共查询到19条相似文献,搜索用时 93 毫秒
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采用分子动力学方法模拟了纳米金属铝在粒径为0.8-3.2 nm 时的熔点、密度和声子热导率的变化, 研究了粒径为1.6 nm的铝纳米颗粒的密度、比热和声子热导率随温度的变化. 采用原子嵌入势较好地模拟了纳米金属铝的热物性及相变行为, 根据能量-温度曲线和比热容-温度曲线对铝纳米颗粒的相变温度进行了研究, 并利用表面能理论、尺寸效应理论对铝纳米颗粒熔点的变化进行了分析. 随着纳米粒径的不断增大, 铝纳米颗粒的熔点呈递增状态, 当粒径在2.2-3.2 nm时, 熔点的增幅减缓, 但仍处于递增趋势. 随着纳米粒径的增大, 铝纳米颗粒的密度呈单调递减, 热导率则呈线性单调递增, 且热导率的变化情况符合声子理论. 随着温度的升高, 粒径为1.6 nm的铝纳米颗粒的密度、热导率均减小. 该模拟从微观原子角度对纳米材料的热物性进行了研究, 对设计基于铝纳米颗粒的相变材料具有指导意义. 相似文献
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应用非平衡分子动力学方法,对水中超空泡流形成机理及减阻效应进行了模拟研究.计算得到了流体密度分布、局部空化数分布、阻力系数及含气百分比等流场细节数据,结果显示空化数判据在分子层面仍然成立,局部低空化数区域与超空泡形成区域在空间上分离;超空泡形成和稳定主要受物体运动速度影响;空化器构型对空泡内含气率有较大影响;从云雾空化状态过渡到超空泡,物体表面摩擦力可以减小50%—90%.与数值模拟结果的对比表明非平衡分子动力学模拟适用于研究微观超空泡机理,能够经济有效地探讨超高速流体运动的一些自然规律.
关键词:
非平衡分子动力学
超空泡
高速流体
摩擦系数 相似文献
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结合卫星“微型核”的特点,研究电介质薄膜中的导热机理以及薄膜厚度对导热系数的影响.以结构较为简单、具有可靠势能函数,实验数据较为丰富和可靠的氩的(fcc)晶体为模型,采用平衡分子动力学方法(EMD)和各向异性非平衡分子动力学方法(NEMD)计算了氩晶体及其法向薄膜的热导率,并与实验结果进行比较.模拟结果表明,氩晶体纳米薄膜的热导率显著小于对应大体积晶体的实验值,具有明显的尺寸效应.在氩薄膜厚度为2.124—5.310nm的模拟范围内,薄膜的法向热导率随着薄膜厚度的增加而呈近似线性增加.
关键词:
热导率
纳米薄膜
尺寸效应
平衡分子动力学
非平衡分子动力学 相似文献
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硅橡胶具有绝缘、耐热等优势,在热界面材料中具有重要的应用.通过非平衡分子动力学方法计算了不同交联密度下的热导率.结果表明随着交联密度的变大,热导率逐渐升高. 80%的交联密度可以使热导率提高40%,这是由于交联形成的空间网状结构缩短了热量沿着原子链传递的长度,使热导率有较大的提升.在相同交联密度下,键位置对热导率影响较小,端部交联和中间交联时热导率没有显著差异.但是交联活性点的间隔增加有利于热导率提高.计算了不同交联密度下的声子态密度,分析交联结构的导热机理. 相似文献
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提出一种计算热导率的非平衡分子动力学(NEMD)方法,通过构造均匀内热源获得抛物线形温度分布,并基于Fourier导热定律计算热导率,与Müller-Plathe发展的反扰动非平衡分子动力学(RNEMD)方法相比,不仅具有能量动量守恒和收敛性好的优点,还克服了常规NEMD方法中热冷源区域存在局域热力学非平衡的问题,并有模拟系统温差影响小的特点.对液态氩的热导率进行模拟并与RNEMD方法的模拟结果进行对比. 相似文献
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使用非平衡分子动力学模拟方法研究了单原子LJ流体的非牛顿流变行为,并在系统中分别施加稳态Couette流场和振荡剪切流场.在Couette流场的模拟中,流体出现剪切变稀和法向应力差效应,不同剪切率下的径向分布函数反映了流体分子由于剪切所导致的微观结构变化,通过分析势能函数发现当剪切率增大时,分子间排斥作用增强,吸引作用减弱.在振荡剪切流场的模拟中,发现剪切应力和剪切率之间的相位差随频率增加而增加,随频率增加复数粘度的实部先增大再减小,虚部单调增加,导致虚部粘度相对实部粘度比例增大,弹性模量和粘性模量之比也随频率增加而增加.这三点现象表明LJ流体出现粘弹性行为,且在高频率下,弹性所占比重增大. 相似文献
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利用结合双温模型的分子动力学模拟方法,研究了飞秒激光与金属相互作用的烧蚀机制.采用中心波长为800 nm,能量密度从0.043 J·cm~(-2)到0.40 J·cm~(-2)不等,脉宽分别为70 fs和200 fs的激光烧蚀金属镍和铝材料.靶材的温度、原子位型以及内部压力随时间的演化展示了材料热物性参量特性和激光参量对烧蚀结果的影响.结果显示材料电子热传导率对飞秒脉宽激光下的影响仍然较大;对比铝和镍的结果可知,铝的电子晶格耦合系数比镍的小,故电子晶格间的温度梯度持续时间较长;铝的电子热传导系数比镍的大,所以材料上下表面电子温度耦合的时间缩短.铝薄膜表面在能量密度为0.40 J·cm~(-2)激光烧蚀下呈现纳米尺寸的晶体结构. 相似文献
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Sensitivity of intrinsic mode functions of Lorenz system to initial values based on EMD method 下载免费PDF全文
Extreme sensitivity to initial values is an intrinsic character of
chaotic systems. The evolution of a chaotic system has a
spatiotemporal structure containing quasi-periodic changes of
different spatiotemporal scales. This paper uses an empirical mode
decomposition (EMD) method to decompose and compare the evolution of
the time-dependent evolutions of the $x$-component of the Lorenz system.
