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The angular diameter, angular size, apparent diameter, or apparent size is an angular distance describing how large a sphere or circle appears from a given point of view. In the vision sciences, it is called the visual angle, and in optics, it is the angular aperture (of a lens). The angular diameter can alternatively be thought of as the angular displacement through which an eye or camera must rotate to look from one side of an apparent circle to the opposite side. Humans can resolve with their naked eyes diameters down to about 1 arcminute (approximately 0.017° or 0.0003 radians). [1] This corresponds to 0.3 m at a 1 km distance, or to perceiving Venus as a disk under optimal conditions.
The angular diameter of a circle whose plane is perpendicular to the displacement vector between the point of view and the center of said circle can be calculated using the formula [2] [3]
in which is the angular diameter in degrees, and is the actual diameter of the object, and is the distance to the object. When , we have , [4] and the result obtained is in radians.
For a spherical object whose actual diameter equals and where is the distance to the center of the sphere, the angular diameter can be found by the following modified formula[ citation needed ]
The difference is due to the fact that the apparent edges of a sphere are its tangent points, which are closer to the observer than the center of the sphere, and have a distance between them which is smaller than the actual diameter. The above formula can be found by understanding that in the case of a spherical object, a right triangle can be constructed such that its three vertices are the observer, the center of the sphere, and one of the sphere's tangent points, with as the hypotenuse and as the sine.[ citation needed ]
The difference is significant only for spherical objects of large angular diameter, since the following small-angle approximations hold for small values of : [5]
Estimates of angular diameter may be obtained by holding the hand at right angles to a fully extended arm, as shown in the figure. [6] [7] [8]
In astronomy, the sizes of celestial objects are often given in terms of their angular diameter as seen from Earth, rather than their actual sizes. Since these angular diameters are typically small, it is common to present them in arcseconds (″). An arcsecond is 1/3600th of one degree (1°) and a radian is 180/π degrees. So one radian equals 3,600 × 180/ arcseconds, which is about 206,265 arcseconds (1 rad ≈ 206,264.806247"). Therefore, the angular diameter of an object with physical diameter d at a distance D, expressed in arcseconds, is given by: [9]
These objects have an angular diameter of 1″:
Thus, the angular diameter of Earth's orbit around the Sun as viewed from a distance of 1 pc is 2″, as 1 AU is the mean radius of Earth's orbit.
The angular diameter of the Sun, from a distance of one light-year, is 0.03″, and that of Earth 0.0003″. The angular diameter 0.03″ of the Sun given above is approximately the same as that of a human body at a distance of the diameter of Earth.
This table shows the angular sizes of noteworthy celestial bodies as seen from Earth:
Celestial object | Angular diameter or size | Relative size |
---|---|---|
Magellanic Stream | over 100° | |
Gum Nebula | 36° | |
Milky Way | 30° (by 360°) | |
Width of spread out hand with arm stretched out | 20° | 353 meter at 1 km distance |
Serpens-Aquila Rift | 20° by 10° | |
Canis Major Overdensity | 12° by 12° | |
Smith's Cloud | 11° | |
Large Magellanic Cloud | 10.75° by 9.17° | Note: brightest galaxy, other than the Milky Way, in the night sky (0.9 apparent magnitude (V)) |
Barnard's loop | 10° | |
Zeta Ophiuchi Sh2-27 nebula | 10° | |
Width of fist with arm stretched out | 10° | 175 meter at 1 km distance |
Sagittarius Dwarf Spheroidal Galaxy | 7.5° by 3.6° | |
Northern Coalsack Nebula | 7° by 5° [10] | |
Coalsack nebula | 7° by 5° | |
Cygnus OB7 | 4° by 7° [11] | |
Rho Ophiuchi cloud complex | 4.5° by 6.5° | |
Hyades | 5°30′ | Note: brightest star cluster in the night sky, 0.5 apparent magnitude (V) |
Small Magellanic Cloud | 5°20′ by 3°5′ | |
Andromeda Galaxy | 3°10′ by 1° | About six times the size of the Sun or the Moon. Only the much smaller core is visible without long-exposure photography. |
