Rotation (green), precession (blue) and nutation in obliquity (red) of a planet
Nutation (from Latin nūtātiō, "nodding, swaying") is a rocking, swaying, or nodding motion in the axis of rotation of a largely axially symmetric object, such as a gyroscope, planet, or bullet in flight, or as an intended behavior of a mechanism. In an appropriate reference frame it can be defined as a change in the second Euler angle. If it is not caused by forces external to the body, it is called free nutation or Euler nutation.^{[1]} A pure nutation is a movement of a rotational axis such that the first Euler angle is constant. In spacecraft dynamics, precession (a change in the first Euler angle) is sometimes referred to as nutation.^{[2]}
Contents

Rigid body 1

Astronomy 2

Earth 3

In popular culture 4

See also 5

References 6

Further reading 7
Rigid body
If a top is set at a tilt on a horizontal surface and spun rapidly, its rotational axis starts precessing about the vertical. After a short interval, the top settles into a motion in which each point on its rotation axis follows a circular path. The vertical force of gravity produces a horizontal torque τ about the point of contact with the surface; the top rotates in the direction of this torque with an angular velocity Ω such that at any moment

\mathbf{\tau} = \mathbf{\Omega} \times \mathbf{L},
where L is the instantaneous angular momentum of the top.^{[3]}
Initially, however, there is no precession, and the top falls straight downward. This gives rise to an imbalance in torques that starts the precession. In falling, the top overshoots the level at which it would precess steadily and then oscillates about this level. This oscillation is called nutation. If the motion is damped, the oscillations will die down until the motion is a steady precession.^{[3]}^{[4]}
The physics of nutation in tops and gyroscopes can be explored using the model of a heavy symmetrical top with its tip fixed. Initially, the effect of friction is ignored. The motion of the top can be described by three Euler angles: the tilt angle θ between the symmetry axis of the top and the vertical; the azimuth φ of the top about the vertical; and the rotation angle ψ of the top about its own axis. Thus, precession is the change in φ and nutation is the change in θ.^{[5]}
If the top has mass M and its center of mass is at a distance l from the pivot point, its gravitational potential relative to the plane of the support is

V = Mgl\cos\theta.
In a coordinate system where the z axis is the axis of symmetry, the top has angular velocities ω_{1}, ω_{2}, ω_{3} and moments of inertia I_{1}, I_{2}, I_{3} about the x, y, and z axes. The kinetic energy is

T = \frac{1}{2}I_1\left(\omega_1^2+\omega_2^2\right) + \frac{1}{2}I_3\omega_3^2.
In terms of the Euler angles, this is

T = \frac{1}{2}I_1\left(\dot{\theta}^2+\dot{\phi}^2\sin^2\theta\right) + \frac{1}{2}I_3\left(\dot{\psi}+\dot{\phi}\cos\theta\right)^2.
If the Euler–Lagrange equations are solved for this system, it is found that the motion depends on two constants a and b (each related to a constant of motion). The rate of precession is related to the tilt by

\dot{\phi} = \frac{b  a\cos\theta}{\sin^2\theta}.
The tilt is determined by a differential equation for u = cos θ of the form

