Read e-book online 2014-2015 Basic and Clinical Science Course (BCSC): Section PDF

By American Academy of Ophthalmology, Dimitri T. Azar MD

ISBN-10: 1615255575

ISBN-13: 9781615255573

Part three has been thoroughly reorganized for simpler use! you can find extra real-life scientific examples, many new figures and new studying workouts to aid gauge your knowing of the fabric. part three offers a accomplished evaluate of scientific optics, together with present purposes of optical phenomena equivalent to lasers, spectacles, IOLs and refractive surgical procedure. offers optics of the human eye; uncomplicated thoughts of geometric optics; ophthalmic tools and speak to lenses. imaginative and prescient rehabilitation is additionally discussed.

Upon of entirety of part three, readers may be capable to:

Outline the foundations of sunshine propagation and snapshot formation and paintings via a few of the primary equations that describe or degree such houses as refraction, mirrored image, magnification and vergence
Define a number of the forms of visible notion and serve as, together with visible acuity, brightness sensitivity, colour notion and distinction sensitivity
Explain the optical rules underlying a variety of modalities of refractive correction: spectacles, touch lenses, intraocular lenses and refractive surgical procedure

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Extra info for 2014-2015 Basic and Clinical Science Course (BCSC): Section 3: Clinical Optics

Sample text

However, if the angle of refraction is 45°, the interface becomes an impenetrable barrier! The interface is transparent to some rays and opaque to others. Physicists have devoted considerable attention to this phenomenon. TIR has great practical value. In the early 1600s, it was difficult to make a good mirror. The best surfaces could specularly reflect only about 80% of incident light, and the rest was diffusely reflected, which made these surfaces nearly useless as imaging devices. However, TIR is just that-total.

Law of Refraction (Specular Transmission) In specular transmission, the transmitted ray's direction bears a definite relation to the incident ray's direction. Again, a surface normal is constructed, and the angle of incidence and the plane of incidence and transmission are defined just as they were for reflection (Fig 1-15). The angle formed by the transmitted ray and the surface normal is the angle of refraction, also known as the angle of transmission. The angle of transmission, (JP is preferred by some authors because the symbol for angle of refraction, (),, might otherwise be confused with that of the angle of reflection, (),.

In this case, the image formed by the first lens became the object for the second lens, which in turn produced a final image. Any number of lenses can be analyzed in the same way. The image produced by the first lens becomes the CHAPTER 1: Geometric Optics • 39 object for the second lens; the image formed by the second lens becomes the object for the third lens; and so forth. 5 cm to the right of Pi', Consider a second 2-lens example (Fig 1-40). 50 D lens. Where is the final image? Applying the LME, the first lens produces an image 50 cm to the right of Pi'.

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2014-2015 Basic and Clinical Science Course (BCSC): Section 3: Clinical Optics by American Academy of Ophthalmology, Dimitri T. Azar MD

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