控制陀螺仪与g 2 / 有关干扰力矩的主要技术途径

一高精度液浮陀螺仪中一般都使用动压气体轴承，动压气体轴承的不等刚度及转子姿态角是陀螺仪ｇ２有关干扰力矩的主要来源，加之由于径向轴承的位移和转子姿态角的出现使问题更加复杂。本文假定框架等刚性的前提下，着重讨论动压气体轴承的某些参数对单自由度液浮陀螺仪与ｇ２有关干扰力矩的影响及其控制此项干扰力矩的技术途径。     

短路匝式传感器干扰力矩分析

短路匝式传感器带来的干扰力矩是引起陀螺仪随机漂移的重要因素之一,减小该项干扰力矩对提高陀螺精度能够起到重要的作用。本文利用电磁感应定律和磁路分析法对干扰力矩进行了推导,并通过Ansoft maxwell软件对短路匝传感器不同参数情况下的干扰力矩进行仿真分析,得出了转子转角、激磁电压和激磁频率对干扰力矩的影响关系曲线,最后合理选择参数以保证干扰力矩在精度允许范围内。该分析结果对减小短路匝传感器的干扰力矩和减小陀螺仪的随机漂移都具有一定参考价值。     

小型静电陀螺仪静电场基本干扰力矩分析

推导了采用装配式电构结构的小型静电陀螺仪静电场基本干扰力矩计算公式,进行了仿真计算,并分析了转子的谐波、转子线位移、支承回路放大系数,转子极轴相对于电极坐标系的偏称对干扰力矩的影响,其结果对小型静电陀螺仪的设计与研制具有参考价值。     

小型静电陀螺仪转子变形及干扰力矩分析

推导了小型静电陀螺仪转子非球形干扰力矩公式，仿真分析了两种不同结构的实心转子的温度变形、离心变形、压力变形及综合变形，计算了其变形产生的干扰力矩及漂移。     

推力轴承对轴承－转子系统的耦合作用研究

研究了推力轴承对轴承－转子系统的耦合作用。在传递矩阵法的基础上，提出一种研究考虑推力轴承影响的轴承－转子系统的动力学的通用方法。研究中考虑了如下几个因素：（１）推力盘的静态倾斜；（２）转子的静变形；（３）径向轴承中负荷的重新分配；（４）偏载对径向轴承性能的影响；（５）推力轴承对系统稳定性的影响。研究结果表明，在某些情况下，推力轴承对径向轴承的动特性、转子的静挠度、系统稳定性等具有显著的影响     

静电陀螺转子径向偏心干扰力矩分析

推导了静电陀螺仪转子径向偏心产生的静电场干扰力矩计算公式，计算分析了该干扰力矩产生的陀螺漂移，其结果对静电陀螺仪的设计与研制具有参考价值。     

数学机械化在转子系统分析中的应用

以转子－轴承系统中两圆盘转子为研究对象,在计及陀累力矩的条件下,通过对两圆盘转子临界转速与振型参数的分析,对吴消去法在转子动力学研究中的应用做了初步探索,将吴消去法的特征列思想 Maple软件的符号计算功能相结合,实现了对两圆盘转子临界转速与振型参数的解析计算与分析。     

转子在线自动平衡及其工程应用研究的进展

转子在线自动平衡技术可以在旋转机械运行期间调整其不平衡量来及时降低振动, 使其始终稳定运行.早期的自动平衡装置始于19世纪末, 包括液体型、环型、球型和摆锤型;20世纪60年代开始研究的自动平衡装置主要包括喷涂型、电腐蚀型、电子光束型、激光型和电化学型;20世纪后期研究的自动平衡装置主要包括电动机型和遥控型;现代的自动平衡装置主要包括液压型、电磁型和电磁轴承型.综述了国内外各种旋转机械在线自动平衡装置的结构和工作原理, 重点介绍了液压型和电磁型自动平衡装置的结构和控制原理.讨论了在线自动平衡技术最新的研究成果, 列举了在线自动平衡技术的工程应用实例, 介绍了应用电磁型自动平衡装置解决柔性弯曲转子和立式超重力机转子振动的试验.转子在线自动平衡技术已经大量应用到机械加工设备, 如磨床等, 显著提高了加工精度;有些还应用于流程工业中大型的旋转机械上, 如汽轮机、风机和压缩机等, 取得了巨大的经济效益.高可靠性的平衡执行机构和高效的控制策略等关键问题尚未完全解决.      

