电动机旋转磁场是发电机旋转磁场的跟随器

三相交流发电机与三相异步电动机都采用星形连接,分析旋转磁场和三相异步电动机的正反转.结果表明:电动机旋转磁场是发电机旋转磁场的跟随器.     

浅谈家用吊扇的调速方法

家用吊扇的核心部分是单相异步电动机,此绕组如图1,有一主绕组(工作绕组)与一串联电容器C的副绕组(启动绕组)相并联.这样做可使二绕组的电流在相位上相差90°,从而形成旋转磁场.转子的转动过程与三相异步电动机相似.     

三相异步电动机变频调速实验装置

三相异步电动机变频调速实验装置黄灿，秦光戎（北京师范大学物理系１００８７５）交流异步电动机应用非常广泛．变频调速是三相交流异步电动机无级变速的一种重要方法．变频调速操作方便，调速范围广，转速稳定，对电网的干扰小并能以最佳转矩启动．与其它调速方式相比具...     

三相异步电动机的断相保护

断相运行问题是三相电动机运行中的最大安全问题之一,且发生频率较高,一旦发生会造成电机损坏,直接影响生产,造成较大的经济损失。通过对电机控制电路的改进和使用单片机控制技术,较好地解决了三相异步电动机的断相保护问题,取得较好的效果。     

介绍一种三相旋转磁场的简易演示方法

三相旋转磁场的建立和三相异步感应电动机的动作原理的演示需要三相交流电源,而一般中学不见得都有三相电源,这里介绍一种不用三相电源进行演示的办法。三相交流电流是在时间上相位互差120°的三种交流电流,这样的交流电流通入到空间互隔120°角的三个线圈(见图1),便能在其中建立起旋转磁场。如果在线圈的中心轴线处,支撑起能够自由迴转的闭合导体(如铝框、铜质小鼠笼),便能旋转起来。三相交流电流可以用三个相位差120°的旋转矢量来表示,即I_A,I_B,I_C(见图2)。在单相     

费拉里斯（Ferraris，Galileo，1847—1897）意大利物理学家（Physicist，Italy）

1885年，费拉里斯根据旋转磁场原理，发明了交流感应电动机，为电力工业的应用和发展开辟了一条广阔的道路。     

如何开三相异步电动机的定子绕组实验

如何开三相异步电动机的定子绕组实验张吉龙（贵州省遵义师专物理系５６３００２）在《电工学》中，“三相异步电动机的定于绕组”部份是非常重要的内容．要使学生掌握好这一内容，必须让学生动手拆装电动机定子绕组．在实验室中进行这一实验，耗时多，材料消耗大，在《电...     

三相异步电动机一相绕组短路后另二相绕组组合运行分析

当三相异步电动机正常运行时因某种原因一相绕组烧毁,通过对剩下二相绕组重新组合的3 种方法进行分析,发现其中二相零接法在适当降低负载功率情况下,电机可连续运行.     

用互馈法测异步电动机的效率

用互馈法测异步电动机的效率陶颐德（江西九江师范专科学校３３２０００）做异步电动机的效率和温升实验时要选配一个适当的负载，对于容量较大的电动机要找到一个较大的合适负载就很困难，而且消耗电能较多．如果用一台相同的或者差不多容量的电动机作为负载，那么不仅可...     

三相交流电机综合演示器

一、作用能演示三相交流电机的基本原理。如单相、三相交流电的产生,旋转磁场的产生,同步、感应电动机的原理与换向,星形及三角形电路的联接。由于采取逐步增添的方法演示三相交流电机的基本原理和充分利用一个模型进行综合演     

Near field acoustic solution of a rotating point source in frequency domain

I.IntroductionAerodyntalcnoiseofturbomaChinrynotoalythectstheenvironmentbutalsosometimesresultsinstructuredamage.Aeroacoustics,asaintewhsciPlineofacousticsandaerodynamics,isattractingmorandmoreatteDtionandresearch.TherearetwoimportalltcontentsonthenoiseproducingmechAnsmsinaeroacousticproblem.OneisaboutthesourcesofnoiseinturbomachinryGenetallytherearethreetyPesofsources:thickness,forceandturbulencestress,correspondingrespectivelyTomonopole,dipoleandquadruplesourcesThelatertwokindsofsourcesh…     

