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1.
声致发光   总被引:1,自引:0,他引:1       下载免费PDF全文
李化茂  冯若 《应用声学》1989,8(5):34-38
本文介绍了声致发光的研究概况、现行的“热点”机制及其面临的问题,最后指出了研究声致发光的意义。  相似文献   

2.
乙二醇溶液中圆锥泡声致发光的发光特性   总被引:1,自引:0,他引:1       下载免费PDF全文
利用一种改进后的U形管圆锥泡声致发光装置,研究了乙二醇溶液中圆锥泡声致发光的发光特性.实验结果表明,利用乙二醇溶液可以得到超强的单个发光脉冲,其脉冲宽度可以达到150 μs,其值远远高于其他方式产生的声致发光的脉冲宽度.测量得到的光谱为一从紫外到可见光波长范围的连续谱,在589 nm附近叠加有钠的3P-3S原子发射谱线.在钠的原子发射谱线两侧测量得到了Na-Ar分子激发态跃迁形成的蓝卫星带,并在声致发光实验中测得了Na-Ar的红卫星带以及钠的3S-4S原子发射谱线. 关键词: 圆锥泡声致发光 光脉冲 光谱 卫星带  相似文献   

3.
柯微娜  程茜  钱梦騄 《物理学报》2008,57(6):3629-3635
光干涉原理和Mie理论计算结果表明,单泡声致发光中气泡前向Mie散射的振荡信号,主要是由于气泡的透射光束和表面反射光束之间光干涉产生的. 这些干涉波峰形成了测量气泡半径的空间标尺,标尺的单位长度δR由散射角θ,检测光波波长和流体光折射率确定,而每个波峰就是标尺的刻线,它们与该时刻的气泡半径大小一一对应. 在30°—50°散射角范围内,利用前向Mie散射实验测定了单泡声致发光中气泡的最大半径,R(t)曲线及平衡半径,表明前向Mie散射是一种便捷的测定气泡运动特性的有效方法. 关键词: 单泡声致发光 前向Mie散射 光干涉  相似文献   

4.
陈岐岱  王龙 《物理》2004,33(12):913-917
介绍两种使用流体动力学实现声致发光的方法:刹管法和U管圆锥泡法.这两种方法的设备简单,操作方便,容易在普通物理实验中进行,所得结果和传统单泡声致发光有所不同.U管圆锥泡法创造了发光功率和单脉冲能量的新记录,并首次用条纹相机得到了时间分辨发射光谱.  相似文献   

5.
圆锥气泡发光的光谱性质   总被引:1,自引:0,他引:1       下载免费PDF全文
在改进的U型管装置中观察到一种圆锥气泡声致发光现象。声致发光产生的单个光脉冲的能量可达到约1.4 毫焦. 脉冲宽度约100 毫秒。发光光谱由连续光谱上叠加C2,CN,和CH的激发态光谱构成。这种圆锥气泡声致发光为单泡声致发光和多泡声致发光提供了一种联系。  相似文献   

6.
徐宁 《物理》2000,29(5):257-258
对单泡声致发光过程采用等离子体描述,考虑了各种等离子体输运过程,假设了声致发光的轫致辐射机制,数值模拟的结果与实验很好地吻合,有力地支持了声致发光的热转向的解释,预言了声致发光中可能出现的极端电现象,对各物理量时空剖面的分析表明,强电场的出现中能产生的Rayleigh-Taylor不稳定性有制约作用,这可能是声致发光约10^12能量汇集的原因之一。  相似文献   

7.
声致发光单泡的Mie散射测量参数的理论计算   总被引:2,自引:0,他引:2       下载免费PDF全文
本文运用Mie散射理论系统地计算了适用于声致发光单泡的Mie散射测量参数,利用Dave倒推算法得出散射光强随半径及散射角的变化曲线I(R),I(θ),结果表明:适合于连续Mie散射测量,脉冲Mie散射测量及Mie散射定标的散射角及接收器张角是各不相同的。文中给出了合适的参数范围。  相似文献   

