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

By American Academy of Ophthalmology, Dimitri T. Azar MD

Part three has been thoroughly reorganized for simpler use! you will find extra real-life medical examples, many new figures and new studying routines to assist gauge your knowing of the fabric. part three presents a complete assessment of scientific optics, together with present purposes of optical phenomena resembling lasers, spectacles, IOLs and refractive surgical procedure. offers optics of the human eye; uncomplicated options of geometric optics; ophthalmic tools and phone lenses. imaginative and prescient rehabilitation can also be discussed.

Upon final touch of part three, readers might be capable to:

Outline the foundations of sunshine propagation and snapshot formation and paintings via many of the primary equations that describe or degree such homes as refraction, mirrored image, magnification and vergence
Define a few of the kinds of visible conception and serve as, together with visible acuity, brightness sensitivity, colour notion and distinction sensitivity
Explain the optical rules underlying quite a few 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

The angle formed by the incident ray and surface normal is the angle of incidence, ei. This is not the angle between the incident ray and the optical interface. The reflected ray and the surface normal form the angle of reflection, (),. The law of reflection states that the reflected ray lies in the same plane as the incident ray and the surface normal (ie, the reflected ray lies in the plane of incidence) and that (Ji =(),. The amount of light reflected from a surface depends on 8; and the plane of polarization of the light.

If so, what are its characteristics? Light has a vergence of -5 D, but as the light crosses the 5 cm to the second lens, its vergence changes (the vergence change on transfer). In order to determine the vergence at the second lens, it is necessary to find the location of the image formed by the fast lens. However, if the first lens does not form an image, how can the vergence at the second lens be calculated? The solution is to use a mathematical trick. Light leaving the first lens has a vergence of -5 D.

A Air Glass Optical interface Figure 1-22 Light traveling from points A to B follows only path 2 because it requires the least time. Light does not travel along either path 1 or path 3. /Illustration developed by Edm ond H. Thall, MD, and Kevin M . M iller, M O, and ren dered by C. H. ) 22 • Clinical Optics but has the shortest distance in glass. Nevertheless, the extreme length of the overall route makes this a fairly slow path. th light will actually follow. Using mathematics beyond the scope of this text, it can be shown that the optimal path is the one predicted by Snell's law.

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