溶胶-凝胶法制备的光学薄膜表面粒度及其分布

本文研究了溶胶-凝胶法制备的光学薄膜表面粒度及其分布,结果表明:膜表面的粒度大小与热处理温度及陈化时间有关,粒度分布函数可为泊松分布,正态分布等.     

浴法抛光中抛光粉粒径对去除效果影响的试验研究

为了分析抛光粉粒径对材料去除效果的影响,选用不同的平均粒径以及不同比例混合氧化铈抛光粉分别对K9玻璃进行了抛光试验。对抛光后的工件表面粗糙度及去除量进行了定量研究。结果表明,在试验条件相同的情况下,不同平均粒径的抛光粉,粒径越小,抛光后的元件表面粗糙度越好。从使用不同比例的混合抛光粉试验中可以看出,粒度的均匀性是影响工件表面粗糙度的重要因素。结合抛光粉粒度分布图和试验结果可以看出,抛光粉粒子的分布范围越小,以及各粒径大小分布在峰值附近的粒子所占体积百分比越接近,加工后的工件表面粗糙度越小。     

用ACM0.1/0粉末磨削后脆性材料的磨损粒度及表面粗糙度

如文献[1]所述,曾用电子显微镜研究用1微米人造氧化铝(M1)磨削脆性材料时,所形成的磨损粒度。按线性尺寸分布的磨损粒度(PA次微米计)反映破坏表面的动力波动不定。这是由于超分子速率摩擦散逸结构[2]所致。我们采用一种粒度比M1细的工业生产ACM0.1/0人选氧化铝粉末磨削表面。下面列举用ACM0.1/0粉末磨削几种脆性光学材料时,所形成产品的磨损尺寸和表面粗糙度的一些数据。     

荧光粉粒度分布的数学模型

荧光粉的粒度分布,必须满足器件的特性,适应涂复的工艺,是荧光粉最重要的参量之一. 国内,已越来越清楚地认识到了荧光粉粒度分布的重要性,对荧光粉粒度分布的研究,也正在大力展开. 荧光粉粒度分布的研究,涉及多方面的内容.本篇文章仅就荧光粉粒度分布的数学模型     

对痕量羊角材料降解产物的表面增强拉曼光谱研究

将一定浓度的硝酸银与柠檬酸三钠混合后,利用微波加热法制备纳米银溶胶,该方法加热速度快、温度分布均匀、反应条件易控制。采用准弹性激光散射技术检测其粒度大小及分布状态的信息,测得其平均粒度为(53.27±2.65)nm,粒度大小集中分布在56 nm左右。然后以之作为表面增强拉曼光谱(SERS)的活性基底,研究测定羊角痕量降解产物的SERS光谱。结果发现,羊角降解产物的表面增强拉曼效应显著,尤其在659,830,850,929,999,1 028,1 280,1 439,1 599 cm-1等多处出现了明显的拉曼振动峰,这些谱峰反映了羊角降解产物的生化成分信息。并且通过对所获得的羊角降解产物SERS信号进行的谱峰归属分析表明,羊角降解产物主要为氨基酸与多肽类物质。运用表面增强拉曼光谱检测角材料的降解产物,获得较高的灵敏度,可测定浓度低至ppm水平的痕量降解产物,本研究表明,SERS可能为羊角等角材料降解产物的检测提供一种快速、直观、准确的新方法。     

表面修饰的钛酸钡纳米粉体的制备

采用水热法制备出表面包裹有硬脂酸的钛酸钡钠米粉体,并运用一系列手段对其微结构进行了表征。结果表明：产物粒径较小,粒度分布较窄,单分散性较好,其表面为非极性,同时表现出良好的流动性能。认为钛酸钡纳米粉体表面极性的改变是由于其表面包裹了一层硬脂酸,并且包裹层降低了粉体间的相互作用力,从而提高了粉体的流动性。     

折反式激光粒度测量方法

激光粒度仪因其快速、非接触等优点被广泛应用于各领域的粒度分布测量,但颗粒散射光的角分布与粒度大小关系复杂。为了获得不同粒度下的相对精度一致,通常会造成粒度分布测量范围小、无法满足宽分布粒度测量要求等问题。根据Mie散射近似的菲涅尔原理,提出采用折反式光路,将颗粒散射信号由分光镜分成两束,经两组组合式镜头和2个光电探测器分别采集透射和反射的散射信号,信号组合后经反演得到颗粒粒度分布,从而提高了可测粒度范围。采用两种标准粒子及其混合物进行了实验,结果表明,单种标准粒子测量结果的体积中位径D50的测量相对误差都不大于7.9%;对混合粒子也能够得到正确的峰值分布。     

硅酸盐荧光粉焙烧中的加盖工艺对产物性能的影响

采用高温固相法合成了Sr2.95SiO5∶0.05Eu荧光粉,借助X射线衍射仪、光谱仪、激光粒度仪、扫描电子显微镜等分析测试方法分别对荧光粉的晶相、激发与发射光谱、粒度分布、表面形貌等进行了表征,进而分析了坩埚的加盖工艺对产物性能的影响.实验结果显示:随着坩埚严密程度的增加,产物在蓝光激发下的发光强度增大.坩埚加盖有利于得到Sr3SiO5相纯度高的产物.加盖后,得到的样品颗粒尺寸较大,但是粒径分布均匀.     

