七年级电功及电功率的学习

关于电功及电功率的教材,在与学习苏联电力化的物理原理有关的知识范围中,占有重要的地位。这些概念的理解、关于它们的量度单位的清楚的观念以及进行有关的简单计算的技能应该是综合技术教育的必要组成部分。可惜,在七年级的物理教科书中,这个学习材料的叙述是形式的、干燥的、很简单的,并且从     

超声波及其应用

超声就是普通的弹性介质的机械扳动,这种振动以一定的速度传播并且具有一定的能量。超声波——是介质的互相更替的稠密和稀疏。超声的传播速度与介质的弹性和介质的密度有关。超声波的波长,也和普通的声波一样,决定于两相隣的稠密或稀疏之间的距离。超声频率的下限     

大气的激光监测

在人口稠密的工业区,大气污染已成为严重的问题,研究污染物以及它们和大气组分的反应已成为迫切的需要了.为了预示与日俱增的污染源对环境的影响和采取及时而有效的措施,需要建立大气的数学模型.这些模型的发展、完善和与之相关的连续监测,要求具有广泛的监测功能. 地球上的生命不仅直接或间接地受近地面的大气组分的影响,而且还受到平流层及平流层以上的大气组分的影响.要用合理的成本来恰当地监测这广阔的区域,为此激光监测是唯一可能提供这种功能的技术. 一、大气遥感技术的特点 激光器的发现促进了人们对物质的非线性特性的研究,以及关…     

开放教学资源下新的教学方式的探讨与尝试

网络时代信息是开放的、共享的和丰富的.网络时代的学习有其自身的特点.作为教育者,我们应该从教学的各个环节作出相应的改变,使我们的教学更加适应时代的发展,从而达到"授之以渔"的教育境界.基于这样的认识,我们在双语物理课的教学中有步骤地指导学生借助互联网上公开的、丰富的信息和学习资源进行课程的学习和课题研究.结果表明这种尝试极大地提高了学生的自我学习的能力和学习兴趣,起到了事半功倍的作用,弥补了课堂教学的不足.     

一种基于迈斯纳效应的超导电机的驱动力的计算

超导体的迈斯纳效应是超导体的特有的性质之一,超导驱动的电机正是利用超导体的这个性质而设计的一种新型电机,由于驱动原理与传统的电机有很大的不同,这种电机的驱动力的计算一直是这种超导电机设计中要解决的主要问题,针对一种结构的电机,利用理论分析和数值计算的方法计算了一种基于超导体迈斯纳效应的超导电机驱动力的大小,为这种电机的设计提供了主要依据。     

物理学和天文学

历史上，物理学和天文学的发展是密切联系的。它们在整个现代科学的发展和技术的发达上起到了先锋的作用。物理学的基本规律和天文学提供的广亵的实验室构成了理想的科学发展的基础。20世纪的一系列科学上的重要突破正是这种优良结合的产物。今天，天文学和物理学又共同面对着更新的前测问题，并一道酝酿着新的科学上的重大进展。它们所取得的每一个进展也必然伴随着技术的创新和提高，也不断更新着人类的认识和文明。     

时间,计时标准和原子时钟

一、时间和它的标准问题在这星球土发展、生存和繁衍的人类,他们起始有时间观念恐怕不比有空间的观念来得迟。这种时间观念存在的表现有时是非常自然的。人是生存在三维空间里的,但是人类思维的发展是动的,辩证地开展的,是四维空间的。人类对于时间的感觉,是从因时而异的物质变化而觉察得的。最简单的物质的变化是一种物体的运动。不要以为颐和园门前的铜狮是     

寂静地震与地震预测的物理问题

寂静地震是指发生了缓慢的位错、但几乎不辐射地震波的“地震” .在目前的地震预测的物理学研究中 ,通常是通过计算历史上曾经发生过的地震所引起的应力变化 ,或者通过研究地震活动的统计性质或“图像动力学” ,来推测一个断层带上发生地震的危险性 .寂静地震的信息的缺失 ,形成了地震预测的物理学研究中的一个很大的“盲区” ,而在相当程度上 ,解决地震预测的物理问题的主要困难和可能的突破的希望 ,也许就在于此 .寂静地震的研究目前还很不深入 .关于寂静地震的性质 ,文章作者提出两个猜想 :(1)寂静地震的频度 ,满足类似于GR定律的幂律分布 ;(2 )最大的寂静地震的地震矩 ,与“可见”的最大地震的地震矩相当 .     

