Angular diameter




The angular diameter, angular size, apparent diameter, or apparent size is an angular measurement 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 angle through which an eye or camera must rotate to look from one side of an apparent circle to the opposite side. Angular radius equals half the angular diameter.




Contents






  • 1 Formula


  • 2 Estimating angular diameter using the hand


  • 3 Use in astronomy


    • 3.1 Non-circular objects


    • 3.2 Defect of illumination




  • 4 See also


  • 5 References


  • 6 External links





Formula




Diagram for the formula of the angular diameter


The angular diameter of a circle whose plane is perpendicular to the displacement vector between the point of view and the centre of said circle can be calculated using the formula[1]


δ=2arctan⁡(d2D),{displaystyle delta =2arctan left({frac {d}{2D}}right),}delta =2arctan left({frac {d}{2D}}right),

in which δ{displaystyle delta }delta is the angular diameter, and d{displaystyle d}d and D{displaystyle D}D are the actual diameter of and the distance to the object. When D≫d{displaystyle Dgg d}Dgg d, we have δd/D{displaystyle delta approx d/D}delta approx d/D, and the result obtained is in radians.


For a spherical object whose actual diameter equals dact,{displaystyle d_{mathrm {act} },}d_{mathrm {act} }, and where D{displaystyle D}D is the distance to the centre of the sphere, the angular diameter can be found by the formula


δ=2arcsin⁡(dact2D){displaystyle delta =2arcsin left({frac {d_{mathrm {act} }}{2D}}right)}delta =2arcsin left({frac {d_{mathrm {act} }}{2D}}right)

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 centre of the sphere. For practical use, the distinction is only significant for spherical objects that are relatively close, since the small-angle approximation holds for x≪1{displaystyle xll 1}xll 1:[2]



arcsin⁡x≈arctan⁡x≈x{displaystyle arcsin xapprox arctan xapprox x}arcsin xapprox arctan xapprox x .


Estimating angular diameter using the hand




Approximate angles of 10°, 20°, 5°, and 1° for the hand outstretched arm's length.


Estimates of angular diameter may be obtained by holding the hand at right angles to a fully extended arm, as shown in the figure.[3][4][5]



Use in astronomy




Angular diameter: the angle subtended by an object


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{displaystyle pi }pi degrees, so one radian equals 3,600*180/π{displaystyle pi }pi arcseconds, which is about 206,265 arcseconds. Therefore, the angular diameter of an object with physical diameter d at a distance D, expressed in arcseconds, is given by:[6]



δ{displaystyle delta }delta = (206,265) d / D arcseconds.

These objects have an angular diameter of 1″:



  • an object of diameter 1 cm at a distance of 2.06 km

  • an object of diameter 725.27 km at a distance of 1 astronomical unit (AU)

  • an object of diameter 45 866 916 km at 1 light-year

  • an object of diameter 1 AU (149 597 871 km) at a distance of 1 parsec (pc)


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 person at a distance of the diameter of Earth.[7]


This table shows the angular sizes of noteworthy celestial bodies as seen from Earth:















































































































































Celestial body
Angular diameter or size
Relative size

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.

Sun
31′27″ – 32′32″
30–31 times the maximum value for Venus (orange bar below) / 1887–1952″

Moon
29′20″ – 34′6″
28–32.5 times the maximum value for Venus (orange bar below) / 1760–2046″

Helix Nebula
about 16′ by 28′

Spire in Eagle Nebula
4′40″
length is 280″

Venus
9.7″ – 1′6″






Jupiter
29.8″ – 50.1″






Saturn
14.5″ – 20.1″






Mars
3.5″ – 25.1″






Mercury
4.5″ – 13.0″






Uranus
3.3″ – 4.1″






Neptune
2.2″ – 2.4″






Ceres
0.33″ – 0.84″






Vesta
0.20″ – 0.64″






Pluto
0.06″ – 0.11″






R Doradus
0.052″ – 0.062″






Betelgeuse
0.049″ – 0.060″






Eris
0.034″ – 0.089″






Alphard
0.00909″


Alpha Centauri A
0.007″


Canopus
0.006″


Sirius
0.005936″


Altair
0.003″


Deneb
0.002″


Proxima Centauri
0.001″


Alnitak
0.0005″

A star like Alnitak at a distance where the Hubble Space Telescope would just be able to see it[8]

6990600000000000000♠6×10−10 arcsec




Comparison of angular diameter of the Sun, Moon and planets. To get a true representation of the sizes, view the image at a distance of 103 times the width of the "Moon: max." circle. For example, if this circle is 5 cm wide on your monitor, view it from 5.15 m away.




