减压活门性能试验台系统方案设计

主要介绍了减压活门性能试验台的实现机理、采用的方案。     

新型精密狭缝的设计

介绍了一种基于弹性铰链的精密狭缝的设计，加工工艺要求和性能测试结果。根据实际需要，狭缝可以采用水冷结构。     

平面形状误差分离方法的比较分析

就十种典型的精密平面形状误差测量－分离方法的权函数及其零点，作了分析比较。按形状误差谐波抑制最小准则，论证了五点式正交逐次三点法、九点式正交逐次三点法、复合三点法、不对称二维混合法和不对称四点法优于其他方法，不对称四点法则较为理想。     

Stability of resonance rotation of a satellite with respect to its center of mass in the orbit plane

The stability of resonance oscillations and rotations of a satellite in the plane of its orbit in the case when the difference of the moments of inertia with respect to the principal axes lying in the orbit plane is small is determined at a given rotation number m by the sign of function Φ_m(e), introduced by F.L. Chernous’ko in 1963. In this paper, convenient analytical representations of functions Φ_m(e) are described in the form of integrals and series of Bessel functions regular at e → 1^?. Values of Φ_m(1) are calculated in explicit form. A theorem about the double asymptotic form of functions Φ_m(e) at m → ∞ and e → 1^? is proved by the saddlepoint method.     

rom 15 sel

with primary goat embryonic fibroblast showed no difference from traditional feederlayer-based culture method used in mouse and human. The putative primary EG colonies were multilayer clumps ofcompact cel     

数控车削加工仿真系统结构研究

根据实际加工情况提出了一种虚拟NC车削加工的仿真系统的设计及实现原理。在Visual C++平台上利用OpenGL技术建立虚拟加工机床数字化模型,用C++语言实现物理仿真相关的各个数学模型的建立,进行虚拟环境下数控车削加工的几何仿真及物理仿真,实现产品的虚拟车削制造。     

INITIALIZATION METHODS FOR GROUP TRACKING

ＩＮＩＴＩＡＬＩＺＡＴＩＯＮＭＥＴＨＯＤＳＦＯＲＧＲＯＵＰＴＲＡＣＫＩＮＧＹａｎｇＣｈｅｕｇｙａｎｇ；ＱｕＪｉａｎｍｉｎｇ；ＭａｏＳｈｉｙｉ（ＢｅｉｊｉｎｇＵｎｉｖｅｒｓｉｔｙｏｆＡｅｒｏｎａｕｔｉｃｓａｎｄＡｓｔｒｏｎａｕｔｉｃｓ，Ｂｅｉｊｎｇ，Ｃ...     

航天产品工艺定型阶段工艺文件的编制与审查

从编制《工艺定型标准化要求》、审定有关工艺定型文件和编写《工艺定型标准化审查报告》等方面浅述航天产品工艺定型阶段应做好的标准化文件的编制与审查,并对其工作内容作了介绍。     

计算机帧时间对半实物仿真的影响

半实物仿真试验中,要求计算机帧时间与计算积分步长相一致,但在实际试验中不容易精确地做到。本文分析了这种不一致给半实物仿真试验带来的影响,给出了解决的办法,文章中还给出了一实例来说明。     

Field formation around negatively biased solar arrays in the LEO-plasma

Heavy emission caused by impacting plasma ions results in a fast discharging effect of the initially large surface potentials on the dielectric solar cells. This eventually counteracts the energization process of the plasma ions to the cover glasses and leaves no significant electric fields. Thus, with an existing thermal plasma, electrons are again able to reach dielectric surfaces. Strong localized electric fields of the order of several 10 kV/cm form near the interconnector-cover glass interface.