2644:
2697:
1706:
through relativistic beaming. During the time it takes the light beam to reach the observer the light source moves in the observer's frame, and the 'true position' of the light source is displaced relative to the apparent position the observer sees, as explained by light-time correction. Finally, the beam in the observer's frame at the moment of observation is tilted compared to the beam in source's frame, which can be understood as an aberrational effect. Thus, a person in the light source's frame would describe the apparent tilting of the beam in terms of aberration, while a person in the observer's frame would describe it as a light-time effect.
2689:
4191:, Bradley's result does not merely give the classical limit of the relativistic case, in the sense that it gives incorrect predictions even at low relative velocities. Bradley's explanation cannot account for situations such as the water telescope, nor for many other optical effects (such as interference) that might occur within the telescope. This is because in the Earth's frame it predicts that the direction of propagation of the light beam in the telescope is not normal to the wavefronts of the beam, in contradiction with
4811:
372:
46:
4167:
of a resting ether did not seem directly convincing to me, since it led to an interpretation of the
Michelson-Morley experiment, which seemed unnatural to me. My direct path to the sp. th. rel. was mainly determined by the conviction that the electromotive force induced in a conductor moving in a magnetic field is nothing other than an electric field. But the result of Fizeau's experiment and the phenomenon of aberration also guided me.
2720:. This instrument had the advantage of a larger field of view and he was able to obtain precise positions of a large number of stars over the course of about twenty years. During his first two years at Wanstead, he established the existence of the phenomenon of aberration beyond all doubt, and this also enabled him to formulate a set of rules that would allow the calculation of the effect on any given star at a specified date.
1702:, which is an angling of the light emitted by a moving light source. It can be considered equivalent to them but in a different inertial frame of reference. In aberration, the observer is considered to be moving relative to a (for the sake of simplicity) stationary light source, while in light-time correction and relativistic beaming the light source is considered to be moving relative to a stationary observer.
3971:
2709:. 35 Camelopardalis was seen to possess an apparent motion which could be consistent with nutation, but since its declination varied only one half as much as that of γ Draconis, it was obvious that nutation did not supply the answer (however, Bradley later went on to discover that the Earth does indeed nutate). He also investigated the possibility that the motion was due to an irregular distribution of the
1804:
3142:
6461:
275:
3073:(yielding an earth-moon round-trip time of only seconds), the lag angle would be imperceptible. What they both overlooked is that aberration (as understood only later) would exactly counteract the lag even if large, leaving this eclipse method completely insensitive to light speed. (Otherwise, shadow-lag methods could be made to sense absolute translational motion, contrary to a basic
2472:
The other, observable, part is an acceleration toward the galactic center of approximately 2.5 × 10 m/s, which yields a change of aberration of about 5 μas/yr. Highly precise measurements extending over several years can observe this change in secular aberration, often called the secular aberration drift or the acceleration of the Solar System, as a small apparent
6597:
1784:
6621:
6573:
6609:
383:. A common analogy is to consider the apparent direction of falling rain. If rain is falling vertically in the frame of reference of a person standing still, then to a person moving forwards the rain will appear to arrive at an angle, requiring the moving observer to tilt their umbrella forwards. The faster the observer moves, the more tilt is needed.
4882:. Now, motion of the aether in the x and y directions does not affect the wavefront, but the motion in the z direction advances it (in addition to the amount it advances at speed c). If the z velocity of the aether varies over space, for example if it is slower for higher x as shown in the figure, then the wavefront becomes angled, by an angle
6585:
3631:
185:, 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
4166:
My own thought was more indirectly influenced by the famous
Michelson-Morley experiment. I learned of it through Lorentz' path breaking investigation on the electrodynamics of moving bodies (1895), of which I knew before the establishment of the special theory of relativity. Lorentz' basic assumption
4061:
immobile, like the electromagnetic aethers of Cauchy, Green and
Maxwell and unlike Fresnel's aether. He obtained Fresnel's dragging coefficient from modifications of Maxwell's electromagnetic theory, including a modification of the time coordinates in moving frames ("local time"). In order to explain
4013:
of the flow are such that the aether has zero velocity far from the Earth, but moves at the Earth's velocity at its surface and within it, he was able to completely account for aberration. The velocity of the aether outside of the Earth would decrease as a function of distance from the Earth so light
2732:
in mid
January the following year. One well-known story was that he saw the change of direction of a wind vane on a boat on the Thames, caused not by an alteration of the wind itself, but by a change of course of the boat relative to the wind direction. However, there is no record of this incident in
2471:
In about 200 million years, the Sun circles the galactic center, whose measured location is near right ascension (α = 266.4°) and declination (δ = −29.0°). The constant, unobservable, effect of the solar system's motion around the galactic center has been computed variously as 150 or 165 arcseconds.
4036:
In the 1880s once electromagnetism was better understood, interest turned again to the problem of aberration. By this time flaws were known to both
Fresnel's and Stokes' theories. Fresnel's theory required that the relative velocity of aether and matter to be different for light of different colors,
3966:
bringing the light along with it. This factor is known as "Fresnel's dragging coefficient". This dragging effect, along with refraction at the telescope's objective, compensates for the slower speed of light in the water telescope in
Bradley's explanation. With this modification Fresnel obtained
2837:
Bradley proposed that the aberration of light not only affected declination, but right ascension as well, so that a star in the pole of the ecliptic would describe a little ellipse with a diameter of about 40", but for simplicity, he assumed it to be a circle. Since he only observed the deviation in
4137:
Lorentz' theory matched experiment well, but it was complicated and made many unsubstantiated physical assumptions about the microscopic nature of electromagnetic media. In his 1905 theory of special relativity, Albert
Einstein reinterpreted the results of Lorentz' theory in a much simpler and more
4122:
in the direction of their motion through the aether. In this way, aberration (and all related optical phenomena) can be accounted for in the context of an immobile aether. Lorentz' theory became the basis for much research in the next decade, and beyond. Its predictions for aberration are identical
3875:
developed a modified explanation to account for the water telescope and for other aberration phenomena. He explained that the aether is generally at rest in the Sun's frame of reference, but objects partially drag the aether along with them as they move. That is, the aether in an object of index of
3643:
adapted
Bradley's explanation for corpuscular light to wavelike light traveling through a medium known as the luminiferous aether. His reasoning was the same as Bradley's, but it required that this medium be immobile in the Sun's reference frame and must pass through the earth unaffected, otherwise
2680:, a star with a right ascension nearly exactly opposite to that of γ Draconis, was 19" more northerly at the beginning of March than in September. The asymmetry of these results, which were expected to be mirror images of each other, were completely unexpected and inexplicable by existing theories.
2534:
Planetary aberration is the combination of the aberration of light (due to Earth's velocity) and light-time correction (due to the object's motion and distance), as calculated in the rest frame of the Solar System. Both are determined at the instant when the moving object's light reaches the moving
2704:
Bradley and
Molyneux discussed several hypotheses in the hope of finding the solution. Since the apparent motion was evidently caused neither by parallax nor observational errors, Bradley first hypothesized that it could be due to oscillations in the orientation of the Earth's axis relative to the
1705:
Consider the case of an observer and a light source moving relative to each other at constant velocity, with a light beam moving from the source to the observer. At the moment of emission, the beam in the observer's rest frame is tilted compared to the one in the source's rest frame, as understood
2216:
is : x = 8.3167 min ≈ 8 min 19 sec = 499 sec. This is possible since the transit time of sunlight is short relative to the orbital period of the Earth, so the Earth's frame may be approximated as inertial. In the Earth's frame, the Sun moves, at a mean velocity v =
390:
In the case of annual aberration of starlight, the direction of incoming starlight as seen in the Earth's moving frame is tilted relative to the angle observed in the Sun's frame. Since the direction of motion of the Earth changes during its orbit, the direction of this tilting changes during the
3612:. While this is different from the more accurate relativistic result described above, in the limit of small angle and low velocity they are approximately the same, within the error of the measurements of Bradley's day. These results allowed Bradley to make one of the earliest measurements of the
3165:
Consider the case where a distant star is motionless relative to the Sun, and the star is extremely far away, so that parallax may be ignored. In the rest frame of the Sun, this means light from the star travels in parallel paths to the Earth observer, and arrives at the same angle regardless of
1713:
towards the Sun, many aberrational effects such as annual aberration on Earth cannot be considered light-time corrections. However, if the time between emission and detection of the light is short compared to the orbital period of the Earth, the Earth may be approximated as an inertial frame and
2954:
Based on these calculations, Bradley was able to estimate the constant of aberration at 20.2", which is equal to 0.00009793 radians, and with this was able to estimate the speed of light at 183,300 miles (295,000 km) per second. By projecting the little circle for a star in the pole of the
220:
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
2838:
declination, and not in right ascension, his calculations for the maximum deviation of a star in the pole of the ecliptic are for its declination only, which will coincide with the diameter of the little circle described by such star. For eight different stars, his calculations are as follows:
2498:
at equatorial coordinates of α = 263° and δ = −20° indicated a secular aberration drift 6.4 ±1.5 μas/yr. Later determinations using a series of VLBI measurements extending over almost 40 years determined the secular aberration drift to be 5.83 ± 0.23 μas/yr in the direction α =
3634:
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
1454:
2672:(1675–1751), a celebrated instrument-maker. This was fixed to a vertical chimney stack in such manner as to permit a small oscillation of the eyepiece, the amount of which (i.e. the deviation from the vertical) was regulated and measured by the introduction of a screw and a plumb line.
4056:
Hendrik
Lorentz spent considerable effort along these lines. After working on this problem for a decade, the issues with Stokes' theory caused him to abandon it and to follow Fresnel's suggestion of a (mostly) stationary aether (1892, 1895). However, in Lorentz's model the aether was
2503:
satellite data of 1.6 million extragalactic sources indicated an acceleration of the solar system of 2.32 ± 0.16 × 10 m/s and a corresponding secular aberration drift of 5.05 ± 0.35 μas/yr in the direction of α = 269.1° ± 5.4°, δ =
2129:
In actuality, Earth's orbit is slightly elliptic rather than circular, and its speed varies somewhat over the course of its orbit, which means the description above is only approximate. Aberration is more accurately calculated using Earth's instantaneous velocity relative to the
4004:
proposed a 'putty-like' aether which acts as a liquid on large scales but as a solid on small scales, thus supporting both the transverse vibrations required for polarized light and the aether flow required to explain aberration. Making only the assumptions that the fluid is
2590:
had suggested that parallactic shifting of the stars should occur according to the heliocentric model, and consequently if stellar parallax could be observed it would help confirm this theory. Many observers claimed to have determined such parallaxes, but Tycho Brahe and
836:
3064:
that if light were not instantaneous, then shadows of moving objects would lag; and if propagation times over terrestrial distances were appreciable, then during a lunar eclipse the Sun, Earth, and Moon would be out of alignment by hours' motion, contrary to observation.
2173:(as viewed from Earth), opposite to the apparent motion of the Sun along the ecliptic (which is from west to east, as seen from Earth). The deflection thus makes the Sun appear to be behind (or retarded) from its rest-frame position on the ecliptic by a position or angle
4037:
and it was shown that the boundary conditions Stokes had assumed in his theory were inconsistent with his assumption of irrotational flow. At the same time, the modern theories of electromagnetic aether could not account for aberration at all. Many scientists such as
2663:
entered this sphere of research in 1725, there was still considerable uncertainty as to whether stellar parallaxes had been observed or not, and it was with the intention of definitely answering this question that they erected a large telescope at Molyneux's house at
3974:
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
2744:
and ecliptic prime meridian, of the tangent of the velocity of the Earth in its orbit for each of the four months where the extremes are found, as well as expected deviation from true ecliptic longitude if Bradley had measured its deviation from right ascension:
3161:
in which light is made of particles. His classical explanation appeals to the motion of the earth relative to a beam of light-particles moving at a finite velocity, and is developed in the Sun's frame of reference, unlike the classical derivation given above.
3967:
Bradley's vacuum result even for non-vacuum telescopes, and was also able to predict many other phenomena related to the propagation of light in moving bodies. Fresnel's dragging coefficient became the dominant explanation of aberration for the next decades.
3847:
performed a similar experiment and found that the aberration was unaffected by the medium in the telescope, providing solid evidence against Young's theory. This experiment was subsequently verified by many others in the following decades, most accurately by
3521:
3996:
to believe that the aether was a totally immobile elastic solid as opposed to Fresnel's fluid aether. There was thus renewed need for an explanation of aberration consistent both with Fresnel's predictions (and Arago's observations) as well as polarization.
