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MTPS蜂窝夹芯结构传热性能及热应力分析 总被引:4,自引:0,他引:4
对于金属防热结构的蜂窝夹芯结构的稳态情况,基于材料的全灰体假设,同时考虑热传导和热辐射两种传热形式对温度场的耦合作用,利用热流量守恒建立了蜂窝芯层温度场的非线性积分方程。离散化后利用数值方法得到方程组的数值解。对于美国兰利研究中心的实验结果,与本文方法的对比计算结果基本吻合。进一步,利用计算结果讨论了给定面板温度边界情况下,下面板、柱体层的灰度、蜂窝结构长径比对夹芯温度场的影响。并根据温度场和近似的应力分析模型,用半解析结果讨论了稳态情况下蜂窝芯层上的热应力。 相似文献
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星外管路多层隔热组件热参数确定方法 总被引:2,自引:0,他引:2
提出了利用整星热平衡试验数据确定星外管路多层组件热参数的方法,解决了以往星外管路热设计在地面热试验验证不充分的难题。以某卫星星外管路为例,通过对星外管路试验状态模型的修正,确定了星外管路多层隔热组件热参数,并分析了星外管路的在轨极端温度。根据确定的星外管路多层隔热组件热参数计算出的星外管路温度,与在轨温度数据符合较好,验证了此方法的有效性。 相似文献
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制备了Cd1-xZnxS三元系半导体材料。利用X射线衍射(XRD)对其结构进行了表征,结果表明实验所得样品均为纤锌矿结构。建立了Cd1-xZnxS混晶替位模型,根据所建模型和晶格振动理论,对Cd1-xZnxS红外光谱特性进行探讨。研究了Cd1-xZnxS三元系半导体材料红外发射率特性,Cd1-xZnxS在3~5μm波段的发射率远远低于8~14μm波段的发射率,这与材料的红外吸收机制和光谱特性有关;Cd1-xZnxS半导体材料的红外发射率随着烧结温度的提高而降低,这是由于温度升高,晶格畸变减小并逐渐趋近于完整晶格。 相似文献
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开展高紫外-可见-近红外反射能力热控填料的制备,研制新型低吸收比(α_S)高发射率(ε_H)无机热控涂层。以自制SBA-15和ZnO前驱体为原料通过溶剂热浸渍和高温煅烧法制备ZnO/SBA-15填料,然后与硅酸钾(K_2SiO_3)制备无机热控涂层;采用SAXD、XRD、SEM、太阳反射光谱分析填料和涂层的性能。结果显示采用硝酸锌作为前驱体、m(ZnO)∶m(SBA-15)=3∶7、950℃下烧结3 h可以得到高紫外-可见-近红外反射能力的填料;ZnO/SBA-15/K_2SiO_3无机涂层的α_S为0.09,ε_H为0.91,涂层结合力等级为1级,经过100次-196~100℃热循环实验后,涂层无脱落和开裂现象。SBA-15改性ZnO可以获得具有高紫外反射率和低α_S的热控填料,ZnO/SBA-15填料制备的无机热控涂层同样具备高紫外反射率、低α_S和高ε_H,可以满足航天器高效散热的需求,应用前景良好。 相似文献
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M.N. Kouahla G. Moreels M. Faivre J. Clairemidi J.W. Meriwether G.A. Lehmacher E. Vidal O. Veliz 《Advances in Space Research (includes Cospar's Information Bulletin, Space Research Today)》2010
A new and original stereo imaging method is introduced to measure the altitude of the OH nightglow layer and provide a 3D perspective map of the altitude of the layer centroid. Near-IR photographs of the OH layer are taken at two sites separated by a 645 km distance. Each photograph is processed in order to provide a satellite view of the layer. When superposed, the two views present a common diamond-shaped area. Pairs of matched points that correspond to a physical emissive point in the common area are identified in calculating a normalized cross-correlation coefficient (NCC). This method is suitable for obtaining 3D representations in the case of low-contrast objects. An observational campaign was conducted in July 2006 in Peru. The images were taken simultaneously at Cerro Cosmos (12°09′08.2″ S, 75°33′49.3″ W, altitude 4630 m) close to Huancayo and Cerro Verde Tellolo (16°33′17.6″ S, 71°39′59.4″ W, altitude 2272 m) close to Arequipa. 3D maps of the layer surface were retrieved and compared with pseudo-relief intensity maps of the same region. The mean altitude of the emission barycenter is located at 86.3 km on July 26. Comparable relief wavy features appear in the 3D and intensity maps. It is shown that the vertical amplitude of the wave system varies as exp (Δz/2H) within the altitude range Δz = 83.5–88.0 km, H being the scale height. The oscillatory kinetic energy at the altitude of the OH layer is comprised between 3 × 10−4 and 5.4 × 10−4 J/m3, which is 2–3 times smaller than the values derived from partial radio wave at 52°N latitude. 相似文献