电弧直读光谱仪的开发与应用

介绍一种国内首创的电弧直读光谱仪。该仪器由交/直流电弧激发光源、凹面光栅分光系统、光电倍增管接收器及智能测控系统所组成。研制成功地质样品专用的"交流电弧直读光谱仪"和高纯金属专用的"直流电弧直读光谱仪"可取代1m或2m光栅摄谱仪,省去了光谱相板、洗相及译谱等繁琐的操作程序。在优化的分析条件下,可直接对粉末状地球化学样品及高纯金属氧化物中的多种微量元素同时进行直读光谱测定,具有灵敏、准确、快速的特点,各项技术指标符合所属领域的"国家标准"及"行业规范"的要求。现已有多家使用单位采用"交流电弧直读光谱仪"分析了十几万件地球化学样品中的银、锡和硼等元素,取得了良好的应用效果。     

An analytical poroelastic model for laboratorial mechanical testing of the articular cartilage (AC)

The articular cartilage (AC) can be seen as a biphasic poroelastic material. The cartilage deformation under compression mainly leads to an interstitial fluid flow in the porous solid phase. In this paper, an analytical poroelastic model for the AC under laboratorial mechanical testing is developed. The solutions of interstitial fluid pressure and velocity are obtained. The results show the following facts. (i) Both the pressure and fluid velocity amplitudes are proportional to the strain loading amplitude. (ii) Both the amplitudes of pore fluid pressure and velocity in the AC depend more on the loading amplitude than on the frequency. Thus, in order to obtain the considerable fluid stimulus for the AC cell responses, the most effective way is to increase the loading amplitude rather than the frequency. (iii) Both the interstitial fluid pressure and velocity are strongly affected by permeability variations. This model can be used in experimental tests of the parameters of AC or other poroelastic materials, and in research of mechanotransduction and injury mechanism involved interstitial fluid flow.     

J-TEXT 扰动场交流电源峰值反馈系统设计

在J-TEXT 装置上设计了一种基于现场可编程逻辑门阵列(FPGA)的数字式峰值检测电路,该电路先对负载电流进行模数(AD)转换,再经有限冲激响应(FIR)滤波器进行数字滤波,然后用峰值算法获取电流峰值,最后经数模转换器(DA)输出电流峰值。在此基础上,完成了扰动场交流电源负载电流峰值反馈系统的设计,实验结果表明系统动态性能好、检测精度高,能很好满足交流电源负载电流反馈控制的需要。     

Particle deposition model for particulate flows at high temperatures in gas turbine components

This study proposes an improved physical model to predict sand deposition at high temperature in gas turbine components. This model differs from its predecessor (Sreedharan and Tafti, 2011) by improving the sticking probability by accounting for the energy losses during particle-wall collision based on our previous work (Singh and Tafti, 2013). This model predicts the probability of sticking based on the critical viscosity approach and collision losses during a particle–wall collision. The current model is novel in the sense that it predicts the sticking probability based on the impact velocity along with the particle temperature. To test the model, deposition from a sand particle laden jet impacting on a flat coupon geometry is computed and the results obtained from the numerical model are compared with experiments (Delimont et al., 2014) conducted at Virginia Tech, on a similar geometry and flow conditions, for jet temperatures of 950 °C, 1000 °C and 1050 °C. Large Eddy Simulations (LES) are used to model the flow field and heat transfer, and sand particles are modeled using a discrete Lagrangian framework. Results quantify the impingement and deposition for 20–40 μm sand particles. The stagnation region of the target coupon is found to experience most of the impingement and deposition. For 950 °C jet temperature, around 5% of the particle impacting the coupon deposit while the deposition for 1000 °C and 1050 °C is 17% and 28%, respectively. In general, the sticking efficiencies calculated from the model show good agreement with the experiments for the temperature range considered.     

Wet-chemical treatment and electronic interface properties of silicon solar cell substrates

On textured n-type silicon substrates for solar cell manufacturing, the relation between light trapping behavior, structural imperfections, energetic distribution of interface state densities and interface recombination losses were investigated by applying surface sensitive techniques. The field-modulated surface photovoltage (SPV), in-situ photoluminescence (PL) measurements, total hemispherical UV-NIR-reflectance measurements and electron microscopy (SEM) were employed to yield detailed information on the influence of wet-chemical treatments on preparation induced micro-roughness and electronic properties of polished and textured silicon substrates. It was shown that isotropic as well as anisotropic etching of light trapping structures result in high surface micro-roughness and density of interface states. Removing damaged surface layers in the nm range by wet-chemical treatments, the density of these states and the related interface recombination loss can be reduced. In-situ PL measurements were applied to optimise HF-treatment times aimed at undamaged, oxide-free and hydrogen-terminated substrate surfaces as starting material for subsequent solar cell preparations.      

