共查询到19条相似文献,搜索用时 171 毫秒
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对含微孔洞疏松度m=1.04的疏松铝进行了冲击加载-卸载实验,利用DISAR(distance interferometer system for any reflector)测得了53至99 GPa五个冲击压力下疏松铝/LiF界面粒子速度波剖面,获得了各压力下的纵波声速和其中三个压力点的体波声速,确定出疏松铝的冲击熔化压力约为81 GPa,确定出高压下冲击熔化前的泊松比约为0.372.通过分析,微孔洞明显降低了冲击熔化压力,引起的非谐振效应明显,状态方程计算中考虑非谐效应,非谐因子l
关键词:
低孔隙度
疏松铝
声速
冲击熔化 相似文献
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为研究微孔洞对锡的高压相变的影响, 对含亚微米孔洞的疏松锡(疏松度m=1.01)进行了冲击加载-卸载实验. 利用DPS(Doppler pins system)测得了31.8-66.1 GPa冲击压力下疏松锡/LiF界面粒子的速度剖面, 获得了各压力下的纵波声速与体波声速, 给出了该疏松锡的冲击熔化起始压力约为49.1 GPa, 获得了各压力下的剪切模量与泊松比. 结合密实锡与疏松锡的高压纵波声速、体波声速与剪切模量, 界定密实锡的冲击熔化压力在53.5-62.3 GPa之间, 高于疏松锡的值, 表明微孔洞明显降低了冲击熔化压力. 对密实锡准确的冲击熔化压力值还需要进一步的实验数据. 测试的固态压力范围内的声速数据没有明显奇异点, 表明疏松锡没有类似密实锡的固态bcc 相变发生. 相似文献
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利用激光干涉测速技术(VISAR)测量LY12铝合金在20—34 GPa冲击压力下经历加载-卸载和加载-再加载过程的样品/窗口界面粒子速度剖面,采用AC方法确定了具有较高精度的动态屈服强度值.实验结果和文献发表的数据具有较好的一致性.通过以平面焊接方式制作组合飞片,克服了组合飞片在气炮发射过程中可能发生分离的技术困难,使铝的动态屈服强度测量压力范围从22 GPa扩展到了34 GPa.同时,根据对不同实验条件下的加载-再加载过程的比较,对再加载弹性前驱波的形成机理进行了讨论,认为位错是形成该现象的主要原因. 相似文献
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冲击相变与熔化作为材料特性的一项重要研究内容,对于多相物态方程构建具有重要意义.本文利用追赶稀疏原理和阻滞法,基于火炮加载技术获得了17.3—28.3 GPa范围内纯铋(Bi)的高精度声速数据和Hugoniot参数,分析了声速软化规律,得到固-液混合相区Bi材料声速随压力的近似线性递减关系C=3.682-0.015p,并进一步确定Bi的冲击熔化压力区间为18—27.4 GPa.同时,Bi/Li F界面速度剖面的预期平台段在固液混合相区表现出渐进爬升的异常特征,分析认为,该现象与Bi材料的非均匀熔化动力学行为及冲击熔化完成时间尺度较长有关. 相似文献
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利用激光干涉测速技术(VISAR)测量LY12铝合金在20—34 GPa冲击压力下经历加载-卸载和加载-再加载过程的样品/窗口界面粒子速度剖面,采用AC方法确定了具有较高精度的动态屈服强度值.实验结果和文献发表的数据具有较好的一致性.通过以平面焊接方式制作组合飞片,克服了组合飞片在气炮发射过程中可能发生分离的技术困难,使铝的动态屈服强度测量压力范围从22 GPa扩展到了34 GPa.同时,根据对不同实验条件下的加载-再加载过程的比较,对再加载弹性前驱波的形成机理进行了讨论,认为位错是形成该现象的主要原因.
关键词:
动态屈服强度
AC方法
弹性前驱波
VISAR 相似文献
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提出了冲击波作用下通过测量沿着准弹性卸载过程纵波波速与体波波速得到等效剪切模量的方法,应用该方法对LY12铝在20—70 GPa冲击压力下的等效剪切模量进行了测量.实验结果表明,等效剪切模量随应力线性减少直至反向屈服时为零,而初始卸载时的等效剪切模量可以由修正的Steinberg-Cochran-Guinan模型进行描述.应用得到的等效剪切模量进行了初步数值模拟,计算结果与实验测量的粒子速度剖面符合很好,重现了准弹性卸载到塑性卸载的光滑过渡.
关键词:
等效剪切模量
波速
准弹性卸载
冲击波
铝 相似文献
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在发生冲击熔化的情况下,金属样品/窗口界面压力下的熔化温度与卸载温度数值相等,且十分接近于界面温度值。根据这一结论,利用二级轻气炮加载手段和光辐射法测温技术,用氟化锂(LiF)单晶作透明窗口,获得了110~140 GPa压力范围内无氧铜的熔化温度。实验表明,无氧铜的高压熔化温度数据与文献发表的无氧铜高压声速实验结果是一致的,铜的高压熔化规律可用Lindemann熔化定律近似描述。采用的熔化温度测量方法不必反演出冲击温度,简化了冲击熔化温度的数据处理方法,为金属冲击熔化温度测量提供了一种潜在的技术途径。 相似文献
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A. A. Akhubekov V. A. Sozaev T. Kh. Tamaev 《Bulletin of the Russian Academy of Sciences: Physics》2009,73(8):1137-1139
The contact melting (CM) of Cd + 0.046 at % Na solid solution with indium, bismuth, and tin is studied. The dependence of
the contact layer lengths on the duration of Cd + 0.046 at % Na CM with indium with electric current through is obtained.