2675:
The instrument was set up in November 1725, and observations on γ Draconis were made starting in December. The star was observed to move 40″ southwards between September and March, and then reversed its course from March to September. At the same time,
3648:
Upon consideration of the phenomena of the aberration of the stars I am disposed to believe that the luminiferous aether pervades the substance of all material bodies with little or no resistance, as freely perhaps as the wind passes through a grove of
3116:
proposed a similar theory, explaining that aberration occurs due to the flow of aether induced by the motion of the Earth. Accumulated evidence against these explanations, combined with new understanding of the electromagnetic nature of light, led
3048:
The original motivation of the search for stellar parallax was to test the Copernican theory that the Earth revolves around the Sun. The change of aberration in the course of the year demonstrates the relative motion of the Earth and the stars.
3039:
1770:"The apparent angular displacement of the observed position of a solar system body from its instantaneous geocentric direction as would be seen by an observer at the geocenter. This displacement is caused by the aberration of light and
2615:, the Pole Star, exhibited variations in its position amounting to 40″ annually. Some astronomers endeavoured to explain this by parallax, but these attempts failed because the motion differed from that which parallax would produce.
386:
The net effect is that light rays striking the moving observer from the sides in a stationary frame will come angled from ahead in the moving observer's frame. This effect is sometimes called the "searchlight" or "headlight" effect.
5121:
5624:
In fact, the light source doesn't need to be stationary, consider for example eclipsing binary stars: they are rotating with high speed —and ever changing and different velocity vectors— around each other, but they appear as
5195:
3044:
Thus, the speed of light to the speed of the Earth's annual motion in its orbit is 10,210 to one, from whence it would follow, that light moves, or is propagated as far as from the Sun to the Earth in 8 minutes 12 seconds.
4021:
Both Fresnel and Stokes' theories were popular. However, the question of aberration was put aside during much of the second half of the 19th century as focus of inquiry turned to the electromagnetic properties of aether.
2141:. If parallax is detectable, the maximum displacement to the south would occur in December, and the maximum displacement to the north in June. It is this apparently anomalous motion that so mystified early astronomers.
3833:
2450:
The secular component of aberration, caused by the motion of the Solar System in space, has been further subdivided into several components: aberration resulting from the motion of the solar system barycenter around
4697:
1286:
5475:"A Letter from the Reverend Mr. James Bradley Savilian Professor of Astronomy at Oxford, and F.R.S. to Dr.Edmond Halley Astronom. Reg. &c. Giving an Account of a New Discovered Motion of the Fix'd Stars"
157:
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
2516:(ICRF3) adopted a recommended galactocentric aberration constant of 5.8 μas/yr and recommended a correction for secular aberration to obtain the highest positional accuracy for times other than the
2467:
objects. The large, constant part of secular aberration cannot be directly observed and "It has been standard practice to absorb this large, nearly constant effect into the reported" positions of stars.
1709:
The relationship between these phenomena is only valid if the observer and source's frames are inertial frames. In practice, because the Earth is not an inertial rest frame but experiences centripetal
1735:"The apparent angular displacement of the observed position of a celestial body resulting from the motion of the observer. Stellar aberration is divided into diurnal, annual, and secular components."
1209:
2356:
4359:
2513:
1117:
4066:(1887), which apparently contradicted both Fresnel's and Lorentz's immobile aether theories, and apparently confirmed Stokes' complete aether drag, Lorentz theorized (1892) that objects undergo "
2196:
This deflection may equivalently be described as a light-time effect due to motion of the Earth during the 8.3 minutes that it takes light to travel from the Sun to Earth. The relation with
81:
about their true positions based on the velocity of the observer: It causes objects to appear to be displaced towards the observer's direction of motion. The change in angle is of the order of
1278:
1943:
375:
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.
1676:
686:
5368:
4542:
5056:
402:
is required to correctly account for aberration. The relativistic explanation is very similar to the classical one however, and in both theories aberration may be understood as a case of
3375:
1762:"The component of stellar aberration resulting from the essentially uniform and almost rectilinear motion of the entire solar system in space. Secular aberration is usually disregarded."
5835:
566:
1791:
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
5728:
Charlot, P.; Jacobs, C. S.; Gordon, D.; Lambert, S.; et al. (2020). "The third realization of the International Celestial Reference Frame by very long baseline interferometry".
5259:
4120:
3610:
1542:
924:
4935:
5643:
3558:
2396:
1490:
872:
635:
1616:
998:
678:
49:
A diagram showing how the apparent position of a star viewed from the Earth can change depending on the Earth's velocity. The effect is typically much smaller than illustrated.
4457:
4408:
2494:
have successfully measured this small effect. The first VLBI measurement of the apparent motion, over a period of 20 years, of 555 extragalactic objects towards the center of
6341:
4967:
3964:
3145:
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
2643:
2619:, from measurements made in 1689 and succeeding years with his mural quadrant, similarly concluded that the declination of Polaris was 40″ less in July than in September.
2247:
4228:
3100:. However, this explanation proved inaccurate once the wave nature of light was better understood, and correcting it became a major goal of the 19th century theories of
5853:
the correction of star places with secular aberration is not at all necessary and is even inconvenient, so long as the solar motion remains uniform and rectilinear.
4758:
3070:
6299:
1576:
958:
5312:
4798:
4582:
4270:
4189:
4162:
and (indirectly) the negative aether drift experiments, already mentioned by him in the introduction of his first relativity paper. Einstein wrote in a note in 1952:
3323:
3184:
3166:
where the Earth is in its orbit. Suppose the star is observed on Earth with a telescope, idealized as a narrow tube. The light enters the tube from the star at angle
2696:
2416:
2214:
2191:
2167:
2108:
2053:
2029:
1897:
506:
2961:
4880:
4848:
4778:
4609:
4290:
3367:
3347:
3303:
3085:
The phenomenon of aberration became a driving force for many physical theories during the 200 years between its observation and the explanation by Albert Einstein.
2281:
486:
459:
3283:
3689:
3232:
2535:
observer on Earth. It is so called because it is usually applied to planets and other objects in the Solar System whose motion and distance are accurately known.
1280:, giving the components of the light beam in the Earth's frame in terms of the components in the Sun's frame. The angle of the beam in the Earth's frame is thus
107:
4990:
5332:
5279:
4717:
4562:
3914:
3894:
3729:
3709:
3252:
3204:
2301:
1986:
1963:
1850:
586:
432:
151:
127:
2955:
ecliptic, he could simplify the calculation of the relationship between the speed of light and the speed of the Earth's annual motion in its orbit as follows:
3663:
were present. An important example is of a telescope filled with water. The speed of light in such a telescope will be slower than in vacuum, and is given by
6108:
Bradley, James; Rigaud, Stephen Peter (1832). Miscellaneous works and correspondence of the Rev. James Bradley, D.D., F.R.S. Oxford: University Press. p. 11.
6478:
3125:
which featured an immobile aether, and he explained that objects contract in length as they move through the aether. Motivated by these previous theories,
5064:
3112:. He proposed that objects partially drag the aether along with them as they move, and this became the accepted explanation for aberration for some time.
4014:
rays from stars would be progressively dragged as they approached the surface of the Earth. The Earth's motion would be unaffected by the aether due to
181:
has historically been used to refer to a number of related phenomena concerning the propagation of light in moving bodies. Aberration is distinct from
5140:
4810:
2512:, incorporating about 66 and 120 months of data, will reduce the random errors of these results by factors of 0.35 and 0.15. The latest edition of the
1687:
292:
4192:
394:
While classical reasoning gives intuition for aberration, it leads to a number of physical paradoxes observable even at the classical level (see
3737:
391:
course of the year, and causes the apparent position of the star to differ from its true position as measured in the inertial frame of the Sun.
2438:
of the observer. Its effect is much smaller than that of annual aberration, and is only 0.32 arcseconds in the case of an observer at the
588:
in the x direction relative to the Sun, then by velocity addition the x component of the beam's velocity in the Earth's frame of reference is
6372:
6246:
6188:
4818:
Stokes' derivation may be summarized as follows: Consider a wavefront moving in the downwards z direction. Say the aether has velocity field
4614:
2740:
The following table shows the magnitude of deviation from true declination for γ Draconis and the direction, on the planes of the solstitial
1753:"The component of stellar aberration resulting from the observer's diurnal motion about the center of the Earth due to the Earth's rotation."
6473:
6045:
Gaia Collaboration; Klioner, S. A.; et al. (2021). "Gaia Early Data Release 3: Acceleration of the Solar System from Gaia astrometry".
2631:
2 which passes practically overhead at the latitude of London (hence its observations are largely free from the complex corrections due to
261:
to develop the theory of special relativity in 1905, which presents a general form of the equation for aberration in terms of such theory.
5281:
s represent the x component of the aether's velocity at the start and end of the ray. Far from the earth the aether has zero velocity, so
1449:{\displaystyle \tan(\phi )={\frac {u_{y}'}{u_{x}'}}={\frac {u_{y}}{\gamma (u_{x}+v)}}={\frac {\sin(\theta )}{\gamma (v/c+\cos(\theta ))}}}
4159:
2688:
246:
6641:
1690:
Aberration, light-time correction, and relativistic beaming can be considered the same phenomenon depending on the frame of reference.
6408:
6332:
6153:
5685:
5653:
5609:
5528:
5411:
2543:
The discovery of the aberration of light was totally unexpected, and it was only by considerable perseverance and perspicacity that
2484:
358:
2595:
concluded that they existed only in the minds of the observers, and were due to instrumental and personal errors. However, in 1680
339:
311:
4063:
2716:
On August 19, 1727, Bradley embarked upon a further series of observations using a telescope of his own erected at the Rectory,
1728:
describes several different types of aberration, arising from differing components of the Earth's and observed object's motion:
250:
5584:
6378:
3234:
to reach the bottom of the tube, where it is detected. Suppose observations are made from Earth, which is moving with a speed
2149:
A special case of annual aberration is the nearly constant deflection of the Sun from its position in the Sun's rest frame by
4001:
2306:
296:
6296:
4299:
3369:
changes with the time of year the observation is made. The apparent angle and true angle are related using trigonometry as:
318:
4150:
He continued to say the experimental results which had influenced him most were the observations of stellar aberration and
3088:
The first classical explanation was provided in 1729, by James Bradley as described above, who attributed it to the finite
4132:
1123:
6563:
5131:
5639:
3993:
2728:
Bradley eventually developed his explanation of aberration in about September 1728 and this theory was presented to the
831:{\displaystyle \tan(\phi )={\frac {u_{y}'}{u_{x}'}}={\frac {u_{y}}{u_{x}+v}}={\frac {\sin(\theta )}{v/c+\cos(\theta )}}}
380:
6543:
Reduction of the Observations Made by Bradley at Kew and Wansted to Determine the Quantities of Aberration and Nutation
1217:
1022:
3644:
the medium (and therefore the light) would move along with the earth and no aberration would be observed. He wrote:
3158:
2460:
1902:
325:
1621:
3630:
3516:{\displaystyle \tan(\phi )={\frac {h\sin(\theta )}{hv/c+h\cos(\theta )}}={\frac {\sin(\theta )}{v/c+\cos(\theta )}}}
5677:
5340:
4462:
4015:
2669:
2592:
2056:
4995:
3285:. Consequently, for the particles of light to reach the bottom of the tube, the tube must be inclined at an angle
285:
1009:
307:
1698:, which is due to the motion of an observed object during the time taken by its light to reach an observer, and
208:. It was first observed in the late 1600s by astronomers searching for stellar parallax in order to confirm the
3659:
However, it soon became clear Young's theory could not account for aberration when materials with a non-vacuum
3640:
511:
5790:
MacMillan, D. S.; Fey, A.; Gipson, J. M.; et al. (2019). "Galactocentric acceleration in VLBI analysis".
3731:
is the refractive index of the water. Thus, by Bradley and Young's reasoning the aberration angle is given by
5204:
4719:
is the modified path length through the water and t is the time it takes the light to travel the distance h,
4073:
3563:
1495:
877:
4233:
3074:
2547:
was able to explain it in 1727. It originated from attempts to discover whether stars possessed appreciable
2464:
1013:
4885:
4361:. Then drag must be accounted for. Without drag, the x and y components of the light in the telescope are
4050:
4049:
unsuccessfully attempted to solve these problems by incorporating either Fresnel or Stokes' theories into
4010:
3861:
3109:
3108:
proposed a correction due to the motion of a medium (the aether) through which light propagated, known as
2632:
1807:
The direction of aberration of a star at the northern ecliptic pole differs at different times of the year
242:
222:
3530:
2361:
1462:
844:
6023:
4969:(assuming the speed of the aether is negligible compared to the speed of light). Then for each distance
4218:
3989:
3113:
3105:
2706:
2700:
Hypothetical observation of γ Draconis and 35 Camelopardalis if their movements were caused by nutation.
