I totally agree that outside influences need to be taken into account. Of course, the first thing to consider is the effect of the Moon's rotation around the Earth, since it is absolutely the most powerful "outside influence" (at least when it comes to gravity). And indeed, the Earth's surface~ionosphere potential varies with the lunar cycle in a way that is predictable by the charged double-layer model. If pressure causes the core to become positively charged, and for the excess electrons to congregate nearer the surface, then at high tide, the pull of the Moon's gravity should relax the pressure, meaning less charge separation on that side of the Earth, with the measurable effect at the surface being fewer excess electrons (i.e., less net negative charge). And this is precisely what happens.
Earthquakes are also more likely to occur at high tide. This destroys the standard model, which maintains that quakes are partially the release of gravitational potential in a buckled crust -- yet the Moon's gravity at high tide
reduces the gravitational potential, meaning that quakes should wait for low tide. But if quakes are the release of electrostatic potential, this makes perfect sense. The buckled crust reduces the pressure on the charged double-layers, enabling charge recombination (i.e., the flow of an electric current). We can measure the changes in E-fields before and during a quake,
and the magnetic field generated by the current. And when the Moon accentuates the buckle by giving an extra gravitational tug, the current is more forceful. Then a force feedback loop kicks in, resulting in a runaway release of energy. The more the crust buckles, the more the charge recombination. The more the electric current, the more the ohmic heating. Expansion of the crust due to ohmic heating then increases the buckle, which closes the loop, and ba-boom -- the energy gets released catastrophically.
celeste wrote:So what do you figure is the gravitational field we need?
I think that the threshold for pressure-driven charge separation is a lot less than anybody else realizes. In the Earth, the lithosphere is rigid, but the asthenosphere (and everything below) is plastic, and "flows" like a liquid. This is "explained" as the rock being under such enormous pressure that a little bit of elasticity graduates to full-blown plasticity. But the elasticity of rock comes from the properties of its crystal lattice, which
shouldn't change under pressure. In the lab, rock under high pressure simply fractures, and additional stresses result in pulverization, not plasticity. So I'm thinking that under really severe pressure, electrons are expelled. The loss of the valence band weakens the lattice, enabling plasticity in a crystal that otherwise wouldn't allow it. So the threshold for charged double-layers is the lithosphere~asthenosphere boundary (> 80 km below the surface).
The implication is that much smaller celestial objects still have charged double-layers, if their gravities generate the same pressure that we get 80 km below the surface. But this doesn't mean that all of them will have magnetic fields. With charged double-layers rotating, one charge generates one magnetic field, and the other charge generates an opposing field. If both layers are rotating at the same rate, those fields just might cancel each other out. So only with differential rotation are we going to see a net magnetic field, and only with oscillations in the differential rotation will we see the polarity of the net field flip. So Ganymede has a magnetic field, but Venus (with twice the radius) does not, when by the standard model it definitely should. I'm thinking that Venus has charged double-layers same as the Earth and Ganymede, but it doesn't have differential rotation, so it doesn't generate a net magnetic field. But the evidence of Venus' electrostatic potentials is obvious. First, there are continuous electrical storms in its atmosphere. Second, if it were not for electrostatics, Venus wouldn't even
have an atmosphere. It doesn't have a magnetosphere to shield it from the solar wind, so by the standard model, its atmosphere should have been swept clean off the planet a long time ago, especially considering the fact that it's closer to the Sun, and the solar wind is more forceful. Yet Venus, which is slightly lighter than Earth, has a thicker atmosphere. Only if Venus' surface has a net charge that attracts the atmosphere will it not get whisked away by the solar wind.
Hence the charged double-layer model seems to handle every challenge thrown at it, including the Sun, the Earth, Venus, Ganymede, ...
As concerns the periodicity of the solar barycenter, here some benchmark papers. I'm still studying this, but the coincidence of the degree of curvature in the Sun's movement and the sunspot cycles is pretty unmistakeable. So I'm thinking that while the energy variations in sunspot cycle are a lot greater than the force of the planets, and therefore the planets are not causing the cycle, the planets might nevertheless regulate the cycle, forcing it to fall into a regular 22 year pattern. This makes sense of the fact that the degree of curvature peaks every 22 years, but the sunspots peak every 11 years. So the idea is that the sunspots would have peaked in roughly that period, but with a little tug from the planets every 22 years, every other sunspot cycle gets enhanced, and this is enough to synchronize the two cycles.
Jose, P. D., 1965: Sun's Motion and Sunspots. The Astronomical Journal, 70 (3): 193-200
Landscheidt, T., 1999: Extrema in Sunspot Cycle Linked to Sun's Motion. Solar Physics, 189 (2): 413-424
Wilson, I. R.; Carter, B. D.; Waite, I. A., 2008: Does a Spin–Orbit Coupling Between the Sun and the Jovian Planets Govern the Solar Cycle? Publications of the Astronomical Society of Australia, 25 (2): 85-93