煤复电阻率频散机理研究

为了研究在0~200 kHz条件下煤复电阻率频散的物理机理,在恒定电流变频条件下,测量煤的复电阻率幅频相频。利用傅里叶逆变换,将煤的复电阻率频域数据变换成时域数据;利用Cole-Cole模型,将复电阻率频散数据进行拟合;借鉴双电层形变假说理论,对比砂岩频散现象,研究煤的复电阻率频散机理。结果表明:在电流频率为0~200 kHz,焦作赵固矿和九里山矿样品复电阻率频散特征与岩石相似,复电阻率幅值随频率增大而减小,复电阻率相位的绝对值随频率的增大先增大后减小,引起频散特征的原因主要是激发极化,电磁感应的影响程度很小。煤复电阻率测量和频散机理的研究成果为复电阻率测井提供了理论依据,具有一定的应用前景。      

基于点云数据的山区建筑物屋顶轮廓线提取研究

山区建筑物由于地势起伏大、周边植被茂盛等特点使得传统屋顶轮廓线提取算法应用效果较差.根据研究区域的地理特征,对轮廓线提取算法进行了改进,即以点云数据的曲率值为影响因子来评价离散程度,对离散程度高的数据选取曲率的最小值为种子点,对离散程度低的数据选取曲率的平均值为种子点.该方法与传统轮廓线提取算法相比,提高了屋顶轮廓线提...     

加强的适合复杂地形的水波方程及其一维数值模型验证

在他人给出的方程的基础上,通过在其动量方程中引入含4个参数的公式,推导出了加强的适合复杂地形的水波方程,新方程的色散、变浅作用以及非线性均比原来适合复杂地形的方程有了改善:色散关系式与斯托克斯线性波的Padé(4,4)阶展开式一致;变浅作用在相对水深(波数乘水深)不大于6时与解析解符合较好;非线性在相对水深不大于1.05时保持在5%的误差之内.基于该方程,在非交错网格下建立的时间差分格式为混合4阶Adams-Bashforth-Moulton的一维数值模型,并在数值计算中利用了五对角宽带解法.数值模拟了潜堤上波浪传播变形,并将数值计算结果与实验结果进行了对比,验证了该数值模型是合理的.     

Explicit Solution to the Wave Dispersion Equation with Higher Accuracy

Based on the previous study results, two higher accuracy explicit solutions to the dispersion equation for wave length are presented in this paper. These two solutions have an accuracy of 0.1% over all wave lengths, which is sufficiently complete for practical application. At the same time, several previous explicit solutions also have been reviewed and compared herein. In comparison with accuracy, the results show that the present two solutions are as good as Wu and Thornton's solution (which has a good accuracy over all wave lengths, but its calculation formula is so complex that it is hard to be used with a hand calculator), and are better than the other solutions, they may be rather useful in practical calculation with a hand calculator or computer.     

输出近百纳焦耳脉冲能量的光子晶体光纤锁模激光器

设计并搭建了一种支持百纳焦耳量级的单脉冲能量输出的锁模光纤激光器.激光器基于σ型腔结构,采用掺Yb偏振型大模场面积光子晶体光纤作为增益介质,利用半导体可饱和吸收镜实现自启动锁模.激光器内没有色散补偿机理,使其工作在全正色散锁模状态.通过在谐振腔内引入多通长腔使激光器的重复频率降低至11.1 MHz,直接获得了平均功率为1.08 W,单脉冲能量为 97 nJ,脉冲宽度为4.17 ps的稳定锁模脉冲输出,经腔外色散补偿,脉冲宽度压缩至740 fs.     

An extended time-dependent numerical model of the mild-slope equation with weakly nonlinear amplitude dispersion

In the present paper, by introducing the effective wave elevation, we transform the extended ellip- tic mild-slope equation with bottom friction, wave breaking and steep or rapidly varying bottom topography to the simplest time-dependent hyperbolic equation. Based on this equation and the empirical nonlinear amplitude dispersion relation proposed by Li et al. (2003), the numerical scheme is established. Error analysis by Taylor expansion method shows that the numerical stability of the present model succeeds the merits in Song et al. (2007)’s model because of the introduced dissipation terms. For the purpose of verifying its performance on wave nonlinearity, rapidly vary- ing topography and wave breaking, the present model is applied to study: (1) wave refraction and diffraction over a submerged elliptic shoal on a slope (Berkhoff et al., 1982); (2) Bragg reflection of monochromatic waves from the sinusoidal ripples (Davies and Heathershaw, 1985); (3) wave transformation near a shore attached breakwater (Watanabe and Maruyama, 1986). Comparisons of the numerical solutions with the experimental or theoretical ones or with those of other models (REF/DIF model and FUNWAVE model) show good results, which indicate that the present model is capable of giving favorably predictions of wave refraction, diffraction, reflection, shoaling, bottom friction, breaking energy dissipation and weak nonlinearity in the near shore zone.     