2529:
2066:
For illustration, consider a star at the northern ecliptic pole viewed by an observer at a point on the
1771:
1695:
230:
226:
212:
of the Solar System. However, it was not understood at the time to be a different phenomenon. In 1727,
186:
2710:
1581:
963:
6180:
6171:
5962:
Titov, O.; Lambert, S. B.; Gontier, A.-M. (2011). "VLBI measurement of the secular aberration drift".
4413:
4364:
4146:
reported some conversations with Einstein, in which Einstein emphasized the importance of aberration:
2398:≈ 0.000099365 rad = 20.49559 sec, very nearly the same as the aberrational correction (here
371:
45:
6501:
6433:
6064:
6015:
5981:
5929:
5878:
5799:
5747:
5560:
5486:
5436:
4199:
between frames. However, Bradley did correctly infer that the effect was due to relative velocities.
4031:
3985:
3122:
2499:
270.2 ± 2.3° and δ = −20.2° ± 3.6°. Optical observations using only 33 months of
1826:
1724:
1699:
238:
190:
39:
35:
591:
6646:
6625:
5427:
Williams, M. E. W. (1979). "Flamsteed's Alleged Measurement of Annual Parallax for the Pole Star".
4143:
4139:
4038:
3849:
3625:
3101:
2713:, thus involving abnormal variations in the refractive index, but again obtained negative results.
2560:
2427:
4940:
3919:
640:
332:
6651:
6613:
6601:
6279:
6271:
6145:
6054:
5997:
5971:
5919:
5815:
5763:
5737:
5709:
5576:
5452:
4171:
While Einstein's result is the same as Bradley's original equation except for an extra factor of
4067:
3840:
3130:
3066:
2628:
2220:
1796:
399:
205:
196:
Aberration is historically significant because of its role in the development of the theories of
159:
31:
2011:(the plane of Earth's orbit) to appear to move back and forth along a straight line, varying by
6538:
4722:
3034:{\displaystyle \cos \left({\frac {1}{2}}\pi -0.00009793\right)=\sin(0.00009793)={\frac {v}{c}}}
680:. Thus the angle of the light in the Earth's frame in terms of the angle in the Sun's frame is
6404:
6368:
6263:
6184:
6179:. Vol. I: A-ak Bayes (15th ed.). Chicago, IL: Encyclopædia Britannica Inc. pp.
6149:
5681:
5649:
5605:
5524:
5407:
5058:, and so the total angle by which it has changed after travelling through the entire fluid is
4151:
4138:
natural conceptual framework which disposed of the idea of an aether. His derivation is given
3844:
3058:
2652:
2517:
2505:
2488:
2111:
1792:
1547:
929:
254:
217:
5284:
4783:
4567:
4255:
4174:
3639:
In the early nineteenth century the wave theory of light was being rediscovered, and in 1804
3308:
3169:
2401:
2199:
2176:
2152:
2093:
2038:
2014:
1882:
491:
241:
of electromagnetism in 1892. The aberration of light, together with Lorentz's elaboration of
6577:
6441:
6255:
6220:
6072:
6068:
5989:
5985:
5937:
5886:
5882:
5844:
5807:
5803:
5755:
5751:
5599:
5568:
5494:
5444:
4213:
4042:
3872:
3660:
2548:
2031:
on either side of their position in the Sun's frame. A star that is precisely at one of the
1872:
1861:
1812:
1686:
201:
182:
74:
4853:
4821:
4763:
4587:
4275:
3352:
3332:
3288:
2252:
2114:, the star's position is displaced to the north by an equal and opposite amount. On either
1744:"The component of stellar aberration resulting from the motion of the Earth about the Sun."
464:
437:
6322:
6303:
6016:"Gaia's measurement of the solar system acceleration with respect to the distant universe"
3839:
which predicts a medium-dependent angle of aberration. When refraction at the telescope's
3257:
3126:
3118:
2660:
2579:
2571:
2563:
2452:
2119:
258:
234:
167:
6326:
5645:
Astronomical Almanac for the Year 2015 and Its Companion, The Astronomical Almanac Online
4611:
is the velocity of the light with these velocity components, then by Bradley's reasoning
3666:
3209:
2668:. They decided to reinvestigate the motion of γ Draconis with a telescope constructed by
1875:
as circular, the maximum displacement of a star due to annual aberration is known as the
84:
6437:
6242:"Descartes' Experimental Proof of the Infinite Velocity of Light and Huygens' Rejoinder"
5933:
5564:
5490:
5440:
4972:
2086:, Earth's orbit carries the observer in a southwards direction, and the star's apparent
6528:
6511:
6397:
6138:
5317:
5264:
5127:
4702:
4547:
4293:
4208:
4046:
4006:
3899:
3879:
3714:
3694:
3613:
3237:
3189:
3089:
3061:
2648:
2624:
2616:
2286:
2004:
1971:
1966:
1948:
1857:
1835:
571:
417:
414:
In the Sun's frame, consider a beam of light with velocity equal to the speed of light
379:
Aberration may be explained as the difference in angle of a beam of light in different
136:
130:
112:
78:
2137:
Note that the displacement due to aberration is orthogonal to any displacement due to
6635:
6467:
6283:
6001:
5819:
5767:
5701:
5456:
4223:
3843:
is taken into account this result deviates even more from the vacuum result. In 1810
2760:
Direction of tangential velocity of Earth on the plane of the ecliptic prime meridian
2729:
2587:
2544:
2473:
2083:
2067:
2032:
1860:
and consequently the aberration also varies periodically, typically causing stars to
1830:
1788:
213:
209:
6357:
5580:
5548:
5116:{\displaystyle \alpha \approx {\frac {1}{c}}\int {\frac {\partial w}{\partial x}}dz}
6589:
6533:
Essays on Several Curious and Useful Subjects in Speculative and Mix'd Mathematicks
2620:
2583:
2567:
2426:
Diurnal aberration is caused by the velocity of the observer on the surface of the
2079:
1853:
1710:
403:
6076:
5993:
5848:
5811:
5759:
3970:
3141:
2430:. It is therefore dependent not only on the time of the observation, but also the
2118:, the displacement in declination is 0. Conversely, the amount of displacement in
17:
5891:
5866:
5190:{\displaystyle {\frac {\partial w}{\partial x}}={\frac {\partial u}{\partial z}}}
6555:
5648:. Washington, DC: U.S. Government Printing Office (published 2014). p. M1.
2635:), and concluded that this star was 23″ more northerly in July than in October.
2596:
2575:
2456:
2087:
2071:
1803:
274:
171:
5549:"Einstein's Investigations of Galilean Covariant Electrodynamics prior to 1905"
5448:
2754:
Direction of tangential velocity of Earth on the plane of the solstitial colure
27:
Phenomenon wherein objects appear to move about their true positions in the sky
5572:
4158:
Other important motivations for Einstein's development of relativity were the
2692:
Hypothetical observation of γ Draconis if its movement was caused by parallax.
2480:
2459:, and aberration resulting from the motion of the Local Group relative to the
2131:
6506:
Miscellaneous Works and Correspondence of the Rev. James Bradley, D.D. F.R.S.
6267:
2734:
2602:
2495:
2435:
1989:
1678:
constant in all frames of reference, unlike the classical derivation above.
163:
54:
6225:
6208:
5499:
5474:
2850:
Maximum deviation in declination of a star in the pole of the ecliptic (")
2035:(at 90° from the ecliptic plane) will appear to move in a circle of radius
3828:{\displaystyle \tan(\phi )={\frac {\sin(\theta )}{v/(c/n)+\cos(\theta )}}}
5924:
2717:
2677:
2431:
2138:
2115:
2008:
154:
30:
Not to be confused with the defects in astronomical instruments known as
6275:
6241:
2358:≈ 0.000099364 rad = 20.49539 sec, which can be solved to give
1783:
6259:
4692:{\displaystyle \tan(\phi )={\frac {h\sin(\alpha )}{vt+h\cos(\alpha )}}}
2612:
2439:
2123:
2060:
1865:
299: in this section. Unsourced material may be challenged and removed.
6445:
2303:= 1 AU = 149,597,870.7 km. This gives an angular correction
2741:
2455:, aberration resulting from the motion of the Galaxy relative to the
2075:
1993:
6584:
6059:
5942:
5907:
5742:
4154:
on the speed of light in moving water. "They were enough," he said.
1008:
The reasoning in the relativistic case is the same except that the
6466:
This article incorporates text from a publication now in the
5976:
5201:
Inserting this into the previous result gives an aberration angle
4252:
More in detail, Fresnel explains that the incoming light of angle
3093:
2695:
2687:
2642:
1997:
1818:
197:
44:
2463:. Secular aberration affects the apparent positions of stars and
193:, although it is often considered separately from these effects.
5833:
Hagihara, Yusuke (1933). "On the Theory of Secular Aberration".
2733:
Bradley's own account of the discovery, and it may therefore be
2608:
6424:
Shankland, R. S. (1963). "Conversations with Albert Einstein".
4272:
is first refracted at the end of the telescope, to a new angle
1714:
aberrational effects are equivalent to light-time corrections.
3349:. As the Earth proceeds in its orbit it changes direction, so
3097:
2763:
Expected deviation from true ecliptic longitude of γ Draconis
2665:
2249:≈ 14,864.7 km in the time it takes light to reach Earth,
1945:
substituting the Earth's average speed in the Sun's frame for
1822:
1682:
Relationship to light-time correction and relativistic beaming
268:
3254:. During the transit of the light, the tube moves a distance
5314:
and at the surface of the earth it has the earth's velocity
4809:
1817:
Annual aberration is caused by the motion of an observer on
162:
around the Sun, by a maximum angle of approximately 20
6116:
6114:
6092:
6090:
6088:
6086:
6209:"An account of a new discovered motion of the fixed stars"
3133:
in 1905, which provides the modern account of aberration.
1016:
between different frames of reference. These formulas are
1856:
periodically during the year as the planet traverses its
5836:
Proceedings of the Physico-Mathematical Society of Japan
3635:
telescope, and the telescope does not need to be tilted.
1618:. This relativistic derivation keeps the speed of light
5406:. Oxford: Pergamon Press. pp. 99–117 und 255–273.
4937:. Now, say in time t the wavefront has moved by a span
3988:(discovered by Fresnel himself) led scientists such as
2351:{\displaystyle \tan(\theta )\approx \theta =\Delta x/R}
5672:
Kovalevsky, Jean & Seidelmann, P. Kenneth (2004).
4354:{\displaystyle \sin(\theta -\phi )=n\sin(\psi -\phi )}
395:
6561:
5343:
5320:
5287:
5267:
5207:
5143:
5067:
4998:
4975:
4943:
4888:
4856:
4824:
4786:
4766:
4725:
4705:
4617:
4590:
4570:
4550:
4465:
4416:
4367:
4302:
4278:
4258:
4177:
4076:
3922:
3902:
3882:
3740:
3717:
3697:
3669:
3566:
3533:
3378:
3355:
3335:
3311:
3291:
3260:
3240:
3212:
3192:
3172:
2964:
2404:
2364:
2309:
2289:
2255:
2223:
2202:
2179:
2155:
2096:
2041:
2017:
1974:
1951:
1905:
1885:
1838:
1624:
1584:
1550:
1498:
1465:
1289:
1220:
1126:
1025:
966:
932:
880:
847:
689:
643:
594:
574:
514:
494:
467:
440:
420:
139:
115:
87:
4814:
The propagating wavefront moving through the aether.