Charon (from the surface of Pluto) | 3°9’ | |
Veil Nebula | 3° | |
Heart Nebula | 2.5° by 2.5° | |
Westerhout 5 | 2.3° by 1.25° | |
Sh2-54 | 2.3° | |
Carina Nebula | 2° by 2° | Note: brightest nebula in the night sky, 1.0 apparent magnitude (V) |
North America Nebula | 2° by 100′ | |
Earth in the Moon's sky | 2° - 1°48′ [12] | Appearing about three to four times larger than the Moon in Earth's sky |
The Sun in the sky of Mercury | 1.15° - 1.76° | [13] |
Orion Nebula | 1°5′ by 1° | |
Width of little finger with arm stretched out | 1° | 17.5 meter at 1 km distance |
The Sun in the sky of Venus | 0.7° | [13] [14] |
Io (as seen from the “surface” of Jupiter) | 35’ 35” | |
Moon | 34′6″ – 29′20″ | 32.5–28 times the maximum value for Venus (orange bar below) / 2046–1760″ the Moon has a diameter of 3,474 km |
Sun | 32′32″ – 31′27″ | 31–30 times the maximum value for Venus (orange bar below) / 1952–1887″ the Sun has a diameter of 1,391,400 km |
Triton (from the “surface” of Neptune) | 28’ 11” | |
Angular size of the distance between Earth and the Moon as viewed from Mars, at inferior conjunction | about 25′ | |
Ariel (from the “surface” of Uranus) | 24’ 11” | |
Ganymede (from the “surface” of Jupiter) | 18’ 6” | |
Europa (from the “surface” of Jupiter) | 17’ 51” | |
Umbriel (from the “surface” of Uranus) | 16’ 42” | |
Helix Nebula | about 16′ by 28′ | |
Jupiter if it were as close to Earth as Mars | 9.0′ – 1.2′ | |
Spire in Eagle Nebula | 4′40″ | length is 280″ |
Phobos as seen from Mars | 4.1′ | |
Venus | 1′6″ – 0′9.7″ | |
International Space Station (ISS) | 1′3″ | [15] the ISS has a width of about 108 m |
Minimum resolvable diameter by the human eye | 1′ | [16] 0.3 meter at 1 km distance [17]
|
About 100 km on the surface of the Moon | 1′ | Comparable to the size of features like large lunar craters, such as the Copernicus crater, a prominent bright spot in the eastern part of Oceanus Procellarum on the waning side, or the Tycho crater within a bright area in the south, of the lunar near side. |
Jupiter | 50.1″ – 29.8″ | |
Earth as seen from Mars | 48.2″ [13] – 6.6″ | |
Minimum resolvable gap between two lines by the human eye | 40″ | a gap of 0.026 mm as viewed from 15 cm away [16] [17] |
Mars | 25.1″ – 3.5″ | |
Apparent size of Sun, seen from 90377 Sedna at aphelion | 20.4" | |
Saturn | 20.1″ – 14.5″ | |
Mercury | 13.0″ – 4.5″ | |
Earth's Moon as seen from Mars | 13.27″ – 1.79″ | |
Uranus | 4.1″ – 3.3″ | |
Neptune | 2.4″ – 2.2″ | |
Ganymede | 1.8″ – 1.2″ | Ganymede has a diameter of 5,268 km |
An astronaut (~1.7 m) at a distance of 350 km, the average altitude of the ISS | 1″ | |
Minimum resolvable diameter by Galileo Galilei's largest 38mm refracting telescopes | ~1″ | [18] Note: 30x [19] magnification, comparable to very strong contemporary terrestrial binoculars |
Ceres | 0.84″ – 0.33″ | |
Vesta | 0.64″ – 0.20″ | |
Pluto | 0.11″ – 0.06″ | |
Eris | 0.089″ – 0.034″ | |
R Doradus | 0.062″ – 0.052″ | Note: R Doradus is thought to be the extrasolar star with the largest apparent size as viewed from Earth |
Betelgeuse | 0.060″ – 0.049″ | |
Alphard | 0.00909″ | |
Alpha Centauri A | 0.007″ | |
Canopus | 0.006″ | |
Sirius | 0.005936″ | |
Altair | 0.003″ | |
Rho Cassiopeiae | 0.0021″ [20] | |
Deneb | 0.002″ | |
Proxima Centauri | 0.001″ | |
Alnitak | 0.0005″ | |
Proxima Centauri b | 0.00008″ | |
Event horizon of black hole M87* at center of the M87 galaxy, imaged by the Event Horizon Telescope in 2019. | 0.000025″ (2.5×10−5) | Comparable to a tennis ball on the Moon |
A star like Alnitak at a distance where the Hubble Space Telescope would just be able to see it [21] | 6×10−10 arcsec |
The angular diameter of the Sun, as seen from Earth, is about 250,000 times that of Sirius. (Sirius has twice the diameter and its distance is 500,000 times as much; the Sun is 1010 times as bright, corresponding to an angular diameter ratio of 105, so Sirius is roughly 6 times as bright per unit solid angle.)
The angular diameter of the Sun is also about 250,000 times that of Alpha Centauri A (it has about the same diameter and the distance is 250,000 times as much; the Sun is 4×1010 times as bright, corresponding to an angular diameter ratio of 200,000, so Alpha Centauri A is a little brighter per unit solid angle).