Addition of sodium is found to drastically affect the temperature of contact melting onset in (Cd + 0.046 at % Na)-Me (Me: In, Sn, Bi) systems. An attempt to interpret the results obtained is made. 相似文献
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L. Soulard 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2008,50(3):241-251
We present a complete molecular dynamics analysis of the micro-spallation, which corresponds to the various events following
the reflexion on a free surface of a unsustained shock wave causing the melting of the material. In a first stage the various
curves required for a purely thermodynamic analysis (Hugoniot, melting curve and isentropes) are calculated by the mean of
both equilibrium and non equilibrium molecular dynamics. Next we define two cases. In the first one the shock pressure is
above the melting pressure (SM case).
In the second one the melting occurs during the release wave following the shock (RM case). These two configurations provide
quite similar results if the melting kinetic of the SM case is slow enough and we observe the formation of a solid micro-spall.
In the other SM cases a direct transition from a liquid to a gas is obtained. As other results we found that (i) the melting
under shock is a stationary process in the front shock referential and so is supported by the Rayleigh line and (ii) the spall
strength of the micro-spallation is negligible. 相似文献
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ICP—AES法直接测定铋矿石中铋 总被引:1,自引:0,他引:1
本文研究了用ICP-AES法直接测定铋矿石中铋含量的方法,优化了仪器的测试条件,并对共存元素的干扰情况进行了研究,该方法简便,快速,可直接用于铋矿石中铋的准确测定,结果满意。 相似文献
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A novel super-resolution near-field optical structure (super-RENS) with bismuth (Bi) mask layer is proposed in this paper. Static optical recording tests with and without super-RENS are carried out using a 650-nm semiconductor laser at recording powers of 14 and 7 mW with pulse duration of 100 ns. The recording marks are observed by high-resolution optical microscopy with a charge-coupled device (CCD)camera. The results show that the Bi mask layer can also concentrate energy into the center of a laser beam at low laser power similar to the traditional Sb mask layer. The results above are further confirmed by another Ar+ laser system. The third-order nonlinear response induced by the plasma oscillation at the Bi/SiN interface during laser irradiation can be used to explain the phenomenon. The calculation results are basically consistent with our experimental results. 相似文献
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E. Haro-Poniatowski R. Serna A. Suárez-García C.N. Afonso M. Jouanne J.F. Morhange 《Applied Physics A: Materials Science & Processing》2004,79(4-6):1299-1302
The synthesis by pulsed laser deposition of a bismuth nano-plane embedded in an amorphous germanium matrix is reported. The structural changes were studied by Raman spectroscopy as a function of temperature. Upon heating, the Bi nano-plane melts and, as the sample is cooled, it re-crystallizes at a temperature well below the melting point. The results show a broad melting–solidification hysteresis cycle (170 K) that is compared to the ones obtained earlier on nanoparticles. Furthermore, a metal-induced crystallization effect was also observed in the germanium matrix. PACS 81.15.Fg; 05.70.Fh; 78.30.En 相似文献
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Corrosion related properties of iron(100) surface in liquid lead and bismuth environments:A first-principles study
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The corrosion of steels in liquid metal lead (Pb) and bismuth (Bi) is a critical challenge in the development of accel-erator driven systems (ADS). Using a first-principles method with a slab model, we theoretically investigate the interaction between the Pb (Bi) atom and the iron (Fe) (100) surface to assess the fundamental corrosion properties. Our investigation demonstrates that both Pb and Bi atoms favorably adsorb on the (100) surface. Such an adsorption decreases the energy required for the dissociation of an Fe atom from the surface, enhancing the dissolution tendency significantly. The seg- regation of six common alloying elements (Cr, A1, Mn, Ni, Nb, and Si) to the surface and their impacts on the corrosion properties are also considered. The present results reveal that Si seems to have a relatively good performance to stabilize the surface and alleviate the dissolving trend caused by Pb and Bi. 相似文献
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J.Y. Li L. Soubeyroux H.L. Zheng C.S. Li Y.F. Lu L. Porcar R. Tournier L. Zhou 《Physica C: Superconductivity and its Applications》2006,450(1-2):56-60
The phase evolution during melting and recrystallization of (Bi,Pb)2Sr2Ca2Cu3O10 ((Bi,Pb)-2223) core in a Ag-sheathed monofilamentary tape has been investigated. The tape was fabricated by PIT process with powders containing nearly pure (Bi,Pb)-2223 phase. Short samples were melted at 805 °C, 808 °C, 812 °C, 816 °C, 831 °C, slowly cooled at 1.5 °C/h under flowing 1.6% O2 balanced with argon and quenched in air at room temperature. X-ray diffraction (XRD) and scanning electron microscopy coupled with energy dispersive spectroscopy (SEM/EDS) were applied for the phase identification. The results show that (Bi,Pb)-2223 core is partially melted into a liquid and alkaline earth cuprates (AECs), mainly 2:1-AEC, at 805 °C, 808 °C, 812 °C, and well reforms directly from the melt during the slow cooling. More (Bi,Pb)-2223 phase is decomposed at temperatures higher than 816 °C, but cannot recrystallize, indicating that a partial melting at some temperatures around a given temperature range is essential to (Bi,Pb)-2223 phase reformation. The melt composition moves from that between “2223” and “2212” stoichiometries towards 2212-like stoichiometry with increasing temperature. This seems to lead to the conclusion that (Bi,Pb)-2223 phase decomposes incongruently into a 2212-like liquid and (Ca,Sr)-cuprates. 2:1-AEC plays the most important role in (Bi,Pb)-2223 melt-recrystallization process. Our results also reveal that plate-like shape (Bi,Pb)-2223 grains can be obtained via melting and recrystallization if the optimum processing conditions are used. 相似文献