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71.
Experimental investigation on evaporation interface temperature and evaporation rate of water in its own vapor at low pressures
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Evaporative phase transitions are widely present in industrial production and daily life such as thin film processes and crystal growth. The evaporation of the liquid layer and the thermocapillary convection affect each other and restrict each other, making the energy transfer mechanism of the evaporation interface very complicated. To understand the evaporation characteristics of water in its low-pressure pure vapor environment, a series of experimental studies were carried out on the temperature distributions and evaporating rate of water evaporation in the annular pool. The cylinder temperature of the annular liquid pool is controlled between 3℃ and 15℃, and the evaporation environment pressure ranges from 394 Pa to 1467 Pa, when the temperature measurement starts, the depth of water is 10 mm. The results show that the temperature of the vapor side on the liquid-vapor interface is higher than that of the liquid side and there is an obvious temperature jump across the vapor-liquid interface. With the decrease of the pressure ratio, the evaporation rate increases, and the interface temperature jump is enlarged. Meanwhile, with the increase of the distance from the cylinder, the local evaporation rate decreases, thus, the temperature jump decreases. At the same pressure ratio, as the cylinder temperature increases, the heat flux from vapor side decreases, the temperature jump decreases at all measurement points. Within the experimental controlled parameters, the maximum temperature jump obtained in the measurements is 2.56℃. Due to the coupling effect of evaporation cooling and thermocapillary convection, there is a uniform temperature layer with a thickness of about 2 mm under the evaporation interface. The thickness of the uniform temperature layer near the cylinder is always larger than that in the middle of the evaporation interface. In the uniform temperature layer, the thermocapillary convection induced by radial temperature gradient transfers heat from the cylinder to the liquid-vapor interface to compensate for the latent heat of evaporation. Below the uniform temperature layer, the temperature rises rapidly due to heat conduction and buoyancy convection. 相似文献
72.
直流电弧等离子体法制备超细Ag粉研究 总被引:2,自引:2,他引:2
采用自行研制的高真空双枪直流电弧金属纳米粉连续制备设备,制备了高纯度的超细银粉,并采用正交试验的方法研究了各工艺参数对粉体产率及粒径分布的影响。利用X射线衍射(XRD)、透射电子显微镜(TEM)和相应选区电子衍射(SAED)以及Simple PCI软件对样品的成分、形貌、晶体结构和粒径分布进行了分析。结果表明:所得银粉纯净无污染,属多晶型结构,平均粒径在38-220nm范围内,粒径分布窄;最大产率比同类研究结果提高了近17倍;电流和充气压力分别是影响产率和粒径分布的显著性因素。 相似文献
73.
真空熔炼AZ91镁合金过程中Mg元素的蒸发行为 总被引:2,自引:0,他引:2
在真空Ar气氛中熔炼AZ91镁合金,测定了不同精炼温度下Mg元素的蒸发速率。结果表明,随着精炼温度的升高,Mg元素的蒸发量增大。通过计算可知,Mg的蒸气压是Al的10^9倍,是Zn的46倍,因此主要是Mg的蒸发而导致合金其他元素含量升高。XRD分析表明,蒸发物是Mg元素。结合Mg元素的蒸发机制,在该试验条件下推导出Mg元素蒸发率的计算公式以及Mg元素的表观传质系数、蒸发率与精炼温度的关系,计算得出Mg元素蒸发率为0.86×10^-3-1.35×10^3g/cm^2·s,Mg元素的表观传质系数在2×10^-5-24×10^-5cm/s范围内。 相似文献
74.
75.
The melting, evaporation and oxidation behaviors as well as the solidification phenomena of tungsten and molybdenum in induction plasma were studied. Scanning electron microscopy was used to examine the morphology and the cross section of plasma-processed powders. X-ray diffraction was used to analyze the oxides formed on the particle surface of these two metals. The influence of spray chamber pressure on the spheroidization and oxidation phenomena was discussed. The results show that fewer Mo particles than W particles are spheroidized at the same powder feed rate under the same plasma spray condition although molybdenum has a lower melting point. A small fraction of tungsten is evaporized and condensed either on the surface of tungsten particles nearby or on the wall of spray chamber. Tungsten oxides were found in tungsten powder processed under soft vacuum condition. Extremely large grains form inside some spheroidized particles of tungsten powder. 相似文献
76.
