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伽利略望远镜和望远显微镜的角视场和线视场

Angular and linear fields of view of Galilean telescopes and telemicroscopes.

作者信息

Katz Milton

机构信息

SUNY College of Optometry, State University of New York, 33 West 42nd Street, New York, NY 10036, USA.

出版信息

Optom Vis Sci. 2007 Jun;84(6):522-31. doi: 10.1097/OPX.0b013e31806db573.

Abstract

PURPOSE

The calculation of the angular fields of view (FOVs) of Galilean telescopes generally necessitates the calculation of the pupils and ports. This, in turn, requires knowledge of the optical design of the telescope, in particular, the focal lengths or powers of the objective and ocular lenses. Equations for finding the FOV that obviate the need to calculate pupils and ports, or even to know the lens powers of the telescope, are presented in this article. The equations can be used to find the FOVs in image space of real Galilean telescopes of known magnification, merely by measuring the distance between the objective and ocular lenses and the diameter of the objective lens. The equations include the effects of eye pupil diameter and eye relief. Linear FOVs (LFOVs) of Galilean telemicroscopes are similarly determined.

METHODS

Two image space angular FOV equations were derived: (1) an equation to determine the angular FOVs of a telescope with various amounts of vignetting and eye relief; and (2) an equivalent equation for the LFOVs of telescopes fitted with lens caps for near vision.

RESULTS

The FOV increases linearly with increasing vignetting. Increasing the eye relief results in a nonlinear decrease in the FOV, shown as a fraction of the normalized value for zero eye relief. Decrements in the FOVs with increasing eye relief as a fraction of the normalized field angle when the eye relief = 0 are shown to be constant regardless of the vignetting level. A transition of the objective lens from field stop to aperture stop occurs when the eye pupil diameter exceeds the diameter of the objective lens divided by the magnification.

CONCLUSIONS

Equations have been derived for Galilean telescopes and telemicroscopes that make it unnecessary to find pupils and ports, or to know the powers of the lenses. They provide a direct and simple evaluation of angular and LFOVs as functions of magnification, objective lens diameter, eye pupil diameter, eye relief, and vignetting, and enable comparisons of actual telescopes.

摘要

目的

计算伽利略望远镜的角视场(FOV)通常需要计算光瞳和出射光瞳。这反过来又需要了解望远镜的光学设计,特别是物镜和目镜的焦距或焦度。本文提出了一些用于计算视场的方程,这些方程无需计算光瞳和出射光瞳,甚至无需知道望远镜的透镜焦度。这些方程可用于仅通过测量物镜和目镜之间的距离以及物镜的直径来计算已知放大倍数的实际伽利略望远镜在像空间中的视场。这些方程考虑了眼瞳直径和出瞳距的影响。伽利略望远显微镜的线性视场(LFOV)也可类似地确定。

方法

推导了两个像空间角视场方程:(1)一个用于确定具有不同渐晕量和出瞳距的望远镜的角视场的方程;(2)一个适用于装有近视力透镜盖的望远镜的线性视场的等效方程。

结果

视场随渐晕增加而线性增加。出瞳距增加会导致视场非线性减小,以零出瞳距时归一化值的分数表示。当出瞳距 = 0时,视场随出瞳距增加而减小的比例,作为归一化视场角的分数,被证明与渐晕水平无关是恒定的。当眼瞳直径超过物镜直径除以放大倍数时,物镜从视场光阑转变为孔径光阑。

结论

已推导出适用于伽利略望远镜和望远显微镜的方程,无需寻找光瞳和出射光瞳,也无需知道透镜的焦度。它们提供了对视场角和线性视场的直接且简单的评估,作为放大倍数、物镜直径、眼瞳直径、出瞳距和渐晕的函数,并能够对实际望远镜进行比较。

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