太阳能无线输电演示仪的研制

应用电磁学理论以及电子技术自制了一套太阳能无线输电演示实验仪。该演示仪由太阳能进行供电,利用电磁耦合共振技术,实现了电能的无线传输。通过增加数码管电压-电流显示电路,可以定量显示电能传输随距离变化的效果,能精确而直观地演示电能无线传输的物理现象。该仪器结构简单、性能稳定、操作方便,可广泛用于课堂演示、课程设计等目的,在实际应用中取得了良好的教学效果。     

微型物理演示实验箱的研制与应用

介绍了电磁学演示实验工具箱的构建方法,本套仪器设计了13个有代表性的电磁学演示实验微型模块。实验仪器安全便捷、易于操作,适合于大学物理课堂教学与实验.     

磁悬浮演示实验仪

应用电磁学理论、机械力学以及电子技术自制了一套磁悬浮演示实验仪.该演示实验仪利用线性霍尔传感器来探测悬浮物体的位移,以达到控制悬浮的目的,添加数码管电压显示电路,定量显示电磁铁的磁性在悬浮过程中随悬浮物位置变化的自动调整,能精确而直观地演示磁悬浮的物理现象.该仪器结构简单、性能稳定、操作方便,能广泛用于课堂演示、课程设...     

创新集成化电磁学演示实验教具的设计与制作

高中物理电磁学部分有许多具有相似性质和相同仪器的演示实验,通过创新设计,将电磁学的部分实验集成化到一个教具中,教师可以根据自身需求,利用开关的闭合,选择不同的实验进行演示.该集成化教具能够帮助教师减少准备实验的时间,具有便捷、演示效果好和成本低等优点.     

利用钕铁硼磁体制作单极电动演示仪器

本文介绍了使用钕铁硼磁体自制的几种单极电动演示仪器,包括：单极电动机、单极电动小车、单极电动风扇。给出了演示仪器的结构图,用经典电磁理论分析了单极电动的原理。该演示仪器制作方法简单且成本低,适合电磁学的教学使用。     

基于线性霍尔传感器的太阳能磁悬浮演示仪

应用电磁学理论、机械力学以及电子技术自制了一套太阳能磁悬浮演示仪,该演示实验仪由太阳能电池供电,利用线性霍尔传感器来探测悬浮物体的位移,以达到控制悬浮的目的,添加数码管电压显示电路,可以定量显示电磁铁的磁性在悬浮过程中随悬浮物位置变化的自动调整,能精确而直观地演示磁悬浮的物理现象该仪器结构简单、性能稳定、操作方便,能广...     

电能无线传输实验仪

正电磁学实验固体物理专业实验电气、电工专业实验仪器简介近年来,电能无线传输技术受到人们越来越多的关注,国内外关于电能无线传输方面的研究在深度和广度两方面都取得了很大进展,并应用于电动汽车充电、无线充电式家用电器和医学仪器等领域。     

自制亥姆霍兹线圈的设计与应用研究

电磁学是高中物理教学的重点和难点,有效地开展实验教学是解决难点的重要手段. 电磁学演示实验 中经常需要磁场,而常规的实验器材因为提供的磁场范围小、不均匀,影响了演示效果. 自制可旋转亥姆霍兹线圈, 结合教学进行应用研究,是提高这类实验演示效果的一个途径     

电磁学教学必须重视演示实验

阐述了电磁学演示实验的重要性及提高高校电磁学演示实验水平的途径.     

杭州精科仪器有限公司

杭州精科仪器有限公司，位于杭州富阳，系浙江省科技型企业。专业从事大专院校物理实验仪器的开发和生产。主要生产力学，热学、声学、电磁学。设计性、演示性物理等方面仪器。     

Parameters of an erosion carbon plasma in the channel of a railgun

The working current dependences of the thermodynamic and electrophysical parameters of a free plasma piston moving with a near-maximal velocity in the channel of an electromagnetic rail launcher with graphite electrodes are obtained. The composition and weight of the plasma depend on the degree of electrode erosion due to discharge current passage (i = 40–80 kA). It is shown that the mean temperature of the plasma piston only slightly depends on the plasma mean pressure and plasma piston weight and increases with current by a near-power law. The measured values of the maximal velocity of the plasma piston front are compared with the calculated value of the sound velocity inside the piston. With the working current and cross-sectional area of the channel fixed, the initial gas density in the channel is found to influence the ratio of the piston maximal velocity to the sound velocity in the plasma. If the initial gas density is low (lower than some critical value), the maximal velocity of the plasma piston front exceeds the sound velocity in the plasma.     

