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1.
纳米流体激光自混频功率谱及其计算   总被引:1,自引:1,他引:0  
激光自混频技术可用于纳米颗粒和纳米流体的探测。在纳米流体自混频信号自相关函数的基础上,理论推导了功率谱函数的表达式。结果表明,纳米流体的激光自混频信号功率谱是洛伦兹线型和高斯线型的卷积,即佛赫特(Voigt)线型。通过数值计算研究了各种典型情况下激光自混频信号功率谱的频谱特征,颗粒定向运动速度决定了多普勒频移和高斯线宽,颗粒粒度决定了洛伦兹线型的宽度,颗粒粒度和速度与功率谱之间的对应关系为纳米流体的测量提供了理论基础。  相似文献   

2.
纳米流体运动特性和颗粒参数的测量对纳米流体换热效率的研究具有重要意义。本文将激光自混频技术应用于纳米流体测量中,给出了自混频信号功率谱密度函数的表达式并实验研究其变化规律。研究结果表明,功率谱密度展宽具有佛克脱函数的形式。激光垂直入射流动样品池时,功率谱密度得到展宽,展宽程度随着定向流速的增大或束腰半径的减小而增大。激光倾斜入射流动样品池时,功率谱密度在展宽的同时还伴随多普勒峰移,其位置随着定向流速的增大或散射矢量与定向流速之夹角的减小而迁移至高频。  相似文献   

3.
 本文在扼要描述了光学元件表面轮廓测量中功率谱密度(PSD)函数的基本概念、公式和应用基础上,重点讨论了光学元件表面低频和中高频空间频率PSD对光场分布的影响,并给出了强激光光学元件表面PSD函数曲线的几个实测结果和分析。  相似文献   

4.
波前功率谱密度(PSD)测量滤波器的设计   总被引:1,自引:1,他引:0  
陈伟  姚汉民  伍凡  范斌  吴时彬  陈强 《光子学报》2006,35(1):130-132
在采用波前功率谱密度评价大口径光学元件时,由于测得的原始数据受到测量系统引入的各种噪音和外界干扰的作用,会使检测准确度下降.对比引入带通滤波技术,对原始数据的有效滤波,减小带外的噪音分量和频谱混叠现象的影响.分别设计了无限脉冲响应带通滤波器和有限脉冲响应带通滤波器,通过模拟分析比较了两者的性能,得出在波前波前功率谱密度用于评价大口径光学元件的面形质量时,采用有限脉冲响应滤波器可以得到更高的测量准确度.  相似文献   

5.
采用正交光功率比值的光子型微波频率测量方案设计   总被引:1,自引:0,他引:1  
通过构建两个正交的光功率比值,以光子技术实施微波频率测量.首先,待测微波信号经外调制器加载到连续光源上,在单边带载波抑制调制下仅得到单个光边带;以光学梳状滤波器对其进行滤波处理,在输出端检测得到随微波频率增大而呈现余弦函数和正弦函数变化趋势的两个光功率;将这两个光功率与参考光功率进行比较后,进而得到余弦函数型和正弦函数...  相似文献   

6.
半导体激光器的线宽通常采用激光外差测量技术,通过差拍信号的功率谱密度函数来确定,受傅里叶变换方法的限制,得到的均是在一定时间段内的静态平均线宽。为了获得半导体激光器在电流调谐过程中的瞬时线宽特性,提出了利用时变功率谱获知调谐瞬时线宽的相干和非相干测量方法,并分别进行了理论分析和实验验证。首先对半导体激光器输出光信号及差拍信号进行了时间-频率域下的数学描述,确定了时变功率谱与调谐瞬时线宽的关系;其次,针对差拍信号的趋向性特征,提出了趋势局部均值分解方法,并研究了利用分解出的乘积函数建立差拍信号及激光器输出光信号的时变功率谱的方法;最后利用非相干和相干测量法分别获得了分布反馈式半导体激光器在50~51及50~100 mA锯齿波电流调谐过程中的瞬时线宽。  相似文献   

7.
动态光散射图像法测量纳米颗粒粒度研究   总被引:4,自引:0,他引:4  
提出了一种基于动态光散射原理的图像法测量纳米颗粒粒径的新方法,采用面阵CCD数以万计的像素同时并行测量处于布朗运动的纳米颗粒空间分布的动态散射光信号,对测得的信号进行数据处理,得到了纳米颗粒粒径。对27、79、482、948nm 4种不同粒径的纳米标准颗粒进行了实验研究,针对面阵CCD拍摄帧率远低于光电倍增管测量频率的特点,采用质量分数为55%高粘度甘油水溶液作为分散介质,在CCD拍摄帧率为8290frame/s时,27nm颗粒的测量误差从以水为分散介质时的15.1%降至1.9%。与目前动态光散射纳米颗粒测量方法相比,该方法大幅度减少了测量时间,仅为现有方法的1%以下,并可大幅度简化测量装置。  相似文献   

8.
随机振动试验是振动环境试验常用的一项重要试验方法。开展随机振动控制算法研究,将有助于提高随机振动试验技术水平。随机振动控制原理如图1所示,其系统的主要功能模块可分为:测量信号的自功率谱密度(PSD)计算;驱动信号的PSD更新;驱动信号相位随机化,转换成FFT谱;IFFT变换生成时域帧信号;时域帧信号搭接。  相似文献   

