Returning to Goloka

due to the interacting gravitational fields of the planets. When a large body,
such as Nibiru and its companion dwarf star Nemesis, comes through our
solar system, it perturbs the orbits of all the planets and in turn the
gravitational fields of the planets perturb its orbit. Basically, the orbit of
Nibiru and Nemesis changes as it comes through our solar system. So at best
we can calculate probabilities of where they will be at what time. The start of
the flyby events has already started, with increased volcanic and earthquake
activity since 2013 and more X-class solar flares as well. The more serious
events are yet to come and will commence approximately 3 months after
Nibiru is clearly visible in the
sky, next to the Sun, every day
by anyone on the planet. Due to
the Kozai mechanism, we
cannot know with certainty
when to expect the full visibility
of Nibiru.
momentum. This conserved quantity can be expressed in terms of the satellite's
eccentricity e and inclination i relative to the plane of the outer binary:
Conservation of Lz means that orbital eccentricity can be "traded for" inclination. Thus,
near-circular, highly inclined orbits can become very eccentric. Since increasing
eccentricity while keeping the semimajor axis constant reduces the distance between
the objects at periapsis, this mechanism can cause comets (perturbed by Jupiter) to
become sungrazing.
Kozai oscillations will be present if Lz is lower than a certain value. At the critical
value of Lz, a "fixed-point" orbit appears, with constant inclination given by
For values of Lz less than this critical value, there is a one-parameter family of orbital
solutions having the same Lz but different amounts of variation in e or i. Remarkably, the
degree of possible variation in i is independent of the masses involved, which only set
the timescale of the oscillations.
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