磁场方向对碳纳米管氢等离子体微波吸收的影响

深入研究了外加磁场的方向对碳纳米管薄膜中氢等离子体电磁波衰减性能的影响。根据磁离子理论和W．K．B半经典近似法,理论推导了外加静磁场方向和微波传播方向之间的夹角θ为任一值时,碳纳米管薄膜磁化氢等离子体的复介电常数和微波衰减吸收系数公式。在不同条件下数值计算了碳纳米管薄膜中磁化氢等离子体的微波衰减吸收随θ的变化关系。理论结果表明：只要适当调控磁场方向,应用外加静磁场能有效改进碳纳米管氢等离子体的微波衰减吸收性能。通过调节氢等离子体密度、电子有效碰撞频率、外加静磁场的强度和方向,能获得碳纳米管薄膜氢等离子体对某一特定频段微波能的强烈吸收。     

波在周期磁化等离子体圆波导中的传播特性

电磁波与等离子体之间的相互作用是等离子体物理学和高功率微波器件研究的重点,加载等离子体可以大幅度提高微波器件的输出功率和效率．文章提出了一种加载周期磁化变化等离子体圆波导的周期慢波结构,即加载轴向周期磁化正弦变化等离子体圆波导的介质周期结构,并研究了电磁波在该介质结构中的传播特性,根据严格的理论推导得出电磁波在其中传播的色散方程,并进行了数值计算和分析．     

等离子体共振表面波的分析

研究具有轴向线性密度特性的非均匀圆柱冷等离子体的表面波,得到了碰撞等离子体时纯表面波在横磁模式下的实频率、衰减速率和特征函数,并且考虑了等离子体共振的情况.结果表明,在等离子体共振时的位置处,特征函数有极大值.     

玻璃钢复合材料板材Lamb波传播特性分析

基于Lamb波在各向异性材料的波动方程和频散原理,采用斜入射法激发A0模态兰姆波。针对板材的铺层角度、各接收点方向和频厚积等因素对衰减规律和传播速度规律有较大影响,采用有限元软件建立玻璃钢复合材料层合板模型,对各影响因素进行数值模拟研究。研究表明:Lamb波传播特性与纤维铺层方式有关,声速及衰减特性沿纤维方向和非纤维方向传播声速和衰减差异较大,并且呈对称现象,频厚积在0.6~1.8 MHz·mm,对传播声速和衰减影响为线性下降且趋于平稳。     

等离子体共振表面波的分析

研究具有轴向线性密度特性的非均匀圆柱冷等离子体的表面波,得到了碰撞等离子体时纯表面波在横磁模式下的实频率、衰减速率和特征函数,并且考虑了等离子体共振的情况.结果表明,在等离子体共振时的位置处,特征函数有极大值.     

惯性约束聚变中等离子体的全息诊断

介绍了用四分幅紫外全息干涉仪，探测惯性约束聚变中电子密度在等离子体中的分布原理和初步试验结果。     

基于 COMSOL Mutiphysics的空芯光纤中氩气放电模拟仿真

为了研究空芯光纤中氩气的放电特性,利用有限元软件 COMSOL Mutiphysics 基于流体模型对长为50mm 空芯光纤中的气体放电过程进行仿真,得到氩气放电过程中等离子体的主要参数分布,如电子密度、离子密度、电势、空间电荷密度、电场强度等。同时分析了气压对放电过程的影响,结果表明,气压对气体放电的影响主要体现在电子密度与阴极侧的电场强度上,随着气压的逐渐增大,阴极侧的电场强度也随之增加,阴极侧电子密度则保持不变,但在空芯光纤中央区域,电子密度的增大较为明显。     

激光烧蚀Si表面的等离子体的电子温度与电子密度

本文研究在大气中用 Nd:YAG 激光烧蚀固体 Si 表面的等离子体。用光学多道分析仪测量了等离子体的时间分辨发射光谱,用 N(Ⅱ)的两条谱线的相对强度计算了激光等离子体的电子温度,根据 N(Ⅱ)3995谱线的 Stark 展宽计算了等离子体的电子密度。     

Langmuir探针测量低温等离子体参数特性实验

介绍了Langmuir探针测量等离子体参数特性的实验原理和方法,采用Langmuir单探针诊断了电子回旋共振等离子体参数的分布特性。结果表明,在一定微波功率下,气压增加,等离子体密度趋于饱和。将Langmuir单探针测量等离子体特性实验引入高年级近代物理实验课程的综合创新实验,使得学生在动手实验的过程中接触到物理学科研究前沿领域的技术与知识,激发学生的创新意识和提高创新能力。     

强激光在等离子体中的传播

在激光与等离子体相互作用中,等离子体波的产生不能忽视,它对电子密度轮廓有一定影响,并且会影响激光在等离子体中的吸收和散射等过程。     

Surface motion of alluvial valley in layered half-space for incident plane P-waves

The indirect boundary element method (IBEM) is used to study the surface motion of an alluvial valley in layered half-space for incident plane P-waves based on Wolf’s theory. Firstly, the free field response can be solved by the direct stiffness method, and the scattering wave response is calculated by Green’s functions of distributed loads acting on inclined lines in a layered half-space. The method is verified by comparing its results with literature and numerical analyses are performed by taking the amplification of incident plane P-waves by an alluvial valley in one soil layer resting on bedrock as an example. The results show that there exist distinct differences between the wave amplification by an alluvial valley embedded in layered half-space and that in homogeneous half-space and there is interaction between the valley and the soil layer. The amplitudes are relatively large when incident frequencies are close to the soil layer’s resonant frequencies.     

