BP网络在语音干扰效果客观评估方法优化中的应用

语音干扰效果评估是当前声学技术研究领域的一个重要课题。在介绍语音干扰效果评估一般方法的基础上,首先利用最小二乘法建立了基于巴克谱测度的语音干扰效果评估模板,通过对该模板进行主、客观分析,引入了BP网络建模方法,大大减小了以往的最小二乘法在语音干扰效果客观评估的建模中的误差,确立了基于BP神经网络的语音干扰效果评估模型,并通过试验数据加以验证。     

YAG脉冲激光焊接的光致等离子体机理研究

针对 YAG脉冲激光焊接 Al及 4 5#钢时产生的光致等离子体 ,采用空心圆电极探测等离子体电信号 ;建立探测器内等离子体区域分析的理论模型 ,并用试验加以验证。研究结果表明 ,在负电压段 ,等离子体电信号的电流随电压增加呈现饱和趋势 ;理论与试验曲线比较证明 ,等离子体温度高于被焊材料气化温度约 30 0 K。     

IGBT芯片静态输出曲线连续测量方法

绝缘栅双极型晶体管(IGBT)芯片的静态输出曲线是考核其能量损耗及指导多芯片并联设计的重要指标之一。现有测量IGBT静态输出曲线的方法多采用商用化的功率器件分析仪,然而商业化功率器件分析仪存在价格昂贵、夹具单一的问题。亟需开发一种简单、快速、有效的静态输出曲线测量方法。面向高压IGBT芯片,提出一种新的静态输出曲线连续测量方法及测试电路,有效减小了IGBT芯片的电导调制效应和温升效应对静态输出曲线的影响。通过实时测量动态过程中的电压及电流,可以快速得到IGBT芯片静态输出曲线。通过对比本文连续法与功率器件分析仪的测量结果,证明了所提方法的有效性。     

Piecewise quadratic trigonometric polynomial curves

Analogous to the quadratic B-spline curve, a piecewise quadratic trigonometric polynomial curve is presented in this paper. The quadratic trigonometric polynomial curve has continuity, while the quadratic B-spline curve has continuity. The quadratic trigonometric polynomial curve is closer to the given control polygon than the quadratic B-spline curve.

     

光纤传感器的标定曲线拟合与误差分析

本文介绍了一种求取实际光纤传感器标定曲线及函数的有效方法。以压电式光纤电压传感器实测数据为例，详细患解出了其标定函数和曲线，并进行了误差分析。     

Integer points on the curve

We completely solve diophantine equations of the form where is a positive integer, using a reduction to some quartic elliptic equations, which can be solved with well known methods.

     

基于贝塞尔曲线和路径的气象模式建模仿真

为了更贴近机载雷达实际的工作情况,符合培训人员工作的需求,介绍了机载雷达训练模拟器的气象模式的建模仿真。首先建立了气象目标控制模型,支持对气象目标显示的控制和调整。通过控制台向显控台发送目标坐标信息,以及对不同强度的气象目标进行不同颜色标记,并基于贝塞尔曲线和路径规划成功实现调用GDI画图来生成不规则形状的气象目标。最后在某型机载雷达训练模拟器实现气象模式的拓展,取得了良好训练效果。     

Fast chromatographic method for the determination of dyes in beverages by using high performance liquid chromatography—Diode array detection data and second order algorithms

A fast chromatographic methodology is presented for the analysis of three synthetic dyes in non-alcoholic beverages: amaranth (E123), sunset yellow FCF (E110) and tartrazine (E102). Seven soft drinks (purchased from a local supermarket) were homogenized, filtered and injected into the chromatographic system. Second order data were obtained by a rapid LC separation and DAD detection. A comparative study of the performance of two second order algorithms (MCR-ALS and U-PLS/RBL) applied to model the data, is presented. Interestingly, the data present time shift between different chromatograms and cannot be conveniently corrected to determine the above-mentioned dyes in beverage samples. This fact originates the lack of trilinearity that cannot be conveniently pre-processed and can hardly be modelled by using U-PLS/RBL algorithm. On the contrary, MCR-ALS has shown to be an excellent tool for modelling this kind of data allowing to reach acceptable figures of merit. Recovery values ranged between 97% and 105% when analyzing artificial and real samples were indicative of the good performance of the method. In contrast with the complete separation, which consumes 10 mL of methanol and 3 mL of 0.08 mol L⁻¹ ammonium acetate, the proposed fast chromatography method requires only 0.46 mL of methanol and 1.54 mL of 0.08 mol L⁻¹ ammonium acetate. Consequently, analysis time could be reduced up to 14.2% of the necessary time to perform the complete separation allowing saving both solvents and time, which are related to a reduction of both the costs per analysis and environmental impact.     

关于椭圆曲线密码的实现

从实现的角度,讨论了椭圆曲线密码实现中的一些问题,涉及有限域的选择,高斯正规基,曲线的选择,点乘的计算方法,签名方案等实际问题。     

On Selfsimilar Jordan Curves on the Plane

We study the attractors of a finite system of planar contraction similarities S _j (j=1,...,n) satisfying the coupling condition: for a set {x ₀,...,x _n} of points and a binary vector (s ₁,...,s _n ), called the signature, the mapping S _j takes the pair {x ₀,x _n} either into the pair {x _j-1,x _j } (if s _j =0) or into the pair {x _j , x _j-1} (if s _j =1). We describe the situations in which the Jordan property of such attractor implies that the attractor has bounded turning, i.e., is a quasiconformal image of an interval of the real axis.