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If light passes from a “thinner” to a “denser” medium, (n2>n1) it is refracted toward the normal. Geometric Optics, Focussing Mirrors, Refraction, Total Internal Reflection, Wavelength, Frequency, Properties, Optics, Mirror Images, Focussing Light, Concave Mirror, Mirror Equations, Index of Refraction, Refrective Index, Snell's Law, Dr A Volya
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Electricity, Magnetism, Light Optics and Modern Physics Dr. Ingo Wiedenhöver Dr. A. Volya Today:
If we look at the wave pattern at one time, we see the above pattern in space. The distance between two maxima is the wavelength λ. Now imagine the wave zooming past you with speed c: It takes period time T for one full cycle. The frequency f is number of cycles per second λ c = T ⇔ = c T ⇔ T = c f = 1 T = c
What does the bottom figure represent?
The different colors of light correspond to em waves of different wavelengths ?: White light contains a mixture of all wavelengths: When white light encounters matter, five things can happen: a) It is absorbed (by black objects) b) It is absorbed and re-emitted in a different direction (by white objects) (by white objects) c) It is absorbed and only some wavelengths are re-emitted (by colored objects) d) It is reflected (by smooth metal surfaces) e) It passes through matter (in transparent objects) or a combination of the above
The light rays emitted from the object are reflected in the mirror. To the observer, they appear to come from the image. object distance =image distance, d =d Light rays are emitted from an object in all directions. We only draw some rays, which reach the observer. We find out, where and how images are formed. “virtual image”
Parabolic Mirrors are used to focus parallel light (approximation: spherical mirrors) Parallel rays which enter on axis all are focussed towards the focal point. The focal length of a spherical mirror is f = r/2. Rays from objects which are very far away are almost parallel!
The focal length, object- and image distances are related by The lateral magnification is the ratio of the size of image over object;
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When light enters a medium, its speed changes, it slows down! The index of refraction, e.g. the speed of light in water
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v = c n
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A fish swims below the surface of the water at P. An observer at O sees the fish at
When light passes from “denser” to “thinner” material, it follows snell's law: The maximum θ 1 , for which refraction possible (θ C
Beyond θ C , there is total internal reflection. Reflected ray 2 = 90 ° n 2 sin 2 = n 1 sin 1 sin 90 ° = 1 sin C = n 2 n 1