The angular diameter of the Sun is about the same as that of the Moon. (The Sun's diameter is 400 times as large and its distance also; the Sun is 200,000 to 500,000 times as bright as the full Moon (figures vary), corresponding to an angular diameter ratio of 450 to 700, so a celestial body with a diameter of 2.5–4″ and the same brightness per unit solid angle would have the same brightness as the full Moon.)
Even though Pluto is physically larger than Ceres, when viewed from Earth (e.g., through the Hubble Space Telescope) Ceres has a much larger apparent size.
Angular sizes measured in degrees are useful for larger patches of sky. (For example, the three stars of the Belt cover about 4.5° of angular size.) However, much finer units are needed to measure the angular sizes of galaxies, nebulae, or other objects of the night sky.
Degrees, therefore, are subdivided as follows:
To put this in perspective, the full Moon as viewed from Earth is about 1⁄2°, or 30′ (or 1800″). The Moon's motion across the sky can be measured in angular size: approximately 15° every hour, or 15″ per second. A one-mile-long line painted on the face of the Moon would appear from Earth to be about 1″ in length.
In astronomy, it is typically difficult to directly measure the distance to an object, yet the object may have a known physical size (perhaps it is similar to a closer object with known distance) and a measurable angular diameter. In that case, the angular diameter formula can be inverted to yield the angular diameter distance to distant objects as
In non-Euclidean space, such as our expanding universe, the angular diameter distance is only one of several definitions of distance, so that there can be different "distances" to the same object. See Distance measures (cosmology).
Many deep-sky objects such as galaxies and nebulae appear non-circular and are thus typically given two measures of diameter: major axis and minor axis. For example, the Small Magellanic Cloud has a visual apparent diameter of 5° 20′ × 3° 5′.
Defect of illumination is the maximum angular width of the unilluminated part of a celestial body seen by a given observer. For example, if an object is 40″ of arc across and is 75% illuminated, the defect of illumination is 10″.
In astronomy, absolute magnitude is a measure of the luminosity of a celestial object on an inverse logarithmic astronomical magnitude scale; the more luminous an object, the lower its magnitude number. An object's absolute magnitude is defined to be equal to the apparent magnitude that the object would have if it were viewed from a distance of exactly 10 parsecs, without extinction of its light due to absorption by interstellar matter and cosmic dust. By hypothetically placing all objects at a standard reference distance from the observer, their luminosities can be directly compared among each other on a magnitude scale. For Solar System bodies that shine in reflected light, a different definition of absolute magnitude (H) is used, based on a standard reference distance of one astronomical unit.
A minute of arc, arcminute (arcmin), arc minute, or minute arc, denoted by the symbol ′, is a unit of angular measurement equal to 1/60 of one degree. Since one degree is 1/360 of a turn, or complete rotation, one arcminute is 1/21600 of a turn. The nautical mile (nmi) was originally defined as the arc length of a minute of latitude on a spherical Earth, so the actual Earth's circumference is very near 21600 nmi. A minute of arc is π/10800 of a radian.
The parsec is a unit of length used to measure the large distances to astronomical objects outside the Solar System, approximately equal to 3.26 light-years or 206,265 astronomical units (AU), i.e. 30.9 trillion kilometres. The parsec unit is obtained by the use of parallax and trigonometry, and is defined as the distance at which 1 AU subtends an angle of one arcsecond. The nearest star, Proxima Centauri, is about 1.3 parsecs from the Sun: from that distance, the gap between the Earth and the Sun spans slightly less than 1/3600 of one degree of view. Most stars visible to the naked eye are within a few hundred parsecs of the Sun, with the most distant at a few thousand parsecs, and the Andromeda Galaxy at over 700,000 parsecs.
In mathematics, a spherical coordinate system is a coordinate system for three-dimensional space where the position of a given point in space is specified by three real numbers: the radial distancer along the radial line connecting the point to the fixed point of origin; the polar angleθ between the radial line and a given polar axis; and the azimuthal angleφ as the angle of rotation of the radial line around the polar axis. (See graphic regarding the "physics convention".) Once the radius is fixed, the three coordinates (r, θ, φ), known as a 3-tuple, provide a coordinate system on a sphere, typically called the spherical polar coordinates. The plane passing through the origin and perpendicular to the polar axis (where the polar angle is a right angle) is called the reference plane (sometimes fundamental plane).
In astronomy, coordinate systems are used for specifying positions of celestial objects relative to a given reference frame, based on physical reference points available to a situated observer. Coordinate systems in astronomy can specify an object's relative position in three-dimensional space or plot merely by its direction on a celestial sphere, if the object's distance is unknown or trivial.
In geometry, a solid angle is a measure of the amount of the field of view from some particular point that a given object covers. That is, it is a measure of how large the object appears to an observer looking from that point. The point from which the object is viewed is called the apex of the solid angle, and the object is said to subtend its solid angle at that point.