油膜支承转子系统动静件碰摩特征分析

以支承在油膜轴承上的Jeffcott转子为对象，分析了油膜力对碰摩转子动力学行为的影响。通过与刚支情形对比，发现油膜力是耦合作用于碰摩转子系统，有时能够抑制振动，有时却加剧振动。因此实际转子碰摩故障诊断过程中，必须在充分考虑支承情况的基础上建立合理的非线性动力学模型，才能为实际转子系统的碰摩故障分析提供必要的理论依据。     

控制力矩陀螺用主动电磁轴承数字控制系统设计与实现

讨论了以TMS320VC33为核心的数字控制系统硬件结构。针对磁悬浮控制力矩陀螺转子的大惯量、小跨距、扁平转子和高速旋转时的陀螺效应，采用积分分离和不完全微分PID加交叉反馈控制策略。实验证明，该系统能够有效地抑制高速转子的陀螺效应，达到控制力矩陀螺电磁轴承高速稳定运行的要求。     

环面节流静压气体球轴承的相似准则

从静压气体润滑基本控制方程组的无量纲化着手,在详细分析静压气体轴承的耦合边界条件及非定常雷诺气体润滑方程特性的基础上,对Constantinescu给出的动压气体轴承相似准则进行补充,得到环面节流静压气体球轴承定常气体润滑膜及非定常气体润滑膜的相似准则.数值实验的结果表明:数值计算结果与相似理论分析结论完全一致;当其它参数不变时,不同球半径的2个球轴承的气膜流场相似;球半径改变对轴承动静态性能的影响可以利用相似理论进行分析.     

微凹坑织构表面对脂润滑关节轴承摩擦特性的影响

为研究脂润滑下表面织构对关节轴承摩擦特性的影响,设计和制造了4组表面高度算术平均值相同、表面微凹坑面积占有率分别为7%、10%、15%和21%的关节轴承内圈表面形貌.使用Talysurf CCI Lite非接触式三维轮廓仪对试件表面进行测量,采用ISO25178定义的表面参数对试件表面形貌进行表征.在改造的HDM-20端面摩擦磨损试验机上,采用2#锂基脂润滑在不同载荷、转速条件下进行了一系列摩擦磨损试验,研究了表面形貌参数与摩擦系数的关系.在本试验中,选取表面高度算术平均值Sa和表面峰态Sku等表面高度参数、表面峰区平均材料体积Vmp、表面中心区平均空体体积Vvc和表面谷区平均空体体积Vvv等表面功能参数以及平均谷体积Sdv等表面特征参数对关节轴承表面形貌进行表征.结果表明:各表面参数对摩擦系数的影响不同,将表面高度参数、功能参数和特征参数这几种表面形貌参数结合对关节轴承表面形貌进行表征,更有利于脂润滑下关节轴承表面形貌的摩擦学设计.     

静电支承球形转子的恒速控制

本讨论静电支承球形转子的恒速控制问题。首先,介绍静电支承系统的基本工作原理,其次,建立静电支承系统的动力学模型。第三,分析采用PID控制器的支承刚度,第四,阐述形成静电旋转力矩的原理。最后,提出利用静电力恒速的方案与基本限制条件。     

Torque on a slip sphere rotating in a semi-infinite micropolar fluid

In this paper, the steady rotational motion of a slip sphere in a semi-infinite micropolar fluid is investigated. The sphere is assumed to rotate about a diameter perpendicular to an impermeable plane wall. The slip and spin boundary conditions are imposed on the spherical particle surface while on the plane wall surface the classical no-slip and no-spin conditions are utilized. A semi-analytical technique based on the principle of superposition together with a numerical method, called the collocation method, is employed to obtain the hydrodynamic torque acting on the spherical particle. Numerical results for the torque are obtained and illustrated graphically.     

Free Convection in Spherical Annular Sectors Filled with a Porous Medium

Calculated free convection flows and heat transfer are presented for concentric spherical annular sectors, filled with a porous medium. Two isothermal walls and an adiabatic radial wall at the sector angle define the sectors. The governing equations (in the stream function and temperature formulation) are solved numerically using ADI (alternative direction implicit) finite-difference method. Over the range of geometric parameters examined, the obtained results for spherical annuli and low Rayleigh number Ra. As Ra increases, multicellular flows develop for small values of the aspect ratio parameter . In addition, analytical solutions of the governing equations were obtained for small values of Ra (1) and it was shown that these solutions agree well with those obtained numerically. Significant differences in the local heat transfer rates on the inner and outer walls of the spherical annuli were observed from these solutions.     

