高速圆柱滚子轴承工作温度研究

将滚子与套圈滚道摩擦生热视为移动热源,建立了高速圆柱滚子轴承温度场计算模型;使用ANSYS的APDL语言发展了轴承工作温度分析的参数化程序,输入热流密度等边界条件,程序能够自动建模精确的分析高速圆柱滚子轴承工作温度.以一个型号轴承为例,分析了不同工况参数对轴承工作温度的影响,结果显示轴承内圈转速、径向载荷和润滑油入口油温对轴承工作温度影响显著.      

Nonlinear Dynamics Behaviors of a Rotor Roller Bearing System with Radial Clearances and Waviness Considered

A rotor system supported by roller beatings displays very complicated nonlinear behaviors due to nonlinear Hertzian contact forces, radial clearances and bearing waviness. This paper presents nonlinear bearing forces of a roller bearing under four-dimensional loads and establishes 4-DOF dynamics equations of a rotor roller bearing system. The methods of Newmark-β and of Newton-Laphson are used to solve the nonlinear equations. The dynamics behaviors of a rigid rotor system are studied through the bifurcation, the Poincar è maps, the spectrum diagrams and the axis orbit of responses of the system. The results show that the system is liable to undergo instability caused by the quasi-periodic bifurcation, the periodic-doubling bifurcation and chaos routes as the rotational speed increases. Clearances, outer race waviness, inner race waviness, roller waviness, damping, radial forces and unbalanced forces-all these bring a significant influence to bear on the system stability. As the clearance increases, the dynamics behaviors become complicated with the number and the scale of instable regions becoming larger. The vibration frequencies induced by the roller bearing waviness and the orders of the waviness might cause severe vibrations. The system is able to eliminate non-periodic vibration by reasonable choice and optimization of the parameters.     

Substorms in the inner plasma sheet

Thin Current Sheets (TCS) are regularly formed prior to substorm breakup, even in the near-Earth plasma sheet, as close as the geostationary orbit. A self-consistent kinetic theory describing the response of the plasma sheet to an electromagnetic perturbation is given. This perturbation corresponds to an external forcing, for instance caused by the solar wind (not an internal instability). The equilibrium of the configuration of this TCS in the presence of a time varying perturbation is shown to produce a strong parallel thermal anisotropy (T T) of energetic electrons and ions (E>50keV) as well as an enhanced diamagnetic current carried by low energy ions (E<50keV). Both currents tend to enhance the confinement of this current sheet near the magnetic equator. These results are compared with data gathered by GEOS-2 at the geostationary orbit, where the magnetic signatures of TCS, and parallel anisotropics are regularly observed prior to breakup. By ensuring quasi-neutrality everywhere we find, when low frequency electromagnetic perturbations are applied, that although the magnetic field line remains an equipotential to the lowest order in T_e/T_i, a field-aligned potential drop exists to the next order in (T_e/T_i). Thus the development of a TCS implies the formation of a field-aligned potential drop ( few hundred volts) to ensure the quasi-neutrality everywhere. For an earthward directed pressure gradient, a field-aligned electric field, directed towards the ionosphere, is obtained, on the western edge of the perturbation (i.e. western edge of the current sheet). Thus field aligned beams of electrons are expected to flow towards the equatorial region on the western edge of the current sheet. We study the stability of these electron beams and show that they are unstable to “High Frequency” (HF) waves. These “HF” waves are regularly observed at frequencies of the order of the proton gyrofrequency (f_H+) just before, or at breakup. The amplitude of these HF waves is so large that they can produce a strong pitch-angle diffusion of energetic ions and a spatial diffusion that leads to a reduction of the diamagnetic current. The signature of a fast ion diffusion is indeed regularly observed during the early breakup; it coincides with the sudden development of large amplitude transient fluctuations, ballooning modes, observed at much lower frequencies (fH+). These results suggest that the HF waves, generated by field-aligned electron beams, provide the dissipation which is necessary to destabilize low frequency (ballooning) modes.     

