Allied Health Professions

Download Fundamental Optical Design by Michael J. Kidger PDF

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By Michael J. Kidger

The heritage of optical layout has engendered theoretical paintings originating in numerous nations, and utilizing various nomenclature and signal conventions. Michael Kidger was once adept at choosing themes that might be worthy within the mainstream of optical layout, lowering idea to the necessities and rewriting it utilizing a typical nomenclature and signal conference. This paintings, released after Kidger's dying with assistance from his colleagues, presents all of the crucial and top components of his classes taught around the globe on lens and optical design.

Contents

- Foreword
- Preface
- checklist of Symbols
- Geometrical Optics
- Paraxial Optics
- Ray Tracing
- Aberrations
- Chromatic Aberration
- Seidel Aberrations
- ideas of Lens Design
- Achromatic Doublet Objectives
- Petzval Lenses and Telephoto Objectives
- Triplets
- Eyepieces and Afocal Systems
- Thermal Imaging Lenses
- Catadioptric Systems
- Index

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Fundamental Optical Design

The heritage of optical layout has engendered theoretical paintings originating in numerous international locations, and utilizing assorted nomenclature and signal conventions. Michael Kidger used to be adept at choosing subject matters that might be invaluable within the mainstream of optical layout, lowering idea to the necessities and rewriting it utilizing a typical nomenclature and signal conference.

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12. Zero-power (afocal) system at finite conjugates. This is important in the design of binoculars. 75 mm. Since the exit pupil of the instrument must be close to the pupil of the user’s eye, we can see that the Lagrange invariant gives us some very important information. 6 Newton's conjugate distance equation We now consider conjugate distance equations, which give us the position of the image in terms of the object position. In Fig. 13, the ray O1FP1O1 is chosen to pass through the first principal focus, and it is therefore parallel to the optical axis in the image space.

80) Therefore, H ( Ei 1  Ei )  hi 1 hi  hi 1 hi hi 1hi  hi hi 1 . 81) Therefore, Ei 1  Ei  1 hi 1hi  hi hi 1 H hi hi 1  1 (hi  du )hi  hi (hi  du ) H hi hi 1  d uhi  uhi . 24) 44 Chapter 2 Ei 1  Ei   d . 83) Since E is zero at the stop, by definition, it follows that we can calculate E at the surfaces adjacent to the stop using Eq. 83), and we can of course extend this to calculate E at all surfaces in a system. Then, using E in Eqs. 78), we can calculate all of the chief ray quantities h , u , and A , without ever tracing a chief ray.

36) Therefore, the cone half-angle, θ, shown in Fig. 12, is given by tan θ = r = e2 − 1 z and cos 2 θ = 1 1 1 = − or k = − . 37) Therefore, an axicon can be represented by a hyperboloid, with a conic constant given by Eq. 37) and a large vertex curvature. 33333 . 12. 3333 (θ = 30 deg) and different curvatures. References 1. W. T. Welford, Aberrations of Optical Systems, Adam Hilger (1986). ” Therefore, we will use the terms “paraxial optics” and “paraxial region” in order to eliminate any confusion.

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