Stellar parallax is the apparent shift of position (parallax) of any nearby star against the background of distant stars. By extension, it is a method for determining the distance to the star through trigonometry, the stellar parallax method. Created by the different orbital positions of Earth, the extremely small observed shift is largest at time intervals of about six months, when Earth arrives at opposite sides of the Sun in its orbit, giving a baseline distance of about two astronomical units between observations. The parallax itself is considered to be half of this maximum, about equivalent to the observational shift that would occur due to the different positions of Earth and the Sun, a baseline of one astronomical unit (AU).
Angular resolution describes the ability of any image-forming device such as an optical or radio telescope, a microscope, a camera, or an eye, to distinguish small details of an object, thereby making it a major determinant of image resolution. It is used in optics applied to light waves, in antenna theory applied to radio waves, and in acoustics applied to sound waves. The colloquial use of the term "resolution" sometimes causes confusion; when an optical system is said to have a high resolution or high angular resolution, it means that the perceived distance, or actual angular distance, between resolved neighboring objects is small. The value that quantifies this property, θ, which is given by the Rayleigh criterion, is low for a system with a high resolution. The closely related term spatial resolution refers to the precision of a measurement with respect to space, which is directly connected to angular resolution in imaging instruments. The Rayleigh criterion shows that the minimum angular spread that can be resolved by an image-forming system is limited by diffraction to the ratio of the wavelength of the waves to the aperture width. For this reason, high-resolution imaging systems such as astronomical telescopes, long distance telephoto camera lenses and radio telescopes have large apertures.
The great-circle distance, orthodromic distance, or spherical distance is the distance between two points on a sphere, measured along the great-circle arc between them. This arc is the shortest path between the two points on the surface of the sphere.
The equation of time describes the discrepancy between two kinds of solar time. The word equation is used in the medieval sense of "reconciliation of a difference". The two times that differ are the apparent solar time, which directly tracks the diurnal motion of the Sun, and mean solar time, which tracks a theoretical mean Sun with uniform motion along the celestial equator. Apparent solar time can be obtained by measurement of the current position of the Sun, as indicated by a sundial. Mean solar time, for the same place, would be the time indicated by a steady clock set so that over the year its differences from apparent solar time would have a mean of zero.
In astronomy, an extraterrestrial sky is a view of outer space from the surface of an astronomical body other than Earth.
Magnification is the process of enlarging the apparent size, not physical size, of something. This enlargement is quantified by a size ratio called optical magnification. When this number is less than one, it refers to a reduction in size, sometimes called de-magnification.
In astronomy, surface brightness (SB) quantifies the apparent brightness or flux density per unit angular area of a spatially extended object such as a galaxy or nebula, or of the night sky background. An object's surface brightness depends on its surface luminosity density, i.e., its luminosity emitted per unit surface area. In visible and infrared astronomy, surface brightness is often quoted on a magnitude scale, in magnitudes per square arcsecond (MPSAS) in a particular filter band or photometric system.
Visual angle is the angle a viewed object subtends at the eye, usually stated in degrees of arc. It also is called the object's angular size.
On Sizes and Distances (of the Sun and Moon) (Greek: Περὶ μεγεθῶν καὶ ἀποστημάτων [ἡλίου καὶ σελήνης], romanized: Peri megethon kai apostematon) is a text by the ancient Greek astronomer Hipparchus (c. 190 – c. 120 BC) in which approximations are made for the radii of the Sun and the Moon as well as their distances from the Earth. It is not extant, but some of its contents have been preserved in the works of Ptolemy and his commentator Pappus of Alexandria. Several modern historians have attempted to reconstruct the methods of Hipparchus using the available texts.
Angular distance or angular separation is the measure of the angle between the orientation of two straight lines, rays, or vectors in three-dimensional space, or the central angle subtended by the radii through two points on a sphere. When the rays are lines of sight from an observer to two points in space, it is known as the apparent distance or apparent separation.
The n-vector representation is a three-parameter non-singular representation well-suited for replacing geodetic coordinates for horizontal position representation in mathematical calculations and computer algorithms.
Geographical distance or geodetic distance is the distance measured along the surface of the Earth, or the shortest arch length.
The position of the Sun in the sky is a function of both the time and the geographic location of observation on Earth's surface. As Earth orbits the Sun over the course of a year, the Sun appears to move with respect to the fixed stars on the celestial sphere, along a circular path called the ecliptic.
Astronomical nutation is a phenomenon which causes the orientation of the axis of rotation of a spinning astronomical object to vary over time. It is caused by the gravitational forces of other nearby bodies acting upon the spinning object. Although they are caused by the same effect operating over different timescales, astronomers usually make a distinction between precession, which is a steady long-term change in the axis of rotation, and nutation, which is the combined effect of similar shorter-term variations.
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