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符号表A无量纲温度幅值L。热扩散长度。1二维效应作用区边界AD温度幅值。试样表面法向Yd样品无量纲厚度AO特征温度q热源热流。材料热扩散率C材料体积比热容qb热源热流幅值。”测量热扩散率d样品厚度T试样上某点温度A材料导热系数h表面等效换热系数几边界温度p温度相位He无量纲换热系数。。光源边界。测量角频率1前言使用周期热流法测量薄膜材料面向热扩散率的基本原理如图1所示,调制光对试样加热,遮光板沿V方向以一定速度V移动,引起试样上热源边界l变化,假设没有热损失,试样上经历沿。方向的一维导热过程,则热电偶测得之温度幅… 相似文献
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生物柴油是新型环境友好型替代能源,其主要成分为碳数分布在C6~C24的长链脂肪酸酯。利用瞬态单丝法导热系数测量系统在272~352 K温度范围内、0.1~15 MPa压力范围内对三种生物柴油组成成分壬酸甲酯、庚酸甲酯和己酸甲酯的液相导热系数进行了实验测量,并将导热系数拟合成关于温度和压力的方程,壬酸甲酯、庚酸甲酯和己酸甲酯导热系数实验值与拟合方程的计算值最大相对偏差分别为?0.18%、0.12%和?0.07%,平均绝对偏差分别为0.06%、0.05%和0.02%。导热系数实验系统测量的扩展不确定度小于2%(置信区间0.95),重复性好于±0.5%。 相似文献
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利用稳态电热拉曼技术测量了碳纳米管纤维对流换热环境下的导热系数. 该方法基于材料拉曼信号与温度之间的关系, 实时探测一维材料在不同电加热(内热源)下的中心点温度, 利用对流环境下的稳态导热模型推导出材料的导热系数, 实现了一维微纳材料热物性的无损化和非接触式测量. 实验发现: 碳纳米管纤维的导热系数远低于单根碳纳米管的导热系数, 但高于碳纳米管堆积床的导热系数. 这表明碳纳米管体材料的热物性主要取决于内部管束的列阵和管束间的接触热阻. 相似文献
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HFC-32饱和气导热系数的实验研究 总被引:5,自引:0,他引:5
1研究背景自《蒙特利尔议定书》签定后,特别是1992年11月哥本哈根会议以来,HCFCS的替代日程已经确定。目前以含有HFC-32的混合物替代HCFC-22的呼声很高,而且国外正开始着手应用。有关HFC-32的饱和气的导热系数现在还没有见文献报导。在本文中,作者自行开发设计了一套双热线法测量导热系数的实验装置,并对HFC-32的饱和气的导热系数进行了测量,经分析测量结果是令人满意的。2实验装置及实验原理热线法是测量导热系数的瞬态方法之一,其基本原理是Carslaw提出的半径趋于零的无限长线热源在无限大介质中的导热方程的解山文献… 相似文献
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基于用稳态法测量不良导体的导热系数实验,为了求得更为精确的导热系数,用origin软件处理实验数据,拟合出温度和时间的曲线,并求得冷却速率及导热系数. 相似文献
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In the present work, an experimental investigation of heat transfer enhancement parameters of the oscillating flow heat exchanger under different frequencies, tidal displacement, and heat fluxes is carried out. The effect of different parameters on experimental effective thermal conductivity and convective heat transfer coefficient in cooling region is studied using correlations given by different researchers. A correlation for experimental effective thermal conductivity in terms of S2√ω is derived based on experimental data. This correlation is useful for predicting the optimum value of S2√ω before onset of turbulence. 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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Gadolinium zirconium oxide (Gd2Zr2O7) films, a promising candidate for thermal barrier coatings and buffer layers in superconductors, are deposited on Al2O3 substrate by using an RF-magnetron sputtering method for the study of thermal conductivity. Thermal conductivity is measured by both methods of time domain thermoreflectance and 3 omega methods, which can give rise to the difference in the heat penetration depth. Since phonon mean free path in Gd2Zr2O7 is smaller than lattice constant due to oxygen vacancy, the film thickness variation in 100–500 nm does not affect thermal conductivity seriously unless interfacial thermal resistance is involved. The interfacial effect can be included or excluded in thermal conductivity depending on the heat penetration depth of heat waves. There is discrepancy between the experimental results of thermal conductivity obtained by the two methods, due to the effect of interfacial thermal resistance. The interfacial effect on thermal conductivity is verified through comparison of the two experimental results, and the Debye–Callaway modeling. 相似文献
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本文建立了低维薄膜材料导热模型,运用非平衡分子动力学模拟的方法,利用lanmmps软件对单层石墨烯纳米带的导热特性进行仿真分析,根据Fourier定律计算热导率,再对石墨烯纳米带的原子施加一定耦合应力场,把应力耦合作用下的石墨烯热导率与正常的石墨烯纳米带进行了对比研究,模拟数据结果表明:在石墨烯纳米带上施加耦合应力时,会导致石墨烯纳米带热导率升高,且随应力增加而增大,模拟范围内热导率升高2.61倍,并且应力方向会对热导率变化产生一定影响,这个研究为纳米尺度上石墨烯相关研究和进一步提升热导率提供了新思路. 相似文献
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Theoretical calculations of thermophysical properties of single-wall carbon nanotube bundles 下载免费PDF全文
Carbon nanotube bundles are promising thermal interfacial materials due to their excellent thermal and mechanical characteristics.In this study,the phonon dispersion relations and density of states of the single-wall carbon nanotube bundles are calculated by using the force constant model.The calculation results show that the inter-tube interaction leads to a significant frequency raise of the low frequency modes.To verify the applied calculation method,the specific heat of a single single-wall carbon nanotube is calculated first based on the obtained phonon dispersion relations and the results coincide well with the experimental data.Moreover,the specific heat of the bundles is calculated and exhibits a slight reduction at low temperatures in comparison with that of the single tube.The thermal conductivity of the bundles at low temperatures is calculated by using the ballistic transport model.The calculation results indicate that the inter-tube interaction,i.e.van der Waals interaction,hinders heat transfer and cannot be neglected at extremely low temperatures.For(5,5) bundles,the relative difference of the thermal conductivity caused by ignoring inter-tube effect reaches the maximum value of 26% around 17 K,which indicates the significant inter-tube interaction effect on the thermal conductivity at low temperatures. 相似文献