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In this paper the conformal transformation method is used to get the inferential reasoning formulas: seepage pressure formula, seepage discharge formula and seepage gradient formula.

本文采用保角变换的方法,通过建立数学模型推导出在均质且理想边界条件下,土石坝基垂直防渗的渗透压力、渗流量和出逸坡降计算公式。

As to the remaining parameters, two methods are developed: first, accepting that the projection function complies with a circular function within at least a part of a given field of view, constrained by the obtained object-to-image radial mapping and a constant focal length, the best-fitting point of the optical origin is tested along the optical axis; secondly, referring to the postulation of the exclusively bilateral mapping between an imaged point and its scenic sight ray, a measuring technique is developed to survey the world coordinates which will fabricate a projecting path to the imaged points located on the imageable region of the image plane in order to directly model the projection geometries involved.

而针对其余参数本文提出两种解题方法:其一是根据『在「部分视野角范围」内,鱼眼相机的投射模型符合一典型的「圆形函数」』以标靶实体与其影像尺寸为限制条件,测试光学轴上的最佳视觉参考点、鉴定最适当的投射模型、焦距、及有效的视野角度范围。其二是根据『一视野线排他性地与对应「呈影点」一一映射』参考一呈影点来搜寻空间中对应视野线的绝对座标后,据以演绎相机内部影像形成的模型。

First, the relative curvature of a certain curve at its first end and the directional angle of the first port tangent vector of that curve as well as the weight factor of the interpolation curve are given, then all the other control vertexes can be gotten by using the conditions of G continuity, and a method to construct transitional curves is also introduced so that we can get the closed interpolation curve which achieves G continuity globally.

首先给定某段曲线的首端相对曲率和该段曲线的首端切矢量的方向角以及插值曲线的权因子,然后利用G2连续条件求出其余控制顶点,并给出了构造过渡曲线的方法,得到了G2连续的闭插值曲线。

The initial value of the convergence half angle in the iterative synthesis is discussed and a more logical function is given for assigning it.

对轴对称收敛型电子枪设计方法进行了整理分析,就阴极半锥角的初始值对迭代综合法的收敛性能所产生的影响进行了讨论,针对低压缩比条件下原来的Vaughan公式失效的问题进行了分析,给出了更为合理的初始值计算公式。

The bending of rectangular plate is divided into the generalized statically determinate bending and the generalized statically indeterminate bending based on the analysis of the completeness of calculating condition at the corner point.

在分析角点求解条件完备性的基础上将矩形板弯曲划分为广义静定问题和广义超静定问题。

In experiment, the bead concentration was adjusted to make the transmission of the light through the cuvette to be about 70%, and the scattering pattern in far field was measured for the angular radius of its first dark ring.

在实验上,把聚苯乙烯小球分散在纯净水中,使其浓度满足光的透过率为70%左右的条件,然后测量单色平行光通过该样品比色皿后的远场衍射图样的第一暗环角半径的数值大小。

The equilibrium equations under local coordinate are obtained through Euler angle transformation. In the modeling of warp, otter door is treated as the end node. The equilibrium equation of otter door is established through d\'Alembert\'s principle. It provides the end boundary condition of the dynamic model of warp.

通过欧拉角的转换关系获得了曳纲微元段矢量动力平衡方程在曳纲局部坐标系下的方程组形式;在建模过程中,将网板视为曳纲的尾部节点,根据达朗伯原理建立了网板的平衡方程,并将其作为曳纲模型的尾部边界条件。

Neutron energy spectrum and angular distribution were computed for T4He reaction neutron source with 260 keV deuteron beam and TiT 1.5 thick target.

采用将厚靶分割成薄靶的方法对厚氚钛靶、260 keV氘束流能量条件下T4He反应中子源的能谱和角分布进行计算。

The lowest loss mode fields and the far field divergency angles of output beams of the UPCUR are calculated by use of Prony method. The relations between the mode discriminability, far field divergency angles and the parameters of the resonator are analyzed. And the theoretical results show that the output beams with diffraction limit quality can be obtained by using the UPUR with small magnification (M=1. 3), which is much better than the traditional unstable resonator under the same conditions.

采用Prony方法计算均匀相位输出耦合镜非稳腔的输出模场分布及远场方向性,分析了模式分辨率和光束远场发散角与系统各参数之间的关系,理论计算得到的结果表明,采用均匀相位输出耦合镜非稳腔,可以在小放大倍率(M=1.3)情况下得到质量达到衍射极限的输出光束,远远好于同等条件下的常规非稳腔,因此这种新型的谐振腔适用于在工业用千瓦级氧碘化学激光器。

In the case of bulk materials, the optimal phase only correlates with experimental conductions. But for nanomaterials, the equivalent resistance and capacitance R(subscript ins and C of MIS structure vary under illumination that will result in great changes in the optimal phase.

对於体相材料,"最佳相位"仅与测量条件有关;对於纳米材料等体系,光照可以改变MIS结构的等效电阻R(下标 ins、等效电容C(下标 ins,从而将引起最佳相位角的显著变化,使"最佳相位"与所研究材料的特性直接关联起来。

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