液体中光击穿所激发声场的理论研究

以液体中光击穿所激发声场为研究对象,在等离子体椭球模型的基础上,为方便理论计算,简化等离子体椭球模型,提出了等离子体椭圆盘模型,对光击穿所激发声场进行了理论研究.得到了等离子体椭圆盘辐射声场的声压规律,并利用椭圆坐标变换,依据马修函数特性和模态的正交性,求得了等离子体椭圆盘振动位移的解析表达式.     

液体中光击穿所激发声场的方向性研究

从液体中光击穿所激发声场的柱体模型和靶盘模型出发,运用声学基础的理论原理,提出了等离子体椭球模型,对光击穿所激发声场的方向性进行了理论研究.通过MATLAB仿真得到此声场的方向特性图,进而分析和比较了能量不同、照射区域大小不同的激光束所激发声场的方向性.研究表明等离子体椭球模型更符合实验情况.     

液体中光击穿所激发声场的方向性研究

从液体中光击穿所激发声场的柱体模型和靶盘模型出发,运用声学基础的理论原理,提出了等离子体椭球模型,对光击穿所激发声场的方向性进行了理论研究.通过MATLAB仿真得到此声场的方向特性图,进而分析和比较了能量不同、照射区域大小不同的激光束所激发声场的方向性.研究表明等离子体椭球模型更符合实验情况.     

液体中光击穿阈值的研究

从等离子体中自由电子密度速率方程出发,考虑到脉冲激光在聚焦区域的特征以及液体中光击穿的实验情况,提出了等离子体椭球模型.通过该模型的建立,对自由电子密度速率方程中电子扩散速率进行了修正,在理论上得到了光击穿的阈值.结果表明,等离子体椭球模型计算出水的击穿阈值更符合实验情况.     

液体中光击穿阈值的研究

从等离子体中自由电子密度速率方程出发,考虑到脉冲激光在聚焦区域的特征以及液体中光击穿的实验情况,提出了等离子体椭球模型.通过该模型的建立,对自由电子密度速率方程中电子扩散速率进行了修正,在理论上得到了光击穿的阈值.结果表明,等离子体椭球模型计算出水的击穿阈值更符合实验情况.     

水下光击穿所激发的声场的方向特性

本文对水中光击穿时所激发的声场的指向特性进行了理论和实验研究。理论分析是根据下述模型:一系列含等离子体的球形小腔体均匀分布在一条短直线段上,并且每一个腔体可看作是一个点脉冲声源。文中给出了声脉冲信号幅度与宽度和接收方向之间的理论关系式,理论分析较好地描述了实验测量结果。     

广义坐标变换在普通物理学中的一些应用

文章举例阐述了广义坐标变换在力学和电磁学中的一些应用.应用广义极坐标变换和广义球坐标变换计算线椭圆环、椭圆盘和椭球刚体对任意轴的转动惯量;应用电多极展开的具体形式结合广义坐标变换,计算均匀带电线椭圆环、椭圆盘和椭球在远场处的电势.     

浅析椭圆盘及椭球体的转动惯量

给出椭圆盘和椭球体对于过质心任意轴的转动惯量公式的新形式,并由此导出椭圆和椭球的一种几何性质     

浅析椭圆盘及椭球体的转动惯量

给出椭圆盘和椭球体对于过质心任意轴的转动惯量公式的新形式,并由此导出椭圆和椭球的一种几何性质。     

高频调制电弧的声学特性及其细化焊缝组织的应用

以等离子体电弧作为声源,利用高频电流进行调制,激发电弧可以产生超声波。研究了高频调制电弧的激发特性和声场特征,发现调制电弧所发射超声波在激励频段内呈现平坦的幅频特性,激励电流是影响电弧超声强度的主要因素,声压幅值与电弧等离子体流力的变化量成正比,声场呈现轴向强两侧弱的特征。同时介绍了利用电弧激发超声波在改善焊缝组织性能方面的应用。     

