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1.
基于密度泛函理论,运用第一原理赝势平面波方法,采用CASTEP量子力学能量软件包研究了Sc占据Ti位与Sc占据A l位的超胞晶格常数、原子形成热、超胞总态密度与电子密度差分图,两种情况对比下,在L10-TiA l合金中,Sc优先占据Ti位,这一结论为进一步研究三元系TiA l-Sc合金提供了理论研究的基础。 相似文献
2.
有机高分子絮凝剂处理高浊度原水效果和机理研究 总被引:2,自引:0,他引:2
本文研究了有机高分子絮凝剂PAM、CTAB及它们的复配PAM+CTAB处理高浊度原水的最佳实验条件、絮凝性能、效果和机理,为有机高分子絮凝剂的选择和管式絮凝器的研制提供了理论依据。 相似文献
3.
CPL技术在FY—1C卫星中的应用 总被引:1,自引:0,他引:1
为使FY 1C卫星上的镉镍电池可向空间散热 ,以降低工作温度 ,采用了毛细泵回路 (CPL)技术。介绍CPL的工作原理、主要组成以及在卫星上控制星载设备温度应用的设计技术 ,给出了在地面进行的各项热性能试验情况。卫星在轨运行测试验证表明 ,卫星温度处于最佳状态 ,镉镍电池组的温度控制在 (4~ 9)℃的范围内 ,6台镉镍电池之间温差小于 3℃ ,满足镉镍电池的特殊温度要求 相似文献
4.
JI Lei* LI Shu-suo HAN Ya-fang JIANG Li-wu School of Materials Science Engineering Beijing University of Aeronautics Astronautics Beijing China 《中国航空学报》2006,19(Z1)
The thermal fatigue behavior of Ni3Al based superalloy IC6E during the cycles between 900 ℃/1 000 ℃ and the room tempera-ture was investigated. The experimental results indicate that the primary and secondary thermal fatigue cracks initiate inside or round the borides and then spread away along grain boundaries and/or in interdendritic areas. The fracture of borides and their separation from the matrix at interfaces are mainly responsible for the crack initiation and its spreading. At temperatures higher than 1 000 ℃, the grain boundary oxidation combined with cyclic stresses accelerates the crack growth. 相似文献
5.
6.
刘先斌%张志刚%汤林志%宫声凯 《宇航材料工艺》2007,37(6):105-108
研究了温度和应变速率对NiAl-30Cr-4Mo共晶合金的拉伸性能的影响.研究结果表明在同一应变速率(1.67×10-4/s)下,随着温度的升高,材料的塑性增加;在韧脆转变温度(BDTT)923 K以上,随着应变速率的降低,合金的拉伸断口韧窝密集程度增大,合金塑性断裂的趋势越明显,且屈服强度随应变速率的降低而下降. 相似文献
7.
对采用研制的焊丝和采用TC18同质焊材钨极氩弧焊焊接TC18钛合金的接头力学性能及微观组织进行了对比研究,结果表明:采用同质焊材焊接TC18钛合金只能保证接头的强度指标,而采用研制的新型焊丝焊接TC18钛合金,可以保证接头具有优良的综合力学性能. 相似文献
8.
Michael J. S. Belton Karen J. Meech Michael F. A’Hearn Olivier Groussin Lucy Mcfadden Carey Lisse Yanga R. Fernández Jana PittichovÁ Henry Hsieh Jochen Kissel Kenneth Klaasen Philippe Lamy Dina Prialnik Jessica Sunshine Peter Thomas Imre Toth 《Space Science Reviews》2005,117(1-2):137-160
In 1998, Comet 9P/Tempel 1 was chosen as the target of the Deep Impact mission (A’Hearn, M. F., Belton, M. J. S., and Delamere, A., Space Sci. Rev., 2005) even though very little was known about its physical properties. Efforts were immediately begun to improve this situation
by the Deep Impact Science Team leading to the founding of a worldwide observing campaign (Meech et al., Space Sci. Rev., 2005a). This campaign has already produced a great deal of information on the global properties of the comet’s nucleus
(summarized in Table I) that is vital to the planning and the assessment of the chances of success at the impact and encounter.
Since the mission was begun the successful encounters of the Deep Space 1 spacecraft at Comet 19P/Borrelly and the Stardust spacecraft at Comet 81P/Wild 2 have occurred yielding new information on the state of the nuclei of these two comets. This
information, together with earlier results on the nucleus of comet 1P/Halley from the European Space Agency’s Giotto, the Soviet Vega mission, and various ground-based observational and theoretical studies, is used as a basis for conjectures on the morphological,
geological, mechanical, and compositional properties of the surface and subsurface that Deep Impact may find at 9P/Tempel 1. We adopt the following working values (circa December 2004) for the nucleus parameters of prime importance to Deep Impact as follows: mean effective radius = 3.25± 0.2 km, shape – irregular triaxial ellipsoid with a/b = 3.2± 0.4 and overall dimensions of ∼14.4 × 4.4 × 4.4 km, principal axis rotation with period = 41.85± 0.1 hr, pole directions
(RA, Dec, J2000) = 46± 10, 73± 10 deg (Pole 1) or 287± 14, 16.5± 10 deg (Pole 2) (the two poles are photometrically, but not
geometrically, equivalent), Kron-Cousins (V-R) color = 0.56± 0.02, V-band geometric albedo = 0.04± 0.01, R-band geometric
albedo = 0.05± 0.01, R-band H(1,1,0) = 14.441± 0.067, and mass ∼7×1013 kg assuming a bulk density of 500 kg m−3. As these are working values, {i.e.}, based on preliminary analyses, it is expected that adjustments to their values may be made before encounter
as improved estimates become available through further analysis of the large database being made available by the Deep Impact observing campaign. Given the parameters listed above the impact will occur in an environment where the local gravity is
estimated at 0.027–0.04 cm s−2 and the escape velocity between 1.4 and 2 m s−1. For both of the rotation poles found here, the Deep Impact spacecraft on approach to encounter will find the rotation axis close to the plane of the sky (aspect angles 82.2 and 69.7
deg. for pole 1 and 2, respectively). However, until the rotation period estimate is substantially improved, it will remain
uncertain whether the impactor will collide with the broadside or the ends of the nucleus. 相似文献
9.
通过采用两片PIC18F448及其外围器件实现了机载环控地面检测系统的数字化设计。通过I^2C总线实现两片单片机之间的数据传输与协调,并利用其CAN接口模块实现多套检测系统的网络化和远程控制操作。 相似文献
10.