Parallactic angle

In spherical astronomy, the parallactic angle is the angle between the great circle through a celestial object and the zenith, and the hour circle of the object.[1] It is usually denoted q. In the triangle zenith—object—celestial pole, the parallactic angle will be the position angle of the zenith at the celestial object. Despite its name, this angle is unrelated with parallax. The parallactic angle is zero or 180° when the object crosses the meridian.

Uses

For ground-based observatories, the Earth atmosphere acts like a prism which disperses light of different wavelengths such that a star generates a rainbow along the direction that points to the zenith. So given an astronomical picture with a coordinate system with a known direction to the North Celestial Pole, the parallactic angle represents the direction of that prismatic effect relative to that reference direction.

Depending on the type of mount of the telescope, this angle may also affect the orientation of the celestial object's disk as seen in a telescope. With an equatorial mount, the cardinal points of the celestial object's disk are aligned with the vertical and horizontal direction of the view in the telescope. With an altazimuth mount, those directions are rotated by the amount of the parallactic angle.[2] The cardinal points referred to here are the points on the limb located such that a line from the center of the disk through them will point to one of the celestial poles or 90° away from them; these are not the cardinal points defined by the object's axis of rotation.

The orientation of the disk of the Moon, as related to the horizon, changes throughout its diurnal motion and the parallactic angle changes equivalently.[3] This is also the case with other celestial objects.

In an ephemeris, the position angle of the midpoint of the bright limb of the Moon or planets, and the position angles of their North poles may be tabulated. If this angle is measured from the North point on the limb, it can be converted to an angle measured from the zenith point (the vertex) as seen by an observer by subtracting the parallactic angle.[3] The position angle of the bright limb is directly related to that of the subsolar point.

Derivation

The vector algebra to derive the standard formula is equivalent to the calculation of the long derivation for the compass course. The sign of the angle is basically kept, north over east in both cases, but as astronomers look at stars from the inside of the celestial sphere, the definition uses the convention that the q is the angle in an image that turns the direction to the NCP counterclockwise into the direction of the zenith.

In the equatorial system of right ascension α and declination δ the star is at

${\displaystyle \mathbf {s} =\left({\begin{array}{c}\cos \delta \cos \alpha \\\cos \delta \sin \alpha \\\sin \delta \end{array}}\right).}$

In the same coordinate system the zenith is found by inserting a=π/2, cos a=0 into the transformation formulas

${\displaystyle \mathbf {z} =\left({\begin{array}{c}\cos \varphi \cos l\\\cos \varphi \sin l\\\sin \varphi \end{array}}\right),}$

where φ is the observer's geographic latitude, a the star's altitude, z=π/2-a the zenith distance, and l the local sidereal time. The North Celestial Pole is at

${\displaystyle \mathbf {N} =\left({\begin{array}{c}0\\0\\1\end{array}}\right).}$

The normalized cross product is the rotation axis that turns the star into the direction of the zenith:

${\displaystyle \mathbf {\omega } _{z}={\frac {1}{\sin z}}\mathbf {s} \times \mathbf {z} ={\frac {1}{\sin z}}\left({\begin{array}{c}\cos \delta \sin \alpha \sin \varphi -\sin \delta \cos \varphi \sin l\\-\cos \delta \cos \alpha \sin \varphi +\sin \delta \cos \varphi \cos l\\\cos \delta \cos \varphi \sin(\alpha -l)\end{array}}\right).}$

Finally ω_z X s is the third axis of the tilted coordinate system and the direction into which the star is moved on the great circle towards the zenith.

