Astronomical nutation

For more details on the general phenomenon in physics, see Nutation.

In astronomy, 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 essentially 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.^[1]

An example of precession and nutation is the variation over time of the orientation of the axis of rotation of the Earth. This is important because the most commonly used frame of reference for measurement of the positions of astronomical objects is the Earth's equator — the so-called equatorial coordinate system. The effect of precession and nutation causes this frame of reference itself to change over time, relative to an arbitrary fixed frame.

Nutation is one of the corrections which must be applied to obtain the apparent place of an astronomical object. When calculating the position of an object, it is initially expressed relative to the mean equinox and equator — defined by the orientation of the Earth's axis at a specified date, taking into account the long-term effect of precession, but not the shorter-term effects of nutation. It is then necessary to apply a further correction to take into account the effect of nutation, after which the position relative to the true equinox and equator is obtained.

Because the dynamic motions of the planets are so well known, their nutations can be calculated to within arcseconds over periods of many decades. There is another disturbance of the Earth's rotation called polar motion that can be estimated for only a few months into the future because it is influenced by rapidly and unpredictably varying things such as ocean currents, wind systems, and hypothesised motions in the liquid nickel-iron outer core of the Earth.

Nutation of the Earth's axis

Causes

Precession and nutation are caused principally by the gravitational forces of the Moon and Sun acting upon the non-spherical figure of the Earth. Precession can be thought of as the effect of these forces when averaged over a very long period of time, and has a timescale of about 26,000 years. Nutation occurs because the forces are not constant, and vary as the Earth revolves around the Sun, and the Moon revolves around the Earth.

The largest term in nutation is caused by the fact that the orbit of the Moon around the Earth is inclined at slightly over 5° to the plane of the ecliptic, and the orientation of this orbital plane varies over a period of about 18.6 years. Because the Earth's equator is itself inclined at an angle of about 23.5° to the ecliptic (the obliquity of the ecliptic, $\epsilon$ ), these effects combine to mean that the inclination of the Moon's orbit to the equator varies between about 18.4° and 28.6° over the 18.6 year period. This causes the orientation of the Earth's axis to vary over the same period, with the true position of the celestial poles describing a small ellipse around their mean position. The maximum radius of this ellipse is approximately 9.2 arcseconds, a figure which is known as the constant of nutation.

Smaller terms in nutation must also be added to this principal term. These are caused by the monthly motion of the Moon around the Earth and the fact that its orbit is eccentric, and similar terms caused by the annual motion of the Earth around the Sun.

Effect on position of astronomical objects

Because nutation causes a change to the frame of reference, rather than a change in position of an observed object itself, it applies equally to all objects. Its magnitude at any point in time is usually expressed in terms of ecliptic coordinates, as nutation in longitude ( $\Delta \psi$ ) and nutation in obliquity ( $\Delta\epsilon$ ). The largest term in nutation is expressed numerically (in arcseconds) as follows:

\Delta \psi =-17.2\sin \Omega

\Delta \epsilon =9.2\cos \Omega

where $\Omega$ is the ecliptic longitude of the ascending node of the Moon's orbit.

Spherical trigonometry can then be used on any given object to convert these quantities into an adjustment in the object's right ascension and declination. For objects that are not close to a celestial pole, nutation in right ascension ( $\Delta \alpha$ ) and declination ( $\Delta \delta$ ) can be calculated approximately as follows:^[2]

\Delta \alpha =(\cos \epsilon +\sin \epsilon \sin \alpha \tan \delta )\Delta \psi -\cos \alpha \tan \delta \Delta \epsilon

\Delta \delta =\cos \alpha \sin \epsilon \Delta \psi +\sin \alpha \Delta \epsilon

History

Nutation was discovered by James Bradley from a series of observations of stars conducted between 1727 and 1747. These observations were originally intended to demonstrate conclusively the existence of the annual aberration of light, a phenomenon that Bradley had unexpectedly discovered in 1725-6. However, there were some residual discrepancies in the stars' positions that were not explained by aberration, and Bradley suspected that they were caused by nutation taking place over the 18.6 year period of the revolution of the nodes of the Moon's orbit. This was confirmed by his 20-year series of observations, in which he discovered that the celestial pole moved in a slightly flattened ellipse of 18 by 16 arcseconds about its mean position.^[3]

Although Bradley's observations proved the existence of nutation and he intuitively understood that it was caused by the action of the Moon on the rotating Earth, it was left to later mathematicians, d'Alembert and Euler, to develop a more detailed theoretical explanation of the phenomenon.^[4]

References

↑ Seidelmann, P. Kenneth, ed. (1992). Explanatory Supplement to the Astronomical Almanac. University Science Books. pp. 99–120. ISBN 0-935702-68-7.
↑ Newcomb, Simon (1906). A Compendium of Spherical Astronomy. Macmillan. pp. 289–292.
↑ Berry, Arthur (1898). A Short History of Astronomy. John Murray. pp. 265–269.
↑ Robert E. Bradley. "The Nodding Sphere and the Bird's Beak: D'Alembert's Dispute with Euler". The MAA Mathematical Sciences Digital Library. Mathematical Association of America. Retrieved 21 April 2014.

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