A particle path formula has been derived for charged particles spiralling in extended magnetic and gravity fields, In part I (Book 1, 3CS 1), a stationary dipole- like magnetic field has been considered in which particles of the highest energies slowly but continuousely diffuse up and fill the tops of very extended field
lineš, while underescape charged paťticles diffuse down and separate from its top-trapped highTenergy part, Below an impact which squeezes the magnetic tubes the field strength H decreases less thon before or even grows with altitude r, in this region.
Consequently the pitch angle of all down spiralling particles increases less now and vice versa; The plasma shifts down, it streams down even without having gained any energy surplus, The bottom of the Van Allen belt shifts down there and rises os Soon
as the impact has ceased, This explains the oocurrence and disappearence of aurorae, When the H(r)-variation changes so that H=const is passed, without gravity the mag¬ netic mirror would immediately switch from the bottom on the top, In the gravity
field first a "hole effect" gradually reverses the path - between H=const and r“^’ Phenomena occurring now apparently violate some basic physical laws.