曲率相关的爆轰波在非结构四边形网格上的数值方法

假设爆轰波阵面的法向速度是曲率的线性函数,在非结构四边形网格上采用水平集方法模拟爆轰波阵面的运动过程.水平集方程的曲率无关项采用正格式离散,曲率项采用伽辽金等参有限元方法空间离散,时间离散采用半隐格式.在笛卡儿网格和随机网格上,含曲率的水平集方程的离散格式为强一阶精度,重新初始化方程的离散格式精度为近似一阶精度.曲率收缩的不光滑界面和多个爆轰波阵面相互作用的算例说明格式可有效地模拟爆轰波与曲率相关的运动.     

薛其坤等《科学》发文,首次在实验上发现量子反常霍尔效应或将推动信息技术进步

由清华大学薛其坤院士领衔,清华大学、中科院物理所和斯坦福大学的研究人员联合组成的团队在量子反常霍尔效应研究中取得重大突破,从实验上首次观测到量子反常霍尔效应,在美国物理学家霍尔于1880年发现反常霍尔效应133年后终于实现了反常霍尔效应的量子化.这是我国     

一种研究敞口容器非稳态导热问题的新方法

在变导热系数条件下,把分段迭代法应用于解决非稳态导热物理问题的集总参数法,为敞口容器恒温热源加热过程中容器内的平均温度变化提供了一个简便的计算方法.利用该方法只需三次分段迭代,即可使得理论计算与实验数据结果吻合.     

原子捕集-火焰原子吸收光谱法测定中草药中痕量镉

考察了火焰条件、捕集管与燃烧器和光束的距离、冷却水流量、捕集时间等实验条件对原子捕集 火焰原子吸收光谱法测定镉的灵敏度的影响 ,实验优选出的最佳实验条件为 :乙炔流量 90L·h- 1 ,捕集管距离燃烧器缝口 5mm ,捕集管距离光束 2mm ,冷却水流量 1 5L·min- 1 ;采用 5 0ng·mL- 1 的镉标准溶液对吸光度与捕集时间的关系进行了考察 ,结果发现 ,在 0～ 6min的捕集时间内二者呈良好的线性关系。在最佳实验条件下 ,捕集时间为 2min时 ,镉的特征浓度为 1 8ng·mL- 1 ,检出限为 0 4 2ng·mL- 1 ,分别较常规火焰原子吸收光谱法的特征浓度和检出限改善了 16倍和 5倍 ,方法的精密度 (RSD)为 1 8%。利用所建立的原子捕集 火焰原子吸收光谱法 ,在最佳实验条件下 ,对人参、丹参、苦参和党参及其水煎液中的痕量镉进行了测定 ,样品的测定回收率在 89 5 %～ 10 4 %之间 ,结果令人满意。     

Numerical analysis of the resonance mechanism of the lumped parameter system model for acoustic mine detection

The method of numerical analysis is employed to study the resonance mechanism of the lumped parameter system model for acoustic mine detection. Based on the basic principle of the acoustic resonance technique for mine detection and the characteristics of low-frequency acoustics, the “soil-mine” system could be equivalent to a damping “mass-spring” resonance model with a lumped parameter analysis method. The dynamic simulation software, Adams, is adopted to analyze the lumped parameter system model numerically. The simulated resonance frequency and anti-resonance frequency are 151 Hz and 512 Hz respectively, basically in agreement with the published resonance frequency of 155 Hz and anti-resonance frequency of 513 Hz, which were measured in the experiment. Therefore, the technique of numerical simulation is validated to have the potential for analyzing the acoustic mine detection model quantitatively. The influences of the soil and mine parameters on the resonance characteristics of the soil–mine system could be investigated by changing the parameter setup in a flexible manner.     

复系统Julia集的同步

非线性系统中的分形集——Julia集, 在工程技术中有着十分重要的应用,定义了不同系统间的Julia集同步的概念, 并引入一种非线性耦合的方法, 对同一系统不同参数的Julia集进行了有效的同步.并以多项式形式和三角函数形式的Julia集同步为例验证了该方法的有效性.     

基于最小化收发器数量的光网络业务量疏导

研究了网格型波分复用中的业务量疏导问题,首先把该问题表示为整数线性规划问题(ILP),优化的目标是使得网络中使用的收发器数量最少由于问题的计算复杂度较高,提出了一种启发式算法来解决该问题,数值结果表明:这种算法可以得到与整数线性规划(ILP)得到的最优解相近的结果,在WDM网络中采用适当的业务量疏导可以减少网络中使用的收发器数量。     

Projection Operator and Propagator for an Arbitrary Half—Integral Spin

Based on the solution to Bargmann-wigner equation for an arbitrary half-integral spin,a direct derivation of the projction operator and propagator for an arbitrary half-intergral spin is presented.The projection operator constructed by Behrends and Fronsdal is confirmed and simplified.The commutation rules and a general expression for the Feynman propagator for a free particle with arbitrary half-integral spin are deduced.Explicit expressions for the propagators for spins 3/2,5/2and 7/2 are provided.     

Pyroelectricity and Spontaneous Polarization in [111] Oriented 0.955 Pb（Zn1/3Nb2/3）O3-0.045PbTiO3 Single Crystals

We report that the measurements of the pyroelectric current of the pre-poled [111]-oriented 0.955 Pb（Zn1/3Nb2/3） O3-0.045 PbTiO3 （PZN-4.5%PT） single crystals can shed some light on the phase transition and spontaneous polarization characters of this material in a similar way to measures of remanent polarization and dielectric properties. The pyroelectric current is measured and the corresponding spontaneous polarization is calculated as a function of temperature with various poling fields added during cooling the sample from 200℃ to room temperature. Critical electric field of 0.061 k V/cm is found to be essential to induce the intermediate ferroelectric orthorhombic phase between the ferroelectric rhombohedral and tetragonal phases. Below the critical field, the polarization increases almost linearly with the increase of poling field. At the critical field, the polarization at 30OC increases abruptly from 14μC/cm^2 for a poling field of O.06kV/cm to 29.5μC/cm^2 for a poling field of 0.061 kV/cm, and afterwards, increases slowly and saturates to 31 μC/cm^2 for poling fields beyond 0.55 kV/cm.