同轴插板式TEM-TE11模式转换器的设计与实验研究

 介绍了同轴插板式TEM－TE₁₁模式转换器的设计:在同轴波导内沿径向插入四块金属板,将同轴TEM模转变为扇形截面波导TE11模,通过控制插板的长度使不同扇形截面波导输出TE₁₁模的相位不同,最后在圆波导内形成TE₁₁模;通过在插板的前端设置角向均匀分布的金属杆,实现了模式转换器的良好匹配。实验测得模式转换器的辐射方向图轴向最大,与数值计算结果吻合良好,表明实验中模式转换器的输出模式与数值计算结果一致,从而验证了同轴插板式模式转换器的可行性。     

E面和H面方向图等化的双模圆锥喇叭设计

 介绍用于Φ7.3 m Cassegrain天线的高功率馈源喇叭的设计。为使E面和H面方向图在照射区域内具有高的等化度,选择双模圆锥喇叭作为馈源的结构形式。由于高功率源采用BJ-32波导输出信号,故馈源系统中还应包含一个矩形到圆形的模式转换器,将TE10模转换为TE11模。设计了双模圆锥喇叭和模式转换器,并进行了功率容量估算。测试结果表明,所设计的馈源达到了设计要求,理论计算结果和实验测试数据吻合良好。     

基于灰色神经网络的测井预测地层破裂压力

在新兴的信息处理技术中,灰色系统预测法和神经网络预测法都可用来解决精细测井解释和油藏描述中的模式识别和参数预测等问题。基于灰色GM(0,N)静态模型和BP神经网络模型,提出了一种新的参数估算方法即灰色神经网络判释法,由此分析了利用测井资料预测地层破裂压力的可行性。以H盆地中部气田为实例,综合应用现场试采测压资料和测井资料,建立了该气田石盒子组马家沟组地层破裂压力的灰色BP神经网络预测模型,成功地处理了该区25口气井(油井)资料。结果表明,该法简便好用,预测精度高,为应用测井资料预测地破裂层压力开拓了一条新的途径。     

模态理论的进展

传统模态理论的基本思想,近年来得到进一步发展和完善,并被引伸到非线性结构振动分析、应力应变振动分析等领域中,发展迅速．本文在总结近年来国内外文献的基础上,根据笔者自己的研究,较系统地介绍了线性位移实模态、复模态分析,广义模态分析,非线性结构系统模态分析,应力应变场模态分析等方面的研究情况．      

"洛管模式"对中国酒店经理人教育培训的启示

比照瑞士洛桑酒店管理学院的教育培训模式,从社会、旅游学院、旅游企业三方面分析造成中国酒店经理人教育培训"学用脱节"、"重量轻质"等问题的原因,并探讨相应对策改革旅游教育的办学理念与模式;明确培养目标,科学合理地设置课程体系与能力结构,优化师资队伍;创办企业大学等.     

一类Hassell模型的定性分析

研究了一类既具有功能性反应又有密度制约的非线性种群模型:=xg(x)-y渍(x), =y(-d+e渍(x)-q(y)),在g(x)和渍(x)是一类非线性函数以及q(y)是线性的情形下,讨论了该系统的平衡点的形态,且得出了极限环存在性、唯一性的一个充分条件。     

纵模分裂式正交偏振双频He-Ne激光器

在激光器谐振腔中放入单轴石英晶体,由于石英晶体对o光和e光的折射率的不同,所以,在同一谐振腔中o光和e光有不同的光程和谐振频率.将其称之为模式分裂效应.利用这一效应可以制成频率达几十兆赫兹的双频激光器.针对原有理论与实验结果之间的某些差异,建立了一套分析该种类型双频激光器的理论.根据所建立的理论着重分析了谐振腔光轴与晶轴夹角α对激光器频差的影响.并绘出了He-Ne激光管L<150nm和150nm相似文献   

Transverse mode competition in defect states of a waveguide with corrugated walls

We investigate the defect states arising in the Bragg and non-Bragg gaps by inserting a straight duct into a waveguide with periodically corrugated walls. In periodic waveguides, the Bragg gap is created by the interference of the same transverse modes whereas the different mode coupling leads to the non-Bragg one. Due to the involved high-order modes, there are two defect states observed in the non-Bragg gap while only one in the Bragg gap, indicating that transverse modes play a significant role in the creation of defect states. Furthermore, the frequency of each defect state highly relies on the defect geometries and their band widths can be optimized by the number of waveguide segments. The proposed transverse mode competition analysis reveals the mechanism of frequency shifting and provides an opportunity for guided wave control engineering, which would definitely benefit their applications in various functional devices, such as filters, sensors, and amplifiers.     

Mechanical properties,lattice thermal conductivity,infrared and Raman spectrum of the fullerite C24

Lightweight carbon materials with excellent thermal and mechanical properties have important applications in aerospace industry. In this study, the stability, mechanical properties, lattice thermal conductivity, electronic structure, infrared and Raman spectrum of sp³ hybridized low-density fullerite C₂₄ were investigated according to density functional theory (DFT) calculations. It was found that the fullerite C₂₄ was both thermodynamic and dynamic stable. Quasi-harmonic approximation and Grüneisen parameter calculations clarified why the fullerite C₂₄ had a positive thermal expansion coefficient at low temperature. The fullerite C₂₄ also exhibited excellent mechanical properties. Interestingly, the Vickers hardness of carbon allotropes was found to almost be linear proportional to the density of a carbon material. HSE06 electronic structure calculations showed that it was a semiconductor with direct bandgap of 2.56 eV. Anharmonic lattice dynamic calculations showed that its thermal conductivity was higher than semiconductor silicon. Besides, Raman and infrared active modes as well as the corresponding spectra were presented.     

高Q值薄壁液芯毛细管微腔电场传感器

为提高电场传感器的抗电磁干扰能力、灵敏度和稳定性,将高Q值薄壁液芯毛细管微腔和电泳效应结合,增强回音壁模共振微腔对外加电场的感知能力,并进行了实验验证.基于时域有限差分法得到了液芯毛细管微腔回音壁模式共振特性随毛细管直径、壁厚等结构参数的变化规律,发现随着壁厚变薄灵敏度增加.采用熔融拉锥法制备了直径为86μm,壁厚约为2μm的薄壁毛细管微腔,通过高精度位移平台实现了锥形光纤和毛细管微腔的高效率耦合,测得回音壁模式Q值为2.8×10^6.毛细管微腔内注入不同浓度的蛋白质溶液,利用电泳原理和蛋白质分子在缓冲溶液里带电的特性,实现的最大电场传感灵敏度为10.6 pm/(kV/m).