Chris Velzel's A Course in Lens Design PDF

By Chris Velzel

ISBN-10: 9401786844

ISBN-13: 9789401786843

ISBN-10: 9401786852

ISBN-13: 9789401786850

A path in Lens layout is an guide within the layout of image-forming optical structures. It teaches how a passable layout may be bought in an easy approach. thought is proscribed to a minimal, and used to aid the sensible layout paintings. The booklet introduces geometrical optics, optical tools and aberrations. It provides an outline of the method of lens layout and of the suggestions utilized in this method. 1/2 its content material is dedicated to the layout of 16 kinds of lenses, defined intimately from starting to finish. This booklet isn't like so much different books on lens layout since it stresses the significance of the preliminary stages of the layout approach: (paraxial) lay-out and (thin-lens) pre-design. The argument for this variation of accessory is that during those levels a lot info might be got concerning the houses of the lens to be designed. this knowledge can be utilized in later stages of the layout. This makes A path in Lens layout an invaluable self-study publication and an appropriate foundation for an introductory path in lens layout. the math customarily used is collage algebra, in a couple of sections calculus is utilized. The booklet will be utilized by scholars of engineering and technical physics and via engineers and scientists.

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Example text

This was confirmed in the work of Anthoni van Leeuwenhoek. 3 mm and M = 48. It turned out that the observable details were of the order of 2 lm. The compound microscope consists of an objective lens that makes a magnified image of the object, and an ocular that projects an image at infinity, so that the eye has a focused image on its retina (see Fig. 6). The angular magnification of the compound microscope is given by M ¼ Mob 250 ; f oc ð2Þ where Mob is the (linear) magnification of the objective and foc the focal length of the ocular.

R This aberration is called field curvature. 6 Astigmatism ÀE ¼ b4 V2 gives dg0 ¼ 2 b4 g02 r yr Á dn0 ¼ 0: n0 u0 ð3:13Þ The wavefront error is proportional to q2 y2r , curvature only in the meridional cross-section. The aberration is a defocus of the meridional rays, proportional to g02 r . This aberration is called astigmatism. ) are equal in form to those for defocus shown in Fig. 5. When both b3 and b4 are =0, we have meridional field curvature 1 Rm ¼ 4ðb3 þ b4 Þ. Sagittal field curvature R1 ¼ 4b3 , where again we have taken n0 u0 ¼ az.

With a height "h of the film plane, the field angle w is given by tan w ¼ "h=s0 . The resolution of lenses used in cameras depends on the application of the camera. 1 mm at a distance of 250 mm. 025 mm. C. 1007/978-94-017-8685-0_2, Ó Springer Science+Business Media Dordrecht 2014 25 26 2 Optical Instruments (Paraxial Approximation) Fig. 1 A simple camera The lens of a film camera (and also a film projection lens) should have a better resolution over a smaller field (8 or 16 mm). With a CCD as target in a camera, the pixel size is related to the required resolution.

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A Course in Lens Design by Chris Velzel

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