Propagation of gravity in the simulation is instantaneous. Anyway thank you Data for the links very interesting reading. But I think the most obvious error in most papers I read is the lack for accounting the variability of mass. Not in the sense of relativity but more like in the sense of UFT.
For the reason I'll explain I think that the companion approach is all about UFT. I was having problems with the simulation from the very beginning if you remember. The two body simulation according to Kepler's law was giving false results. If I put the companion mass to 3.4 % of the Sun and set the semimajor axis of the companion orbit to 1.7 ly then the orbital period was over 32 million years and not 28.2 as it should be. I was forced to reduce the semimajor axis to 1.5 ly which then produces the correct orbital period.
But I noticed even back then that adding 50% mass to the Sun would correct the problem.
Nevertheless yesterday I made once again the simulation of the whole orbit of the companion and included the planets to plot the trajectory. I knew that if I increase the mass of the Sun then the planets will shrink their orbits and the simulation would be messed up. So I added mass to the companion star to be precise I put the mass of the companion equal to 56 % mass of the Sun (So to say I transferred the additional mass from the Sun to the companion). And lo and behold the period was correct! Actually only half period because as soon as the companion approached the solar system it kinda ripped it apart. But the period was in perfect agreement with what the Cs said (and all other orbital parameters) and also it is in good agreement with Keplers law (thank you Saša).
If you remember the C's have given the 56 % value back in 1998 in fact it was in the same session where they mention the Libra constellation.
I thought that the 56 % value has to be wrong because as I said it would disrupt the solar system. Moreover in more recent transcript the value was 3.4 percent.
I've introduced a new "style" in this session: giving some of those present their forum names for familiarity. Session Date: January 30th 2010 Laura, Ark, Ottershrew, Joe, Andromeda, Belibaste, Nomad, Burma Jones, PoB, Alada, Ailén, Scottie, Psyche Q: (L) [Talking to others in the room with...
cassiopaea.org
But as I said the 56 % value gives proper orbital parameters. So I was thinking about this and I reread Pierre's book for inspiration and the chapter about grounding captured my attention. And a thought occured to me that what if the companion is somehow connected to the Sun. I mean by some beam or something and there is some kind of energy transfer. The Sun would increase gravity and thus inhibit more flares and the companion perhaps the opposite. So that temporarily it would lose some gravity.
If I visualize the solar system as a large capacitor then surely there has to occur something when the companion enters the heliosphere. Something similar to when one touches plasma ball and a plasma filament is created. So I was thinking that well there has to be at least some region where the current is more dense compared to ambient values. So I fired up SOTT WorldView and selected only the events which I thought were linked to electric activity. And the result is in Fig. 63. And one can clearly observe once again the seasonality. This time the peaks are during summer months.
So is it possible that if the companion is close to the plane of ecliptic and it is connected somehow to the Sun that each time the Earth crosses between the Sun and the companion all the Earth changes tied to electricity are exacerbated?