Linear Cables
Stabilization and elevator cables on the launch loop are very long, and propagation delay is a big issue. In most systems people are familiar with, cables are short enough and forces change slowly enough that propagation delay is not a major issue. With a launch loop, forces can change rapidly (milliseconds) while the propagation delays are 10s of seconds.
For example, when an instantaneous force change is applied to one end of a very long cable, the end does not stretch a little, it moves, and keeps moving until the force has had time to propagate to a stationary attachment and back. For a 100km stabilization cable, and a 10km/s speed of sound, that can be 20 seconds, in which time many meters of cable moves.
| Material | density | elastic | strength | CTE | Vsound | Support | 100km | Therm exp | notes | 
| 
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 | modulus | 
 | 
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 | Length | Round Trip | 100Km*100K | 
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| 
 | gm/cm3 | GPa | GPa | um/m-K | km/s | km | seconds | m | 
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| 
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 | 
 | 
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| Steel SAE980x | 7.9 | 200 | 0.65 | 12 | 5.0 | 8.4 | 40 | 120 | 
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| Pure Kevlar | 1.44 | 124 | 3.62 | -2.7 | 9.3 | 250 | 22 | -27 | 
 | 
| Pure Spectra | 0.97 | 168 | 2.58 | -12 | 13.2 | 270 | 15 | -120 | continuous creep | 
| Pure Diamond | 3.52 | 1140 | >60 | 1.2 | 18.0 | 1700 | 11 | 12 | 
 | 
| Pure nanotube | ~1.4 | ~1000 | ~60 | -9? | 26.0 | 4400 | 8 | -90 | 
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| composites: | 
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| 80% Kevlar | 
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| 80% Spectra | 
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| 80% nanotube | 
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note: Nanotube properties are controversial. The CTE simulation Prakash is used here, but other simulations differ wildly.
