Airy Disk Diffraction
1diffraction by disk
Большой англо-русский и русско-английский словарь >diffraction by disk
2diffraction by disk
Англо-русский технический словарь >diffraction by disk
3diffraction by disk
Универсальный англо-русский словарь >diffraction by disk
4diffraction disk
дифракционныйкружок, диск ЭйриБольшой англо-русский и русско-английский словарь >diffraction disk
5diffraction disk
Англо-русский словарь технических терминов >diffraction disk
6diffraction by a disk
Универсальный англо-русский словарь >diffraction by a disk
7diffraction disk
Универсальный англо-русский словарь >diffraction disk
8diffraction disk
English-russian dictionary of physics >diffraction disk
- Airy Disk - An Overview ScienceDirect Topics
- Airy Disk Diffraction Limit
- Circular Aperture Diffraction
- Diffraction Pattern And Aberrations - Telescope Optics
См. также в других словарях:
Sep 10, 2018 The result is an Airy pattern, illustrated to the right in the tutorial, where the central Airy disk is surrounded by an alternating series of interlaced dark and light zones of diminishing intensity where the wavelets interfere both constructively (light zones) and destructively (dark zones). The diffraction pattern caused when light passes through an aperture is called the Airy Disk. Find out how the Airy Disk can impact your image at Edmund Optics. The aperture diffraction pattern above was photographed with Fuji Sensia 100ASA slide film and then digitized. With the time exposure necessary to show the side lobes, the central peak was washed out nearly white. The only retouching of the digital image was to paint in the washed out part of the central maximum (Airy's disc). Sep 11, 2018 Airy Pattern Basics. The three-dimensional diffraction pattern formed by a circular aperture near the focal point in a well-corrected microscope is symmetrically periodic along the axis of the microscope as well as radially around the axis. When this diffraction pattern is sectioned in the focal plane, it is observed as the classical two-dimensional diffraction spectrum known as the Airy pattern.
Airy Disk - An Overview ScienceDirect Topics
diffraction by disk — difrakcija per apskritą ekraną statusas T sritis fizika atitikmenys: angl. diffraction by disk; disk diffraction vok. Beugung am Kreisscheibe, f; Beugung am runden Schirme, f rus. дифракция на круглом экране, f pranc. diffraction par un écran… … Fizikos terminų žodynas
disk diffraction — difrakcija per apskritą ekraną statusas T sritis fizika atitikmenys: angl. diffraction by disk; disk diffraction vok. Beugung am Kreisscheibe, f; Beugung am runden Schirme, f rus. дифракция на круглом экране, f pranc. diffraction par un écran… … Fizikos terminų žodynas
diffraction par un écran rond — difrakcija per apskritą ekraną statusas T sritis fizika atitikmenys: angl. diffraction by disk; disk diffraction vok. Beugung am Kreisscheibe, f; Beugung am runden Schirme, f rus. дифракция на круглом экране, f pranc. diffraction par un écran… … Fizikos terminų žodynas
Diffraction — Computer generated intensity pattern formed on a screen by diffraction from a square aperture … Wikipedia
disk — 1. A round, flat plate; any approximately flat circular structure. 2. SYN: lamella (2). 3. In dentistry, a circular piece of thin paper or other material, coated with an abrasive substance, used for cutting and polishing tee … Medical dictionary
diffraction disk — noun : spurious disk … Useful english dictionary
Airy disk — Computer generated image of an Airy disk. The gray scale intensities have been adjusted to enhance the brightness of the outer rings of the Airy pattern … Wikipedia
Atmospheric diffraction — is manifested in the following principal ways:* Fourier optics is the bending of light rays in the atmosphere, which results in remarkable visual displays of astronomical objects, such as depictions on this page.* Radio wave diffraction is the… … Wikipedia
spurious disk — noun : the small apparently circular disk of a star as seen in a telescope that limits the resolving power of the telescope and varies inversely with the diameter of the objective called also diffraction disk … Useful english dictionary
airy disk — noun Usage: usually capitalized A : the bright central spot in the system of diffraction rings formed by an optical system with light from a point source (as a star) … Useful english dictionary
Beugung am Kreisscheibe — difrakcija per apskritą ekraną statusas T sritis fizika atitikmenys: angl. diffraction by disk; disk diffraction vok. Beugung am Kreisscheibe, f; Beugung am runden Schirme, f rus. дифракция на круглом экране, f pranc. diffraction par un écran… … Fizikos terminų žodynas