\dot{u}^2 = f(u)
where f is a cubic polynomial that depends on parameters a and b as well as constants that are related to the energy and the gravitational torque. The roots of f are cosines of the angles at which the rate of change of θ is zero. One of these is not related to a physical angle; the other two determine the upper and lower bounds on the tilt angle, between which the gyroscope oscillates.^{[6]}
Astronomy
The nutation of a planet happens because of gravitational attraction of other bodies that cause the precession of the equinoxes to vary over time so that the speed of precession is not constant. The nutation of the axis of the Earth was discovered in 1728 by the British astronomer James Bradley, but this nutation was not explained in detail until 20 years later.^{[7]}
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 nickeliron outer core of the Earth.
Values of nutations are usually divided into components parallel and perpendicular to the ecliptic. The component that works along the ecliptic is known as the nutation in longitude. The component perpendicular to the ecliptic is known as the nutation in obliquity. Celestial coordinate systems are based on an "equator" and "equinox", which means a great circle in the sky that is the projection of the Earth's equator outwards, and a line, the Vernal equinox intersecting that circle, which determines the starting point for measurement of right ascension. These items are affected both by precession of the equinoxes and nutation, and thus depend on the theories applied to precession and nutation, and on the date used as a reference date for the coordinate system. In simpler terms, nutation (and precession) values are important in observation from Earth for calculating the apparent positions of astronomical objects.
Earth
Nutation makes a small change to the angle at which the Earth tilts with respect to the Sun, changing the location of the major circles of latitude that are defined by the Earth's tilt (the equator, tropical circles and polar circles).
In the case of the Earth, the principal sources of tidal force are the Sun and Moon, which continuously change location relative to each other and thus cause nutation in Earth's axis. The largest component of Earth's nutation has a period of 18.6 years, the same as that of the precession of the Moon's orbital nodes.^{[1]} However, there are other significant periodical terms that must be calculated depending on the desired accuracy of the result. A mathematical description (set of equations) that represents nutation is called a "theory of nutation". In the theory, parameters are adjusted in a more or less ad hoc method to obtain the best fit to data. Simple rigid body dynamics do not give the best theory; one has to account for deformations of the Earth, including mantle inelasticity and changes in the core–mantle boundary.^{[8]}
The principal term of nutation is due to the regression of the moon's nodal line and has the same period of 6798 days (18.61 years). It reaches plus or minus 17″ in longitude and 9″ in obliquity. All other terms are much smaller; the nextlargest, with a period of 183 days (0.5 year), has amplitudes 1.3″ and 0.6″ respectively. The periods of all terms larger than 0.0001″ (about as accurately as one can measure) lie between 5.5 and 6798 days; for some reason (as with ocean tidal periods) they seem to avoid the range from 34.8 to 91 days, so it is customary to split the nutation into longperiod and shortperiod terms. The longperiod terms are calculated and mentioned in the almanacs, while the additional correction due to the shortperiod terms is usually taken from a table.
In popular culture
In the 1961 movie The Day The Earth Caught Fire, the nearsimultaneous detonation of two superhydrogen bombs near the poles causes a change in the Earth's nutation, as well as an 11 degree shift in the axis of rotation and a change in the Earth's orbit around the sun.
The verb to nutate was used by MIT physicist Peter Fisher on the television show Late Night with Conan O'Brien on February 8, 2008. Fisher used the term to describe the motion of a spinning ring as it began to slow down and wobble.
See also
References

^ ^{a} ^{b} Lowrie, William (2007). Fundamentals of geophysics (2nd ed.). Cambridge [u.a.]: Cambridge Univ. Press. pp. 58–59.

^ Kasdin, N. Jeremy; Paley, Derek A. (2010). Engineering dynamics : a comprehensive introduction. Princeton, N.J.: Princeton University Press. pp. 526–527.

^ ^{a} ^{b} Feynman, Leighton & Sands 2011, pp. 20–7

^ Goldstein 1980, p. 220

^ Goldstein 1980, p. 217

^ Goldstein 1980, pp. 213–217

^ 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.

^ "Resolution 83 on nonrigid Earth nutation theory".
Further reading

Feynman, Richard P.; Leighton, Robert B.; Sands, Matthew (2011). The Feynman lectures on physics (New millennium ed.). New York: BasicBooks.

Goldstein, Herbert (1980). Classical mechanics (2d ed.). Reading, Mass.: AddisonWesley Pub. Co.

Lambeck, Kurt (2005). The earth's variable rotation : geophysical causes and consequences (Digitally printed 1st pbk. ed.). Cambridge: Cambride University Press.

Munk, Walter H.; MacDonald, Gordon J.F. (1975). The rotation of the earth : a geophysical discussion. Reprint. with corr. Cambridge, Eng.: Cambridge University Press.
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