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* Launch vehicles will travel on a magnetically levitated and coupled sled . Aerodynamically shaped launch vehicles are 5000 kg riding above a 2000 kg magnet sled |
* '''Launch loops are assembled over and float the ocean for safety and security''' . A good place is 8 degrees south, 120 degrees west, west of Ecuador and south of San Diego . The "most boring weather in the world" according to one meteorologist * '''Launch vehicles will travel on a magnetically levitated and coupled sled''' . Aerodynamically shaped launch vehicles are 5000 kg, and ride above a 2000 kg magnet sled |
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. After payload release, sleds are decelerated and reused * Launch loops must be very long |
. Magnet sleds will use a lot of expensive Neodymium magnets . Nanostructured iron nitride may be a cheap, earth-abundant replacement someday; theoretical for now . After payload release, sleds are decelerated, retested, repaired, and reused * '''Launch loops must be very long''' . at 30 m/s² (≈ 3 gees) payload acceleration to 11.1 km/s exit velocity: . 370 seconds of acceleration, and a 2053 km launch path. . at 150 m/s² (≈ 15 gees), the empty sled stops in 74 seconds over 411 km |
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. at 30 m/s² (≈ 3 gees) payload acceleration to 11.1 km/s exit velocity, that is: . 370 seconds of acceleration, and a 2053 km launch path. . at 150 m/s² (≈ 15 gees), the empty sled stops in 74 seconds over 411 km. * The launch loop rotor masses 3 kg/m, with a 4 cm hexagonal cross section |
* '''The launch loop rotor masses 3 kg/m, with a 4 cm hexagonal cross section''' |
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* Launch loop launch altitude is 80 km | * '''Loop failure''' . The entire rotor stores almost 2e15 joules . A "1 megaton" bomb releases 4.2e15 joules instantly . The rotor circulates in 430 seconds . The rotor "power rate" is 4100 GW . A failing launch loop releases some rotor at the point of failure . most will be deflected and fanned into the ocean at two places, boiling a '''LOT''' of seawater '''''fast''''' . some material may be thrown into Earth escape orbit . a very small amount of material will re-enter . the bolts should be designed to disintegrate into small fragments during re-entry or ocean penetration * '''The launch loop track and stabilization cables mass 6.5 kg/m''' . the track contains velocity transformer coils, which couple sled magnets to the rotor * '''Stabilization cables to the surface transmit N/S and radial forces''' . cables must be aluminum-sheathed to carry lightning strokes . perhaps they can be actively charged to "cloud neutrality", but this seems unlikely * '''Launch loop launch altitude is 80 km''' |
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. The tenuous atmosphere above 80 km will deorbit smaller (and hard to track) space debris . Larger objects must be dodged or intercepted. |
. The tenuous atmosphere above 80 km will de-orbit smaller (and hard to track) space debris . Larger debris objects must be dodged or intercepted. * '''Launch loop ''inclines'' descend from the tracks to turnaround ''ambits'' at the ends . an upwards curve supports "west station" at 30 km altitude . the inclines enter '''upward deflector''' structures at the ocean surface at a 20 degree angle . presuming a 6 km turn radius, and a 100 meter superstructure: . the deflector structures will descend 300 meters below the ocean surface . they will deflect the rotor back up to 50 meters below the surface and wave agitation . they will be able to release a failing rotor into the ocean floor * '''Launch loop ambits will deflect six "tracks" of separated bolts''' . turn radius estimated 6000 meters . The ambits will have GW power plants and 10 km long linear motors . The ambits will be associated with "spare bolt racetracks" . These will also store burst power . High speed inspection stations will photograph each bolt at speed, to micrometer resolution . Bolt measurements will be "synopsized" by large parallel computers, and compared to previous measurements . Significant changes will cause a bolt to be diverted into a "used bolt racetrack . The ambits and deflection magnets will resemble a low-tech version of the [[ https://en.wikipedia.org/wiki/Large_Hadron_Collider | Large Hadron Collider ]] . Loop design will shamelessly steal technologies and best practices from LHC . If no particles are discovered after the Higgs, thousands of brilliant technicians may be available * Launch loops require [[ http://server-sky.com | Server Sky ]] constellations overhead . Providing redundant and precision interferometric positioning to the loop controllers . Providing redundant whole system control in case of failure . Capturing diagnostic information for modelling and optimization . Tracking vehicles and managing orbital traffic . Tracking incoming debris objects and planning mitigations === Power Storage === * '''At realistic launch market growth rates, it will be decades before launch loops are profitable''' . Space solar power has been '''just around the corner'' for half a century . Missions to Mars will be robotic, and humans can't compete economically . Mars will never be a practical "second Earth" (the asteroids might). . Deep space missions to deflect asteroids are way too expensive . Asteroid mining missions are proposed only by non-geologists and non-miners . We will do all of these things someday, but advocates must first start talking economic sense. * '''Grid scale energy storage is an urgent need''' . Grid demand varies hourly and seasonally . Wind and solar is intermittent and unpredictable . Nuclear is steady but not "peakable" . Carbon fuel stinks * '''Loop technology can store huge amounts of power''' . The fast loop described above stores 500 GW-hours . A slower, heavier loop running at 7900 m/s will "orbit" in its tunnel without vertical deflection forces . A kilogram of 7.9 km/s rotor stores 17 kWh. . Cycled 200 times per year, buying power at \$3/MWh and selling at \$10/MWh, a kilogram earns \$24 per year . purchase and automated forming cost might be \2 per kg ... '''≫≫profit!≪≪''''' . Most of the system losses are in the ambits; a longer "straightaway" adds storage with little loss . power storage loops can span the Pacific Ocean, time-shifting power across 10 time zones. . Much heavier rotors can store more energy . Power storage rotors can be simpler and safer than launch rotors * Lessons learned from power storage will speed the design of launch loops * Manufacturing lines for power storage can be used to build launch loops |
Short Intro
Launch loops are assembled over and float the ocean for safety and security
- A good place is 8 degrees south, 120 degrees west, west of Ecuador and south of San Diego
- The "most boring weather in the world" according to one meteorologist
- A good place is 8 degrees south, 120 degrees west, west of Ecuador and south of San Diego
Launch vehicles will travel on a magnetically levitated and coupled sled
- Aerodynamically shaped launch vehicles are 5000 kg, and ride above a 2000 kg magnet sled
Magnet sleds (perhaps 50 meters long) couple to the rotor through a velocity transformer track
- Magnet sleds will use a lot of expensive Neodymium magnets
- Nanostructured iron nitride may be a cheap, earth-abundant replacement someday; theoretical for now
- After payload release, sleds are decelerated, retested, repaired, and reused
Launch loops must be very long
- at 30 m/s² (≈ 3 gees) payload acceleration to 11.1 km/s exit velocity:
- 370 seconds of acceleration, and a 2053 km launch path.