The results indicate that the sensitivity of
intrinsic mode function (IMF) component is dependent on initial
values, which provides some scientific evidence for the possibility
of long-range climatic prediction. 相似文献
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A new Co–Fe-based ferromagnetic bulk metallic glass (BMG) was synthesized by copper mould casting method. The thermal stability and crystallization processes were investigated by differential scanning calorimetry (DSC) and X-ray diffraction (XRD). The soft magnetic behavior was studied by DC magnetic measurements. The high glass formation ability was interpreted in terms of the effective suppression of nucleation and growth of the intermetallic compounds which appear in the multicomponent system during solidification. The high thermal stability indicates that the new Co–Fe-based BMG could be used as high-temperature magnetic material. The low coercivity which was as low as 8 A/m for the as-cast sample was found in the Co–Fe-based metallic glass cylinder with a diameter of 1.5 mm. 相似文献
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基于经验模态分解和小波阈值的冲击信号去噪 总被引:2,自引:0,他引:2
冲击信号是非线性的并且容易受到噪声污染。为研究冲击信号去噪的问题,本文针对经验模态分解(Empirical Mode Decomposition,EMD)去噪和小波阈值去噪方法存在的不足,提出了基于EMD的小波阈值去噪方法。单纯的EMD去噪方法会在去除高频噪声的同时压制高频的有效信息。本文将EMD与小波阈值去噪相结合,利用连续均方误差准则确定含噪较多的高频固有模态函数(Intrinsic Mode Function, IMF),对高频IMF分量进行小波阈值去噪,以分离并保留这些分量中的有效信息,同时保持低频IMF分量不变。对模拟数据和实际冲击信号进行去噪处理,结果表明,基于EMD的小波阈值去噪方法的去噪效果优于单纯的EMD去噪方法和小波阈值去噪方法。 相似文献
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The Ab initio investigations on structural, electronic, optical and thermal properties of MoB have been reported using full potential linearised-augmented plane wave method within the framework of density functional theory. The exchange and correlation potentials were calculated using the Perdew-Burke-Ernzerhof-Sol generalised gradient approximation. The calculated equilibrium lattice constants and cell volume are in excellent agreement with the experimental results as compared to the available theoretical data. Electronic band structure shows that MoB is metallic in nature. From the partial densities of states of MoB it has been found that major contribution on the Fermi level is due to Mo-4d states. Among the reported optical parameters the large value of reflectivity at low energy shows that MoB can be used as a coating material in IR region. Maximum absorption in extreme UV region shows that it can be used in production of electricity through solar power in space vehicles. Various thermal properties have been calculated in a wide temperature range at high pressures. Change in thermal expansion coefficient with respect to temperature shows that anharmonic effect in MoB is very weak at high temperature. The optical and thermal properties of MoB are presented for the first time in this work. 相似文献
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Samples of Bi2V0.9Co0.1-xZnxO5.35, 0.02 ≤ x ≤ 0.08 with layered Aurivillius structure were synthesized successfully by sol-gel citrate method. Structural and electrical characterization of compositions has been investigated by X-ray diffraction, thermogravimetric analysis–differential scanning calorimetric (TGA–DSC) analysis and AC impedance spectroscopy. The tetragonal γ phase has been observed for all investigated samples. The AC impedance response of samples has been measured in the frequency range of 20 Hz to 1 MHz. The impedance for pellets decreases as thermal energy increases. The contribution of grain to the conduction process is more than that of grain boundary. The ionic conductivity and dielectric permittivity are found to be composition-dependent and increase with increasing Zn concentration. The maximum electrical conductivity observed for the composition x = 0.08 is σ = 4.51 × 10?4 S cm?1 at 300 °C. 相似文献