Quote:
Originally Posted by Roadam
There is no need for any elevators as space ships would just sit on the cable at one of the stations and turn on the magnetic brakes.
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Now that you mention it, it does seem that rather than what Lofstrom described in his 1985 paper,
“THE LAUNCH LOOP: A LOW COST EARTH-TO-HIGH-ORBIT LAUNCH SYSTEM”The vehicles are brought up these cables rather than up the west incline to simplify the spacing controllers on the incline. Other benefits of this approach are minimized incline weight, shorter upward transit times, and less likelihood of sheath damage.
it would be better to use the sloping sections of the loop as elevators, using the same magnetic induction brake that the to-be-launched ship uses on the main track.
Lofstrom’s reasons for proposing an elevator appear to center around two features: the necessary differences between the lower, sloping sheath, which must be much thicker in order to maintain a vacuum and be weatherproof, and the upper, which is in near vacuum at 80,000 m altitude, so need only provide magnetic bearing to keep the rotor in a smooth path; and not wanting to put load on rotor in its sloping section, which would be difficult to manage for the systems many guide cables.
I don’t understand why a load of the launch ship at 1 g (9.8 m/s/s) on different part of the sloping section from a vehicle moving under 300 m/s (we’d likely want to avoid going super-sonic in any substantial atmosphere) is less troublesome than a 1 g load on a fixed point (the west station), followed by the force of accelerating the launched ship at a bit over 3 g (30 m/s/s) on the upper track for a bit over 6 minutes to a final speed of up to escape velocity (11400 m/s) or more.
Perhaps Lofstrom’s main reason is the “shorter upward transit times ” he mentions. I get a travel time of about 1 hour traverse nearly 1000 km at a barely subsonic speed of 300 m/s, vs the 80 km vertical elevator trip, at a reasonable elevator speed of 10 m/s, of a bit over 2 hours. Loftstrom might plan a slower sloping section speed, or a faster elevator.
A major difference between the system described in Lofstrom’s 1985 paper and
this 2002 slideshow (from which
the wikipedia article appears to get its graphics and description) is that the 1985 proposes a flat, ribbon-like iron rotor, while by 2002, it’s proposing one with a circular cross section.
Quote:
Originally Posted by Roadam
Also I am not yet sure how does author achieve levitation, as ferromagnetic metals are usually attractive.
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That part, I understand.
The rotor is magnetized. The sheath is conductive. When the magnetic field of a particular section moves past a section of the conductive sheath, it induces a current, causing that section to have a magnetic field. Their magnetic polarities, it turns out, are in opposite directions, resulting in mutual repulsion.
It’s similar to how an
Inductrack maglev train works, except that the rotor doesn’t have its magnets arranged into the more optimal pattern of a Halbach array. This is OK, as it results only in the levitating force being lower for a given rotor speed. In a Inductrack maglev train, this results in a higher “liftoff” speed at which the train cars begin levitating, a bad thing. The rotor in launch loop, however, move at a very high speed, so will induce a lot of current and repulsive magnetic fields in the sheath’s conductor, even with its magnetic fields less-than optimally arranged.
Given all of our uncertainties and guesswork, it might be worth our while to contact Keith Lofstrom. If
his personal webpage is any indication, he seems an approachable, techish person. I imagine he’s interested in promoting discussion of the launch loop concept, and wouldn’t mind helping.
If nobody else wants the honor, I’ll email him an invitation at the address give on his personal webpage.
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