1) limit point
极限点
1.
Based on the measurement process and learning of measuring error, a novel method of using the limit point to evaluate the static characteristics of the nonlinear transducer is presented.
基于对测量过程、测量误差的认识 ,提出了一种利用极限点法评估非线性传感器静态特性的一种新方法。
2.
The limit point is analysed by establishing the mathematic model of cyclinder and taper orthoyonal.
通过建立圆柱与圆锥正交时的数学模式，对极限点进行几何分析，用微积分的方法求出极限点的坐标及变化规
3.
The tangent stiffness matrix is obtained from the engineering strain and the principle for determining the limit point and bifurcation point is given.
由工程应变推导出几何非线性的切线刚度矩阵,并给出判断分歧点与极限点的准则,最后用一数值例题说明该方法的分析过程。
2) limit-point
极限点
1.
In this paper we studied the deficiency indices of powers of a class of J -symmetric differential operators,got some sufficient conditions which guarantee the powers be limit-point.
研究了一类 J对称微分算子的亏指数 ,并给出了极限点的充分条件 ,从而将文〔1〕的结果推广到了复系数的情
2.
It was concluded that singular dirac operator L was limit-point when the potential was continuous.
Dirac方程是量子力学的基本方程,讨论Dirac算式的自伴域在数学物理中有广泛的应用,文中根据Dirac算式的最大定义域、最小定义域和Dirac算式在区间[0,b]上的自伴域的结果,利用自伴延拓的Calkin描述通过对b取极限的讨论推导出Dirac算式在区间[0,+∞)上的自伴域D(T(L))={f∈D(L)|f1(0)cosα+f2(0)sinα},并证明了当势函数q1(x),q2(x)为区间[0,+∞)上的实值连续函数,则L必是极限点。
3) limit points
极限点
1.
The construction of the sets of limit points on indeterminate formula f(x)/g(x)andf (x)/g (x) in 0/0 and */0 are being described in this paper.
讨论了0/0型和*/∞型不定式f(x)／g(x)的极限点集以及相应的f'(x)／g'(x)的极限点集的结构。
4) Utmost dew point
极限露点
5) ω-limit point
ω-极限点
6) limiting zero point
极限零点
1.
By deriving limiting zero point of the equation,some sufficient conditions that guarantee the existence and uniqueness of traveling wave solution of this equation are obtained.
通过讨论方程的极限零点和非极限零点,获得了保证其行波解存在惟一性的充分条件。
补充资料：轨道的极限点
轨道的极限点
limit point of a trajectory
轨道的极限点[俪t因血It of a hajectol寸;npe及e。‘，a，TO叹Ka TPae灯oP皿HJ 动力系统.厂的轨道{尹x}的极限点是点 x。二*叭.f“‘(l)又仪极限点(戊一俪itPO毗))或 ‘。二沪曳户‘(2)(。极限点(。·腼t point))，这里序列{r*}*。、满足:(l)中当火~的时￡*-今一田，或(2)中当k，的时t、~+的，并且(l)或(2)中的极限存在. 对于动力系统(d”lam屺 al system)厂(或者换句话说，对于f(t，x)，见11])的轨道{frx}，:极限点(田极限点)与动力系统f一‘(逆向时间系统)的轨道{f一‘x}的山极限点(“极限点)相同.轨道{尹、}的所有田极限点(以极限点)的集合Q二(A二)称为这个轨道的田极限集(田一】inlit set)(仪极限集(:一如lit set))(见轨道的极限集(1如it set ofatrajec-tory)).
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条