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一般变换
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  general transform
     General transform characters of lens
     透镜的一般变换特性
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  general function transform
     Jacobi elliptic function expansion method under a general function transform and its applications
     一般变换下的Jacobi椭圆函数展开法及应用
短句来源
     The new exact solutions to Klein-Gordon equation under a general function transform
     一般变换下Klein-Gordon方程新的精确解
短句来源
     Double Jacobian elliptic function expansion method under a general function transform and its applications
     一般变换下双Jacobi椭圆函数展开法及应用
短句来源
  general transformation
     In this paper, a general transformation formula for multiple series is proved.
     本文证明了多重级数的一般变换公式。
短句来源
     For some nonlinear equations, the general transformation would degenerate to the travelling wave reduction under certain conditions.
     对于某些非线性方程 ,在一定条件下一般变换退化为行波约化 .
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  “一般变换”译为未确定词的双语例句
     ON THE GENERAL TRANSFORMATIONS FOR WEAK SADDLES AND WEAK FOCUSES
     关于细鞍点与细焦点的一般变换
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     In order to calculate repeat integral and simplify it, general conversion formula through which the new variable is replaced by the old variable is introduced and included in the repeat integral symbol.
     为计算与化简重积分,需要在积分号下引进新变量代替旧变量的一般变换公式。
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     The General Transforms on the Weak Saddle of Quadratic Differential System
     二次系统中细鞍点的一般变换
短句来源
     RESEARCH INTO THE GENERAL GROUP OF TRANSFORMATIONS ON THE SET S
     集合S上一般变换群的研究
短句来源
     In this article, design of the holographic lens for generalized tranform simplified by Fourier optical system is presented. As a example, one dimensional 8×8 walsh hadamard transform was realized by the system. The design of holographic and experimental results are given.
     本文利用傅里叶光学系统简化了光学一般变换全息透镜的设计,以一维八序Walsh-Hadamard变换为例,用计算机设计和产生了变换所需的透镜,并进行引了光学实验,得到了预定变换结果。
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  general transform
The Michael transform, which simplifies structure 2 to precursor 3, can be found by general transform selection procedures.
      
  general transformation
A general transformation is presented that preserves the form of the three-dimensional boundary layer equations in an arbitrary orthogonal curvilinear coordinate system.
      
It appears that this is a general transformation available for analytes bearing the 2-hyroxyl-phenol (catechol) and/or the 2-amino-phenol moieties.
      
Leaving aside for the moment the spin and isospin degrees of freedom the most general transformation group, which leaves the hamiltonian invariant, is determined to be the unitary group in3 A dimensions (
      
Finally, for the case of scalar bosons, a more general transformation is defined which leaves theS-matrix invariant, but gives rise to a purely instantaneous interaction in the ladder approximation.
      
We adopt a local, purely thermodynamic approach recently developed in connection with the construction of a general transformation theory in thermodynamics.
      
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By using the irreducible tensor method of representing SHG coefficients, we have proposed in this paper a general transformation formula for SHG coefficients of the macroscopic crystal and those of its microscopic anionic groupings. It thus leads to a series of calculation formulas suitable generally for calculating the contributions of the anionic groupings of different orientations in the crystal to the macroscopic SHG coefficients. It has been shown that this method can be used conveniently to calculate the...

By using the irreducible tensor method of representing SHG coefficients, we have proposed in this paper a general transformation formula for SHG coefficients of the macroscopic crystal and those of its microscopic anionic groupings. It thus leads to a series of calculation formulas suitable generally for calculating the contributions of the anionic groupings of different orientations in the crystal to the macroscopic SHG coefficients. It has been shown that this method can be used conveniently to calculate the SHG coefficients of various iodates. The agreements of our calculation values with the experimental ones are quite satisfactory. Our work has provided a dear stero-structural criterion for searching of new types of SHG materials.

本文使用倍频系数的不可约张量表示法,得到了离子基团的微观倍频系数与晶体宏观倍频系数间的一般变换公式,从而为晶体中不同取向的基因对宏观倍频系数的贡献提供了普遍的计算公式。应用这一计算方法可方便地计算各种碘酸盐的倍频系数,结果相当满意。本文对于探索新型倍频材料,提供了明确的空间结构条件。

When the spacetime is experienced a Lorentz transformation the formula of temperature transformation is not unique.The simplest and the most reasonable formula for the temperature transformation is T=T01-β2The traditional formula δQ=δQ01-β2 for the transformation of heat is questionable: it is not satisfied when the heat is transferred between two bodies in relative motion.Hence,all the derivations of temperature transformation formula depending on δQ=δQ01-β2 are questionable,too.After the general transformation...

When the spacetime is experienced a Lorentz transformation the formula of temperature transformation is not unique.The simplest and the most reasonable formula for the temperature transformation is T=T01-β2The traditional formula δQ=δQ01-β2 for the transformation of heat is questionable: it is not satisfied when the heat is transferred between two bodies in relative motion.Hence,all the derivations of temperature transformation formula depending on δQ=δQ01-β2 are questionable,too.After the general transformation formula of δQ is derived,together with the temperature transformation formula T=T0v1-β2,it can be established that the total entropy change of a general thermodymmic process if positive and independent of the inertial reference frame we choose,i.c.,entropy is qn invariant increasing with time monotonically.

当时空经受洛伦兹变换时,温度变换的公式并不唯一确定。最简单最合理的温度变换式是T=T_0(1-β~2)~(1/2)。 传统上关于热量的变换公式δQ=δQ_0(1-β~2)~(1/2)不适用于有相对运动的物体间所传递的热量。因此,所有依赖于δQ=δQ_0(1-β~2)~(1/2)而推导出来的温度变换式,其推导方法都是有毛病的。 在求得热量δQ的一般变换式后,结合T=T_0(1-β~2)~(1/2)就可以证明一个一般热力学过程的总熵变恒大于零,并且与所选取的惯性参考系无关。就是说,熵是不变量且随时间单调地增加。

In this article, design of the holographic lens for generalized tranform simplified by Fourier optical system is presented. As a example, one dimensional 8×8 walsh hadamard transform was realized by the system. The design of holographic and experimental results are given.

本文利用傅里叶光学系统简化了光学一般变换全息透镜的设计,以一维八序Walsh-Hadamard变换为例,用计算机设计和产生了变换所需的透镜,并进行引了光学实验,得到了预定变换结果。

 
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