How does the diffraction pattern known as the Airydiskget generated by shining light through a pinhole? Or moregenerally,what causes diffraction of light? Diffraction of light occursbecauseof its transverse wave nature. We have already said that whenlighthits an object, it is diffracted. This phenomenon is bestunderstood by an examination of Huygens' Principle. In 1678, the Dutchpysicist Christiaan Huygens wrote a treatise on the wave theory oflight in which he presented a theory now known as Huygens'Principle. It states that every point ona wave front can be thought of as a new point source for wavesgenerated in the direction the wave is traveling or beingpropagated. OR-- the wavefront of a propagating wave oflight at any instant conforms to the envelope of spherical waveletsemanating from every point on the wavefront at the prior instant (withthe understanding that the wavelets have the same speed as the overallwave). Fresnel later elaborated on Huygens' Principle by statingthat the amplitude of the wave at any given point equals thesuperposition of the amplitudes of all the secondary wavelets at thatpoint (with the understanding that the wavelets have the same frequencyas the original wave). These are termed Huygens’ wavelets. The formation of the Airydisk can best be described by looking at how imaging of a luminouspointoccurs in a lens system such as is found in the compound microscope.Thefollowing diagram shows what happens.
If a luminous point at A is projected through thefrontlens of an objective O1, and assuming that the light ismonochromatic,light coming from point A will define wave surfaces as spheres (e.g., So)with their centers at A. Assuming the objective to be a perfectlens,the light going through it will also produce wave surfaces as spheresaswell (e.g., Si).The centers of these spheres are at point A'0which is a geometrical image of A.
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At any point on the wave surface ofSi according to Huygen's Principle, the image A'0is formed as if all the points of the wave surface were actual sourcesof light with the same vibratory state. But any point on the wavesurfacesuch as M emits vibrations not only towards A'0, but also inother directions. In fact all the points on the wave surface Sidiffract the light which spreads over the image surrounding the point A'0. The diagram below at the left shows that all the vibrations emanatingfromany point on the wave surface Si will reach point A'0in the same vibratory state. Only two waves from points M and M0are shown to keep the figure simple. As the waves have thesame vibration, the amplitudes are additive and since amplitude is seenby the eye as brightness, at point A'0, we have a verybrightspot.Thediagram on the right shows vibrations going to a point A'1fromM and M0. The amplitudes are opposite each other when theyreachthe plane (indicated by line P and extending out from the page) whereourdiffraction image is generated. We would now have a dark area atpoint A'1 because the luminous amplitudes cancel each otherout and add up to zero. The same situation would happen if A'1were on the other side at the same distance from A'0. And in fact if one considered the whole plane of line P as shown by thesquare in perspective, the image would be a dark ring with a radius A'1-A'0with A'0 at the center as shown by the circle. Ifthe vibrations coming from points M and M0 were imaged at apoint A'2 on line P twice as from point A'0as A'1, the amplitudes of the vibrations would once again beadditive and one would then see a bright ring in the plane of lineP. It also follows that the intensities of the vibrations at all thepointson the plane of line P results from vibrations from all the points onwavesurface Si, not just those from points M and M0.
Airy Disk Diffraction Limit
If all this information is taken together, then theimageseen in the plane of line P would be a very bright central circulardisksurrounded by alternately bright and dark rings whose intensitydecreasesrapidly as distance increases: the Airy disk. It canalso be seen that the distances between the bright and dark rings willchange with changes in the wavelength of light.
It must be remembered that any object observed inthemicroscope is subject to the phenomena described here and this hasimportantconsequences for the generation of enlarged images in the microscopeandis why the concept of numericalaperture is so important in microscopy.
Circular Aperture Diffraction
*Diagrams redrawn from Francon, M. 1961. Progressin Microscopy. Pergamon Press: London (also Row, PetersonandCo.: Elmsford, NY).