基于低维相变薄膜的显示器件光学性质的研究

采用传输矩阵模型研究了基于低维相变薄膜的显示器件的光学特性与器件结构的关系。显示器件的类型有反射型和透射型,器件结构的关键参数包括Ge_2Sb_2Te_5(GST)层的厚度、ITO层的厚度、GST层的晶态与非晶态的变化。结果表明:对于反射型器件,ITO层的厚度对器件的反射光谱影响较大,可以通过改变ITO层的厚度达到改变器件颜色的效果;GST层的厚度为12 nm时,GST的晶态与非晶态的变化使器件有最好的颜色对比度且消耗较低的电功率。对于透射型器件,通过使用超薄的GST薄膜,器件的透明度可以保持很高,器件的透明度在GST的厚度超过几纳米后迅速下降。     

赝标Goldstone玻色子的手征拉氏量的 Gasser-Leutwyler系数

基于我们提出的参数化的完全穿衣服的夸克传播子,我们预言了未知的赝标Goldstone玻色子的手征拉氏量的Gasser-Leutwyler系数Li。预言的G-L系的数值与在文献中广泛应用的经验值和其他许多具有QCD特征的理论模型所预言的值一致。说明参数化的夸克传播子的适用性和可靠性。     

压电诱导型声光调制器中的电光效应

本文通过解压电效应的基本方程,应用一维近似理论,结合边界条件,得出压电共振晶体中电场是不均匀的,它将导致“电光栅”的产生。“电光栅”与“声光栅”可以相互耦合,产生“高次光栅”。压电诱导声光(PESD)调制器中的一次电光效应更有助于对入射光束的衍射和调制。实验结果证实本文结论。 关键词：     

The Separation Mechanism of Particles in a Smoke by an Electric Field

It was found that smoke particles smaller than 100nm and of different crystal structures can be separated by an electric field. Tungsten oxide smoke curved in the electric field towards the positive electrode plate. The morphology of the particles and dispersion of particles became good in the electric field. By burning of Pb in a mixture gas of Ar (80%) and O₂ (20%), red and yellow layer structure particles were simultaneously produced. The flow direction of red and yellow smokes changed by applying an electric field (200V/cm). Red particles flowed towards the negative plate and yellow particles flowed towards the positive plate, i.e. two different structures were separated. Simultaneous growth conditions of SnO and SnO₂ were observed and also found that they can be separated by the use of electric field as well as lead oxides. The curve of the smoke is discussed as that the surface net charge was affected by the electric field on the basis of produced particle structure and morphology.     

Linear Interaction (Transformation) of de Broglie Waves of the Γ- and X-Valleys and Intraband Optical Transitions in GaAs/AlAs Quantum-Well Heterostructures in a Lateral Electric Field

We discuss the linear interaction between the de Broglie waves of different electron valleys in heterostructures where a constant electric field is applied along the heterointerfaces (lateral field). The probabilities of phononless and dipole optical transitions of electrons between the - and X-subbands in GaAs/AlAs quantum-well heterosructures with a lateral electric field are calculated. It is shown that the electric field has a strong effect on the probabilities of phononless and direct optical dipole -X electron transitions. Moreover, a lateral electric field changes the spectrum of the intersubband -X light absorption, i.e., there is an intersubband analogue of the Franz-Keldysh effect. The considered linear interaction of de Broglie waves is compared with the well-known cases of linear wave interaction in a magnetized plasma, the Zener breakdown, and the Franz-Keldysh effect in solids.     

带电细圆环与导体球壳系统的场分布

先依电象法,推导均匀带电圆环在金属导体球壳内的"象电荷";再在球坐标系下,根据电场强度的计算公式与Tay-lor展开式,计算出均匀带电细圆环在全空间的电场分布的级数形式解;进而结合唯一性定理和电场的叠加原理,获得带电细圆环与导体球壳系统的空间场分布.     

High-frequency properties of KNiPO<Subscript>4</Subscript> in alternating magnetic and electric fields

The dependences of the antiferromagnetic resonance frequencies on the constant magnetic field H and constant electric field E are calculated for a KNiPO₄ crystal with spontaneous electric polarization and antiferromagnetic order. It is demonstrated that the KNiPO₄ crystal is characterized by an exchange-enhanced effect of the electric field E on the antiferromagnetic resonance frequencies. This effect is not revealed in the magnetoelectric materials studied earlier. It is established that oscillations of both magnetization and electric polarization exhibit resonance response at antiferromagnetic resonance frequencies. The expressions for these responses in alternating magnetic and electric fields are presented.     

