基于集合卡尔曼变换的东中国海声学 敏感区判定方法*

为改善海洋与水声环境预报质量,针对常规观测成本高、资料利用率低等问题,将适应性观测方法应用于海洋声学领域。结合海洋-声学耦合模式与集合卡尔曼转换敏感区诊断方法,以东中国海宫古海峡北部区域为验证区,计算并分析不同条件下海洋环境敏感区与声学敏感区分布,通过观测系统模拟试验验证适应性观测对验证区预报的提升效果。结果表明,两种敏感区位置随时间间隔增加均向验证区上游移动,海洋环境敏感区相比于声学敏感区分布更为集中,且平移特征更明显;对海洋环境敏感区和声学敏感区添加适应性观测均能提升海洋与水声环境的预报质量,提升效果随时间间隔增加而减小,在某种类型敏感区的适应性观测对相对应参数的预报质量提升效果优于对其他类型敏感区进行观测的效果。     

耦合时间精度对模拟飞行器自由运动特性的影响

将亚迭代技术引入流体动力学和刚体动力学方程的耦合求解,获得细长三角翼极限环运动的规律.探讨耦合时间精度对飞行器非定常运动特性的影响,细长三角冀的大迎角自由滚运动最终形成极限环振荡的周期性自维持运动,不同攻角自由滚振幅阶跃式的变化特点较好地吻合了自由滚试验的规律.对于多系统耦合问题,亚迭代耦合求解(耦合时间精度为二阶)对物理时间步长的依赖性不明显;而存在一阶时间滞后的解耦推进方法的数值结果强烈地依赖于物理时间步长选取,稍大的时间步长将导致非物理的数值结果.     

CaAl_2Si_2O_8∶Eu,Ce,Tb单基三元掺杂荧光材料的制备及其光谱学特征研究

采用高温固相法制备了CaAl_2Si_2O_8∶Eu,Ce,Tb单基三元掺杂的荧光材料。使用X射线衍射仪(XRD)、拉曼光谱仪(Raman)和荧光分光光度计(PL)等测试手段对该荧光材料进行表征。采用XRD表征了样品的物相组成,测试结果表明稀土离子Eu~(2+)置换Ca~(2+)并没有引起CaAl_2Si_2O_8基质晶格结构的变化。拉曼光谱分析证实了样品中硅氧四面体和铝氧四面体的存在,表明了Eu~(2+)替代Ca~(2+)的数量与晶体形态畸变程度有关,Eu~(2+)进入基质晶格的数量影响着硅(铝)氧四面体的数量。PL测试结果表明样品在325nm光激发下,其发射峰主要表现为426nm(蓝光区)的强宽带发射峰和541nm(绿光区)的弱发射峰,其中426nm处的宽带发射峰可通过高斯拟合成三个位于393,419和474nm的拟合峰;对比分析荧光性能以及同等合成条件下样品荧光强度的不同,确定了该荧光材料在三掺Eu∶Ce∶Tb的摩尔比为1∶1∶1.5时所发射荧光最强。CIE色度图坐标显示三种掺杂比例下制备的荧光材料均发射蓝色荧光,光显色性好,色温低,是一种适合作为紫外-近紫外激发的LED用蓝色荧光材料。     

基于综合监控的设备状态修方案研究

随着工业控制领域的不断发展,综合监控系统已经日趋成熟并于工业现场运行较长时间。而基于综合监控系统获取的大量历史数据的分析和实时数据的使用并没有开展深入的探讨。本方案提出了一种基于综合监控系统的状态修方案,把综合监控系统的历史数据经过一定的清洗,建模导入到大数据平台,通过相应的算法分析,从而改善维修决策模型并建立设备评价体系;把实时数据实时的传递到设备状态页面,减轻了传统巡检工作,保证了设备检查效果;把设备报警数据通过分类,分项,直接派生检修工单,实现了设备维修的自动化。     

