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integral component相关的网络例句

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与 integral component 相关的网络例句 [注:此内容来源于网络,仅供参考]

First,we consider the lower semicontinuity property fora functional with linear growth in LDΩthe second, in the SBD space,we discussthe lower semicontinuity of an integral functional that the integrand is a Carathéodoryfunction and that satisfies a symmetric quasi-convex assumption, by the compactnesstheorem of the SBD space,blow-up method and Morrey theorem,prove that integral functional is lower semicontinuous with respect to L~1- convergence;then by using theone-dimentional sections method and the structure theorem of the BD functions, dis-cuss the lower semicontinuity of the integral functional in the whole BD space.

首先我们考虑LD空间满足线性增长的积分泛函的下半连续性;其次在SBD函数空间讨论了被积函数为Carathéodory函数时的积分泛函在满足对称拟凸条件时的下半连续性,主要利用SBD函数空间的紧性定理和blow-up方法以及Morrey定理等给出了积分泛函关于L~1-强收敛的下半连续性;然后利用BD函数的一维截断方法和结构定理,讨论了在BD全空间上的积分泛函的下半连续性。

This paper discussed working principle of the ideal electronic integrator which was constituted of operational amplifier. Integral drift parameter and integral time constant as main factors influencing the accuracy of integral output were analyzed.

摘 要:讨论了由运算放大器构成的理想电子积分器的工作原理,分析了积分漂移、积分时间常数等主要因素对积分输出误差的影响及改善措施。

Nextly, the definition of Perron integral and Denjoy integral for fuzzy-number-valued functions in the plane are given, and by using them, we discuss the characterization theorems of the primitive functions for fuzzy Henstock integral in the sense of the special derivate bases.

其次,定义了平面上的模糊Perron积分及模糊Denjoy积分,并利用这两种积分对平面上两种特殊形式的导数基意义下的模糊Henstock积分原函数进行了刻划。

All the measurement results of magnetic field of optical klystron before and after shimming are given, including the distribution of field integral and phase error on axis, field integral and RMS phase error for different gaps and transverse distribution of field integral.

详述了合肥储存环的光学速调管辐射段磁场垫补的三种方式,测量了垫补前后不同间隙下积分场分布、位相误差及横向均匀度,各项指标都达到了要求。

In the path integral formalism, we represent the generating functional and Green functions of Φ〓 theory by taking account of that the partial and the functional derivatives commute. Also we discuss the effective action for noncommutative scalar fields, and show how the noncommutative phase factors appear in path integral formalism. We realize that the two approaches (path integral and canonical quantizations) are completely equivalent each other.

在用路径积分方法对非对易标量场进行研究时,我们利用偏微商和泛函微商的可交换性,给出了Φ〓场格林函数和格林函数生成泛函的具体表达形式,得出了非对易相因子在路径积分方法中的具体表现形式,并对连通格林函数和有效作用量等问题做了讨论。

We introduce the concept of irregular incremental integral samples. Therefore, we present the reconstruction of signal from regular and irregular incremental integral samples in spline subspaces and show the essence of the concept of incremental integral samples. The obtained results improve and generalize the Aldroubi, Moon, Zhou and Sun's results.

我们引入了非均匀增量积分采样的概念,并讨论了在样条子空间中从均匀增量积分采样和非均匀增量积分采样中的重构,从而揭示了增量积分采样的实质,获得的结果推广并改进了Aldroubi、Moon、周性伟、孙文昌等人的工作。

The integral with respect to scattering angle is separated andcan be carried out exactly without meeting the usual divergent difficulty. The five-foldBoltzmann integral is reduced to a simple three-fold integral.

通过一种变量变换的方法,成功地将玻耳兹曼碰撞项中的有关散射角积分,分离并解析地积出,将五重积分形式的玻耳兹曼碰撞项化为较简单的三重积分。

They arebirth stochastic integral functionals,death stochastic integral func-tionals and stochastic integral functionals at time t in level dependentQBD processes,respectively.

教授和王梓坤教授等人关于在通常生灭过程上随机积分泛函的主要结论,而且不同于Ho,Y.C。

Then introduced a triple integral calculation of the basic concepts and methods of calculating the triple integral in three-dimensional volume, as well as the mechanical application of triple integral example .

随后介绍了三重积分的基本概念和计算方法,三重积分计算立体体积以及力学中三重积分的应用举例。

Then introduces the basic concept and triple integral calculation method, the three-dimensional volume and triple integral calculation of triple integral mechanics.

随后介绍了三重积分的基本概念和计算方法,三重积分计算立体体积以及力学中三重积分的应用举例。

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But this is impossible, as long as it is engaging in a market economy, there are risks in any operation.

但是,这是不可能的,只要是搞市场经济,是有风险的任何行动。

We're on the same wavelength.

我们是同道中人。

The temperature is usually between 300 and 675 degrees Celsius.

温度通常在摄氏300度到675度之间。