By Karl Dieter Moeller

ISBN-10: 0387953604

ISBN-13: 9780387953601

This publication is meant for a one semester path in optics for juniors and seniors in technological know-how and engineering; it makes use of Mathcad(R) scripts to supply a simulated laboratory the place scholars can examine through exploration and discovery rather than passive absorption.

The textual content covers all of the average themes of a conventional optics path, together with: geometrical optics and aberration, interference and diffraction, coherence, Maxwell's equations, wave publications and propagating modes, blackbody radiation, atomic emission and lasers, optical homes of fabrics, Fourier transforms and toes spectroscopy, photo formation, and holography. It comprises step-by-step derivations of all easy formulation in geometrical, wave and Fourier optics.

The simple textual content is supplemented by means of over one hundred seventy Mathcad records, every one suggesting courses to unravel a specific challenge, and every associated with a subject matter in or program of optics. the pc records are dynamic, permitting the reader to determine immediately the results of adjusting parameters within the equations. scholars are hence inspired to invite "what...if" inquiries to asses the actual implications of the formulation.

The publication is written for the learn of specific tasks yet can simply be tailored to a version of comparable reports. The three-fold association of textual content, functions, and records makes the booklet appropriate for "self-learning" via by way of scientists or engineers who wish to refresh their wisdom of optics. All documents are published out and come on a CD and will good function beginning issues to discover recommendations to extra complicated difficulties as skilled via engineers of their functions.

The Mathcad(r) scripts at the CD are supplied in either Mathcad(r) 7 and Mathcad(r) 2000, and as PDF documents.

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**Extra info for Optics - Learning By Computing With Model Examples Using Mathcad, Matlab, Mathematica, And Maple**

**Example text**

4 Negative Lens. 13 (a) Image formation of an object larger than the diameter of the lens. The extended plane of the lens is used; (b) image formation for an object at infinity. The axis B of the system is the ray from the center of the object through the center of the lens. the PF-ray is assumed to come from the top of an object at finite distance; the corresponding image is indicated. 13b). 6 Thin Lens and Two Different Media on the Outside We go back to the thin lens equation and choose different indices of refraction at the two media on both sides of the lens.

1 Refraction and Translation Matrices A thick lens has two spherical surfaces separated by a dielectric material of a certain thickness. 8. 19 Multiple lens system. The lenses may have different radii of curvature and different refractive indices. but now take it into account. One may calculate the image formation of the thick lens by first finding the image produced by the first surface. Then one uses this image as an object in the second imaging process and finds the image produced by the second surface.

Calculate the final image distance for two lenses at distance D 50. Assume that the object distance from the first lens is −20. Give the magnification, and make a sketch of object and image, assuming that the object is erect. Consider the following cases. a. First lens f1 10; second lens f2 10. b. First lens f1 10; second lens f2 −10. c. First lens f1 −10; second lens f2 10. d. First lens f1 −10; second lens f2 −10. 2. Distance between the lenses is smaller than 2f . Calculate the final image distance for two lenses at distance D 6.

### Optics - Learning By Computing With Model Examples Using Mathcad, Matlab, Mathematica, And Maple by Karl Dieter Moeller

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