Effect of surface modification of metal hydride electrode on performance of MH/Ni batteries 总被引:1,自引:0,他引:1
A novel method was applied to the surface modification of the metal hydride(MH)electrode of MH/Ni batteries.Both sides of the electrode were plated with a thin silver film about 0.1μm thick using vacuum evaporation plating technology,and the effect of the electrode on the performance of MH/Ni batteries was examined.It is found that the surface modification can enhance the electrode conductivity and decrease the battery ohimic resistance.After surface modification,the discharge capacity at 5C(7.5A)is increased by 212 mA.h and the discharge voltage is increased by 0.11 V,the resistance of the batteries is also decreased by 32%.The batteries with modified electrode exhibit satisfactory durability.The remaining capacity of the modified batteries is 89%of the initial capacity even after 500 cycles.The inner pressure of the batteries during overcharging is lowered and the charging efficiency of the batteries is improved. 相似文献
77.
78.
A series of Co/Si/(Co/Cu/Co) multilayers and Co/Si/Co sandwiches were prepared by high vacuum electron-beam evaporation. It was found that a Si spacer (≥0.9 nm) could greatly decrease the interlayer coupling in Co/Si/Co sandwiches and there was no magnetoresistance(MR) or spin-valve MR in them due to the high resistivity of Si spacer. While in Co/Si/(Co/Cu/Co) multilayers, we observed a spin-valve MR of about 0.5% through a nominal 2.7 nm Si spacer at room temperature. The spin-valve MR in Co/Si/(Co/Cu/Co) multilayers was attributed to the enhanced spin polarization of conduction electrons caused by the top Co/Cu/Co sandwich with GMR mechanism and high spin-dependent scattering at Co/Cu interface. 相似文献
79.
薄膜厚度对HfO2薄膜残余应力的影响 总被引:1,自引:0,他引:1
HfO2薄膜是用电子束蒸发方法制备的,利用ZYGO干涉仪测量了基片镀膜前后曲率半径的变化,计算了薄膜应力。对样品进行了XRD测试,讨论了膜厚对薄膜残余应力的影响。结果发现不同厚度HfO2薄膜的残余应力均为张应力,应力值随薄膜厚度的增加而减小,当薄膜厚度达到一定值后,应力值趋于稳定。从微观结构变化对实验结果进行了分析,发现微结构演变引起的本征应力变化是引起薄膜残余应力改变的主要因素。 相似文献
80.
We report the stress relaxation behavior of arc-evaporated TiCxN1−x thin films during isothermal annealing between 350 and 900°C. Films with x=0, 0.15, and 0.45, each having an initial compressive intrinsic stress σint=−5.4 GPa, were deposited by varying the substrate bias Vs and the gas composition. Annealing above the deposition temperature leads to a steep decrease in the magnitude of σint to a saturation stress value, which is a function of the annealing temperature. The corresponding apparent activation energies for stress relaxation are Ea=2.4, 2.9, and 3.1 eV, for x=0, 0.15, and 0.45, respectively. TiC0.45N0.55 films with a lower initial stress σint=−3 GPa, obtained using a high substrate bias, show a higher activation energy Ea=4.2 eV. In all the films, stress relaxation is accompanied by a decrease in defect density indicated by the decreased width of X-ray diffraction peaks and decreased strain contrast in transmission electron micrographs. Correlation of these results with film hardness and microstructure measurements indicates that the stress relaxation is a result of point-defect annihilation taking place both during short-lived metal-ion surface collision cascades during deposition, and during post-deposition annealing by thermally activated processes. The difference in Ea for the films of the same composition deposited at different Vs suggests the existence of different types of point-defect configurations and recombination mechanisms. 相似文献