Comprehensive research on self phase modulation based optical delay systems

This paper comprehensively investigates the properties of self phase modulation based optical delay systems consisting of dispersion compensation fibre and highly nonlinear fibres. It researches into the impacts of power level launched into highly nonlinear fibres, conversion wavelength, dispersion slope, modulation format and optical filter bandwidth on the overall performance of optical delay systems. The results reveal that, if the power launched into highly nonlinear fibres is fixed, the time delay generally varies linearly with the conversion wavelength, but jumps intermittently at some conversion wavelengths. However, the time delay varies semi-periodically with the power launched into highly nonlinear fibres. The dispersion slope of highly nonlinear fibres has significant influence on the time delay, especially for the negative dispersion slope. The time delay differs with modulation formats due to the different combined interaction of nonlinearity and dispersion in fibres. The bandwidth of the optical filters also greatly affects the time delay because it determines the bandwidth of the passed signal in the self phase modulation based time delay systems. The output signal quality of the overall time delay systems depends on the conversion wavelength and input power level. The optimisation of the power level and conversion wavelength to provide the best output signal quality is made at the end of this paper.     

从阵列声波测井波形处理地层纵、横波时差的新方法

阵列声波测井波形中包含丰富的地层纵、横波速度信息.如何从这些波形中提取出这些速度信息,得到比较准确的地层纵、横波时差是资料应用人员非常关心的问题.目前,最常用的纵、横时差处理方法是STC———慢度—时间相关法.该方法只有在波形的速度频散不严重时比较有效.而井内声波传播的基本特征是具有频散特征.利用Ma-trix pencil方法可以求出阵列声波测井波形的二维谱.借助于波形的二维谱,本文给出一种求地层的纵、横波时差的方法.本方法充分利用井内声波传播的规律,有效地减小了频散对纵、横波时差计算的影响,得到的纵、横波时差值精度比较高.     

Alteration and primary geochemical dispersion associated with the Bulletin lode-gold deposit, Wiluna, Western Australia

The Bulletin lode-gold deposit is within the northernmost part of the Norseman–Wiluna greenstone belt in the Archaean Yilgarn Block, Western Australia. It is located within a brittle–ductile shear zone and hosted by tholeiitic metavolcanic rocks. Syn-metamorphic wallrock alteration envelops the gold mineralisation and is pervasive throughout the entire shear zone and extends up to 150 m into the undeformed wallrocks. Alteration is characterised by the sequence of distal chlorite–calcite, intermediate calcite–dolomite, outer proximal sericite and inner proximal dolomite–sericite zones. The thickness of the alteration envelope, and the occurrence of dolomite in the alteration sequence, can be used as a rough guide to the width, extent and grade of gold mineralisation, because a positive correlation exists between these variables. Mass transfer evaluations indicate that chemical changes related to the wallrock alteration are similar in all host rocks: in general, Ag, As, Au, Ba, CO₂, K, Rb, S, Sb, Te and W are enriched, Na and Y are depleted, and Al, Cr, Cu, Fe, Mg, Mn, Nb, Ni, P, Se, V, Zn and Zr are immobile, while Ca, Si and Sr show only minor or negligible relative changes. The degree of mobility of each component increases with proximity to gold mineralisation. The largest potential exploration targets are possibly defined by regional As (>6 ppm) and Sb (>0.6 ppm) anomalies. These anomalies, if real, extend laterally for >150 m from the mineralised shear zone into areas of apparently unaltered rocks. Anomalies defined by Te (>10 ppb), W (>0.6 ppm), carbonation indices, local enrichment of Sb (>2.0 ppm) and As (>28 ppm), and potassic alteration indices also form significant exploration targets extending beyond the HJB shear zone and the Au anomaly (>6 ppb) and, locally, into apparently unaltered rock. Gold, itself, has a restricted dispersion, with an anomaly extending for 1–35 m from ore, and being restricted to within the shear zone itself. Amongst individual geochemical parameters, only As and Sb define significant, consistent and smooth trends (vectors) when laterally approaching the ore. However, the respective dimensions of individual geochemical anomalies can be used as an extensive, though stepwise, vector towards ore.     

伪谱算法在声波数值模拟中的数值频散分析

本文推导了声波方程频散函数, 分析了伪谱法的空间网格大小和采样周期对数值频散的影响, 通过数值模拟实验得到了最佳空间参数选择方法。 结果表明: 伪谱方法稳定数值模拟的最大空间采样间距选取原则是使中波长(奈奎斯特频率的一半)的采样点数为2个; 对于所有维度, 稳定性随空间采样间距的增加而增加, 但不易变化太大, 变化太大时需要适当减小震源子波的主频, 以满足空间合理采样; 空间采样间距的大小设置, 需要考虑满足采样定理和稳定性计算条件, 并且稳定性条件对空间采样间距的要求更加严格; 伪谱法数值模拟的最佳(数值频散最小)空间参数选择为中波长2个采样点, 对应主波长约6~7个采样点。 以上研究对于采用伪谱法进行声波方程数值模拟过程中, 如何合理选择模拟参数提供一些参考。