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Molecular dynamics simulations of melting of perfect crystalline hexahydro-1,3,5-trinitro-1,3,5-s-triazine

机译:完美结晶六氢-1,3,5-三硝基-1,3,5-s-三嗪熔融的分子动力学模拟

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The melting mechanism of superheated perfect crystalline hexahydro-l,3,5-trinitro-l,3,5-s-triazine(alpha-RDX)has been investigated using molecular dynamics simulations with the fully flexible force field developed by Smith and Bharadwaj [J.Phys.Chem.B 103,3570(1999)].Sequential 50 ps equilibration simulations of the constant stress-constant temperature ensemble were performed at 10 K intervals over the range of 300-650 K,corresponding to a heating rate of 2.0 X 10~(11)K/s.A solid-solid phase transition is observed between 480 and 490 K,followed by melting,which occurs between 500 and 510 K.The solid-solid phase transition,both displacive and rotational,is characterized by an abrupt decrease in the lengths of the unit cell edges a and b and an increase of the length of edge c.The molecular conformation in the new phase is AAE,although the axial nitro groups have different changes:one shift is more axial and the other is more equatorial.Phases other than alpha-RDX have been observed experimentally,however,there are insufficient data for comparisons to ascertain that the new phase observed here corresponds to a real phase.At the high heating rate(2.0 X 10~(11)K/s)used in the simulations,the melted RDX reaches full orientational disorder at about 540 K and translational freedom at around 580 K.If the simulation at the melting temperature(510 K)is run sufficiently long complete rotational freedom is achieved in a few hundreds of picoseconds,while complete translational freedom requires much longer.These results show that given a sufficiently high heating rate,the system can exist for significant periods of time in a near-liquid state in which the molecules are not as free to rotate and diffuse as in the true liquid state.The bond lengths and bond angles undergo little change upon melting,while there are significant changes in the dihedral angles.The molecular conformation of RDX changes from AAE to EEE upon melting.The ramification of this for formulating force fields that accurately describe melting is that it is important that the torsional motions are accurately described.
机译:Smith和Bharadwaj利用分子动力学模拟研究了完全结晶的六氢-l,3,5-三硝基-l,3,5-s-三嗪(α-RDX)的熔融机理。 J.Phys.Chem.B 103,3570(1999)]。在300-650 K的范围内,以10 K的间隔进行了恒定应力-恒定温度集合的顺序50 ps平衡模拟,对应于加热速率2.0 X 10〜(11)K / s在480 K至490 K之间观察到固-固相变,随后发生熔化,发生在500至510 K之间。在新相中的分子构象是AAE,尽管轴向的硝基有不同的变化:一个位移更轴向,另一个位移另一个轴向上的单位构象是AAE。更赤道。已观察到除alpha-RDX以外的相位然而,根本上没有足够的数据用于比较,无法确定此处观察到的新相对应于真实相。在模拟中使用的高加热速率(2.0 X 10〜(11)K / s)下,RDX熔化达到如果在540 K左右的熔融温度下运行足够长的时间,则完全旋转方向的自由度将在数百皮秒内达到,而完全平移的自由度则需要更长的时间。这些结果表明,在足够高的加热速率下,该系统可以在接近液态的状态下存在相当长的一段时间,在这种状态下,分子没有像真正的液态状态那样自由旋转和扩散。角在熔化时几乎没有变化,而二面角却有很大变化。RDX的分子构象在熔化时从AAE变为EEE。准确地描述融化是重要的,准确描述扭转运动。

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