Defintion  "Looking Inward to a cfp" / "Looking Outward to a pvs" Looking "inward":
> #2  "The Flow of Observers Postulate"
When one is at rest with pvs everything is Galilean.
There does not exist any masses/particles/forces/etc in pvs, but
nonetheless, the laws of physics in that space is Galilean and all
Lorentz factors are equivalent to one. Thus, without morph effects
everything becomes Galielan. When one introduces "stuff",
masses/particles/forces/etc, then the space becomes Einsteinian. Remarks
The ameasured and aderived quantities can and do differ depending on whether one is using outward equations or inward equations. If a quantity is ameasured and aderived to be the same in all outward and inward equations, then we say the quantity is wayward. Note that one can never observe an external outsider! Rather, one must become an external outsider and look inward towards others. Also notice that both escape Lorentz velocities v_{e} and captured Lorentz velocities v_{c} are all inward bound. Thus, any equation that has a Lorentz factor must also be inward bound. Examples >(1) (+) _{d}F_{P} = _{m}m*a_{}>(2) (±) v = a*t >(3) () _{d}F = _{d}m*a