1204:{\displaystyle u_{y}'=u_{y}/\gamma (1+u_{x}v/c^{2})}
6342:
A History of the Theories of Aether and Electricity
6328:
A History of the theories of aether and electricity
4292:within the telescope. This may be accounted for by
2090:is therefore displaced to the south by an angle of
2055:about its true position, and stars at intermediate
6496:Explanatory Supplement to the Astronomical Almanac
6396:
6170:
6137:
5362:
5326:
5306:
5273:
5253:
5189:
5115:
5050:
4984:
4961:
4929:
4874:
4842:
4792:
4772:
4752:
4711:
4691:
4603:
4576:
4556:
4536:
4451:
4402:
4353:
4284:
4264:
4183:
4114:
3958:
3908:
3888:
3827:
3723:
3703:
3683:
3604:
3552:
3515:
3361:
3341:
3317:
3297:
3277:
3246:
3226:
3198:
3178:
3157:Bradley conceived of an explanation in terms of a
3033:
2410:
2390:
2350:
2295:
2275:
2241:
2208:
2185:
2161:
2102:
2047:
2023:
1980:
1957:
1937:
1891:
1844:
1670:
1610:
1570:
1536:
1484:
1448:
1272:
1203:
1111:
992:
952:
918:
866:
830:
672:
629:
580:
560:
500:
480:
453:
426:
145:
121:
101:
6358:"The Optics and Electrodynamics of Moving Bodies"
4229:Timeline of electromagnetism and classical optics
2570:had received confirmation by the observations of
1273:{\displaystyle \gamma =1/{\sqrt {1-v^{2}/c^{2}}}}
1112:{\displaystyle u_{x}'=(u_{x}+v)/(1+u_{x}v/c^{2})}
1012:formulas must be used, which can be derived from
2007:, annual aberration causes stars exactly on the
1938:{\displaystyle \kappa =\theta -\phi \approx v/c}
6498:(University Science Books, 1992), 127–135, 700.
6213:Philosophical Transactions of the Royal Society
4195:. It also does not preserve the speed of light
4164:
4148:
3646:
1671:{\displaystyle {\sqrt {u_{x}^{2}+u_{y}^{2}}}=c}
6482:. Vol. 1 (11th ed.). pp. 54–61.
6331:(1. ed.). Dublin: Longman, Green and Co.
3053:Retrodiction on Descartes' lightspeed argument
2705:celestial sphere – a phenomenon known as
1694:Aberration is related to two other phenomena,
5957:
5955:
5953:
5363:{\displaystyle \alpha \approx {\frac {v}{c}}}
4537:{\displaystyle (c/n)\cos(\psi )-(1-1/n^{2})v}
2777:← (moving toward perihelion at fast velocity)
2757:Deviation from true declination of γ Draconis
2504:−31.6° ± 4.1°. It is expected that
2442:, where the rotational velocity is greatest.
8:
6356:Janssen, Michel & Stachel, John (2010).
6317:
6315:
6313:
6311:
6202:
6200:
5785:
5783:
5781:
5779:
5777:
5667:
5665:
5051:{\displaystyle \alpha \approx (dw/dx)(dz/c)}
2283:≈ 499 sec for the orbit of mean radius
5908:"Astrometric effects of secular aberration"
5514:
5512:
5510:
5397:
5395:
5393:
5391:
2811:→ (moving toward aphelion at slow velocity)
6120:
6096:
5723:
5721:
5719:
1899:. It may be calculated using the relation
6516:Mathematical and Philosophical Dictionary
6224:
6058:
5975:
5941:
5923:
5890:
5741:
5498:
5468:
5466:
5350:
5342:
5319:
5292:
5286:
5266:
5243:
5234:
5221:
5206:
5167:
5144:
5142:
5087:
5074:
5066:
5037:
5014:
4997:
4992:the ray descends, it is bent by an angle
4974:
4942:
4916:
4887:
4855:
4823:
4785:
4765:
4744:
4735:
4724:
4704:
4636:
4616:
4595:
4589:
4569:
4549:
4522:
4513:
4472:
4464:
4423:
4415:
4374:
4366:
4301:
4277:
4257:
4176:
4104:
4095:
4089:
4077:
4075:
3944:
3935:
3921:
3901:
3881:
3793:
3782:
3759:
3739:
3716:
3696:
3673:
3668:
3594:
3565:
3544:
3532:
3484:
3461:
3426:
3397:
3377:
3354:
3334:
3310:
3290:
3267:
3259:
3239:
3216:
3211:
3191:
3171:
3021:
2976:
2963:
2623:, in 1674, published his observations of
2403:
2374:
2363:
2340:
2308:
2288:
2265:
2254:
2222:
2201:
2178:
2154:
2095:
2040:
2016:
1973:
1950:
1927:
1904:
1884:
1837:
1654:
1649:
1636:
1631:
1625:
1623:
1600:
1583:
1554:
1549:
1526:
1497:
1476:
1464:
1414:
1385:
1364:
1347:
1341:
1327:
1314:
1308:
1288:
1262:
1253:
1247:
1235:
1230:
1219:
1192:
1183:
1174:
1153:
1147:
1131:
1125:
1100:
1091:
1082:
1064:
1049:
1030:
1024:
982:
965:
936:
931:
908:
879:
858:
846:
799:
776:
758:
747:
741:
727:
714:
708:
688:
664:
648:
642:
615:
599:
593:
573:
561:{\displaystyle \tan(\theta )=u_{y}/u_{x}}
552:
543:
537:
513:
493:
472:
466:
445:
439:
419:
359:Learn how and when to remove this message
138:
114:
91:
86:
6131:
6129:
5542:
5540:
3969:
3629:
3140:
2840:
2747:
1802:
1782:
1685:
370:
6568:
6399:Electrodynamics from Ampére to Einstein
5521:Parallax:The Race to Measure the Cosmos
5387:
5373:which is the known aberration result.
5254:{\displaystyle \alpha =(u_{2}-u_{1})/c}
4459:, but drag modifies the x component to
4245:
4142:, and is now the accepted explanation.
4115:{\displaystyle {\sqrt {1-v^{2}/c^{2}}}}
3605:{\displaystyle \tan(\theta -\phi )=v/c}
2724:Development of the theory of aberration
2578:and the mathematical investigations of
2514:International Celestial Reference Frame
1795:corresponding to these cases, and with
1757:
1748:
1537:{\displaystyle \sin(\theta -\phi )=v/c}
919:{\displaystyle \tan(\theta -\phi )=v/c}
1988:. Its accepted value is 20.49552
1739:
6247:Archive for History of Exact Sciences
5604:(2nd ed.). Springer. p. 8.
5553:Archive for History of Exact Sciences
4123:to those of the relativistic theory.
3916:is partially dragged with a velocity
3136:
2655:as reduced by Busch to the year 1730.
2070:. Such an observer will see the star
568:. If the Earth is moving at velocity
7:
5429:Journal for the History of Astronomy
4930:{\displaystyle \tan(\alpha )=tdw/dx}
4800:one obtains Bradley's vacuum result.
4193:Maxwell's theory of electromagnetism
2483:of extragalactic objects using both
2418:is in radian and not in arcsecond).
2078:, once every day (strictly speaking
297:adding citations to reliable sources
5708:. Macmillan, 1906 – republished by
5706:A Compendium of Spherical Astronomy
4760:. Upon solving these equations for
4160:moving magnet and conductor problem
3553:{\displaystyle \theta =90^{\circ }}
2391:{\displaystyle \theta =v/c=\kappa }
2126:and at maximum on either solstice.
1852:of Earth (in the Sun's rest frame)
1485:{\displaystyle \theta =90^{\circ }}
867:{\displaystyle \theta =90^{\circ }}
637:, and the y velocity is unchanged,
434:, with x and y velocity components
247:moving magnet and conductor problem
5906:Kopeikin, S.; Makarov, V. (2006).
5523:. New York, New York: Henry Holt.
5404:Nineteenth-century aether theories
5178:
5170:
5155:
5147:
5098:
5090:
4051:Maxwell's new electromagnetic laws
3052:
2334:
2224:
2059:will appear to move along a small
1821:as the planet revolves around the
221:became a major motivation for the
25:
6339:Whittaker, Edmund Taylor (1953).
4544:if the Earth moves with velocity
4025:
3081:Historical theories of aberration
2485:Very Long Baseline Interferometry
1611:{\displaystyle \theta -\phi =v/c}
993:{\displaystyle \theta -\phi =v/c}
251:negative aether drift experiments
6619:
6607:
6595:
6583:
6571:
6459:
6384:from the original on 2022-10-09.
6335:from the original on 2016-02-15.
5587:from the original on 2009-01-11.
4452:{\displaystyle (c/n)\cos(\psi )}
4403:{\displaystyle (c/n)\sin(\psi )}
3984:However, the fact that light is
2539:Discovery and first observations
2217:29.789 km/s, by a distance
1879:, conventionally represented by
273:
3852:in 1871, with the same result.
3137:Bradley's classical explanation
2659:Consequently, when Bradley and
284:needs additional citations for
204:and, ultimately, the theory of
6240:Sakellariadis, Spyros (1982).
6169:Hoiberg, Dale H., ed. (2010).
5912:The Astronomical Journal (USA)
5867:"Aberration in proper motions"
5402:Schaffner, Kenneth F. (1972).
5240:
5214:
5045:
5028:
5025:
5005:
4901:
4895:
4683:
4677:
4654:
4648:
4630:
4624:
4528:
4501:
4495:
4489:
4480:
4466:
4446:
4440:
4431:
4417:
4397:
4391:
4382:
4368:
4348:
4336:
4321:
4309:
3950:
3923:
3819:
3813:
3801:
3787:
3774:
3768:
3753:
3747:
3585:
3573:
3507:
3501:
3476:
3470:
3452:
3446:
3415:
3409:
3391:
3385:
3329:position of the star at angle
3015:
3009:
2322:
2316:
1517:
1505:
1440:
1437:
1431:
1408:
1400:
1394:
1376:
1357:
1302:
1296:
1198:
1161:
1106:
1069:
1061:
1042:
1010:relativistic velocity addition
899:
887:
822:
816:
791:
785:
702:
696:
630:{\displaystyle u_{x}'=u_{x}+v}
527:
521:
1:
6494:P. Kenneth Seidelmann (Ed.),
5849:10.11429/ppmsj1919.15.3-6_155
5642:(21 March 2014). "Glossary".
4133:History of special relativity
3129:then developed the theory of
6140:A Short History of Astronomy
6047:Astronomy & Astrophysics
5640:U.S. Nautical Almanac Office
5473:Bradley, James (1727–1728).
4962:{\displaystyle dz\approx ct}
3959:{\displaystyle (1-1/n^{2})v}
3149:differs from its true angle
2822:→ (moving toward perihelion)
2814:increase of less than 20.2"
2780:decrease of more than 20.2"
2639:James Bradley's observations
2638:
1578:this may be approximated by
673:{\displaystyle u_{y}'=u_{y}}
381:inertial frames of reference
6426:American Journal of Physics
6403:. Oxford: Clarendon Press.
6077:10.1051/0004-6361/202039734
5994:10.1051/0004-6361/201015718
5812:10.1051/0004-6361/201935379
5760:10.1051/0004-6361/202038368
4064:Michelson–Morley experiment
4026:Lorentz' length contraction
3866:
3159:corpuscular theory of light
2607:stated, as a result of ten
2555:Search for stellar parallax
2461:cosmic microwave background
2242:{\displaystyle \Delta x=vt}
308:"Aberration" astronomy
6668:
6472:Eppenstein, Otto (1911). "
6395:Darrigol, Olivier (2000).
5964:Astronomy and Astrophysics
5892:10.1051/0004-6361:20030560
5871:Astronomy and Astrophysics
5792:Astronomy and Astrophysics
5730:Astronomy and Astrophysics
5678:Cambridge University Press
5674:Fundamentals of Astrometry
5449:10.1177/002182867901000203
4130:
4029:
3979:
3859:
3623:
2788:← (moving toward aphelion)
2647:Bradley's observations of
2593:Giovanni Battista Riccioli
2527:
1992:(sec) or 0.000099365
1810:
29:
6642:Electromagnetic radiation
6558:on Bradley's observations
6363:. In John Stachel (ed.).
6345:(2. ed.). T. Nelson.
6172:"aberration, constant of"
5598:Richard A. Mould (2001).
5573:10.1007/s00407-004-0085-6
5519:Hirschfeld, Alan (2001).
4753:{\displaystyle t=h/v_{l}}
2479:Recently, highly precise
1492:, this result reduces to
874:, this result reduces to
243:Maxwell's electrodynamics
6323:Whittaker, Edmund Taylor
5547:Norton, John D. (2004).
5132:Cauchy–Riemann equations
3096:in its orbit around the
2453:the center of our Galaxy
1571:{\displaystyle v/c\ll 1}
1004:Relativistic explanation
953:{\displaystyle v/c\ll 1}
73:) is a phenomenon where
6479:Encyclopædia Britannica
6297:Encyclopædia Britannica
6177:Encyclopædia Britannica
6136:Berry, Arthur (1961) .