The electric “Meissner effect” in spin superconductor

Spin superconductivity results from the condensation of spin-triplet but charge neutralparticles (e.g., triplet excitons). We present a Laplace-type equation describingelectrostatic properties of spin superconductors. With the phenomenological equationsobtained, we show that there exists an electric “Meissner effect” against the spatialvariation of the electric field along the magnetic moment direction, in particular,(?·?)(?·E). Severaldistinctive characteristics of this electric “Meissner effect” emerge in spinsuperconductors. Firstly, the variation of the electric field(?·?)(?·E) has an abruptdecrease at the boundary, which is analogous to the screen effect for electric fieldE in a uniform dielectric material. Secondly, thesuper-spin current distributes inside or near the boundaries of a spin superconductor,which depends on the magnitude of gradient for the external driven electric field.     

线电荷与介质圆柱所形成的电场

在线电荷电场的电势调和展开式的基础上,得出线电荷电场内存在介质圆柱时电势的级数解.并以此来分析长直线电荷与介质圆柱所形成的电场的电像,从而给出电势与电像有关的解析表达式,进一步得出等势线(面)与电场线方程,并利用软件MATLAB绘制出电场线和等势线图予以验证.     

Effect of an electric field on photoluminescence of cadmium selenide nanocrystals

We have demonstrated a difference in the nature of the effect of a strong external electric field (>10⁵ V/cm) on the photoluminescence of cadmium selenide nanoparticles of different shapes. We have determined a correlation between the magnitude of the external electric field and the average photoluminescence decay time for two types of nanoparticles: "quantum dots" and nanorods. We discuss the mechanism for the effect of an electric field on the photoluminescence of both types of nanoparticles.     

Untersuchung von elektrischer Hyperfeinstruktur-Wechselwirkung in Hafniumammoniumhexafluorid-Einkristallen durch γγ-Winkelkorrelationsmessungen

The angular correlation of the 133 keV-482 keV-yy-cascade in the decay of Hf¹⁸¹ is strongly attenuated if solid sources of hafniumammoniumhexafluoride are used. The unperturbed correlation was observed however when a single crystal of hafniumammoniumhexafluoride was used whose main axis pointed into the direction of one of the two detectors. This proves that the perturbation is static and that the maximum component of the electric field gradient at the position of the hafnium nucleus coincides with the direction of the main axis of the crystal. The anisotropy of the angular correlation was measured as a function of the direction of the crystal axis. The results agree with the theoretical predicted functions for a strong electric quadrupole interaction. Then we combined the intrinsic electric field with an external magnetic field. The magnetic field direction was chosen parallel to thez-axis of the electric field gradient and perpendicular to the plane of the detectors. The theory for axially symmetric field gradients predicts a maximum of the anisotropy of the angular correlation for a magnetic field strength at which resonance exists between electric and magnetic precession. For a strong electric interaction the maxium anisotropy has half the value of the unperturbed correlation. In our case the electric quadrupole interaction was so strong that we could not reach the resonance even when we applied external magnetic fields up to 48000 gauss. The observed anisotropies were too large however to be fitted by theoretical curves which were calculated under the assumption that the field gradient has axial symmetry. Therefore we developed the theory for non-axially symmetric electric field gradients. Now a fit was possible and gave unique solutions for the strength of the electric hyperfine interaction as well as for the asymmetry coefficient of the electric field gradient tensor. The accuray of these results was not very high but the strength of the electric hyperfine interaction was found to be small enough to make a direct observation of the electric spin rotation by the differential angular correlation method possible. The observed pattern confirmed the non-axially symmetry of the electric field gradient and we derived the following parameters:

$$\omega _{E_0 } = \left( {570 \pm 30} \right)MHz\left( {\omega _{E_0 } = electric interaction frequency = \frac{{6eQ \cdot \left| {V_{zz} } \right|}}{{4I \cdot \left( {2I - 1} \right) \cdot \rlap{--} h}}} \right)$$     

Tunable magnetic interaction by an applied electric field in a Co-adsorbed SiC monolayer

The magnetic properties of Co-adsorbed SiC monolayer under an external electric field are investigated using first-principles method. In the absence of the electric field, the interaction between two Co atoms is ferromagnetic, which is originated by the p?d hybridization between Co and its neighboring C and Si atoms. When an electric field was introduced along the c axis, the interaction between two Co dopants switched from ferromagnetic to antiferromagnetic, which could be dominated by the competition between p?d exchange and superexchange. Moreover, the magnetic anisotropy prefers to parallel to the a axis and it seems not to be turn into the c axis under the electric field.