1·The far point of a normal eye is at infinity.
正常眼的远点在无穷远处。
2·He only catches up with it at infinity (infinitude).
他仅能在无限的地方赶上它。
3·Anti-de sitter space, although it is infinite, has a "boundary, " located out at infinity.
反德西特空间虽然无穷大，却有个位于无穷远的“边界”。
4·At infinity, there's no stored potential energy, and it drops off more and more negative as one over r.
在无限远处，没有储存的势能，并且它向负方向减少，当距离超过R时。
5·We have defined potential energy 0 to be zero at infinity, and that is why all bound orbits have negative total energy.
我们规定，无限大时,势能为，这就是为什么所有的,规则轨道总能量为负。
6·To construct a progression at infinity as an expansion of function in the continuous interval, a good result was achieved.
给出了一种不含导数的函数展开方法，在函数的连续区间内构造一个无穷级数作为函数的展开式。
7·The decay rate of the corresponding strong solution at infinity is also given for some kinds of initial data with exponential decay.
若其初值以指数方式衰退，且空间可微，则此强解在之后的时间内也将以指数方式衰退。
8·The mode currents form a weighted orthogonal set over the conductor surface, and the mode fields form an orthogonal set over the sphere at infinity.
经典特征模理论提供了一套在导体表面形成加权正交系的特征电流，在无穷远球面上形成正交系的特征场。
9·Cross ratio and element at infinity are two important concepts with projective geometry and primary tools in considerate projective property of figures.
交比和无穷远元素是射影几何中的两个重要概念，它们是探讨图形射影性质的主要工具。
10·The limit of the integrand f ( x ) of abnormal integral, which is convergent in the infinite range of integration, is not certainly equal zero at infinity.
摘要无穷限反常积分收敛时，其被积函数在无穷远处的极限不一定为零。