八电极静电陀螺支承系统的建模

八电极静电支承系统沿着四个非正交轴对转子施加静电力,这些作用力相互影响,因此需要对支承坐标进行垂直解耦。针对采用八电极方案的静电陀螺,给出了电极电容的计算公式和位移解算方法,推导了静电力计算公式,最后建立了八电极静电陀螺支承系统的模型并利用Simulink对系统进行仿真。仿真结果表明,在系统中加入解算矩阵和"3-4"变换矩阵后,可以使X、Y、Z三个轴向上对转子位移的控制相互独立,为转子的可靠支承奠定了基础。     

带有轴间动力学解耦的三轴转台自适应控制

针对某型号转台存在的轴间非线性耦合，运用非线性解耦的方法进行了解耦设计，并基于解耦后的系统提出用超稳定性和正性的方法进行自适应模型跟随控制器设计，来解决系统在运行过程中参数发生变化对控制性能影响的问题。仿真结果表明，当系统参数在一定范围变化甚至被控对象模型阶次发生变化时，所设计的自适应模型跟随控制器仍能保证系统具有良好的控制性能。     

大型柔性构件振动控制的特征结构配置

根据大型柔性构件存在着建立运动方程自由度多,整体结构参数不宜测量等特点,文中研究了基于子结构的振动特征结构配置．为克服以往在拼装子结构时由于界面耦合作用,造成振动能量相互传递,破坏原有各子控制器设计性能的缺陷,作者提出了通过在界面上安装控制执行器,以割断子结构间能量传递的分散解耦控制法,保证了子控制器的设计特性在装配后不会改变     

紧耦合天线的反相耦合相消隔离技术

提高紧耦合天线的隔离度是雷达、通信和电子对抗等许多领域中提升系统性能的技术之一,目前的方法大多以牺牲天线辐射效率为代价。研究了一种基于反相耦合相消理念的去耦方法,可以在极小间距情况下实现天线单元之间的高隔离度,并且保持较高的天线增益。利用一种微带双天线结构来验证这一方法,这种结构的两个天线都工作于1.8 GHz,相互间的间隔为10 mm(1/16波长),仿真和实验结果说明,两个天线间的隔离可以低于-20 dB。经仿真结果显示该结构中的天线增益要大于0 dB,与不经隔离设计时的同结构同尺寸天线差别约1 dB。初步实现了在较小地影响辐射性能的前提下实现紧耦合天线之间的高隔离目标。     

基于DSP的三相光伏并网逆变器控制系统设计与实现

三相电压型光伏并网逆变器,直接控制其三相电流较困难.同步旋转坐标下基于PWM技术的PI控制方法动态响应快,且可实现对指令的无静差跟踪,但是d、q两相直流电流之间还存在耦合关系,不利于控制设计,同时还存在电网电压的影响,为了消除这些影响,运用了前馈解耦控制算法,结合空间矢量SVPWM给出了逆变器的电流控制策略.浮点数字信...     

线性调频连续波激光雷达测量方法研究

线性调频连续波激光雷达在光电器件响应速度有限的条件下,要满足较高的距离分辨率的测量要求,就需要比同体制微波雷达大得多的相对带宽。这就导致线性调频连续波微波雷达的距离与速度去耦合方法不能被直接应用。针对探测近距高速运动目标和实时性高的要求,根据激光雷达目标回波的特点,提出了一种快速线性调频信号参数估计方法,利用均匀分成两段的中频信号的傅里叶变换来获取目标的距离与速度信息。在目标距离50m,速度1000m/s,中频信噪比为0的仿真条件下,雷达测距误差小于15mm,测速误差小于10m/s。仿真实验表明,该方法具有较高的测量精度和较强的抗干扰能力。     

高速PCB板谐振仿真与分析

谐振是电源完整性一大问题,PCB电源平面间谐振振幅过大,会导致电源分配系统(PDS)工作异常,甚至成为EMI辐射源,故在PCB详细设计阶段需开展谐振仿真分析并消除谐振,从而提高设计成功率。为消除谐振,首先利用SIWAVE软件对电源地平面间谐振情况进行仿真分析,找出谐振点,然后合理选用布局去耦电容,消除400 MHz以下频段谐振影响。通过调整PCB叠层及层间距消除400 MHz以上频段谐振影响。通过实例仿真分析,依据工程经验,实现了快速估算去耦电容的计算方法,并证明了其正确性。     

Sweep direction and efficiency of the swept-frequency two pulse phase modulated scheme for heteronuclear dipolar-decoupling in solid-state NMR

We present here a bimodal Floquet theoretical and experimental investigation of the direction of sweep in the swept-frequency two pulse phase modulated (SW(f)-TPPM) scheme used for heteronuclear dipolar decoupling in solid-state NMR. The efficiency of the decoupling turns out to be independent of the sweep direction.     

Johnson‐Lindenstrauss lemma for circulant matrices**

We prove a variant of a Johnson‐Lindenstrauss lemma for matrices with circulant structure. This approach allows to minimize the randomness used, is easy to implement and provides good running times. The price to be paid is the higher dimension of the target space k = O(ε^?2 log³ n) instead of the classical bound k = O(ε^?2 log n). © 2011 Wiley Periodicals, Inc. Random Struct. Alg., 2011     

New insights from variable-temperature and variable-pressure studies into coupling and decoupling processes for ion transport in polymer electrolytes and glasses

A fresh analysis of literature data shows how the influences of temperature and pressure on ion transport and structural relaxation in glass-forming systems may be combined within the framework of ‘master plots’ based on the equation E_A = M · V_A, to reveal new insights into coupling and decoupling effects in a wide range of systems. E_A,σ and V_A,σ are, respectively, instantaneous activation energies and volumes for ionic conductivity and the parameter, M_σ, is a corresponding ‘process modulus’. For structural relaxations occurring at the glass transition, the appropriate modulus is given by M_s = T_g · dP/dT_g. We can now identify typical behaviour patterns for fragile liquids on the one hand, and typical inorganic glasses on the other. Thus, the parameters, M_σ and M_s, for fragile systems such as molten Ca(NO₃)₂:KNO₃ (CKN) or a typical polymer electrolyte such as a complex of LiCF₃SO₃ in PPG, are found to remain constant over a wide range of temperatures down to T_g, despite changes in the temperature (and pressure) dependences of the ionic conductivities, as indicated for example by a return to Arrhenius behaviour in the case of CKN, or by so-called Stickel plots and changes in the VTF parameters for the polymer electrolytes. If E* and V* are activation energies and volumes assigned to elementary steps, when again E* = M · V*, we can go further and identify the microscopic processes driving forward structural relaxation. In the case of inorganic glasses, where usually we find the decoupling index R_τ ≈ 10¹², we identify two distinct decoupling paradigms represented by strong and fragile systems respectively, where in both cases the activation volumes for ion transport are very similar to the corresponding ionic volumes. In the former case (typified by the strongly cross-linked silicate and aluminosilicate systems), the negative activation volumes for structural relaxation (negative values of dT_g/dP) are clearly indicative of a ‘water-like’ behaviour attributable to the collapse of the network under pressure. On the other hand, for the more fragile fast-ion conducting silver iodomolybdate glass, the experimental results show that M_s (at T_g) ≈ M_σ (in glass), implying some recoupling of structural relaxation to ion transport. Arguments based on the dynamic structure model lead us to predict that a similar close link should exist between M_s (at T_g) and M_σ in the relatively fragile lithium and sodium borate glasses, thus highlighting the need for more information concerning the effects of pressure on the glass transition temperatures of common inorganic glasses.