- at 150 m/s² (≈ 15 gees), the empty sled stops in 74 seconds over 411 km
- A 2500 km launch path means a 6000 km total rotor length
- at 30 m/s² (≈ 3 gees) payload acceleration to 11.1 km/s exit velocity:
The launch loop rotor masses 3 kg/m, with a 4 cm hexagonal cross section
Each hexagonal is a row of iron-faced bolts, each perhaps 10 meters long.
Loop failure
- The entire rotor stores almost 2e15 joules
- A "1 megaton" bomb releases 4.2e15 joules instantly
- The rotor circulates in 430 seconds
- The rotor "power rate" is 4100 GW
- A failing launch loop releases some rotor at the point of failure
most will be deflected and fanned into the ocean at two places, boiling a LOT of seawater fast
- some material may be thrown into Earth escape orbit
- a very small amount of material will re-enter
- the bolts should be designed to disintegrate into small fragments during re-entry or ocean penetration
- The entire rotor stores almost 2e15 joules
The launch loop track and stabilization cables mass 6.5 kg/m
- the track contains velocity transformer coils, which couple sled magnets to the rotor
Stabilization cables to the surface transmit N/S and radial forces
- cables must be aluminum-sheathed to carry lightning strokes
- perhaps they can be actively charged to "cloud neutrality", but this seems unlikely
- cables must be aluminum-sheathed to carry lightning strokes
Launch loop launch altitude is 80 km
- Post-release payload drag and blunt nose heating will be significant but not extreme
- The tenuous atmosphere above 80 km will de-orbit smaller (and hard to track) space debris
- Larger debris objects must be dodged or intercepted.
Launch loop inclines descend from the tracks to turnaround ambits at the ends
- an upwards curve supports "west station" at 30 km altitude
the inclines enter
- presuming a 6 km turn radius, and a 100 meter superstructure:
- the deflector structures will descend 300 meters below the ocean surface
- they will deflect the rotor back up to 50 meters below the surface and wave agitation
- they will be able to release a failing rotor into the ocean floor
Launch loop ambits will deflect six "tracks" of separated bolts The ambits and deflection magnets will resemble a low-tech version of the Large Hadron Collider
Launch loops require Server Sky constellations overhead
- Providing redundant and precision interferometric positioning to the loop controllers
- Providing redundant whole system control in case of failure
- Capturing diagnostic information for modelling and optimization
- Tracking vehicles and managing orbital traffic
- Tracking incoming debris objects and planning mitigations
Power Storage
At realistic launch market growth rates, it will be decades before launch loops are profitable
Space solar power has been
- Missions to Mars will be robotic, and humans can't compete economically
- Mars will never be a practical "second Earth" (the asteroids might).
- Deep space missions to deflect asteroids are way too expensive
- Asteroid mining missions are proposed only by non-geologists and non-miners
- We will do all of these things someday, but advocates must first start talking economic sense.
Grid scale energy storage is an urgent need
- Grid demand varies hourly and seasonally
- Wind and solar is intermittent and unpredictable
- Nuclear is steady but not "peakable"
- Carbon fuel stinks
Loop technology can store huge amounts of power
- The fast loop described above stores 500 GW-hours
- A slower, heavier loop running at 7900 m/s will "orbit" in its tunnel without vertical deflection forces
- A kilogram of 7.9 km/s rotor stores 17 kWh.
- Cycled 200 times per year, buying power at \$3/MWh and selling at \$10/MWh, a kilogram earns \$24 per year
purchase and automated forming cost might be \2 per kg ... ≫≫profit!≪≪
- Most of the system losses are in the ambits; a longer "straightaway" adds storage with little loss
- power storage loops can span the Pacific Ocean, time-shifting power across 10 time zones.
- Much heavier rotors can store more energy
- Power storage rotors can be simpler and safer than launch rotors