旋转运动点声源近场声学频域解

本文在任意运动点源声辐射频域解基础上，得到旋转运动声源近场声学的一个近似解。如果旋转半径相对于场声波是紧致的，此解就可以表示为在远场解基础上叠加三项近场修正项。根据此解，本文得到适合于近场的自由空间Ｇｒｅｅｎ函数，由此讨论了声源旋转导致的声场方向性特征，研究了声源位置及源频率以及旋转频率等对近场声学结构的影响。     

Dynamics of a nonmagnetic drop suspended in a magnetic fluid in a rotating magnetic field

The behavior of a nonmagnetic drop suspended in a magnetic fluid and subjected to the action of a rotating magnetic field is studied experimentally. The configurations of the drop in the form of prolate and oblate ellipsoids of revolution in the rotating field are investigated, and disintegration of the drop in the rotating field and the development of comb instability of its surface under certain conditions are observed.     

Thermodynamic properties of rotating trapped ideal Bose gases

Ultracold atomic gases can be spined up either by confining them in rotating frame, or by introducing “synthetic” magnetic field. In this paper, thermodynamics of rotating ideal Bose gases are investigated within truncated-summation approach which keeps to take into account the discrete nature of energy levels, rather than to approximate the summation over single-particle energy levels by an integral as it does in semi-classical approximation. Our results show that Bose gases in rotating frame exhibit much stronger dependence on rotation frequency than those in “synthetic” magnetic field. Consequently, BEC can be more easily suppressed in rotating frame than in “synthetic” magnetic field.     

Black holes: a physical route to the Kerr metric

As a consequence of Birkhoff's theorem, the exterior gravitational field of a spherically symmetric star or black hole is always given by the Schwarzschild metric. In contrast, the exterior gravitational field of a rotating (axisymmetric) star differs, in general, from the Kerr metric, which describes a stationary, rotating black hole. In this paper I discuss the possibility of a quasi–stationary transition from rotating equilibrium configurations of normal matter to rotating bla ck holes.     

Dynamics of superparamagnetic filaments with finite magnetic relaxation time

In this paper we formulate a model of superparamagnetic filaments with internal dissipative torques due to the action of a rotating magnetic field. It is shown that spirals are formed at both ends of the filament due to the action of the internal torques. These spirals propagate to the center of the filament and collide, forming a compact cluster that rotates in accordance with the rotating magnetic field. These results are in agreement with recent experiments with chains of superparamagnetic beads in a rotating magnetic field.     

Diffusion of magnetotactic bacterium in rotating magnetic field

Swimming trajectory of a magnetotactic bacterium in a rotating magnetic field is a circle. Random reversals of the direction of the bacterium motion induces a random walk of the curvature center of the trajectory. In assumption of the distribution of the switching events according to the Poisson process the diffusion coefficient is calculated in dependence on the frequency of the rotating field and the characteristic time between the switching events. It is confirmed by the numerical simulation of the random walk of the bacterium in the rotating magnetic field.     

虚光子过程对“两个二能级原子-单模光场”相互作用系统场熵演化特性的影响

利用全量子理论,研究了非旋波近似下两个二能级原子与单模光场相互作用过程中受激场场熵的演化规律,通过与旋波近似下的相应结果进行比较,进一步揭示出非旋波近似条件下虚光子过程对场熵演化特性的影响.     

Rotating relativistic electron beam-plasma interaction and formation of a field-reversed configuration

Experimental results on interaction of a rotating relativistic electron beam with plasma and neutral gas are presented. The rotating relativistic electron beam has been propagated up to a distance of 150 cm in a plasma. The response of the plasma to the rotating electron beam is found to be of magnetic diffusion type over a plasma density range 10¹¹–10¹³ cm⁻³. Excitation of the axial and azimuthal return currents by the rotating beam and subsequent trapping of the azimuthal return current layer by the magnetic mirror field are observed. A field-reversed configuration has been formed by the rotating relativistic electron beam when injected into neutral hydrogen gas. We have observed field reversal up to three times the initial field in an axial length of 100 cm.     

Phase diagrams for the precession states of the nanoparticle magnetization in a rotating magnetic field

Using the analytical and numerical solutions of the Landau–Lifshitz equation, we calculate the phase diagrams for the precession states of the nanoparticle magnetization in a rotating magnetic field. We show that there are three different scenarios for the magnetization switching. The bias magnetic field applied antiparallel to the nanoparticle magnetization strongly decreases the switching amplitudes and frequencies of the rotating field.