The plane tangential to the celestial sphere at the star is spanned by the unit vectors to the north,

${\displaystyle \mathbf {u} _{\delta }=\left({\begin{array}{c}-\sin \delta \cos \alpha \\-\sin \delta \sin \alpha \\\cos \delta \end{array}}\right),}$

and to the east

${\displaystyle \mathbf {u} _{\alpha }=\left({\begin{array}{c}-\sin \alpha \\\cos \alpha \\0\end{array}}\right).}$

These are orthogonal:

${\displaystyle \mathbf {u} _{\delta }\cdot \mathbf {u} _{\alpha }=0;\quad \mathbf {u} _{\delta }^{2}=\mathbf {u} _{\alpha }^{2}=1.}$

The parallactic angle q is the angle of the initial section of the great circle at s, east of north,[4]

${\displaystyle \omega _{z}\times \mathbf {s} =\cos q\,\mathbf {u} _{\delta }+\sin q\,\mathbf {u} _{\alpha }.}$

${\displaystyle \cos q=(\omega _{z}\times \mathbf {s} )\cdot \mathbf {u} _{\delta }={\frac {1}{\sin z}}(\cos \delta \sin \varphi -\sin \delta \cos \varphi \cos h),}$

${\displaystyle \sin q=(\omega _{z}\times \mathbf {s} )\cdot \mathbf {u} _{\alpha }={\frac {1}{\sin z}}\sin h\cos \varphi .}$

(The previous formula is the sine formula of spherical trigonometry.[5]) The values of sin z and of cos φ are positive, so using atan2 functions one may divide both expressions through these without losing signs; eventually

${\displaystyle \tan q={\frac {\sin h\cos \varphi }{\cos \delta \sin \varphi -\sin \delta \cos \varphi \cos h}}={\frac {\sin h}{\cos \delta \tan \varphi -\sin \delta \cos h}}}$

yields the angle in the full range -π ≤ q ≤ π. The advantage of this expression is that it does not depend on the various offset conventions of A; the uncontroversial offset of the hour angle h takes care of this.

For a sidereal target, by definition a target where δ and α are not time-dependent, the angle changes with a period of a sidereal day T_s. Let dots denote time derivatives; then the hour angle changes as[6]

${\displaystyle {\dot {h}}={\frac {2\pi }{T_{s}}}}$

and the time derivative of the tan q expression is

${\displaystyle {\dot {q}}{\frac {1}{\cos ^{2}q}}={\frac {\cos \varphi [\cos h\cos \delta \sin \varphi -\sin \delta \cos \varphi ]}{(\cos \delta \sin \varphi -\sin \delta \cos \varphi \cos h)^{2}}}{\dot {h}};}$

${\displaystyle {\dot {q}}={\frac {\cos \varphi [\cos h\cos \delta \sin \varphi -\sin \delta \cos \varphi ]}{\sin ^{2}z}}{\dot {h}}={\frac {\cos \varphi \cos a\cos A}{\sin ^{2}z}}{\dot {h}}={\frac {\cos \varphi \cos A}{\sin z}}{\dot {h}}.}$

See also

• Libration
• Equatorial mount
• Altazimuth mount

Further reading

• Taff, Laurence G. (1981). Computational spherical astronomy. Wiley. Bibcode:1981csa..book.....T. ISBN 0471-873179.
• Karttunen, Hannu; Kröger, Pekka; Oja, Heikki; Poutanen, Markku; Donner, Karl Johan, eds. (1987). Fundamental Astronomy. Springer. Bibcode:2003fuas.book.....K. ISBN 0-387-17264-5.

References

1. "AIPS++ Glossary". Associated Universities Inc., Washington, D.C. Retrieved 21 December 2009.
2. Meadows, Peter. "Solar Observing: Parallactic Angle". Retrieved 15 December 2009.
3. Meeus, Jean (1998). Astronomical Algorithms (Second ed.).
4. Newcomb, Simon (1906). A compendium of spherical astronomy. Dover Publications. p. 133. Bibcode:1960csaw.book.....N.
5. Abramowitz, Milton; Stegun, Irene Ann, eds. (1983) [June 1964]. "Chapter 4.3.149". Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables. Applied Mathematics Series. 55 (Ninth reprint with additional corrections of tenth original printing with corrections (December 1972); first ed.). Washington D.C.; New York: United States Department of Commerce, National Bureau of Standards; Dover Publications. ISBN 978-0-486-61272-0. LCCN 64-60036. MR 0167642. LCCN 65-12253.
6. Avila, G.; Wirenstrand, K. (1991). Field and Pupil Rotations for the VLT 8m Unit Telescopes (PDF). ESO.