一个地球自转变化问题引起的思考

探索汽车向北行驶时引起地球动能变化的动力学原因.     

细数“嫦娥一号”的八大宝贝

2007年10月24日18时5分,中国第一颗探月卫星“嫦娥一号”在四川西昌卫星发射中心成功升空。在克服了可靠性、无法预知的空间环境风险和技术方面可能的不确定性等诸多威胁,历时十天,经过多次变轨、中途修正、近月制动、捕获月球等数百个动作,“嫦娥一号”终于扑入了月球的怀抱。又经过多次调整,“嫦娥一号”进入了周期为127分钟、高为200千米的环月轨道。     

工科专业大学物理教学中的课程思政——以“角动量守恒定律”为例

以工科专业的大学物理中“刚体定轴转动的角动量定理和角动量守恒定律”为例,展示了如何在不同的课堂教学环节进行思政教育的融入.在引课环节、知识讲授环节和知识应用环节,主要从以下几个方面对学生进行思政教育：激发学生的民族自信心和自豪感,鼓励学生树立科技报国的远大志向;培养学生勇于探索、多角度考虑问题的素养,建立唯物主义世界观;鼓励学生不畏困难、不断超越自我的奋斗精神.思政教育的融入使得课堂教学更加饱满,达到了“教书”和“育人”的双重目的.     

带电粒子在电场中做锥摆式运动的分析

对在点电荷的电场中作匀速圆周运动的带电粒子，在加上一匀强电场后运动状况的复杂性进行分析，并阐述了要使该粒子作锥摆式运动的条件。     

电磁场角动量守恒定律的又一例

处于外磁场中圆柱形带电体，当外磁场变化时，带电体将旋转，本文分别用电磁体系的能量守恒和角动量守恒对其进行讨论，说明它们的一致。     

课程思政理念融入高校物理教学的实践探析——以“角动量守恒”为例

课程思政理念融入物理教学是高校实现“三全育人”要求的重要途径,可以培养学生科学的思维方式和严谨的科学认知态度,全面提升学生科学素养.以大学物理课程中“角动量守恒”一节为例,详细介绍了教学设计思路和在物理教学中如何融入思政育人元素,实现课程育人与思政育人的协同作用.     

天体的旋进与角动量守恒

通过非惯性系中的角动量定理和惯性系中的角动量守恒定律分析天体的旋进,指出地轴的旋进与卫星轨道平面的旋进这两种现象同根同源,相互依存.     

一种刚体角动量守恒演示仪的设计制作

本文就一种刚体角动量守恒演示仪的制作进行了阐述,为相关仪器的制作提供了参考,交流了制作经验.     

“嫦娥一号”上的科学探测仪器

“嫦娥一号”上搭载了8种24台件科学探测仪器，重130kg，即微波探测仪系统、γ射线谱仪、X射线谱仪、激光高度计、太阳高能粒子探测器、太阳风离子探测器、CCD立体相机、干涉成像光谱仪．     

嫦娥一号卫星干涉成像光谱仪时序设计

介绍了基于Actel反熔丝FPGA的嫦娥一号卫星干涉成像光谱仪时序控制模块设计.概述了时序控制模块的功能要求,详细描述了时序控制模块外部时序接口和内部时序接口,给出了时序控制模块设计的参量配置、逻辑结构和简要结果.各项地面试验和一年的在轨飞行结果表明该设计合理可靠.     

Nontopological finite temperature induced fermion number

We show that while the zero temperature induced fermion number in a chiral sigma model background depends only on the asymptotic values of the chiral field, at finite temperature the induced fermion number depends also on the detailed shape of the chiral background. We resum the leading low temperature terms to all orders in the derivative expansion, producing a simple result that can be interpreted physically as the different effect of the chiral background on virtual pairs of the Dirac sea and on the real particles of the thermal plasma. By contrast, for a kink background, not of sigma model form, the finite T induced fermion number is temperature dependent but topological.     

关于《一道习题的两种解法》的补充

《物理通报》1998年第7期刊登了邓文清同志《一道习题的两种解法》的文章，原文给出了两种解法．作为该文的补充，笔者再给出一种解法．     

Soliton and boundary condition induced fractional fermion number

We show that for a fermion in a bounded background potential in a finite box, eigenvalues of the total charge are independent of whether the potential is solitonic and depend only on the boundary condition: half-odd integral or integral for charge conjugation (C) invariant boundary conditions and an arbitrary fraction forC non-invariant boundary conditions. Fractional fermion numbers for infinite space Jackiw-Rebbi and Goldstone-Wilczek Hamiltonians are reproduced in finite space by using boundary conditions different from the periodic ones of Rajaraman and Bell.     

The systematics of possibly narrow quark states with baryon number one

We discuss the systematics of hadronic colour singlets consisting of four quarks and an antiquark. For the configurations that could give narrow colour isomer states we compute relative mass splittings between different flavour multiplets, discuss production possibilities and cross sections. Such states have, perhaps, already been observed.     

Double transmission peaks electromagnetically induced transparency induced by simultaneously exciting the electric and magnetic resonance in one unit cell

In this paper, we investigate a metamaterial formed by a planar array of a metallic L-shaped structure and a cut wire(CW), which behaves as an analogue of the electromagnetically induced transparency(EIT). The double transmission peaks are formed by the destructive interference of two bright-modes and a quasi-dark mode. The two bright-modes are respectively excited by the L-shaped structure and CW. The unit structure itself performs a quasi-dark mode. The group refractive indexes are over 20 in the first transmission peak, and 117 in the second transmission peak, thus offering potential applications in slow light devices. Finally, all the above characteristics are achieved in just one simple unit cell.     

激光冲击强化“残余应力洞”的形成机制

利用ABAQUS有限元软件进行了单个圆形高斯光斑的激光冲击强化数值模拟,分析材料表面光斑中心区域形成的"残余应力洞"现象,并通过分析材料的动态力学响应特征揭示了"残余应力洞"的形成机制。结果表明:在冲击波加载时,光斑边界处会产生很强的剪切应力,形成向四周传播的表面稀疏波和向材料内部传播的剪切波。当稀疏波同时传播到光斑中心,发生相遇、汇聚,使材料产生急剧的上下位移过程,造成冲击波加载塑性变形后的二次塑性变形。二次塑性变形中形成了较大的剪切塑性应变,并降低了冲击波加载阶段产生的轴向和径向塑性应变,使残余压应力降低,从而形成"残余应力洞"。