8.
鲁米诺增强声致发光应用研究的进展与问题   总被引:2,自引:0,他引:2       下载免费PDF全文
李化茂  冯若 《应用声学》1998,17(3):37-39
本文结合自己的工作,介绍了化学发光剂鲁米诺增强声致发光应用研究中的几种典型情况,并相应地 一些得到探讨的问题。  相似文献   

9.
李玉同  张杰 《物理》2002,31(5):293-297
空泡广泛存在于自然界中,理论和实验表明,空泡在坍塌时可以将能量密度提高-10^12倍,发出皮秒级超短脉冲闪光,文章对液体介质中的空泡规律和常用研究方法进行了描述,主要内容包括空泡动力学、声致发光、冲击波产生、激光空泡及空泡应用前景介绍。  相似文献   

10.
11.
A modified U-tube conical bubble sonoluminescence device is used to study the conical bubble photoluminescence. The spectra of conical bubble sonoluminescence at different concentrations of rhodamine 6G (Rh6G) solution in 1,2- propanediol have been measured. Results show that the sonoluminescence from the conical bubbles can directly excite Rh6G, which in turn can fluoresce. The light emission of this kind is referred to as conical bubble photoluminescence. The maximum of fluorescence spectral line intensity in the conical bubble photoluminescence has a red shift in relative to that of the standard photo-excited fluorescence, which is due to the higher self-absorption of Rh6G, and the spectral line of conical bubble photoluminescence is broadened in width compared with that of photo-excited fluorescence.  相似文献   

12.
钱祖文  肖灵 《中国物理 B》2008,17(10):3785-3791
The numerical results obtained by Rayleigh-Plesset (R-P) equation failed to agree with the experimental Mie scattering data of a bubble in water without inappropriately increasing the shear viscosity and decreasing the surface tension coefficient. In this paper, a new equation proposed by the present authors (Qian and Xiao) is solved. Numerical solutions obtained by using the symbolic computation program from both the R-P equation and the Qian-Xiao (Q-X) equation clearly demonstrate that Q-X equation yields best results matching the experimental data (in expansion phase). The numerical solutions of R-P equation also demonstrate the oscillation of a bubble in water depends strongly upon the surface tension and the shear viscosity coefficients as well as the amplitude of driving pressure, so that the uniqueness of the numerical solutions may be suspected if they are varied arbitrarily in order to fit the experimental data. If the bubble's vibration accompanies an energy loss such as the light radiation during the contract phase, the mechanism of the energy loss has to be taken into account. We suggest that by use of the bubble's vibration to investigate the state equations of aqueous solutions seem to be possible. We also believe that if one uses this equation instead of R-P equation to deal with the relevant problems such as the 'phase diagrams for sonoluminescing bubbles', etc., some different results may be expected.  相似文献   

13.
安宇 《中国物理 B》2008,17(8):2984-2988
Using the equations of fluid mechanics with proper boundary conditions and taking account of the gas properties, we can numerically simulate the process of single bubble sonoluminescence, in which electron-neutral atom bremsstrahlung, electron-ion bremsstrahlung and recombination radiation, and the radiative attachment of electrons to atoms and molecules contribute to the light emission. The calculation can quantitatively or qualitatively interpret the experimental results. We find that the accumulated heat energy inside the compressed gas bubble is mostly consumed by the chemical reaction, therefore, the maximum degree of ionization inside Xe bubble in water is much lower than that in sulfuric acid, of which the vapour pressure is very low. In addition, in sulfuric acid much larger pa and R0 are allowed which makes the bubbles in it much brighter than that in water.  相似文献   

14.
Finite-amplitude vibration of a bubble and sonoluminescence   总被引:1,自引:0,他引:1       下载免费PDF全文
钱祖文  肖灵  郭良浩 《中国物理》2004,13(7):1059-1064
Numerical solutions of the differential equation for a bubble performing finite-amplitude vibration are given in detail for a variety of situations. The results demonstrate that in lower acoustic pressure (maximum Mach number very low) its vibration has bounce. When acoustic pressure is in excess of 1.18atm and the instantaneous radius of the bubble approaches its equivalent Van der Waals radius, the maximum velocity and acceleration on the surface of a bubble have a huge increase in a very short period, which seems to favour the sonoluminescence. In vacuum environment (0.1atm), an intensive sonoluminescence could be generated.  相似文献   