PN结电容与正向直流偏压的关系

半导体PN结具有电容的性质．在正向直流偏压下,理论计算表明,PN结扩散电容的对数与正向偏压成正比．实验发现,当正向偏压小于30mV时,这种线性关系是成立的;当正向偏压大于30mV时,会偏离这种线性关系．由于PN结还具有电阻特性,对交流信号的相位有影响．随着正向偏压增大,交流信号的相位变化出现一极值．如果将PN结等效为一个电容和一个电阻并联,就可以定性解释这种变化关系．     

AC susceptibility of magnetic markers in suspension for liquid phase immunoassay

AC susceptibility of magnetic markers in solution was studied for biosensor applications. First, frequency dependence of the susceptibility was measured, and size distribution of the markers was estimated by analyzing the experimental result with the so-called singular value decomposition (SVD) method. The size distribution estimated with the magnetic measurement agreed with that obtained from conventional optical measurement. Next, susceptibility measurement was applied to the liquid-phase immunoassay without bound/free (B/F) separation. We performed the detection of biotin-coated polymer beads in suspension using avidin-coated magnetic markers. Changes of the susceptibility and the size distribution caused by the binding reaction were shown.     

醋酸铜热解制备无氯Cu2O/AC催化剂及其催化氧化羰基化

以醋酸铜为前驱物, 采用浸渍法负载后进行热处理使醋酸铜热解, 获得了负载型无氯Cu2O/AC(活性炭)催化剂, 并通过催化甲醇直接气相氧化羰基化合成碳酸二甲酯(DMC). 在氮气和惰性气体气氛下, 一水合醋酸铜Cu(CH3COO)2·H2O在30~450 ℃范围内产生3个失重过程, 其中在150~300 ℃范围内Cu(CH3·COO)2热解生成Cu2O; 而在300~450 ℃范围内生成单质Cu. 在200~350 ℃范围内, 将Cu(CH3COO)2·H2O/AC加热处理4 h后, 催化剂上逐步形成了Cu2O, 到350 ℃时, 水合醋酸铜几乎全部转化为Cu2O, 并有极少量单质Cu形成. 在300~350 ℃热处理4 h后, 催化剂中铜主要以Cu2O形式存在, 并表现出良好的氧化羰基化催化活性. 在n(CO)∶n(MeOH)∶n(O2)=4∶10∶1及SV=5600 h-1条件下, 于300 ℃热处理4 h所制备的催化剂的甲醇转化率达到6.21%, DMC的时空收率为128.16 mg·g-1·h-1, 选择性为64.26%.     

Uncompensated magnetization in the layered molecular antiferromagnet {N(n-C5H11)4[MnFe(ox)3]}∞

Studies on the magnetic properties of the molecular antiferromagnetic material {N(n-C₅H₁₁)₄[Mn^IIFe^III(ox)₃]}_∞, carried out by various physical techniques (AC/DC magnetic susceptibility, magnetization, heat capacity measurements and Mössbauer spectroscopy) at low temperatures, have been presented. Different experimental observations complement each other and provide a clue for the observation of an uncompensated magnetization below the Néel temperature and short-range correlations persisting high above T_N. It is understood that the honeycomb layered structure of the compound contains non-equivalent magnetic sub-lattices, (Mn^II–ox–Fe^III_A–...) and (Mn^II–ox–Fe^III_B–...), where different responses of the Fe^III_A and Fe^III_B spin sites towards an external magnetic field might be responsible for the observation of the uncompensated magnetization in this compound at T < T_N. The present magnetic system is an S = 5/2 2-D Heisenberg antiferromagnet system with the intralayer exchange parameter J/k_B = −3.29 K. A very weak interlayer exchange interaction was anticipated from the spin wave modeling of the magnetic heat capacity for T < 0.5T_N. The positive sign of the coupling between the layers has been concluded from the Mössbauer spectrum in the applied magnetic field. Frustration in the magnetic interactions gives rise to the uncompensated magnetic moment in this compound at low temperatures.     

Conductive diamond hollow fiber membranes

Boron-doped diamond hollow fiber membrane (BDD–HFM) was fabricated as a novel type of porous conductive diamond. BDD–HFM was obtained by deposition of BDD polycrystalline film onto a quartz filter substrate consisting of quartz fibers, followed by etching of the substrate in HF/HNO₃ aqueous solution. Cross-sectional scanning electron microscope (SEM) observation showed the inner diameter and wall thickness of the BDD hollow fibers were in the range of 0.4–2 and 0.2–2 μm, respectively. The BDD–HFM electrode exhibited a relatively large double-layer capacitance (ca. 13 F g⁻¹) in 0.1 M H₂SO₄. Electrochemical AC impedance properties were simulated using an equivalent circuit model containing a transmission line model, which indicated characteristics of a porous electrode material.