激光衍射粒度分析仪粒度分布求解方法的研究

本文介绍了激光衍射粒度分析仪的基本原理,给出了光电探测器上的光能分布公式,对其求解方法进行了详细分析,提出了利用改进的最小二乘法求解粒度分布的新方法.最后分别利用函数限制解法和自由分布解法对两种情况的粒度分布进行了数值模拟计算.     

夫琅和费衍射颗粒粒度测量中的改进Chin-Shifrin反演算法

在基于线阵CCD的夫琅和费衍射颗粒粒度测量中,采用Chin-Shifrin积分变换反演算法使得反演的粒度分布出现假峰现象.为解决此问题,提出在该Chin-Shifrin积分变换反演算法中引入矩形窗函数,并在分析颗粒粒径与衍射光强导数最小值之间关系的基础上,确定矩形窗函数中心点位置及左右边界,利用该矩形窗函数对粒度分布进行截断处理,消除虚假峰,提高反演颗粒粒度分布的准确性.分别对两种标准颗粒进行了测量,并对不同算法的反演结果进行了对比.实验结果表明:引入矩形窗函数的改进Chin-Shifrin算法,能够有效排除粒度分布中的多假峰;粒度分布测量相对误差小于3%,重复性小于4%.     

Calculating the soot particle size distribution function in turbulent diffusion flames using a sectional method

Soot formation in a turbulent jet diffusion flame is modeled using an unsteady flamelet approach in post-process. In the present work, we apply a detailed kinetic soot model with a sectional method, and study the evolution of the particle size distribution. Detailed information on the evolution of the soot particle size distribution function is acquired. It is found that the particle size distribution function is bimodal throughout the flame. The transition from the small to large particle size distributions is strongly influenced by surface growth and oxidation reactions. We find that large particles are most likely to be emitted from the flame.     

风沙流对高压绝缘子电位和电场分布的影响

研究风沙流对高压绝缘子电位和电场分布的影响,基于有限体积法建立绝缘子风沙气固两相流模型和风沙天气下绝缘子的风-沙-电耦合场模型,计算不同风沙天气下绝缘子表面沙尘的空间分布和沉积及其对绝缘子沿面电位和电场的影响,结果表明：风沙天气下绝缘子沿面电位和电场畸变受风速和粒径影响显著,电位的畸变幅度随风速和粒径的增加而升高,电场的畸变幅度随风速和粒径的增大而减少;风沙天气下绝缘子表面不同的沙尘空间分布和沉积导致绝缘子不同位置沿面电位和电场畸变不同.     

Analogous materials for studying spent nuclear fuel: The influence of particle size distribution on the specific surface area of irradiated nuclear fuel

Knowledge of the reactive surface that a given material presents to reactive species is one of the fundamental factors for the discussion of experimental data from the alteration of a solid at laboratory scale, or the extrapolation to different environmental conditions. The reactive surface depends on several factors such as the origin of the solid, for example, history of irradiation, the particle size distribution and the history of its reactive surface.Here we discuss the relation between the particle size distribution and the specific surface area for different uranium oxides, namely, irradiated fuel, SIMFUEL and several fresh - non-irradiated - uranium oxides. The analysis is made comparing our own data with values reported in the literature. Our analysis strongly suggests that it is necessary to establish the surface area time evolution in order to model its behaviour in different scenarios where the alteration process will happen. Moreover, this is required in both, dry and wet conditions. A first step to get this function is the determination of the particle size distribution dependence of the specific surface area.     

不同粒径沙地表面双向反射特性研究

由于自然环境遭到人为因素的破坏,我国沙地面积正在逐步扩大,确定沙地的性质与面积已经成为改善环境的重要的指示性信息.遥感技术以其特有的优势可以为沙地监测提供科学有效的信息.本文以不同粒径沙地表面为研究对象,测量其双向反射信息,分析粒径大小对沙地表面反射特性的影响;基于现有的模型对不同粒径大小沙地表面的反射信息进行计算,与实测信息进行对比.研究结果表明,粒径大小对沙地表面反射的反射分布特性有明显的影响;通过对比测量的反射信息与模型计算的反射信息发现,利用双向反射模型可以准确地计算出不同粒径沙地表面的反射信息.本研究不仅确定了粒径大小对反射信息的影响,也为遥感技术估算沙地表面粒径大小以及研究地表固有光学特性提供参考.     