6069:2021A&A...649A...9G
5986:2011A&A...529A..91T
5883:2003A&A...404..743K
5865:Kovalevsky, J. (2003).
5804:2019A&A...630A..93M
5752:2020A&A...644A.159C
5307:{\displaystyle u_{2}=0}
4793:{\displaystyle \theta }
4577:{\displaystyle \alpha }
4265:{\displaystyle \theta }
4234:Relativistic aberration
4184:{\displaystyle \gamma }
3318:{\displaystyle \theta }
3179:{\displaystyle \theta }
3075:principle of relativity
3071:Rømer's lightspeed data
2411:{\displaystyle \kappa }
2209:{\displaystyle \kappa }
2186:{\displaystyle \kappa }
2162:{\displaystyle \kappa }
2145:Solar annual aberration
2103:{\displaystyle \kappa }
2048:{\displaystyle \kappa }
2024:{\displaystyle \kappa }
1892:{\displaystyle \kappa }
1772:light-time displacement
1014:Lorentz transformations
960:may be approximated by
501:{\displaystyle \theta }
488:, and thus at an angle
63:astronomical aberration
6539:de:August Ludwig Busch
6523:Astronomical Discovery
6226:10.1098/rstl.1727.0064
6207:James Bradley (1729).
5500:10.1098/rstl.1727.0064
5364:
5334:. Thus we finally get
5328:
5308:
5275:
5255:
5191:
5117:
5052:
4986:
4963:
4931:
4876:
4844:
4815:
4794:
4774:
4754:
4713:
4693:
4605:
4578:
4558:
4538:
4453:
4404:
4355:
4286:
4266:
4185:
4169:
4156:
4116:
3976:
3960:
3910:
3890:
3862:Aether drag hypothesis
3829:
3725:
3705:
3685:
3657:
3636:
3606:
3554:
3517:
3363:
3343:
3319:
3299:
3279:
3248:
3228:
3200:
3180:
3154:
3057:In the prior century,
3035:
2701:
2693:
2656:
2633:atmospheric refraction
2412:
2392:
2352:
2297:
2277:
2243:
2210:
2187:
2163:
2104:
2082:). At the time of the
2049:
2025:
1982:
1959:
1939:
1893:
1877:constant of aberration
1846:
1808:
1800:
1691:
1672:
1612:
1572:
1538:
1486:
1450:
1274:
1205:
1113:
994:
954:
920:
868:
832:
674:
631:
582:
562:
502:
482:
455:
428:
404:addition of velocities
376:
147:
123:
103:
50:
6024:European Space Agency
5365:
5329:
5309:
5276:
5256:
5192:
5118:
5053:
4987:
4964:
4932:
4877:
4875:{\displaystyle x,y,z}
4845:
4843:{\displaystyle u,v,w}
4813:
4795:
4775:
4773:{\displaystyle \phi }
4755:
4714:
4694:
4606:
4604:{\displaystyle v_{l}}
4579:
4559:
4539:
4454:
4405:
4356:
4287:
4285:{\displaystyle \psi }
4267:
4219:Astronomical nutation
4186:
4152:Fizeau's measurements
4117:
3973:
3961:
3911:
3891:
3867:Fresnel's aether drag
3830:
3726:
3706:
3686:
3633:
3607:
3555:
3518:
3364:
3362:{\displaystyle \phi }
3344:
3342:{\displaystyle \phi }
3320:
3300:
3298:{\displaystyle \phi }
3280:
3249:
3229:
3201:
3186:and travels at speed
3181:
3144:
3110:"partial aether drag"
3106:Augustin-Jean Fresnel
3036:
2699:
2691:
2646:
2611:' observations, that
2530:Light-time correction
2413:
2393:
2353:
2298:
2278:
2276:{\displaystyle t=R/c}
2244:
2211:
2188:
2164:
2134:of the Solar System.
2105:
2050:
2026:
1983:
1960:
1940:
1894:
1847:
1806:
1786:
1768:Planetary aberration:
1696:light-time correction
1689:
1673:
1613:
1573:
1539:
1487:
1451:
1275:
1206:
1114:
995:
955:
926:, which in the limit
921:
869:
833:
675:
632:
583:
563:
503:
483:
481:{\displaystyle u_{y}}
456:
454:{\displaystyle u_{x}}
429:
410:Classical explanation
374:
187:light-time correction
148:
124:
104:
61:(also referred to as
48:
6502:Stephen Peter Rigaud
5341:
5318:
5285:
5265:
5205:
5141:
5130:it will satisfy the
5065:
4996:
4973:
4941:
4886:
4854:
4822:
4784:
4764:
4723:
4703:
4615:
4588:
4568:
4548:
4463:
4414:
4365:
4300:
4276:
4256:
4175:
4074:
4032:Lorentz ether theory
4016:D'Alembert's paradox
3920:
3900:
3880:
3738:
3715:
3695:
3667:
3564:
3531:
3376:
3353:
3333:
3309:
3289:
3278:{\displaystyle vh/c}
3258:
3238:
3210:
3190:
3170:
2962:
2847:Annual Variation (")
2586:. As early as 1573,
2524:Planetary aberration
2402:
2362:
2307:
2287:
2253:
2221:
2200:
2177:
2153:
2094:
2039:
2015:
1972:
1949:
1903:
1883:
1836:
1827:orbital eccentricity
1725:Astronomical Almanac
1700:relativistic beaming
1622:
1582:
1548:
1496:
1463:
1287:
1218:
1124:
1023:
964:
930:
878:
845:
687:
641:
592:
572:
512:
492:
465:
438:
418:
293:improve this article
223:aether drag theories
191:relativistic beaming
137:
113:
85:
40:chromatic aberration
36:spherical aberration
6438:1963AmJPh..31...47S
5934:2006AJ....131.1471K
5565:2004AHES...59...45N
5491:1727RSPT...35..637B
5479:Phil. Trans. R. Soc
5441:1979JHA....10..102W
4144:Robert S. Shankland
4011:boundary conditions
3980:Stokes' aether drag
3896:moving at velocity
3684:{\displaystyle c/n}
3626:Luminiferous aether
3620:Luminiferous aether
3227:{\displaystyle h/c}
3102:luminiferous aether
3069:commented that, on
1733:Stellar aberration:
1659:
1641:
1544:, and in the limit
1335:
1322:
1139:
1038:
735:
722:
656:
607:
233:(in 1845), and for
102:{\displaystyle v/c}
71:velocity aberration
6302:2013-11-11 at the
6260:10.1007/BF00348308
5629:spot all the time.
5360:
5324:
5304:
5271:
5251:
5187:
5134:, one of which is
5113:
5048:
4985:{\displaystyle dz}
4982:
4959:
4927:
4872:
4840:
4816:
4790:
4770:
4750:
4709:
4689:
4601:
4574:
4554:
4534:
4449:
4400:
4351:
4282:
4262:
4181:
4127:Special relativity
4112:
4068:length contraction
3977:
3956:
3906:
3886:
3856:Aether drag models
3825:
3721:
3701:
3681:
3654:Thomas Young, 1804
3637:
3602:
3550:
3513:
3359:
3339:
3325:, resulting in an
3315:
3295:
3275:
3244:
3224:
3196:
3176:
3155:
3131:special relativity
3092:and the motion of
3031:
2711:Earth's atmosphere
2702:
2694:
2657:
2446:Secular aberration
2422:Diurnal aberration
2408:
2388:
2348:
2293:
2273:
2239:
2206:
2183:
2159:
2100:
2057:ecliptic latitudes
2045:
2021:
1978:
1955:
1935:
1889:
1842:
1809:
1801:
1797:ecliptic longitude
1793:ecliptic latitudes
1758:Secular aberration
1749:Diurnal aberration
1692:
1668:
1645:
1627:
1608:
1568:
1534:
1482:
1446:
1323:
1310:
1270:
1201:
1127:
1109:
1026:
990:
950:
916:
864:
828:
723:
710:
670:
644:
627:
595:
578:
558:
498:
478:
451:
424:
400:special relativity
377:
210:heliocentric model
206:special relativity
143:
119:
99:
67:stellar aberration
51:
32:optical aberration
18:Stellar aberration
6556:Courtney Seligman
6446:10.1119/1.1969236
6374:978-1-4020-1308-9
6190:978-1-59339-837-8
6121:Eppenstein (1911)
6097:Eppenstein (1911)
6026:. 3 December 2020
5358:
5327:{\displaystyle v}
5274:{\displaystyle u}
5185:
5162:
5105:
5082:
4850:as a function of
4712:{\displaystyle h}
4687:
4557:{\displaystyle v}
4110:
4070:" by a factor of
3909:{\displaystyle v}
3889:{\displaystyle n}
3823:
3724:{\displaystyle n}
3704:{\displaystyle c}
3511:
3456:
3247:{\displaystyle v}
3199:{\displaystyle c}
3029:
2984:
2952:
2951:
2835:
2834:
2678:35 Camelopardalis
2653:35 Camelopardalis
2492:space observatory
2296:{\displaystyle R}
2112:September equinox
1981:{\displaystyle c}
1958:{\displaystyle v}
1845:{\displaystyle v}
1779:Annual aberration
1740:Annual aberration
1660:
1444:
1380:
1336:
1268:
826:
771:
736:
581:{\displaystyle v}
427:{\displaystyle c}
398:). The theory of
369:
368:
361:
343:
255:Fizeau experiment
253:, as well as the
146:{\displaystyle v}
122:{\displaystyle c}
75:celestial objects
16:(Redirected from
6659:
6624:
6623:
6622:
6612:
6611:
6610:
6600:
6599:
6598:
6588:
6587:
6576:
6575:
6574:
6567:
6483:
6465:
6463:
6462:
6450:
6449:
6421:
6415:
6414:
6402:
6392:
6386:
6385:
6383:
6362:
6353:
6347:
6346:
6336:
6319:
6306:
6294:
6288:
6287:
6237:
6231:
6230:
6228:
6204:
6195:
6194:
6174:
6166:
6160:
6159:
6143:
6133:
6124:
6118:
6109:
6106:
6100:
6094:
6081:
6080:
6062:
6042:
6036:
6035:
6033:
6031:
6012:
6006:
6005:
5979:
5959:
5948:
5947:
5945:
5927:
5925:astro-ph/0508505
5918:(3): 1471–1478.
5903:
5897:
5896:
5894:
5862:
5856:
5855:
5830:
5824:
5823:
5787:
5772:
5771:
5745:
5725:
5714:
5713:
5698:
5692:
5691:
5669:
5660:
5659:
5636:
5630:
5622:
5616:
5615:
5601:Basic Relativity
5595:
5589:
5588:
5544:
5535:
5534:
5516:
5505:
5504:
5502:
5485:(406): 637–661.