测量布儒斯特角时折射波功率增大的研究

分析了测量布儒斯特角时出现折射波功率大于入射波功率的异常现象原因:在喇叭口面上折射波场的相位偏差小于入射波场的相位偏差,喇叭接收折射波的增益大于接收入射波增益。提出了改进方法。     

Study of interaction between shock wave and unsteady boundary layer

This paper reports theoretical and experimental study of a new type of interaction of a moving shock wave with an unsteady boundary layer. This type of shock wave-boundary layer interaction describes a moving shock wave interaction with an unsteady boundary layer induced by another shock wave and a rarefaction wave. So it is different from the interaction of a stationary shock wave with steady boundary layer, also different from the interaction of a reflected moving shock wave at the end of a shock tube with unsteady boundary layer induced by an incident shock. Geometrical shock dynamics is used for the theoretical analysis of the shock wave-unsteady boundary layer interaction, and a double-driver shock tube with a rarefaction wave bursting diaphragm is used for the experimental investigation in this work. Projects (No. X61151) supported by Centre for Engineering Research at Zhejiang University of Technology, China     

Study of interaction between shock wave and unsteady boundary layer

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Contour detection-based realistic finite-difference-time-domain models for microwave breast cancer detection

In this paper, a collection of three-dimensional(3D)numerical breast models are developed based on clinical magnetic resonance images(MRIs). A hybrid contour detection method is used to create the contour, and the internal space is filled with different breast tissues, with each corresponding to a specified interval of MRI pixel intensity. The developed models anatomically describe the complex tissue structure and dielectric properties in breasts. Besides, they are compatible with finite-difference-time-domain(FDTD)grid cells. Convolutional perfect matched layer(CPML)is applied in conjunction with FDTD to simulate the open boundary outside the model. In the test phase, microwave breast cancer detection simulations are performed in four models with varying radiographic densities. Then, confocal algorithm is utilized to reconstruct the tumor images. Imaging results show that the tumor voxels can be recognized in every case, with 2 mm location error in two low density cases and 7 mm─8 mm location errors in two high density cases, demonstrating that the MRI-derived models can characterize the individual difference between patients' breasts.     

微波综合实验仪的设计

设计了一种微波综合性学生实验仪器,能进行电子自旋共振、微波特性研究和光速的精确测量。设备由微波振荡源、晶体检波器、微波频率计、驻波测量线、示波器、全反射铜板、多孔径铜质反射器等元器件组成,介绍了微波电子综合实验仪的工作原理及制作方法。该设计节约了资源,提高了仪器的利用效率,在近代物理实验应用中有着良好的发展前景。     

TM波在密度周期变化等离子体圆波导中的传播特性

提出了一种加载密度周期变化等离子体圆波导的周期慢波结构即加载密度轴向正弦变化等离子体圆。波导的介质周期慢波结构,并研究了TM波在该介质结构中的传播特性,根据严格的理论推导得出TM波在其中传播的色散方程并进行了数值计算和分析．     

反绝热近似下金属络合物链的二聚化行为

运用玻色化方法研究了一维半充满状态的金属络合物的基态和激发态在反绝热近似下的临界性质.结果表明在反绝热情况下系统的基态是电荷密度波相，其电荷密度波相的强度随电声耦合参量的变化而变化.同时也讨论了系统二聚化序参量的变化规律.     

Effects of differently polarized microwave radiation on the microscopic structure of the nuclei in human fibroblasts

To investigate the influence of microwave radiation on the human fibroblast nuclei, the effects of three variants of electromagnetic wave polarization, linear and left-handed and right-handed elliptically polarized, were examined. Experimental conditions were: frequency (f) 36.65 GHz, power density (P) at the surface of exposed object 1, 10, 30, and 100 μW/cm², exposure time 10 s. Human fibroblasts growing in a monolayer on a cover slide were exposed to microwave electromagnetic radiation. The layer of medium that covered cells during microwave exposure was about 1 mm thick. Cells were stained immediately after irradiation by 2% (w/v) orcein solution in 45% (w/v) acetic acid. Experiments were made at room temperature (25 °C), and control cell samples were processed in the same conditions. We assessed heterochromatin granule quantity (HGQ) at 600× magnification. Microwave irradiation at the intensity of 1 μW/cm² produced no effect, and irradiation at the intensities of 10 and 100 μW/cm² induced an increase in HGQ. More intense irradiation induced more chromatin condensation. The right-handed elliptically polarized radiation revealed more biological activity than the left-handed polarized one.     

Wave protection effect of periodic row of bottom-hinged flap-type wave energy converters

A flap-type wave energy converter (WEC) is combined with a nearshore breakwater to expand the application of WECs both economically and environmentally. Based on the linear potential theory, an eigenfunction expansion solution is developed for a periodic row of bottom-hinged flap-type WECs exposed to normal waves. Additionally, the viscous effect is considered using the ship rolling solution method with a viscous damping term included in the equation of motion, and the viscous damping expression is also described. The proposed solution is verified by comparison with published literatures. The results including the wave energy conversion efficiency, the reflected and transmitted proportion of the incident wave energy are presented for a range of wave periods and geometric ratios. It is demonstrated that better wave protection effects can be attained with smaller gaps between the WECs, where the transmitted proportion of the incident wave energy is lower. An optimal geometric ratio thus exists for a given wave power absorption and a specific wave period.