The highest density emission is equatorially, but the planets emit all around. It's not an all or nothing game; the density changes as you move latitudinally. Miles has recently shown that the polar aurorae are are big clue to where the 'cross-over' point is between net out and net in. (See the paper here: http://milesmathis.com/aurora.pdf).

 

I'm not sure how to calculate the tilt in an assumed Saturnian system. Miles does it in his paper on Bode by using relative numbers and not absolute and because he has the sun as a baseline. I think it would depend a lot upon which bodies were considered primary. If Saturn is the baseline away from the sun, each new body would have to adjust and settle into a stable orbit as it encountered the other body's charge fields. Even with relative numbers, I would think it would possible to write a program that could set the bodies all up on a single axis and move them around until a relative stability is achieved. The complexity increases as you add more and more bodies however. And I don't think I have the skill to do it (yet).

 

Miles' Heat paper (http://milesmathis.com/core.pdf) goes some way toward calculating the emission of the earth but I'm not sure it gives absolute or complete numbers, but it seems to be a start. Due to the small size of the charge photons, I wouldn't expect to see any holes necessarily in the atmosphere. Any gas is going to be largely immune to such effects I would think since it is obviously very fluid and can fill any gaps quickly. The ionosphere is another question and may relate to the aurora paper above. But Miles has stated that the charge field is interpenetrable to a large degree. He does however argue that the unexpected negative tide on the moon's earth-facing side is strong evidence for a bombarding field from the earth.

 

It may be that ions cool the poles; but that only begs the question of what is driving the ions to the poles? Either way you arrive back at the incoming polar charge field that carried the ions along. If ions are moving, they need a potential to drive them; the charge field creates that potential. The ions are riding in the river of the photons.