field aberration - traducción al ruso
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field aberration - traducción al ruso

PHENOMENON IN ASTRONOMY
Astronomical aberration; Stellar aberration; Constant of aberration; Aberration of starlight; Stellar Aberration; Planetary Aberration; Planetary aberration; Annual aberration; Aberration of light (non-dependence of star's velocity); Abberation of light; Aberration of light
  • Stars at the [[ecliptic pole]]s appear to move in circles, stars exactly in the ecliptic plane move in lines, and stars at intermediate angles move in ellipses. Shown here are the apparent motions of stars with the [[ecliptic latitude]]s corresponding to these cases, and with [[ecliptic longitude]] of 270°.
  • γ Draconis]] and [[35 Camelopardalis]] as reduced by Busch to the year 1730.
  • Hypothetical observation of γ Draconis and 35 Camelopardalis if their movements were caused by nutation.
  • Hypothetical observation of γ Draconis if its movement was caused by parallax.
  • Figure 2: As light propagates down the telescope, the telescope moves requiring a tilt to the telescope that depends on the speed of light. The apparent angle of the star ''φ'' differs from its true angle ''θ''.
  • Young reasoned that aberration could only be explained if the aether were immobile in the frame of the Sun. On the left, stellar aberration occurs if an immobile aether is assumed, showing that the telescope must be tilted. On the right, the aberration disappears if the aether moves with the telescope, and the telescope does not need to be tilted.
  • Conceptual illustration of Stokes' aether drag theory. In the rest frame of the Sun the Earth moves to the right through the aether, in which it induces a local current. A ray of light (in red) coming from the vertical becomes dragged and tilted due to the flow of aether.
  • The propagating wavefront moving through the aether.
  • Light rays striking the earth in the Sun's rest frame compared to the same rays in the Earth's rest frame according to special relativity. The effect is exaggerated for illustrative purposes.

field aberration      
сферическая аберрация
lens aberration         
  • Figure 1
  • Figure 2
  • Figure 4
  • Figure 5
  • Figure 6
  • Reflection from a spherical mirror. Incident rays (red) away from the center of the mirror produce reflected rays (green) that miss the focal point, F. This is due to [[spherical aberration]].
  • Fig. 3a: Barrel distortion
  • Fig. 3b: Pincushion distortion
  • newspaper=ESO Announcement}}</ref>
  • Image plane of a flat-top beam under the effect of the first 21 Zernike polynomials. The beam goes through an aperture of the same size, which is imaged onto this plane by an ideal lens.
DEPARTURE OF THE PERFORMANCE OF AN OPTICAL SYSTEM FROM THE PREDICTIONS OF PARAXIAL OPTICS
Optical abberation; Actinic Rays; Aberration, optical; Lens aberrations; Lens Aberrations; Optical aberrations; Optical Aberrations; Lens aberration; Aberration (optics); Aberration in optical systems; Seidel aberration; Seidel aberrations; Optical abberration; Curvature of image; Curvature of field; Monochromatic aberration

общая лексика

аберрация объектива

lens aberration         
  • Figure 1
  • Figure 2
  • Figure 4
  • Figure 5
  • Figure 6
  • Reflection from a spherical mirror. Incident rays (red) away from the center of the mirror produce reflected rays (green) that miss the focal point, F. This is due to [[spherical aberration]].
  • Fig. 3a: Barrel distortion
  • Fig. 3b: Pincushion distortion
  • newspaper=ESO Announcement}}</ref>
  • Image plane of a flat-top beam under the effect of the first 21 Zernike polynomials. The beam goes through an aperture of the same size, which is imaged onto this plane by an ideal lens.
DEPARTURE OF THE PERFORMANCE OF AN OPTICAL SYSTEM FROM THE PREDICTIONS OF PARAXIAL OPTICS
Optical abberation; Actinic Rays; Aberration, optical; Lens aberrations; Lens Aberrations; Optical aberrations; Optical Aberrations; Lens aberration; Aberration (optics); Aberration in optical systems; Seidel aberration; Seidel aberrations; Optical abberration; Curvature of image; Curvature of field; Monochromatic aberration
аберрация объектива

Definición

грип
ГРИП, ГРИПП, гриппа, ·муж. (·франц. grippe) (мед.). Инфекционная болезнь - катарральное воспаление дыхательных путей, сопровождаемое лихорадочным состоянием; то же, что инфлуэнца
.

Wikipedia

Aberration (astronomy)

In astronomy, aberration (also referred to as astronomical aberration, stellar aberration, or velocity aberration) is a phenomenon which produces an apparent motion of celestial objects about their true positions, dependent on the velocity of the observer. It causes objects to appear to be displaced towards the direction of motion of the observer compared to when the observer is stationary. The change in angle is of the order of v/c where c is the speed of light and v the velocity of the observer. In the case of "stellar" or "annual" aberration, the apparent position of a star to an observer on Earth varies periodically over the course of a year as the Earth's velocity changes as it revolves around the Sun, by a maximum angle of approximately 20 arcseconds in right ascension or declination.

The term aberration has historically been used to refer to a number of related phenomena concerning the propagation of light in moving bodies. Aberration is distinct from parallax, which is a change in the apparent position of a relatively nearby object, as measured by a moving observer, relative to more distant objects that define a reference frame. The amount of parallax depends on the distance of the object from the observer, whereas aberration does not. Aberration is also related to light-time correction and relativistic beaming, although it is often considered separately from these effects.

Aberration is historically significant because of its role in the development of the theories of light, electromagnetism and, ultimately, the theory of special relativity. It was first observed in the late 1600s by astronomers searching for stellar parallax in order to confirm the heliocentric model of the Solar System. However, it was not understood at the time to be a different phenomenon. In 1727, James Bradley provided a classical explanation for it in terms of the finite speed of light relative to the motion of the Earth in its orbit around the Sun, which he used to make one of the earliest measurements of the speed of light. However, Bradley's theory was incompatible with 19th century theories of light, and aberration became a major motivation for the aether drag theories of Augustin Fresnel (in 1818) and G. G. Stokes (in 1845), and for Hendrik Lorentz's aether theory of electromagnetism in 1892. The aberration of light, together with Lorentz's elaboration of Maxwell's electrodynamics, the moving magnet and conductor problem, the negative aether drift experiments, as well as the Fizeau experiment, led Albert Einstein to develop the theory of special relativity in 1905, which presents a general form of the equation for aberration in terms of such theory.

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