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⇤ ← Revision 1 as of 2009-07-11 16:59:14
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| 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 the attachment and back. For a 100km stabilization cable, that can be 20 seconds, in which time many meters of cable moves. |
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. |
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| || Material || density || modulus || strength || CTE || Vsound || Length || Round Trip || 100Km*100K || || || gm/cm^3^ || GPa || MPa || um/m-K || m/s || m || seconds || m || || Steel SAE980x || 7.9 || 200 || 650 || 12 || 5000 || 8400 || 40 || 120 || || 80% Kevlar || || 80% Spectra || || 80% nanotube || |
|| Material || density || elastic || strength || CTE || Vsound || Support || 100km || Therm exp || || || || modulus || || || || Length || Round Trip || 100Km*100K || || || gm/cm^3^ || GPa || MPa || um/m-K || km/s || km || seconds || m || || || || || || || || || || || || Steel SAE980x || 7.9 || 200 || 650 || 12 || 5.0 || 8.4 || 40 || 120 || || Pure Kevlar || 1.44 || 124 || 3620 || -2.7 || 9.3 || 250 || 22 || -27 || || Pure Spectra || 0.97 || 168 || 2580 || || 13.2 || 270 || 15 || || || Pure Diamond || 3.52 || 1140 || >60000 || 1.2 || 18.0 || 1740 || 11 || 12 || || Pure nanotube || || || || || || || || || || composites: || || || || || || || || || || 80% Kevlar || || || || || || || || || || 80% Spectra || || || || || || || || || || 80% nanotube || || || || || || || || || |
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 |
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modulus |
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Length |
Round Trip |
100Km*100K |
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gm/cm3 |
GPa |
MPa |
um/m-K |
km/s |
km |
seconds |
m |
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Steel SAE980x |
7.9 |
200 |
650 |
12 |
5.0 |
8.4 |
40 |
120 |
Pure Kevlar |
1.44 |
124 |
3620 |
-2.7 |
9.3 |
250 |
22 |
-27 |
Pure Spectra |
0.97 |
168 |
2580 |
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13.2 |
270 |
15 |
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Pure Diamond |
3.52 |
1140 |
>60000 |
1.2 |
18.0 |
1740 |
11 |
12 |
Pure nanotube |
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composites: |
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|| 80% Kevlar || || || || || || || || ||
80% Spectra |
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80% nanotube |
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