5470:
5461:
5460:
5424:
5418:
5417:
5399:
5375:
5369:
5367:
5366:
5361:
5359:
5351:
5333:
5331:
5330:
5325:
5313:
5311:
5310:
5305:
5297:
5296:
5280:
5278:
5277:
5272:
5260:
5258:
5257:
5252:
5247:
5239:
5238:
5226:
5225:
5196:
5194:
5193:
5188:
5186:
5184:
5176:
5168:
5163:
5161:
5153:
5145:
5126:If the fluid is
5122:
5120:
5119:
5114:
5106:
5104:
5096:
5088:
5083:
5075:
5057:
5055:
5054:
5049:
5041:
5018:
4991:
4989:
4988:
4983:
4968:
4966:
4965:
4960:
4936:
4934:
4933:
4928:
4920:
4881:
4879:
4878:
4873:
4849:
4847:
4846:
4841:
4807:
4801:
4799:
4797:
4796:
4791:
4779:
4777:
4776:
4771:
4759:
4757:
4756:
4751:
4749:
4748:
4739:
4718:
4716:
4715:
4710:
4698:
4696:
4695:
4690:
4688:
4686:
4657:
4637:
4610:
4608:
4607:
4602:
4600:
4599:
4583:
4581:
4580:
4575:
4563:
4561:
4560:
4555:
4543:
4541:
4540:
4535:
4527:
4526:
4517:
4476:
4458:
4456:
4455:
4450:
4427:
4409:
4407:
4406:
4401:
4378:
4360:
4358:
4357:
4352:
4291:
4289:
4288:
4283:
4271:
4269:
4268:
4263:
4250:
4214:Stellar parallax
4190:
4188:
4187:
4182:
4121:
4119:
4118:
4113:
4111:
4109:
4108:
4099:
4094:
4093:
4078:
3965:
3963:
3962:
3957:
3949:
3948:
3939:
3915:
3913:
3912:
3907:
3895:
3893:
3892:
3887:
3873:Augustin Fresnel
3834:
3832:
3831:
3826:
3824:
3822:
3797:
3786:
3777:
3760:
3730:
3728:
3727:
3722:
3710:
3708:
3707:
3702:
3690:
3688:
3687:
3682:
3677:
3661:refractive index
3655:
3611:
3609:
3608:
3603:
3598:
3559:
3557:
3556:
3551:
3549:
3548:
3522:
3520:
3519:
3514:
3512:
3510:
3488:
3479:
3462:
3457:
3455:
3430:
3418:
3398:
3368:
3366:
3365:
3360:
3348:
3346:
3345:
3340:
3324:
3322:
3321:
3316:
3304:
3302:
3301:
3296:
3284:
3282:
3281:
3276:
3271:
3253:
3251:
3250:
3245:
3233:
3231:
3230:
3225:
3220:
3205:
3203:
3202:
3197:
3185:
3183:
3182:
3177:
3040:
3038:
3037:
3032:
3030:
3022:
2999:
2995:
2985:
2977:
2841:
2748:
2684:Early hypotheses
2417:
2415:
2414:
2409:
2397:
2395:
2394:
2389:
2378:
2357:
2355:
2354:
2349:
2344:
2302:
2300:
2299:
2294:
2282:
2280:
2279:
2274:
2269:
2248:
2246:
2245:
2240:
2215:
2213:
2212:
2207:
2192:
2190:
2189:
2184:
2168:
2166:
2165:
2160:
2109:
2107:
2106:
2101:
2054:
2052:
2051:
2046:
2030:
2028:
2027:
2022:
1987:
1985:
1984:
1979:
1964:
1962:
1961:
1956:
1944:
1942:
1941:
1936:
1931:
1898:
1896:
1895:
1890:
1851:
1849:
1848:
1843:
1831:orbital velocity
1813:Stellar parallax
1677:
1675:
1674:
1669:
1661:
1658:
1653:
1640:
1635:
1626:
1617:
1615:
1614:
1609:
1604:
1577:
1575:
1574:
1569:
1558:
1543:
1541:
1540:
1535:
1530:
1491:
1489:
1488:
1483:
1481:
1480:
1455:
1453:
1452:
1447:
1445:
1443:
1418:
1403:
1386:
1381:
1379:
1369:
1368:
1352:
1351:
1342:
1337:
1331:
1318:
1309:
1279:
1277:
1276:
1271:
1269:
1267:
1266:
1257:
1252:
1251:
1236:
1234:
1210:
1208:
1207:
1202:
1197:
1196:
1187:
1179:
1178:
1157:
1152:
1151:
1135:
1118:
1116:
1115:
1110:
1105:
1104:
1095:
1087:
1086:
1068:
1054:
1053:
1034:
999:
997:
996:
991:
986:
959:
957:
956:
951:
940:
925:
923:
922:
917:
912:
873:
871:
870:
865:
863:
862:
837:
835:
834:
829:
827:
825:
803:
794:
777:
772:
770:
763:
762:
752:
751:
742:
737:
731:
718:
709:
679:
677:
676:
671:
669:
668:
652:
636:
634:
633:
628:
620:
619:
603:
587:
585:
584:
579:
567:
565:
564:
559:
557:
556:
547:
542:
541:
507:
505:
504:
499:
487:
485:
484:
479:
477:
476:
460:
458:
457:
452:
450:
449:
433:
431:
430:
425:
364:
357:
353:
350:
344:
342:
301:
277:
269:
227:Augustin Fresnel
202:electromagnetism
152:
150:
149:
144:
128:
126:
125:
120:
108:
106:
105:
100:
95:
21:
6667:
6666:
6662:
6661:
6660:
6658:
6657:
6656:
6632:
6631:
6630:
6620:
6618:
6608:
6606:
6596:
6594:
6582:
6572:
6570:
6562:
6552:
6491:
6489:Further reading
6486:
6471:
6460:
6458:
6454:
6453:
6423:
6422:
6418:
6411:
6394:
6393:
6389:
6381:
6375:
6360:
6355:
6354:
6350:
6338:
6337:
6321:
6320:
6309:
6304:Wayback Machine
6295:
6291:
6239:
6238:
6234:
6206:
6205:
6198:
6191:
6168:
6167:
6163:
6156:
6135:
6134:
6127:
6119:
6112:
6107:
6103:
6095:
6084:
6044:
6043:
6039:
6029:
6027:
6014:
6013:
6009:
5961:
5960:
5951:
5905:
5904:
5900:
5864:
5863:
5859:
5832:
5831:
5827:
5789:
5788:
5775:
5727:
5726:
5717:
5700:
5699:
5695:
5688:
5671:
5670:
5663:
5656:
5638:
5637:
5633:
5623:
5619:
5612:
5597:
5596:
5592:
5546:
5545:
5538:
5531:
5518:
5517:
5508:
5472:
5471:
5464:
5426:
5425:
5421:
5414:
5401:
5400:
5389:
5384:
5379:
5378:
5339:
5338:
5316:
5315:
5288:
5283:
5282:
5263:
5262:
5230:
5217:
5203:
5202:
5177:
5169:
5154:
5146:
5139:
5138:
5097:
5089:
5063:
5062:
4994:
4993:
4971:
4970:
4939:
4938:
4884:
4883:
4852:
4851:
4820:
4819:
4808:
4804:
4782:
4781:
4762:
4761:
4740:
4721:
4720:
4701:
4700:
4658:
4638:
4613:
4612:
4591:
4586:
4585:
4566:
4565:
4546:
4545:
4518:
4461:
4460:
4412:
4411:
4363:
4362:
4298:
4297:
4274:
4273:
4254:
4253:
4251:
4247:
4242:
4205:
4173:
4172:
4135:
4129:
4100:
4085:
4072:
4071:
4034:
4028:
3982:
3940:
3918:
3917:
3898:
3897:
3878:
3877:
3869:
3864:
3858:
3778:
3761:
3736:
3735:
3713:
3712:
3693:
3692:
3665:
3664:
3656:
3653:
3628:
3622:
3562:
3561:
3540:
3529:
3528:
3527:In the case of
3480:
3463:
3419:
3399:
3374:
3373:
3351:
3350:
3331:
3330:
3307:
3306:
3305:different from
3287:
3286:
3256:
3255:
3236:
3235:
3208:
3207:
3188:
3187:
3168:
3167:
3139:
3127:Albert Einstein
3123:electron theory
3119:Hendrik Lorentz
3083:
3055:
2975:
2971:
2960:
2959:
2825:19.5" northward
2791:19.5" southward
2726:
2686:
2661:Samuel Molyneux
2641:
2557:
2541:
2532:
2526:
2518:reference epoch
2448:
2424:
2400:
2399:
2360:
2359:
2305:
2304:
2285:
2284:
2251:
2250:
2219:
2218:
2198:
2197:
2175:
2174:
2151:
2150:
2147:
2122:is 0 on either
2120:right ascension
2092:
2091:
2037:
2036:
2013:
2012:
1970:
1969:
1947:
1946:
1901:
1900:
1881:
1880:
1834:
1833:
1815:
1781:
1720:
1684:
1620:
1619:
1580:
1579:
1546:
1545:
1494:
1493:
1472:
1461:
1460:
1459:In the case of
1404:
1387:
1360:
1353:
1343:
1285:
1284:
1258:
1243:
1216:
1215:
1188:
1170:
1143:
1122:
1121:
1096:
1078:
1045:
1021:
1020:
1006:
962:
961:
928:
927:
876:
875:
854:
843:
842:
841:In the case of
795:
778:
754:
753:
743:
685:
684:
660:
639:
638:
611:
590:
589:
570:
569:
548:
533:
510:
509:
490:
489:
468:
463:
462:
441:
436:
435:
416:
415:
412:
365:
354:
348:
345:
302:
300:
290:
278:
267:
259:Albert Einstein
235:Hendrik Lorentz
168:right ascension
135:
134:
111:
110:
83:
82:
79:apparent motion
43:
28:
23:
22:
15:
12:
11:
5:
6665:
6663:
6655:
6654:
6649:
6644:
6634:
6633:
6629:
6628:
6616:
6604:
6592:
6580:
6560:
6559:
6551:
6550:External links
6548:
6547:
6546:
6536:
6529:Thomas Simpson
6526:
6521:H. H. Turner,
6519:
6512:Charles Hutton
6509:
6499:
6490:
6487:
6485:
6484:
6455:
6452:
6451:
6416:
6409:
6387:
6373:
6365:Going Critical
6348:
6307:
6289:
6232:
6196:
6189:
6161:
6154:
6125:
6110:
6101:
6082:
6037:
6007:
5949:
5943:10.1086/500170
5898:
5877:(2): 743–747.
5857:
5839:. 3rd Series.
5825:
5773:
5715:
5702:Newcomb, Simon
5693:
5686:
5661:
5654:
5631:
5617:
5610:
5590:
5536:
5529:
5506:
5462:
5435:(2): 102–116.