强电场下气泡形变对液体绝缘的影响

 基于液体气泡击穿的椭球模型,推导了气泡形变的流体动力学方程;利用软件Comsol模拟了气泡受力后的形变;根据模拟结果,结合气体击穿的帕邢定律,讨论了气泡形变对液体绝缘的影响。结果表明:气泡在静电引力和表面张力的作用下,沿电场线方向拉伸成椭球,椭球长短轴之比与外加电场强度和气泡初始半径成正比;形变导致电场方向气体通道延长,气泡更容易击穿,外加气压是避免气泡击穿的有效途径之一,外加气压的大小与电场强度和气泡初始半径成正比。     

Non-contact acoustic tests based on nanosecond laser ablation: Generation of a pulse sound source with a small amplitude

A method to generate a pulse sound source for acoustic tests based on nanosecond laser ablation with a plasma plume is discussed. Irradiating a solid surface with a laser beam expands a high-temperature plasma plume composed of free electrons, ionized atoms, etc. at a high velocity throughout ambient air. The shockwave generated by the plasma plume becomes the pulse sound source. A laser ablation sound source has two features. Because laser ablation is induced when the laser fluence reaches 10¹²–10¹⁴ W/m², which is less than that for laser-induced breakdown (10¹⁵ W/m²), laser ablation can generate a lower sound pressure, and the sound source has a hemispherical radiation pattern on the surface where laser ablation is generated. Additionally, another feature is that laser-induced breakdown sound sources can fluctuate, whereas laser ablation sound sources do not because laser ablation is produced at a laser beam–irradiation point. We validate this laser ablation method for acoustic tests by comparing the measured and theoretical resonant frequencies of an impedance tube.     

The two-fluid model with superfluid entropy

Summary The two-fluid model of liquid helium is generalized to the case that the superfluid fraction has a small entropy content. We present theoretical arguments in favour of such a small superfluid entropy. In the generalized two-fluid model various sound modes of He II are investigated. In a superleak carrying a persistent current the superfluid entropy leads to a new sound mode which we call sixth sound. The relation between the sixth sound and the superfluid entropy is discussed in detail.     

A simple scattering model for measuring particle mass fractions in multiphase flows

In this paper we present a simple theoretical model of how pulsed ultrasound is attenuated by the particles in a solid/liquid flow. The theoretical model is then used to predict the attenuation of sound, given the mass fraction, the density, and the size distribution of the solid particles. The model is verified experimentally for suspensions of 0-10% (by mass) Dolomite ((Ca,Mg)CO3) particles and water. The experimental results show that the attenuation of sound due to particles varies linearly with mass fraction, and that the proposed theoretical model can be used to predict this attenuation. In all experiments the transmitter and receiver array were clamped onto the pipe wall, thus providing a completely non-invasive and non-intrusive measurement technique.     

Optical breakdown in a liquid: The slow phase of the dynamics of cavity collapse and a noncontact technique for pressure measurement in a liquid

It is demonstrated that, in the case of optically probing the breakdown region, a pulsed signal is formed due to the acoustic pulses produced by the breakdown and collapse of the cavitation cavity. The measured dependence of the delay time of the second pulse on the hydrostatic pressure in the liquid and the pressure of saturated vapor agrees well with the theoretical dependence corresponding to the hydrodynamic model of the cavity. On the basis of the optical cavitation effect, a technique is proposed for a noncontact measurement of hydrostatic pressure in a liquid enclosed in a sealed cell. The range of applicability of the technique is evaluated.     

Initiation of Electrical Breakdown by Ionic Bombardment in a Vacuum Gap after Arc Extinction

This report presents a theoretical model of development of the post-arc gap breakdown in vacuum as a result of surface processes following cathode bombardment by energetic ions flowing from residual plasma after zero arc current. The most important surface processes for this model are sputtering and secondary electron emission. For a considerable group of metals, the sputtering yield Sr and secondary electron emission ?c can assume relatively high values when the ions have a high energy. Based on the ion flux from the plasma and the time of its flow as well as the ionization of sputtered atoms, a quantitative criterion for a breakdown will be derived. It has been proven that breakdown will occur if there is at least a minimum ion charge Qi which is dependent on the product of Sr · ?c. Qualitative consistency was also demonstrated between experimental results and the conclusion derived from our breakdown criterion.