The Palaeozoic reversal sequence is represented by complex rhythms with characteristic times of (5-7)×10
7, (1-4)×10
7 and (1-2)×10
6y. The first order units recognized are Arginian (R) 590-535m. y., Siberian (Rn) 535-485m. y., Baikalian (Nr) 485-430m. y., Sayanian (Rn) 430-360m. y., Donetsk (Rn) 360-300m. y., Kiaman (R) 300-240m. y., and Illawarra (NR) 240-215m. y. Three types of Palaeozoic field transitions have been recognized: 1. “sudden” reversals (single or repeated), 2. reversals with a considerable dispersion of palaeomagnetic directions, 3. reversals with loop-wise rotations of the field. The latter may result from the concurrence of axial and equatorial dipoles. Reversals usually occur with a 4 to 10 times lower field intensity. The time span for the complete transition ranges from 8×10
3 to 3×10
5y. Peculiarities of the reversals have been traced over strike distances of 1600km. Angular constituents of paleosecular variation have components with characteristic times of (4-8)×10
3y. and 3×10
4y. The latter is characterized by standard deviations of 6 to 10 degrees in stable field epochs and up to 20 degrees in intervals of frequent reversals.
The field of the geocentric axial dipole is a good first approximation of time-averaged field. However, the occasional presence of an irreversible equatorial dipole, controls the shape of geomagnetic reversals of the 3rd type.
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