5419:
5412:
5386:
5385:
5383:
5380:
5377:
5376:
5371:
5370:
5357:
5354:
5349:
5346:
5323:
5303:
5300:
5295:
5291:
5270:
5250:
5246:
5242:
5237:
5233:
5229:
5224:
5220:
5216:
5213:
5210:
5199:
5198:
5183:
5180:
5175:
5172:
5166:
5160:
5157:
5152:
5149:
5124:
5123:
5112:
5109:
5103:
5100:
5095:
5092:
5086:
5081:
5078:
5073:
5070:
5047:
5044:
5040:
5036:
5033:
5030:
5027:
5024:
5021:
5017:
5013:
5010:
5007:
5004:
5001:
4981:
4978:
4958:
4955:
4952:
4949:
4946:
4926:
4923:
4919:
4915:
4912:
4909:
4906:
4903:
4900:
4897:
4894:
4891:
4871:
4868:
4865:
4862:
4859:
4839:
4836:
4833:
4830:
4827:
4802:
4789:
4769:
4747:
4743:
4738:
4734:
4731:
4728:
4708:
4685:
4682:
4679:
4676:
4673:
4670:
4667:
4664:
4661:
4656:
4653:
4650:
4647:
4644:
4641:
4635:
4632:
4629:
4626:
4623:
4620:
4598:
4594:
4573:
4553:
4533:
4530:
4525:
4521:
4516:
4512:
4509:
4506:
4503:
4500:
4497:
4494:
4491:
4488:
4485:
4482:
4479:
4475:
4471:
4468:
4448:
4445:
4442:
4439:
4436:
4433:
4430:
4426:
4422:
4419:
4399:
4396:
4393:
4390:
4387:
4384:
4381:
4377:
4373:
4370:
4350:
4347:
4344:
4341:
4338:
4335:
4332:
4329:
4326:
4323:
4320:
4317:
4314:
4311:
4308:
4305:
4281:
4261:
4244:
4243:
4241:
4238:
4237:
4236:
4231:
4226:
4221:
4216:
4211:
4209:Apparent place
4204:
4201:
4180:
4128:
4125:
4107:
4103:
4098:
4092:
4088:
4084:
4081:
4027:
4024:
3981:
3978:
3955:
3952:
3947:
3943:
3938:
3934:
3931:
3928:
3925:
3905:
3885:
3868:
3865:
3857:
3854:
3845:François Arago
3837:
3836:
3821:
3818:
3815:
3812:
3809:
3806:
3803:
3800:
3796:
3792:
3789:
3785:
3781:
3776:
3773:
3770:
3767:
3764:
3758:
3755:
3752:
3749:
3746:
3743:
3720:
3700:
3680:
3676:
3672:
3651:
3621:
3618:
3614:speed of light
3601:
3597:
3593:
3590:
3587:
3584:
3581:
3578:
3575:
3572:
3569:
3547:
3543:
3539:
3536:
3525:
3524:
3509:
3506:
3503:
3500:
3497:
3494:
3491:
3487:
3483:
3478:
3475:
3472:
3469:
3466:
3460:
3454:
3451:
3448:
3445:
3442:
3439:
3436:
3433:
3429:
3425:
3422:
3417:
3414:
3411:
3408:
3405:
3402:
3396:
3393:
3390:
3387:
3384:
3381:
3358:
3338:
3314:
3294:
3274:
3270:
3266:
3263:
3243:
3223:
3219:
3215:
3206:taking a time
3195:
3175:
3138:
3135:
3121:to develop an
3090:speed of light
3082:
3079:
3059:René Descartes
3054:
3051:
3042:
3041:
3028:
3025:
3020:
3017:
3014:
3011:
3008:
3005:
3002:
2998:
2994:
2991:
2988:
2983:
2980:
2974:
2970:
2967:
2950:
2949:
2946:
2944:
2940:
2939:
2936:
2933:
2929:
2928:
2925:
2922:
2918:
2917:
2914:
2911:
2907:
2906:
2903:
2900:
2896:
2895:
2892:
2889:
2885:
2884:
2881:
2878:
2874:
2873:
2870:
2867:
2863:
2862:
2859:
2856:
2852:
2851:
2848:
2845:
2833:
2832:
2829:
2826:
2823:
2820:
2816:
2815:
2812:
2809:
2806:
2803:
2799:
2798:
2795:
2792:
2789:
2786:
2782:
2781:
2778:
2775:
2772:
2769:
2765:
2764:
2761:
2758:
2755:
2752:
2725:
2722:
2685:
2682:
2640:
2637:
2617:John Flamsteed
2566:theory of the
2556:
2553:
2540:
2537:
2525:
2522:
2447:
2444:
2428:rotating Earth
2423:
2420:
2407:
2387:
2384:
2381:
2377:
2373:
2370:
2367:
2347:
2343:
2339:
2336:
2333:
2330:
2327:
2324:
2321:
2318:
2315:
2312:
2292:
2272:
2268:
2264:
2261:
2258:
2238:
2235:
2232:
2229:
2226:
2205:
2182:
2158:
2146:
2143:
2099:
2044:
2033:ecliptic poles
2020:
2005:circular orbit
1977:
1967:speed of light
1954:
1934:
1930:
1926:
1923:
1920:
1917:
1914:
1911:
1908:
1888:
1871:Approximating
1862:appear to move
1858:elliptic orbit
1841:
1789:ecliptic poles
1780:
1777:
1776:
1775:
1765:
1764:
1763:
1754:
1745:
1719:
1716:
1683:
1680:
1667:
1664:
1657:
1652:
1648:
1644:
1639:
1634:
1630:
1607:
1603:
1599:
1596:
1593:
1590:
1587:
1567:
1564:
1561:
1557:
1553:
1533:
1529:
1525:
1522:
1519:
1516:
1513:
1510:
1507:
1504:
1501:
1479:
1475:
1471:
1468:
1457:
1456:
1442:
1439:
1436:
1433:
1430:
1427:
1424:
1421:
1417:
1413:
1410:
1407:
1402:
1399:
1396:
1393:
1390:
1384:
1378:
1375:
1372:
1367:
1363:
1359:
1356:
1350:
1346:
1340:
1334:
1330:
1326:
1321:
1317:
1313:
1307:
1304:
1301:
1298:
1295:
1292:
1265:
1261:
1256:
1250:
1246:
1242:
1239:
1233:
1229:
1226:
1223:
1212:
1211:
1200:
1195:
1191:
1186:
1182:
1177:
1173:
1169:
1166:
1163:
1160:
1156:
1150:
1146:
1142:
1138:
1134:
1130:
1119:
1108:
1103:
1099:
1094:
1090:
1085:
1081:
1077:
1074:
1071:
1067:
1063:
1060:
1057:
1052:
1048:
1044:
1041:
1037:
1033:
1029:
1005:
1002:
989:
985:
981:
978:
975:
972:
969:
949:
946:
943:
939:
935:
915:
911:
907:
904:
901:
898:
895:
892:
889:
886:
883:
861:
857:
853:
850:
839:
838:
824:
821:
818:
815:
812:
809:
806:
802:
798:
793:
790:
787:
784:
781:
775:
769:
766:
761:
757:
750:
746:
740:
734:
730:
726:
721:
717:
713:
707:
704:
701:
698:
695:
692:
667:
663:
659:
655:
651:
647:
626:
623:
618:
614:
610:
606:
602:
598:
577:
555:
551:
546:
540:
536:
532:
529:
526:
523:
520:
517:
497:
475:
471:
448:
444:
423:
411:
408:
367:
366:
281:
279:
272:
266:
263:
229:(in 1818) and
142:
131:speed of light
118:
98:
94:
90:
26:
24:
14:
13:
10:
9:
6:
4:
3:
2:
6664:
6653:
6650:
6648:
6645:
6643:
6640:
6639:
6637:
6627:
6617:
6615:
6605:
6603:
6593:
6591:
6586:
6581:
6579:
6569:
6565:
6557:
6554:
6553:
6549:
6544:
6540:
6537:
6534:
6530:
6527:
6524:
6520:
6517:
6513:
6510:
6507:
6503:
6500:
6497:
6493:
6492:
6488:
6481:
6480:
6475:
6469:
6468:public domain
6457:
6456:
6447:
6443:
6439:
6435:
6431:
6427:
6420:
6417:
6412:
6410:0-19-850594-9
6406:
6401:
6400:
6391:
6388:
6380:
6376:
6370:
6366:
6359:
6352:
6349:
6344:
6343:
6334:
6330:
6329:
6324:
6318:
6316:
6314:
6312:
6308:
6305:
6301:
6298:
6293:
6290:
6285:
6281:
6277:
6273:
6269:
6265:
6261:
6257:
6253:
6249:
6248:
6243:
6236:
6233:
6227:
6222:
6218:
6214:
6210:
6203:
6201:
6197:
6192:
6186:
6182:
6178:
6173:
6165:
6162:
6157:
6155:9780486202105
6151:
6147:
6142:
6141:
6132:
6130:
6126:
6123:, p. 55.
6122:
6117:
6115:
6111:
6105:
6102:
6099:, p. 54.
6098:
6093:
6091:
6089:
6087:
6083:
6078:
6074:
6070:
6066:
6061:
6056:
6052:
6048:
6041:
6038:
6025:
6021:
6017:
6011:
6008:
6003:
5999:
5995:
5991:
5987:
5983:
5978:
5973:
5969:
5965:
5958:
5956:
5954:
5950:
5944:
5939:
5935:
5931:
5926:
5921:
5917:
5913:
5909:
5902:
5899:
5893:
5888:
5884:
5880:
5876:
5872:
5868:
5861:
5858:
5854:
5850:
5846:
5842:
5838:
5837:
5829:
5826:
5821:
5817:
5813:
5809:
5805:
5801:
5797:
5793:
5786:
5784:
5782:
5780:
5778:
5774:
5769:
5765:
5761:
5757:
5753:
5749:
5744:
5739:
5735:
5731:
5724:
5722:
5720:
5716:
5711:
5707:
5703:
5697:
5694:
5689:
5687:0-521-64216-7
5683:
5679:
5676:. Cambridge:
5675:
5668:
5666:
5662:
5657:
5655:9780707741499
5651:
5647:
5646:
5641:
5635:
5632:
5628:
5621:
5618:
5613:
5611:0-387-95210-1
5607:
5603:
5602:
5594:
5591:
5586:
5582:
5578:
5574:
5570:
5566:
5562:
5559:(1): 45–105.
5558:
5554:
5550:
5543:
5541:
5537:
5532:
5530:0-8050-7133-4
5526:
5522:
5515:
5513:
5511:
5507:
5501:
5496:
5492:
5488:
5484:
5480:
5476:
5469:
5467:
5463:
5458:
5454:
5450:
5446:
5442:
5438:
5434:
5430:
5423:
5420:
5415:
5413:0-08-015674-6
5409:
5405:
5398:
5396:
5394:
5392:
5388:
5381:
5374:
5355:
5352:
5347:
5344:
5337:
5336:
5335:
5321:
5301:
5298:
5293:
5289:
5268:
5248:
5244:
5235:
5231:
5227:
5222:
5218:
5211:
5208:
5181:
5173:
5164:
5158:
5150:
5137:
5136:
5135:
5133:
5129:
5110:
5107:
5101:
5093:
5084:
5079:
5076:
5071:
5068:
5061:
5060:
5059:
5042:
5038:
5034:
5031:
5022:
5019:
5015:
5011:
5008:
5002:
4999:
4979:
4976:
4956:
4953:
4950:
4947:
4944:
4924:
4921:
4917:
4913:
4910:
4907:
4904:
4898:
4892:
4889:
4869:
4866:
4863:
4860:
4857:
4837:
4834:
4831:
4828:
4825:
4812:
4806:
4803:
4787:
4767:
4745:
4741:
4736:
4732:
4729:
4726:
4706:
4680:
4674:
4671:
4668:
4665:
4662:
4659:
4651:
4645:
4642:
4639:
4633:
4627:
4621:
4618:
4596:
4592:
4584:is angle and
4571:
4551:
4531:
4523:
4519:
4514:
4510:
4507:
4504:
4498:
4492:
4486:
4483:
4477:
4473:
4469:
4443:
4437:
4434:
4428:
4424:
4420:
4394:
4388:
4385:
4379:
4375:
4371:
4345:
4342:
4339:
4333:
4330:
4327:
4324:
4318:
4315:
4312:
4306:
4303:
4295:
4279:
4259:
4249:
4246:
4239:
4235:
4232:
4230:
4227:
4225:
4224:Proper motion
4222:
4220:
4217:
4215:
4212:
4210:
4207:
4206:
4202:
4200:
4198:
4194:
4178:
4168:
4163:
4161:
4155:
4153:
4147:
4145:
4141:
4134:
4126:
4124:
4105:
4101:
4096:
4090:
4086:
4082:
4079:
4069:
4065:
4060:
4054:
4052:
4048:
4044:
4040:
4033:
4023:
4019:
4017:
4012:
4009:and that the
4008:
4003:
3998:
3995:
3991:
3987:
3972:
3968:
3953:
3945:
3941:
3936:
3932:
3929:
3926:
3903:
3883:
3874:
3863:
3855:
3853:
3851:
3846:
3842:
3816:
3810:
3807:
3804:
3798:
3794:
3790:
3783:
3779:
3771:
3765:
3762:
3756:
3750:
3744:
3741:
3734:
3733:
3732:
3718:
3698:
3678:
3674:
3670:
3662:
3650:
3645:
3642:
3632:
3627:
3619:
3617:
3615:
3599:
3595:
3591:
3588:
3582:
3579:
3576:
3570:
3567:
3560:, this gives
3545:
3541:
3537:
3534:
3504:
3498:
3495:
3492:
3489:
3485:
3481:
3473:
3467:
3464:
3458:
3449:
3443:
3440:
3437:
3434:
3431:
3427:
3423:
3420:
3412:
3406:
3403:
3400:
3394:
3388:
3382:
3379:
3372:
3371:
3370:
3356:
3336:
3328:
3312:
3292:
3272:
3268:
3264:
3261:
3241:
3221:
3217:
3213:
3193:
3173:
3163:
3160:
3152:
3148:
3143:
3134:
3132:
3128:
3124:
3120:
3115:
3114:George Stokes
3111:
3107:
3103:
3099:
3095:
3091:
3086:
3080:
3078:
3076:
3072:
3068:
3063:
3060:
3050:
3046:
3026:
3023:
3018:
3012:
3006:
3003:
3000:
2996:
2992:
2989:
2986:
2981:
2978:
2972:
2968:
2965:
2958:
2957:
2956:
2947:
2945:
2942:
2941:
2937:
2934:
2931:
2930:
2926:
2923:
2920:
2919:
2915:
2912:
2909:
2908:
2904:
2901:
2898:
2897:
2893:
2890:
2887:
2886:
2882:
2879:
2876:
2875:
2871:
2868:
2865:
2864:
2860:
2857:
2854:
2853:
2849:
2846:
2843:
2842:
2839:
2830:
2827:
2824:
2821:
2818:
2817:
2813:
2810:
2807:
2804:
2801:
2800:
2796:
2793:
2790:
2787:
2784:
2783:
2779:
2776:
2773:
2770:
2767:
2766:
2762:
2759:
2756:
2753:
2750:
2749:
2746:
2743:
2738:
2736:
2731:
2730:Royal Society
2723:
2721:
2719:
2714:
2712:
2708:
2698:
2690:
2683:
2681:
2679:
2673:
2671:
2670:George Graham
2667:
2662:
2654:
2650:
2645:
2636:
2634:
2630:
2626:
2622:
2618:
2614:
2610:
2606:
2604:
2598:
2594:
2589:
2588:Thomas Digges
2585:
2581:
2577:
2573:
2569:
2565:
2562:
2554:
2552:
2550:
2546:
2538:
2536:
2531:
2523:
2521:
2519:
2515:
2511:
2510:data releases
2509:
2502:
2497:
2493:
2491:
2486:
2482:
2477:
2475:
2474:proper motion
2469:
2466:
2465:extragalactic
2462:
2458:
2454:
2445:
2443:
2441:
2437:
2433:
2429:
2421:
2419:
2405:
2385:
2382:
2379:
2375:
2371:
2368:
2365:
2345:
2341:
2337:
2331:
2328:
2325:
2319:
2313:
2310:
2290:
2270:
2266:
2262:
2259:
2256:
2236:
2233:
2230:
2227:
2203:
2194:
2180:
2172:
2156:
2144:
2142:
2140:
2135:
2133:
2127:
2125:
2121:
2117:
2113:
2097:
2089:
2085:
2084:March equinox
2081:
2077:
2073:
2069:
2068:Arctic Circle
2064:
2062:
2058:
2042:
2034:
2018:
2010:
2006:
2001:
1999:
1995:
1991:
1975:
1968:
1952:
1932:
1928:
1924:
1921:
1918:
1915:
1912:
1909:
1906:
1886:
1878:
1874:
1873:Earth's orbit
1869:
1867:
1863:
1859:
1855:
1839:
1832:
1828:
1824:
1820:
1814:
1805:
1798:
1794:
1790:
1787:Stars at the
1785:
1778:
1773:
1769:
1766:
1761:
1759:
1755:
1752:
1750:
1746:
1743:
1741:
1737:
1736:
1734:
1731:
1730:
1729:
1727:
1726:
1717:
1715:
1712:
1707:
1703:
1701:
1697:
1688:
1681:
1679:
1665:
1662:
1655:
1650:
1646:
1642:
1637:
1632:
1628:
1605:
1601:
1597:
1594:
1591:
1588:
1585:
1565:
1562:
1559:
1555:
1551:
1531:
1527:
1523:
1520:
1514:
1511:
1508:
1502:
1499:
1477:
1473:
1469:
1466:
1434:
1428:
1425:
1422:
1419:
1415:
1411:
1405:
1397:
1391:
1388:
1382:
1373:
1370:
1365:
1361:
1354:
1348:
1344:
1338:
1332:
1328:
1324:
1319:
1315:
1311:
1305:
1299:
1293:
1290:
1283:
1282:
1281:
1263:
1259:
1254:
1248:
1244:
1240:
1237:
1231:
1227:
1224:
1221:
1193:
1189:
1184:
1180:
1175:
1171:
1167:
1164:
1158:
1154:
1148:
1144:
1140:
1136:
1132:
1128:
1120:
1101:
1097:
1092:
1088:
1083:
1079:
1075:
1072:
1065:
1058:
1055:
1050:
1046:
1039:
1035:
1031:
1027:
1019:
1018:
1017:
1015:
1011:
1003:
1001:
987:
983:
979:
976:
973:
970:
967:
947:
944:
941:
937:
933:
913:
909:
905:
902:
896:
893:
890:
884:
881:
859:
855:
851:
848:
819:
813:
810:
807:
804:
800:
796:
788:
782:
779:
773:
767:
764:
759:
755:
748:
744:
738:
732:
728:
724:
719:
715:
711:
705:
699:
693:
690:
683:
682:
681:
665:
661:
657:
653:
649:
645:
624:
621:
616:
612:
608:
604:
600:
596:
575:
553:
549:
544:
538:
534:
530:
524:
518:
515:
495:
473:
469:
446:
442:
421:
409:
407:
405:
401:
397:
392:
388:
384:
382:
373:
363:
360:
352:
341:
338:
334:
331:
327:
324:
320:
317:
313:
310: –
309:
305:
304:Find sources:
298:
294:
288:
287:
282:This section
280:
276:
271:
270:
264:
262:
260:
256:
252:
248:
244:
240:
239:aether theory
236:
232:
228:
224:
219:
215:
214:James Bradley
211:
207:
203:
199:
194:
192:
188:
184:
180:
175:
173:
169:
165:
161:
156:
140:
132:
116:
96:
92:
88:
80:
76:
72:
68:
64:
60:
56:
47:
41:
37:
33:
19:
6626:Solar System
6542:
6532:
6522:
6515:
6505:
6495:
6477:
6432:(1): 47–57.
6429:
6425:
6419:
6398:
6390:
6367:. Springer.
6364:
6351:
6340:
6327:
6292:
6251:
6245:
6235:
6216:
6212:
6176:
6164:
6139:
6104:
6050:
6046:
6040:
6030:14 September
6028:. Retrieved
6019:
6010:
5967:
5963:
5915:
5911:
5901:
5874:
5870:
5860:
5852:
5843:(3–6): 175.
5840:
5834:
5828:
5795:
5791:
5733:
5729:
5705:
5696:
5673:
5644:
5634:
5626:
5620:
5600:
5593:
5556:
5552:
5520:
5482:
5478:
5432:
5428:
5422:
5403:
5372:
5200:
5128:irrotational
5125:
4817:
4805:
4780:in terms of
4248:
4196:
4170:
4165:
4157:
4149:
4136:
4058:
4055:
4035:
4020:
4007:irrotational
3999:
3983:
3870:
3838:
3691:rather than
3658:
3647:
3641:Thomas Young
3638:
3526:
3326:
3164:
3156:
3150:
3146:
3087:
3084:
3056:
3047:
3043:
2953:
2836:
2739:
2727:
2715:
2703:
2674:
2658:
2627:, a star of
2621:Robert Hooke
2600:
2568:Solar System
2564:heliocentric
2558:
2542:
2533:
2507:
2500:
2489:
2478:
2470:
2449:
2425:
2195:
2170:
2169:towards the
2148:
2136:
2128:
2080:sidereal day
2065:
2002:
1876:
1870:
1816:
1767:
1756:
1747:
1738:
1732:
1723:
1721:
1711:acceleration
1708:
1704:
1693:
1458:
1213:
1007:
840:
413:
393:
389:
385:
378:
355:
346:
336:
329:
322:
315:
303:
291:Please help
286:verification
283:
231:G. G. Stokes
195:
178:
176:
70:
66:
62:
58:
52:
6614:Outer space
6602:Spaceflight
6254:(1): 1–12.
6219:: 637–661.
4294:Snell's law
3876:refraction
2877:η Ursa Maj.
2597:Jean Picard
2576:Tycho Brahe
2457:Local Group
2088:declination
2003:Assuming a
265:Explanation
216:provided a
172:declination
77:exhibit an
6647:Astrometry
6636:Categories
6474:Aberration
6060:2012.02036
5743:2010.13625
5382:References
5261:where the
4131:See also:
4059:completely
4030:See also:
3860:See also:
3624:See also:
3013:0.00009793
2993:0.00009793
2866:β Draconis
2855:γ Draconis
2735:apocryphal
2649:γ Draconis
2625:γ Draconis
2603:Uranibourg
2561:Copernican
2549:parallaxes
2528:See also:
2496:our galaxy
2481:astrometry
2132:barycenter
1996:(rad) (at
1990:arcseconds
1811:See also:
508:such that
319:newspapers
179:aberration
164:arcseconds
59:aberration
6652:Radiation
6578:Astronomy
6284:118187860
6268:0003-9519
6002:119305429
5977:1009.3698
5820:198471325
5768:225068756
5457:118565124
5348:≈
5345:α
5228:−
5209:α
5179:∂
5171:∂
5156:∂
5148:∂
5099:∂
5091:∂
5085:∫
5072:≈
5069:α
5003:≈
5000:α
4951:≈
4899:α
4893:
4788:θ
4768:ϕ
4681:α
4675:
4652:α
4646:
4628:ϕ
4622:
4572:α
4508:−
4499:−
4493:ψ
4487:
4444:ψ
4438:
4395:ψ
4389:
4346:ϕ
4343:−
4340:ψ
4334:
4319:ϕ
4316:−
4313:θ
4307:
4296:, giving
4280:ψ
4260:θ
4179:γ
4083:−
4043:Heaviside
4000:In 1845,
3986:polarized
3930:−
3871:In 1818,
3841:objective
3817:θ
3811:
3772:θ
3766:
3751:ϕ
3745:
3583:ϕ
3580:−
3577:θ
3571:
3546:∘
3535:θ
3505:θ
3499:
3474:θ
3468:
3450:θ
3444:
3413:θ
3407:
3389:ϕ
3383:
3357:ϕ
3337:ϕ
3313:θ
3293:ϕ
3174:θ
3007:
2990:−
2987:π
2969:
2921:35 Camel.
2819:September
2629:magnitude
2601:Voyage d'
2599:, in his
2436:longitude
2406:κ
2386:κ
2366:θ
2335:Δ
2329:θ
2326:≈
2320:θ
2314:
2225:Δ
2204:κ
2181:κ
2157:κ
2110:. On the
2098:κ
2043:κ
2019:κ
1922:≈
1919:ϕ
1916:−
1913:θ
1907:κ
1887:κ
1864:in small
1825:. Due to
1592:ϕ
1589:−
1586:θ
1563:≪
1515:ϕ
1512:−
1509:θ
1503:
1478:∘
1467:θ
1435:θ
1429:
1406:γ
1398:θ
1392:
1355:γ
1300:ϕ
1294:
1241:−
1222:γ
1159:γ
974:ϕ
971:−
968:θ
945:≪
897:ϕ
894:−
891:θ
885:
860:∘
849:θ
820:θ
814:
789:θ
783:
700:ϕ
694:
525:θ
519:
496:θ
349:July 2019
218:classical
177:The term
55:astronomy
6379:Archived
6333:Archived
6325:(1910).
6300:Archived
6276:41133639
5736:: A159.
5704:(1960).
5585:Archived
5581:17459755
4203:See also
3652:—
3327:apparent
2910:α Persei
2899:τ Persei
2768:December
2718:Wanstead
2707:nutation
2520:2015.0.
2487:and the
2432:latitude
2139:parallax
2116:solstice
2009:ecliptic
1965:and the
1866:ellipses
1799:of 270°.
1333:′
1320:′
1137:′
1036:′
733:′
720:′
654:′
605:′
183:parallax
160:revolves
155:velocity
6564:Portals
6545:(1838).
6535:(1740).
6525:(1904).
6518:(1795).
6508:(1832).
6470::
6434:Bibcode
6065:Bibcode
6020:esa.int
5982:Bibcode
5970:: A91.
5930:Bibcode
5879:Bibcode
5800:Bibcode
5798:: A93.
5748:Bibcode
5561:Bibcode
5487:Bibcode
5437:Bibcode
4039:Maxwell
3975:aether.
3067:Huygens
2932:Capella
2888:α Cass.
2613:Polaris
2572:Galileo
2545:Bradley
2440:Equator
2124:equinox
2074:at the
2072:transit
2061:ellipse
1994:radians
396:history
333:scholar
129:is the
6464:
6407:
6371:
6282:
6274:
6266:
6187:
6152:
6053:: A9.
6000:
5818:
5766:
5684:
5652:
5608:
5579:
5527:
5455:
5410:
4699:where
4002:Stokes
3990:Cauchy
3711:where
3649:trees.
3062:argued
2742:colure
2584:Newton
2580:Kepler
2506:later
2076:zenith
1854:varies
1829:, the
1214:where
335:
328:
321:
314:
306:
257:, led
249:, the
245:, the
109:where
6590:Stars
6382:(PDF)
6361:(PDF)
6280:S2CID
6272:JSTOR
6146:Dover
6055:arXiv
5998:S2CID
5972:arXiv
5920:arXiv
5816:S2CID
5764:S2CID
5738:arXiv
5710:Dover
5577:S2CID
5453:S2CID
4564:. If
4240:Notes
4140:above
4047:Hertz
3994:Green
3094:Earth
2948:40.4
2938:40.0
2927:40.2
2916:40.2
2905:41.0
2894:40.8
2883:40.4
2872:40.2
2861:40.4
2831:none
2797:none
2785:March
2751:Month
2609:years
1998:J2000
1819:Earth
1718:Types
340:JSTOR
326:books
198:light
69:, or
38:, or
6405:ISBN
6369:ISBN
6264:ISSN
6185:ISBN
6150:ISBN
6032:2022
5682:ISBN
5650:ISBN
5606:ISBN
5525:ISBN
5408:ISBN
4410:and
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