This photo compares the apparent sizes of Jupiter and its four Galilean moons (Callisto at maximum elongation) with the apparent diameter of the full Moon during their conjunction on 10 April 2017.


The table shows that the angular diameter of Sun, when seen from Earth is approximately 32′ (1920″ or 0.53°), as illustrated above.


Thus the angular diameter of the Sun 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:



  • 360 degrees (°) in a full circle

  • 60 arc-minutes (′) in one degree

  • 60 arc-seconds (″) in one arc-minute


To put this in perspective, the full Moon as viewed from Earth is about ​12°, 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



d≡2Dtan⁡2){displaystyle dequiv 2Dtan left({frac {delta }{2}}right)}dequiv 2Dtan left({frac {delta }{2}}right).

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).



Non-circular objects


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


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″.



See also



  • Angular diameter distance

  • Angular resolution

  • Solid angle

  • Visual acuity

  • Visual angle

  • Visual Angle Illusion

  • List of stars with resolved images



References





  1. ^ This can be derived using the formula for the length of a cord found at "Archived copy". Archived from the original on 2014-12-21. Retrieved 2015-01-23.CS1 maint: Archived copy as title (link).mw-parser-output cite.citation{font-style:inherit}.mw-parser-output .citation q{quotes:"""""""'""'"}.mw-parser-output .citation .cs1-lock-free a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/6/65/Lock-green.svg/9px-Lock-green.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .citation .cs1-lock-limited a,.mw-parser-output .citation .cs1-lock-registration a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/d/d6/Lock-gray-alt-2.svg/9px-Lock-gray-alt-2.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .citation .cs1-lock-subscription a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/a/aa/Lock-red-alt-2.svg/9px-Lock-red-alt-2.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .cs1-subscription,.mw-parser-output .cs1-registration{color:#555}.mw-parser-output .cs1-subscription span,.mw-parser-output .cs1-registration span{border-bottom:1px dotted;cursor:help}.mw-parser-output .cs1-ws-icon a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/4/4c/Wikisource-logo.svg/12px-Wikisource-logo.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output code.cs1-code{color:inherit;background:inherit;border:inherit;padding:inherit}.mw-parser-output .cs1-hidden-error{display:none;font-size:100%}.mw-parser-output .cs1-visible-error{font-size:100%}.mw-parser-output .cs1-maint{display:none;color:#33aa33;margin-left:0.3em}.mw-parser-output .cs1-subscription,.mw-parser-output .cs1-registration,.mw-parser-output .cs1-format{font-size:95%}.mw-parser-output .cs1-kern-left,.mw-parser-output .cs1-kern-wl-left{padding-left:0.2em}.mw-parser-output .cs1-kern-right,.mw-parser-output .cs1-kern-wl-right{padding-right:0.2em}


  2. ^ "Archived copy" (PDF). Archived (PDF) from the original on 2015-02-18. Retrieved 2015-01-23.CS1 maint: Archived copy as title (link)


  3. ^ "Archived copy". Archived from the original on 2015-01-21. Retrieved 2015-01-21.CS1 maint: Archived copy as title (link)


  4. ^ "Photographing Satellites". 8 June 2013. Archived from the original on 21 January 2015.


  5. ^ Wikiversity: Physics and Astronomy Labs/Angular size


  6. ^ Michael A. Seeds; Dana E. Backman (2010). Stars and Galaxies (7 ed.). Brooks Cole. p. 39. ISBN 978-0-538-73317-5.


  7. ^ http://www.google.com/search?hl=en&hs=3cj&q=arctan%286ft+%2F+12756.3+Km%29+in+arcseconds&btnG=Search


  8. ^ 800 000 times smaller angular diameter than that of Alnitak as seen from Earth. Alnitak is a blue star so it gives off a lot of light for its size. If it were 800 000 times further away then it would be magnitude 31.5, at the limit of what Hubble can see.




External links



  • Small-Angle Formula

  • Visual Aid to the Apparent Size of the Planets




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