末敏弹减速运动和稳态扫描段运动特性的研究

对末敏弹这一全新反坦克武器在减速运动和稳态扫描段的运动特性进行了仔细的研究。恰当地引入了降落伞的附加质量和附加惯性矩,完整地分析了伞体和弹体所受的外力和外力矩,建立了由伞体和弹体组成的末敏弹系统二体运动模型。编制了完整的计算程序。给出了末敏弹扫描角速度、扫描角和扫描曲线随时间的变化,以及扫描覆盖区随高度的变化。计算结果与试验结果有很好的一致性。该模型可进一步用于末敏弹系统的弹道修正、参数优化和弹道模拟。     

第2009卡林顿周太阳活动的初步分析

介绍了第 2 0 0 9卡林顿周大黑子群AR484,AR486和AR488产生的太阳活动以及这些太阳活动对地球空间环境造成的影响。依据对太阳活动的统计研究 ,简要分析了三个大黑子群活动的差异。分析结果指出 ,关注某一时期太阳活动的活动经度带以及太阳活动在某一半球的主次是解决太阳活动短期预报非常重要的思路     

一种低复杂度的Multi-h CPM相干解调算法及FPGA实现

多调制指数连续相位调制（Multi-h Continuous Phase Modulation,Multi-h CPM）是一种恒包络调制,具有多个周期出现的调制指数,因此其频谱效率和功率效率比单调制指数CPM更高,但其接收机的复杂度也随之增加。本文在倾斜相位（Tilted Phase,TP）的基础上采用频率脉冲截断（Frequency Pulse Truncation,FPT）和状态空间分割（State Space Partition,SSP）相结合的方法来降低多调制指数连续相位调制的复杂度,使相位状态由512降低到16,理论损耗约为0.8 dB。同时,对降低复杂度的解调算法在现场可编程门阵列（Field Programmable Gate Arrays, FPGA）上进行了验证。仿真和在线测试的误码率曲线接近理论分析曲线,和常用的128状态解调算法相比,资源消耗降低了约59%。     

C/C-Cu复合材料的烧蚀形貌和烧蚀机理

以PAN预氧化纤维整体毡为增强体,经碳化、等温CVI致密化后制备多孔的C/C复合材料预制体,利用气体压力浸渗法将Cu引入C/C预制体中制备C/C-Cu复合材料。采用氢氧(H2-O2)焰考核C/C-Cu复合材料的烧蚀性能,经扫描电镜和电子能谱对不同烧蚀区域的微观结构和成分进行分析,结果表明:预制体密度为0.96 g/cm3的C/C-Cu复合材料的线烧蚀率和质量烧蚀率分别为4.75μm/s、0.223 mg/s,烧蚀性能优良;其烧蚀表面具有不同的宏观形貌,在烧蚀中心区产生了明显的凹坑,主要烧蚀机制为C/C预制体的氧化和铜基体的机械冲刷;烧蚀过渡区聚集了大量的铜基体,其烧蚀机制为Cu的热氧化和机械冲刷;烧蚀边缘区材料表面变黑,主要因为C/C的氧化。为了提高C/C-Cu的烧蚀性能,需要发挥C/C预制体的"钉扎"作用,阻止Cu在高温下被气流冲刷而发生流动。     

超声速涡轮叶型全局气动优化设计

针对涡轮叶型全局优化设计计算时间长、样本空间大等难点提出一种可行的优化设计方法,该方法将控制叶型的17个参数作为优化变量,采用第二代多目标遗传算法进行全局自动寻优。基于此方法,搭建了涡轮叶型全局优化设计平台。利用此平台,分别采用轴向稠度固定和自由优化两种方式对超声速涡轮叶型进行了优化设计。数值计算结果表明,两组优化设计叶型在设计工况下总压损失系数比参考叶型分别低19.5%和10.0%,流道中的激波强度更弱,且在变工况条件下都具有较好的气动性能。深入分析流场与激波结构后发现,外尾激波相比于内尾激波对总损失的影响更大,通过减小气流膨胀转折角或内尾激波气流转折角能够有效削弱外尾激波强度。     

轴向充磁圆筒型永磁直线同步电机气隙磁场解析计算

介绍了一种基于许-克变换法的轴向充磁结构圆筒型永磁直线同步电机(TPMLSM)气隙磁场解析计算方法。首先采用许-克变换法计算出无齿槽时电机的气隙磁场;然后利用许-克变换法求取初级铁心开槽时的气隙相对比磁导函数,分析铁心开槽对气隙磁场的影响;最后通过无齿槽时的气隙磁场与有齿槽时的气隙磁场相对比磁导函数得到有齿槽时电机的气隙磁场分布。同时给出了该种充磁结构TPMLSM气隙磁场解析计算表达式,并以1台36/12极槽配合轴向充磁TPMLSM样机进行试验。试验结果证明空载气隙磁场的有限元分析值与解析值较吻合,空载电动势(EMF)计算值、试验测试值、有限元分析值一致。