The occurrence of this phenomenon with respect to the earth results in the Milankovitch cycles, and a (*) relativistic form of this phenomenon results from the noncommutativity of infinitesimal Lorentz transformations.
The occurrence of this phenomenon with respect to the earth results in the Milankovitch cycles, and a (*) relativistic form of this phenomenon results from the noncommutativity of infinitesimal Lorentz transformations. A more common form of this phenomenon is exploited in such techniques as NMR and has a frequency given by the product of the gyromagnetic ration and the applied magnetic field. It is the term given to the tumbling of an object about an unstable Euler axis, and when applied to a top subject to a torque, it is given by the time-dependence of one of the Euler angles. Coming in Larmor, Thomas, torque-free, and torque-induced forms, for ten points, identify this periodic motion of a rigid body, which on earth is responsible for the shift in the positions of stars over a period of 26,000 years.
The occurrence of this phenomenon with respect to the earth results in the Milankovitch cycles, and a (*) relativistic form of this phenomenon results from the noncommutativity of infinitesimal Lorentz transformations.
{precession} (accept “precession of the equinoxes” before *)