9.
提出了一种基于图像动态光散射原理测量二维纳米颗粒粒度的新方法,称为平移转动-图像动态光散射(TR-IDLS)法。采用会聚的偏振高斯光束照射样品池中处于布朗运动的二维纳米粒子,分别采集纳米粒子的水平偏振散射光信号和垂直偏振散射光信号。根据两个偏振方向上散射光光强波动的时间相关函数,计算出纳米颗粒的平移和转动扩散系数的分布,进而从扩散系数中获得颗粒的长宽比、等效直径和厚度的分布。采用该方法测量了球形标准纳米颗粒和片状云母颗粒的粒径。采用电镜获得了片状云母颗粒的形状和等效直径,并与TR-IDLS方法的实验结果进行比较,验证了TR-IDLS方法的可行性。  相似文献   

10.
本文以聚苯乙烯纳米颗粒作为测量对象,分别采用最为常见的扫描电子显微镜法(SEM)和动态光散射法(DLS)测量其粒径。结果表明:电子显微镜法可观察颗粒形貌及结构,但测量误差偏大;动态光散射法可精确测量颗粒粒径及其分布状态。分析讨论了这两种测量方法的优缺点,对纳米颗粒测量具有重要的指导作用。  相似文献   

11.
Two-factor dependences of the maximum and half-width of a surface plasmon resonance band on both the average diameter of nanoparticles and the scatter in their particle-size distributions were defined for colloidal silver and gold aqueous solutions based on modeling the extinction effectiveness factor by Mie theory. The obtained three-dimensional surfaces determined the shape of calibration curves used to define the average particle diameters and the scatter in their particle-size distributions from measurements of the maximum and half-width of the surface plasmon resonance band in spectra of the silver and gold colloidal solutions. The calibration curves were correlated with experimental samples of aqueous ultradispersed media containing silver and gold nanoparticles.  相似文献   

12.
The size of nanoparticles is measured by laser diode self-mixing interferometry, which employs a sensitive, compact, and simple optical setup. However, the signal processing of the interferometry is slow or expensive. In this article, a fast and economic signal processing technique is introduced, in which the self-mixing AC signal is transformed into DC signals with an analog circuit consisting of 16 channels. These DC signals are obtained as a spectrum from which the size of nanoparticles can be retrieved. The technique is examined by measuring the standard nanoparticles. Further experiments are performed to compare the skimmed milk and whole milk, and also the fresh skimmed milk and rotten skimmed milk.  相似文献   

13.
14.
The self-mixing vibration signals are observed in the laser diode when the optical beam is back-scattered into the laser cavity which causes laser output power modulated. Based on these properties, a laser diode self-mixing vibrometer with wide dynamic range is proposed. This current investigation further reports new work to improve the accuracy and range of the measured vibration signals. Numerical simulations and experimental results are given and discussed. The experimental results show that the frequency measurement range can be achieved up to 22 kHz with 0.241% maximum relative error while utilizing the reflecting film. For amplitude measurement utilizing the same reflecting film, the error of measurement result is 4.77 nm which has approached nanometer order of magnitude.  相似文献   

15.
Xu P  Hu Z  Jiang N  Ma L  Hu Y 《Optics letters》2012,37(11):1992-1994
We propose a novel and practical method to exactly measure the transient reflectance spectra (TRS) of the adaptive filters based on dynamic population gratings. The modulating signals applied to the laser source play an important role. We specially designed a train of triangular amplitude modulated pulses with a small duty to modulate the laser frequency, and then the TRS was obtained from the grating responses to this pulse train. The measured half-zero-point bandwidths of the filter with and without 2.6 m cavity length are 20 and 60 MHz, respectively. Our research also indicates that the relatively high input power and a short cavity length may enhance the antiperturbation ability of lasers.  相似文献   

16.
基于颗粒物米氏散射特性、激光自混合三镜腔理论和激光器稳态条件,推导出在大气颗粒物光反馈下激光器频率、功率、线宽的理论表达式,建立了大气颗粒物光反馈下的激光自混合理论模型。同时,数值模拟和分析了大气颗粒物物理参数对激光自混合干涉信号的影响。结果表明,在一定粒径范围内,激光自混合反馈强度随大气颗粒物粒径增大先增大后减小,且反馈强度峰值出现的位置随颗粒物折射率实部的增大、虚部的减小向粒径较大处移动;自混合系统的外腔长度影响自混合干涉信号的波动深度,激光器输出光信号的幅值随外腔长度增大呈指数衰减;自混合干涉信号波动频率与大气颗粒物运动速度呈线性关系。分析结果对基于激光自混合效应的大气颗粒物多物理参数传感具有重要作用。  相似文献   

17.
Laser-induced breakdown detection (LIBD) is a well established technique for measuring size and concentration of inorganic colloids in liquids. However, most applications of LIBD are restricted to the measurement of mean sizes, which is problematic in cases of wide colloid size distributions (PSD) as typically is the case in natural systems. Evaluation of PSDs from LIBD is possible but requires detailed control of the power density within the laser focus. In the present work we describe the mathematical treatment how to calculate this power density from the beam characteristics of the light source and the optical properties of the focusing optics. The results are compared to measured spatial distributions of breakdown events of three LIBD setups.  相似文献   

18.
N. Prosperini 《Physica A》2007,383(2):595-602
In this contribution, particle size distributions (PSD) of soil samples are analyzed by fractal methods. Different scaling domains, characterizing different ranges of particle sizes, are identified. Numerical models based on cellular automata are presented with the aim to understand the basic mechanisms responsible for the occurrence of multiple scaling domains in soil PSD. Numerical simulations are in good agreement with natural data and furnish a conceptual framework to explain the features observed in the PSD of studied soil samples.  相似文献   

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