Problems regarding Saturn’s rings | Saturn’s ring problems explained through superconducting effects |
1) Anomalous purity of water ice (99.9 %) | Superconductivity of ice in Saturn’s rings [13] , Meissner-Ochsenfeld effect [14] |
2) The existence of a temperature boundary beyond the asteroid belt, where the planets may have rings | Superconducting transition temperature (Tc) |
3) Great flattening of the rings system. Sharp edges and rings discontinuities. Arcs | The phenomenon of expulsion of the superconductors out of the areas with greater density of magnetic flow [15] |
4) Fine periodical structure of the Saturn’s rings, density waves | The phenomenon of the formation of a periodic structure in a super-diamagnetic liquid film under the influence of normally oriented magnetic field |
5) “Ring rain” of the submicron particles | Disappearance of the super-diamagnetic properties of superconducting particles at a greater depth than London’s penetration depth of the magnetic field (50 - 500 nm) |
6) Forming and development of the “spokes” of Saturn’s B ring | Loss of superconductivity due to the critical magnetic field Hc |
7) High reflection and low brightness of the ring particles in the radiofrequency range | Critical frequency for the superconductor, above which electromagnetic waves are absorbed, and below which they are completely reflected (1011 Hz) |
8) The wide band pulse radiation of the rings (20 kHz - 40.2 MHz) | Non-stationary Josephson phenomenon: generation of electromagnetic waves by Josephson’s weak links with the parameter 4.83594 × 1014 Hz/V [16] |
9) Existence of Kilometric radiation of the Saturn rings (ν < 1.2 MHz) | The electric field appears due to the movement of the superconducting fluid within the magnetic field |
10) Color differentiation of Saturn’s rings in a small scale | Dependence of the force of magnetic levitation from the volume of superconducting phase in the bulk matter (observed in experiment) |
11) Phenomenon of anomalous inversion of reflection of the radio waves with the circular polarization (λ ≥ 1 cm) | Positive charge of the superconducting carriers (protons) [17] |
12) Possible distribution of particles by size in Saturn’s rings in the radial direction | Dependence of magnetic separation of the superconducting particles by size, and also, strength, extension, and the range of the applied magnetic field [18] |
13) The existence of an atmosphere of molecular oxygen around the rings of Saturn | Magnetic levitation of gas molecules due to diamagnetic expulsion forces induced in superconducting particles by molecular magnetic moments (observed in experiment). Flux pinning [19] |
14) Saturn’s magnetic field alignment with the planet’s rotation axis (<0.06˚) | London moment [20] |
15) Increasing the purity of the ice in the radial direction from Saturn | The dependence of the force of expulsion of a superconductor from a magnetic field on the volume of the super conducting phase (observed in experiment) |
16) “Dirt” concentrated in the ring’s gaps | The phenomenon of expulsion of the superconductors out of the areas with greater density of magnetic flow |
17) Deviation in the qualitative composition of the “rain” from the composition of the rings [21] | London’s penetration depth , flux pinning, super-diamagnetic expulsion |
18) “Plateaus” in Saturn’s C ring | Tao effect: Electric-field induced formation of superconducting granular balls [22] |
19) Age of the rings | London moment, super-diamagnetic expulsion, flux pinning |
20) Roll-off in the spectrum (100 μm - 0.5 mm) [23] [24] | Superconducting energy gap (10−4 eV - 10−3 eV) |
21) “Propellers” in Saturn’s A ring [25] | Gyromagnetic effect [26] , London moment, super-diamagnetic expulsion |
22) Origin, dynamics and evolution of the rings | All phenomena above |