal, electrical, and mechanical properties of these carbon nanomaterials computationally and experimentally. In the present research, we investigate graphene layers and nanostructured carbons with random configurations. The REBO and AIREBO potential are used alongside LAMMPS to simulate tritium interactions with sheets of graphene. Custom MATLAB codes were used to create the graphene structure as well as randomly distribute 100 tritium atoms along a plane above and parallel to the graphene sheet. The tritium atoms are held in place while the graphene sheets undergo multiple stages of equilibration. The velocities of tritium atoms are selected so that incident energies may be 0.1, 0.2, 0.5, 1, 2, 5, 10, 20, 50, 100, 200, or 500 eV during a single simulation. Reflection is shown to be the dominant interaction at low incident energy. Adsorption rates increase with increasing incident energy until energies reach 5 eV. After 5 eV, adsorption rates decrease as incident energy increases. At incident energies greater than 5 eV, adsorption rates increase with the number of graphene layers. At low incident energies (< 1 eV), no isotopic effects on interactions are observed since the predominant interaction is derived from the force of π electrons. Simulations were performed with different incident angles of tritium. Adsorption rates are always the highest when tritium atoms travel vertically towards graphene (θ = 0°) while they are the lowest when the angle is the largest (θ = 60°) with only a few exceptions (5 eV and 10 eV). AIREBO potential shows a significant difference in adsorption of tritium on graphene from REBO potential. AIREBO potential consistently showed lower adsorption rates and higher reflection rates when compared to REBO potential. The results obtained in this research study will be used to develop novel nanomaterials that can be employed for tritium control.
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