Physical Classical optics is a more comprehensive model of light, which includes wave effects such as diffraction and interference that cannot be accounted for in geometric Classical optics.
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Physical Classical optics is a more comprehensive model of light, which includes wave effects such as diffraction and interference that cannot be accounted for in geometric Classical optics.
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Practical applications of Classical optics are found in a variety of technologies and everyday objects, including mirrors, lenses, telescopes, microscopes, lasers, and fibre Classical optics.
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Greek philosophy on Classical optics broke down into two opposing theories on how vision worked, the intromission theory and the emission theory.
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Classical optics commented on the parity reversal of mirrors in Timaeus.
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Classical optics based his work on Plato's emission theory wherein he described the mathematical rules of perspective and described the effects of refraction qualitatively, although he questioned that a beam of light from the eye could instantaneously light up the stars every time someone blinked.
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Classical optics summarized much of Euclid and went on to describe a way to measure the angle of refraction, though he failed to notice the empirical relationship between it and the angle of incidence.
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Classical optics used this law to compute optimum shapes for lenses and curved mirrors.
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Classical optics rejected the "emission theory" of Ptolemaic optics with its rays being emitted by the eye, and instead put forward the idea that light reflected in all directions in straight lines from all points of the objects being viewed and then entered the eye, although he was unable to correctly explain how the eye captured the rays.
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Classical optics was able to correctly deduce the role of the retina as the actual organ that recorded images, finally being able to scientifically quantify the effects of different types of lenses that spectacle makers had been observing over the previous 300 years.
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Wave Classical optics was successfully unified with electromagnetic theory by James Clerk Maxwell in the 1860s.
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The understanding of the interaction between light and matter that followed from these developments not only formed the basis of quantum Classical optics but was crucial for the development of quantum mechanics as a whole.
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Quantum Classical optics gained practical importance with the inventions of the maser in 1953 and of the laser in 1960.
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Classical optics is divided into two main branches: geometrical optics and physical optics.
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In geometrical Classical optics, light is considered to travel in straight lines, while in physical Classical optics, light is considered as an electromagnetic wave.
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Geometrical Classical optics can be viewed as an approximation of physical Classical optics that applies when the wavelength of the light used is much smaller than the size of the optical elements in the system being modelled.
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Geometric Classical optics is often simplified by making the paraxial approximation, or "small angle approximation".
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All of the results from geometrical Classical optics can be recovered using the techniques of Fourier Classical optics which apply many of the same mathematical and analytical techniques used in acoustic engineering and signal processing.
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Techniques known as adaptive Classical optics have been used to eliminate the atmospheric disruption of images and achieve results that approach the diffraction limit.
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Quantum Classical optics is not just theoretical; some modern devices, such as lasers, have principles of operation that depend on quantum mechanics.
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Specialty areas of Classical optics research include the study of how light interacts with specific materials as in crystal Classical optics and metamaterials.
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Today, the pure science of Classical optics is called optical science or optical physics to distinguish it from applied optical sciences, which are referred to as optical engineering.
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Many people benefit from eyeglasses or contact lenses, and Classical optics are integral to the functioning of many consumer goods including cameras.
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