Estimation of surface area concentration of workplace incidental nanoparticles based on number and mass concentrations

Surface area was estimated by three different methods using number and/or mass concentrations obtained from either two or three instruments that are commonly used in the field. The estimated surface area concentrations were compared with reference surface area concentrations (SA_REF) calculated from the particle size distributions obtained from a scanning mobility particle sizer and an optical particle counter (OPC). The first estimation method (SA_PSD) used particle size distribution measured by a condensation particle counter (CPC) and an OPC. The second method (SA_INV1) used an inversion routine based on PM1.0, PM2.5, and number concentrations to reconstruct assumed lognormal size distributions by minimizing the difference between measurements and calculated values. The third method (SA_INV2) utilized a simpler inversion method that used PM1.0 and number concentrations to construct a lognormal size distribution with an assumed value of geometric standard deviation. All estimated surface area concentrations were calculated from the reconstructed size distributions. These methods were evaluated using particle measurements obtained in a restaurant, an aluminum die-casting factory, and a diesel engine laboratory. SA_PSD was 0.7–1.8 times higher and SA_INV1 and SA_INV2 were 2.2–8 times higher than SA_REF in the restaurant and diesel engine laboratory. In the die casting facility, all estimated surface area concentrations were lower than SA_REF. However, the estimated surface area concentration using all three methods had qualitatively similar exposure trends and rankings to those using SA_REF within a workplace. This study suggests that surface area concentration estimation based on particle size distribution (SA_PSD) is a more accurate and convenient method to estimate surface area concentrations than estimation methods using inversion routines and may be feasible to use for classifying exposure groups and identifying exposure trends.     

Raman scattering from gas-evaporated silicon small particles

Raman scattering measurements are reported on silicon small particles prepared by gas-evaporation technique. The crystalline structure is also observed for the sample having 70 A particles in average size. Four resolved component modes with Gaussian distribution function are identified with the three usual modes (LA, TO and allowed-TO) and a new surface mode. The surface mode of silicon particle, whose relative integrated intensity decrease with an increase of the particle size, is presented for the first time.     

Describing Hydrodynamic Particle Removal from Surfaces Using the Particle Reynolds Number

The fundamental processes related to the removal of fine particles from surfaces in a hydrodynamic flow field are not adequately understood. A critical particle Reynolds number approach is proposed to assess these mechanisms for fine particles when surface roughness is small compared to particle diameter. At and above the critical particle Reynolds number, particle removal occurs, while below the critical value, particles remain attached to a surface. The system under consideration consists of glass particles adhering to a glass surface in laminar channel flow. Our results indicate rolling is the removal mechanism, which is in agreement with the literature. Theoretical results of the critical particle Reynolds number model for rolling removal are in general agreement with experimental data when particle size distribution, particle and surface roughness, and system Hamaker constant are taken into account.     

多分散Au-Ag合金纳米球的光谱消光法反演

贵金属纳米颗粒具有局域表面等离子体共振特性而引起了广泛的关注,其中Au-Ag合金纳米颗粒具有良好的结构稳定性、光热性能以及潜在的抗癌功效而得到普遍研究。在众多应用中的特性与其粒径和浓度密切相关,然而目前常用的电子显微镜观察法和动态光散射法不能同时获得粒径和浓度信息,因此采取有效手段测量颗粒粒径和浓度信息至关重要。基于光谱消光法,利用非负的Tikhonov正则化方法解决反演问题,并根据Mie理论计算消光矩阵。针对噪声问题,采取两种情况研究多分散Au-Ag合金纳米球粒径分布与浓度的反演问题。未添加噪声情况下,颗粒系Ⅰ的反演相对误差小于颗粒系Ⅱ,在波长范围300～500 nm之间的反演相对误差最小,对应平均粒径、粒径标准差和颗粒数浓度的反演相对误差分别为0%,-0.03%和0%。添加随机噪声情况下,将0.5%和1.0%的随机噪声添加进颗粒系Ⅰ中的消光谱,经过数据比较发现在波长范围200～600 nm之间的反演相对误差最小。当添加0.5%的随机噪声时,粒径分布、粒径标准差和颗粒数浓度的变化范围分别为79.76～80.15 nm, 5.60～6.61 nm和0.995 8×1010～1.005 9×1010个·cm-3;当添加1.0%的随机噪声时,粒径分布、粒径标准差和颗粒数浓度的变化范围分别为78.87～80.27 nm, 5.36～9.00 nm和0.992 4×1010～1.027 7×1010个·cm-3。反演结果随着随机噪声的增大,变化范围也明显增大即反演相对误差增大,并且每次添加相同随机噪声后的反演结果不同。为了减少随机噪声导致的不稳定性,对100次反演结果进行平均得到平均粒径、粒径标准差和颗粒数浓度。当随机噪声从0.5%增大至1.0%时,其反演结果的相对误差均增大,但是反演得到的粒径分布、粒径标准差和颗粒数浓度相对误差均小于6%,这说明通过反演算法得到的反演结果具有较好的稳定性。研究表明,光谱消光法为反演多分散Au-Ag合金纳米球粒径分布与浓度提供了一种简单、快速的表征手段,也对研究非球形纳米颗粒有启示作用。