Simon Bridge
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Those aren't references supporting what you say - they are just references to you saying it...
The PE calc looks like the difference between gravitational PE and Centrifugal effect.
If you just fired something straight up, in a rotating reference frame, it does not go straight. Put it on a radial track, though, and push it straight up, then the rotation gives you some help ... though you lose energy from the thing rotating. Now your rotating reference frame no longer has a constant angular speed wrt an inertial frame - did you take this into account?
The further you run the mass up the track, the more energy you draw off from the rotation. This is the same effect as an ice-skater pushing their arms out to slow their spin. At some stage, you'll slow to a stop.
At the end of the track, above geostationary, the mass seems to accelerate madly away for a bit - but isn't that just a classical relativity effect? The mass just heads off at a constant velocity in the inertial frame.
There is a common mistake people make when they consider rotational gravity - they may have someone start out in the "low g" section of a cylindrical habitat moving slowly radially and then figure that since gravity depends on the distance from the center, that the person experiences an increasing gravitational pull as they move outwards.
The PE calc looks like the difference between gravitational PE and Centrifugal effect.
If you just fired something straight up, in a rotating reference frame, it does not go straight. Put it on a radial track, though, and push it straight up, then the rotation gives you some help ... though you lose energy from the thing rotating. Now your rotating reference frame no longer has a constant angular speed wrt an inertial frame - did you take this into account?
The further you run the mass up the track, the more energy you draw off from the rotation. This is the same effect as an ice-skater pushing their arms out to slow their spin. At some stage, you'll slow to a stop.
At the end of the track, above geostationary, the mass seems to accelerate madly away for a bit - but isn't that just a classical relativity effect? The mass just heads off at a constant velocity in the inertial frame.
There is a common mistake people make when they consider rotational gravity - they may have someone start out in the "low g" section of a cylindrical habitat moving slowly radially and then figure that since gravity depends on the distance from the center, that the person experiences an increasing gravitational pull as they move outwards.