干涉型光纤水听器PGC解调的参数估计方法

对于干涉型光纤水听器外调制式相位生成载波(PGC)解调方案,光干涉强度和调制深度两个参数的波动会影响解调结果。为了消除影响,本文提出利用椭圆曲线拟合以及频域搜索的参数估计方法。根据理论分析,当调制深度在[0,3.83]区间内两种方法有效,可以适应实际情况中调制深度缓慢且小范围波动的情况。为了分析验证两种方法,本文利用不同类型的待测信号进行了数值仿真,根据仿真结果,在声信号引起的相位较大的情况下,两种方法都能对参数进行正确估计;利用频域搜索的方法适用的动态范围更大;当相关参数缓慢波动时,频域搜索法能正确跟踪估计相关参数。     

CaAlSiN_3∶Eu~(2+)荧光粉掺杂PC透光罩的制备及其在植物灯中的应用

为了实现传统白光LED光源与植物照明用光源之间的快速转换,采用高温熔融造粒的方式制备了不同质量分数CaAlSiN_3∶Eu~(2+)(CASN∶Eu~(2+))掺杂的荧光聚碳酸酯(PC)透光罩,并进行了结构和光学分析。制备了荧光PC透光罩配备的T8型LED灯管,测试了其EL光谱、相关光学性质以及对于生菜的种植效果。结果表明,CASN∶Eu~(2+)荧光粉在掺杂过程中性质稳定,该灯管随着配备的透光罩的荧光粉掺杂浓度的提高,相对应的WLED的色坐标从(0.3272,0.3467)变化到(0.3895,0.3824),色温从5757K下降到3807K,显色指数从70.3上升到77.6,但光效略有减弱。配备了荧光粉质量分数为4‰透光罩的T8型白光LED灯管的光质更适合生菜生长。     

LARGE-TIME BEHAVIOR OF SOLUTIONS TO THE INFLOW PROBLEM OF THE NON-ISENTROPIC MICROPOLAR FLUID MODEL

We investigate the asymptotic behavior of solutions to the initial boundary value problem for the micropolar fluid model in a half line R+ :=(0,∞).Inspired by t...     

Guided Waves in a Multi-Layered Cylindrical Elastic Solid Medium

We investigate the guided waves in a multi-layered cylindrical elastic solid medium. The dispersion function of guided waves is usually complex and the dispersion curves of all modes are not conveniently obtained. Here we present an effective method to obtain the dispersion curves of all modes. First, the dispersion function of the guided waves is transformed into a real function. The dispersion curves are then calculated for all the modes of the guided waves by the bisection method. The modes with the orders n = 0, 1, and 2 are analysed in two- and three-layer media. The existence condition of Stoneley wave is discussed. The modes of the guided waves are also investigated in a two-layer medium, in which the velocity of shear wave in the outer layer is less than that in the inner layer.     

Raman and X-Ray Investigation of Pyrope Garnet （Mg0.76Fe0.14Ca0.10）3Al2Si3O12 under High Pressure

The compressional behavlour of natural pyrope garnet is investigated by using angle-dlspersive synchrotron radiation x-ray diffraction and Raman spectroscopy in a diamond anvil cell at room temperature. The pressureinduced phase transition does not occur under given pressure. The equation of state of pyrope garnet is determined under pressure up to 25.3 GPa. The bulk modulus KTO is 199 GPa, with its first pressure derivative K′TO fixed to 4. The Raman spectra of pyrope garnet are studied. A new Raman peak nearly at 743 cm^-1 is observed in a bending vibration of the SiO4 tetrahedra frequency range at pressure of about 28 GPa. We suggest that the new Raman peak results from the lattice distortion of the SiO4 tetrahedra. All the Raman frequencies continuously increase with the increasing pressure. The average pressure derivative of the high frequency modes （650-1000 cm^-1） is larger than that of the low frequency （smaller than 650 cm^-1）. Based on these data, the mode Grǖneisen parameters for pyrope are obtained.     

First-Principles Prediction of High-Pressure Phase of CaC6

The lattice dynamics of rhombohedral GaG6 is studied as a function orpressure to probe Its high pressure phase with low superconducting transition temperature using the density functional liner-response theory. The pressureinduced phase transition in CaC6 is attributable to the softening transverse acoustic （TA） phonon mode at the zone boundary X （0.5, 0.0, 0.5） point. The high pressure phase is then explored by performing fully structural optimization in the supercell which accommodates the atomic displacements corresponding to the eigenvectors of the unstable mode of TA（X）. The high-pressure phase is predicted to be a monoclinic unit cell with space group P21/m.