On the Chaotic Dynamics of a Spherical Pendulum with a Harmonically Vibrating Suspension

The equations of motion for a lightly damped spherical pendulum are considered. The suspension point is harmonically excited in both vertical and horizontal directions. The equations are approximated in the neighborhood of resonance by including the third order terms in the amplitude. The stability of equilibrium points of the modulation equations in a four-dimensional space is studied. The periodic orbits of the spherical pendulum without base excitations are revisited via the Jacobian elliptic integral to highlight the role played by homoclinic orbits. The homoclinic intersections of the stable and unstable manifolds of the perturbed spherical pendulum are investigated. The physical parameters leading to chaotic solutions in terms of the spherical angles are derived from the vanishing Melnikov–Holmes–Marsden (MHM) integral. The existence of real zeros of the MHM integral implies the possible chaotic motion of the harmonically forced spherical pendulum as a result from the transverse intersection between the stable and unstable manifolds of the weakly disturbed spherical pendulum within the regions of investigated parameters. The chaotic motion of the modulation equations is simulated via the 4th-order Runge–Kutta algorithms for certain cases to verify the analysis.     

The Discrete Cosserat Eigenfunctions for a Spherical Shell

The Papkovich-Neuber potential method is applied to obtain the discrete Cosserat eigenvalues and eigenvectors for the boundary value problems of displacement and traction for a spherical shell. The eigenvalues presented herein correct those obtained by the Cosserats. This revised version was published online in August 2006 with corrections to the Cover Date.     

Evolution of a Small Distortion of the Spherical Shape of a Gas Bubble under Strong Expansion-Compression

The evolution of a small distortion of the spherical shape of a gas bubble which undergoes strong radial expansion-compression upon a single oscillation of the ambient liquid pressure under a harmonic law are analyzed by numerical experiments. It is assumed that the distortions of the spherical bubble shape are axisymmetric and have the form of individual spherical surface harmonics with numbers of 2–5. Bubble-shape oscillations prior to the beginning of expansion are taken into account. Generally, the distortion value during bubble expansion-compression depends on the phase of bubble-shape oscillation at the beginning of the expansion (initial phase). Emphasis is placed on the dependence of the maximum distortions in the initial phase at certain characteristic times of bubble expansion-compression on the amplitude of the external excitation, liquid viscosity, and distortion mode (harmonic number). The parameters of the problem are typical of the stable periodic sonolumiescence of an individual air bubble in water at room temperature. An exception is the liquid pressure oscillation amplitude, which is varied up to values that are five times the static pressure. That large excitation amplitudes are beyond the stability threshold of periodic oscillations of spherical bubbles. Their consideration is of interest from the point of view of increasing the compression ratio of the bubble gas, i. e., increasing the maximum temperature and density achievable in the final compression stage.__________Translated from Prikladnaya Mekhanika i Tekhnicheskaya Fizika, Vol. 46, No. 4, pp. 17–28, July–August, 2005.     

Flows through Porous Media Containing a Shielded Spherical Inclusion

Compact formulas are obtained for constructing flow potentials in media containing a spherical inclusion shielded by a high- or low-permeability film (fracture or barrier) using the known potentials of steady-state incompressible fluid flows through homogeneous porous media. The formulas obtained can be extended both to inhomogeneous porous media in which the permeability functions have different constant factors inside and outside the inclusion and to bounded zones. The type of singular points of the potentials (sources, sinks, etc.) and the boundary conditions assigned in media without an inclusion are conserved for media containing a shielded inclusion. As an example, translational flow past a spherical shielded polluted zone is studied. This is of interest in connection with environmental problems.     

球壳结构馈通增长的瑞利-泰勒不稳定性

利用小扰动分析法 ,导出不可压缩球壳结构的馈通增长方程 ,数值模拟了高压气体驱动外表面有初始扰动的明胶球壳的瑞利 泰勒不稳定性模型。计算结果表明 :对于低波数扰动 ,外界面比较稳定 ,内表面的馈通增长较快 ,具有比较明显的三个演化阶段和波形反转现象。高波数扰动的增长恰好与低波数相反。球壳会聚结构比柱壳会聚结构的界面稳定性要好些。