Semi-active particle-based damping systems controlled by magnetic fields

This paper reports the design of a semi-active particle-based damping system in which a dry magnetic particle bed is used to dissipate the energy of a vibrating piston. The system is magnetized by a magnetic field generated by an electromagnetic coil. Hysteresis-free, ferromagnetic materials are selected for both the piston and particles. The damping efficiency increases as the magnetization of the piston and particles increases up to saturation. Semi-active control is achieved by varying the electric current supplied to the coil, which changes the magnetization and allows for real-time tunability of the damping rate. During the process of magnetization and demagnetization, the damping is reversible and temperature-independent over a wide temperature range. This system can be useful in aerospace, automobile and structural engineering applications, particularly in harsh environments.     

Simulation of laser oscillation in a two-layer microcavity with a semiconductor nanostructure shell

A theoretical model that describes the transformation of electromagnetic radiation by microcavities in the form of microspheres with a semiconductor nanostructure shell is developed. It is established that the regime of bistable two-mode laser oscillation due to morphology-dependent resonances with different quality factors and spatial distributions of the electromagnetic field can be implemented in a two-layer microcavity with a semiconductor-nanostructure shell. The region of two-mode oscillation and the relation between the intensities of oscillating modes depend on the indices of refraction and the sizes of the microparticle core and shell.     

Finite-temperature Casimir effect in piston geometry and its classical limit

We consider the Casimir force acting on a d-dimensional rectangular piston due to a massless scalar field with periodic, Dirichlet and Neumann boundary conditions and an electromagnetic field with perfect electric-conductor and perfect magnetic-conductor boundary conditions. The Casimir energy in a rectangular cavity is derived using the cut-off method. It is shown that the divergent part of the Casimir energy does not contribute to the Casimir force acting on the piston, thus renders an unambiguously defined Casimir force acting on the piston. At any temperature, it is found that the Casimir force acting on the piston increases from −∞ to 0 when the separation a between the piston and the opposite wall increases from 0 to ∞. This implies that the Casimir force is always an attractive force pulling the piston towards the closer wall, and the magnitude of the force gets larger as the separation a gets smaller. Explicit exact expressions for the Casimir force for small and large plate separations and for low and high temperatures are computed. The limits of the Casimir force acting on the piston when some pairs of transversal plates are large are also derived. An interesting result regarding the influence of temperature is that in contrast to the conventional result that the leading term of the Casimir force acting on a wall of a rectangular cavity at high temperature is the Stefan–Boltzmann (or black-body radiation) term which is of order T ^d+1, it is found that the contributions of this term from the two regions separating the piston cancel with each other in the case of piston. The high-temperature leading-order term of the Casimir force acting on the piston is of order T, which shows that the Casimir force has a nontrivial classical ℏ→0 limit. Explicit formulas for the classical limit are computed.     

Szilard's demon revisited

We show that piston fluctuations are of crucial importance in the analysis of a Szilard engine. Some engines which do not require information in order to perform a Szilard cycle actually do not work. We pinpoint the mechanism and stages which require work investment when a measuring instrument is reset.     

The covariant electromagnetic Casimir effect for real conducting cylindrical shells

Using covariant quantization of the electromagnetic field, the Casimir force per unit area experienced by a long conducting cylindrical shell, under both Dirichlet and Neumann boundary conditions, is calculated. The renormalization procedure is based on the plasma cut-off frequency for real conductors. The real case of a gold (silver) cylindrical shell is considered and the corresponding electromagnetic Casimir pressure is computed. It is discussed that the Dirichlet and Neumann problems should be considered separately without adding their corresponding results.     

金属包裹纳米微粒的光学特性研究(英文)

金属包裹纳米粒子是一种纳米量级的介质球核外包裹薄金属层的纳米粒子.在本文中,Au包裹Au₂S纳米粒子被抽象成微型电磁谐振腔,其谐振波长决定于Au₂S介质球核的半径.运用经典电磁理论可以得到谐振波长和谐振能量.由于Au包层很薄(2nm),这种微型谐振腔的耦合方式是有别于传统方式的透射耦合,因此Au包层的厚度决定了谐振的能量以及谐振腔品质因子Q.此外,本文还讨论了吸收峰的线宽.     

Simulation of the wave-absorbing model of a carbonyl iron / silver-coated core–shell structure

The microwave-absorbing performances of carbonyl iron powder / silver core–shell composite particles are studied on the basis of the electromagnetic scattering theory and the energy conservation law. In addition, a calculation method for reflection loss of the carbonyl iron powder / silver core–shell composite particles with microwave is proposed. The calculated reflection loss of the carbonyl iron powder / silver core–shell composite particles is compared with the experimental results. The findings show that the trend of reflection loss of the carbonyl iron powder / silver composite particles can be predicted which can subsequently provide a relevant reference for future experiment and calculation of the absorbing mechanism of electromagnetic wave-microscopic carbonyl iron powder / silver core–shell composite particles.