15.
陈岐岱  王龙 《中国物理》2004,13(4):564-570
Large size single transient cavitation bubbles of maximum diameter up to 3 cm with sonoluminescence have been generated in water by the ‘tube arrest' method. A simplified one-dimensional model of bubble growing and water column motion is proposed. The results of numerical simulation are compared with the experimental data of the bubble size and oscillation period as the key parameters.  相似文献   

16.
Sonoluminescence     
《应用光谱学评论》2013,48(3):399-436
Abstract

Sonoluminescence is the light emission phenomenon from collapsing bubbles in liquid irradiated by an ultrasonic wave. In the present review, theoretical and experimental studies of the two types of sonoluminescence [single‐bubble sonoluminescence (SBSL) and multibubble sonoluminescence (MBSL)] are described. SBSL is a sonoluminescence from a single stably pulsating bubble trapped at the pressure antinode of a standing ultrasonic wave. MBSL is a sonoluminescence occurring from many bubbles in liquid irradiated by an ultrasonic wave. The theoretical and experimental studies suggest that SBSL originates in emissions from plasma inside the heated bubble at the bubble collapse, whereas MBSL originates both in emissions from plasma and in chemiluminescence inside heated bubbles at the bubble collapse. Unsolved problems of sonoluminescence have also been explained in detail.  相似文献   

17.
M.A. Margulis 《Ultrasonics》1985,23(4):157-169
Contemporary ideas on the nature of cavitation are reviewed in this paper. The general theories of sonoluminescence and sonochemical reactions, the origin, stability and splitting of cavitation bubbles, the dynamics of cavitation field evolution, the peculiarities of cavitation effects at low intensity and low-frequency acoustic oscillations, the sonoluminescence quenching effect and some questions on the energetics of cavitation fields are discussed. The electrical theory of the splitting of cavitation bubbles may, as shown in the paper, become an alternative to the thermal theories of cavitation in the future.  相似文献   

18.
Dynamics and measurement of cavitation bubble   总被引:1,自引:1,他引:0  
Based on the introduction of international progress, our investigations on acoustic cavitation have been reported. Firstly we considered the cavity’s dynamics under the drive of the asymmetrical acoustic pressure. An aspheric dynamical model was proposed and a new stable and aspheric solution was found in numerical simulation of the theoretical framework of the aspheric model. Then, a dual Mie-scattering technique was developed to measure the cavity’s aspheric pulsation. A significant asynchronous pulsation signal between two Mie-scattering channels was caught in the case of large cavity driven by low acoustic pressure. As a direct deduction, we observed an evidence of cavity’s aspheric pulsation. Furthermore, we studied the dependency of the asynchronous pulsation signal on the various parameters, such as the amplitude and frequency of the driving acoustic pressure, and the surface tension, viscosity and gas concentration of the liquid. Finally, we introduced a new numeric imaging technique to measure the shapes of the periodic pulsation cavities. The time-resolution was in the order of 20 ns, one order of magnitude lower than that in the previous work, say, 200 ns.  相似文献   

19.
Based on a quasi-adiabatic model,the parameters of the bubble interior for a moving single bubble sonoluminescence (m-SBSL) in water are calculated.By using a complete form of the hydrodynamic force,a unique circular path for the m-SBSL in water is obtained.The effect of the ambient pressure variation on the bubble trajectory is also investigated.It is concluded that as the ambient pressure increases,the bubble moves along a circular path with a larger radius and all bubble parameters,such as gas pressure,interior temperature and light intensity,increase.A comparison is made between the parameters of the moving bubble in water and those in N-methylformamide.With fluid viscosity increasing,the circular path changes into an elliptic form and the light intensity increases.  相似文献   

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