|
Size: 2799
Comment:
|
Size: 3479
Comment:
|
| Deletions are marked like this. | Additions are marked like this. |
| Line 5: | Line 5: |
| || || Aluminum || Maraging Steel || goodness || || density ρ kg/m³ || 2700 || 8100 || || || rms. atomic number || 13 || 27.2 || 2.09 :-) || || avg. atomic weight || 26 || 58.6 || 2.25 :-) || || resistivity nΩ-m || 28.2 || 181 || 0.156 :-( || || thermal conductance W/m-K || 237 || 24.8 || 0.105 :-( || || thermal expansion μm/m-K || 23.1e-6 || 10.3e-6 || 2.24 :-) || || Youngs modulus E, GPa || 70 || 210 || 3.0 :-) || ||<-4> Derived 5m²/kg || || Thickness t μm || 74.1 || 24.7 || || || Bending Stiffness (1) E t || 5.2e6 || 5.2e6 || || Bending Stiffness (2) E t³ || 28.4e-3 || 3.16e-4 || 0.111 :-( || || Resistance mΩ/□ || 0.38 || 7.32 || 0.019 :-( || || Thermal conduction mW/K || 17.6 || 0.63 || 0.036 :-( || |
|| || Aluminum || Maraging Steel || goodness || || density ρ kg/m³ || 2700 || 8100 || || || rms. atomic number || 13 || 27.2 || 2.09 :-) || || avg. atomic weight || 26 || 58.6 || 2.25 :-) || || resistivity nΩ-m || 28.2 || 181 || 0.156 :-( || || thermal conductance W/m-K || 237 || 24.8 || 0.105 :-( || || thermal expansion μm/m-K || 23.1e-6 || 10.3e-6 || 2.24 :-) || || Youngs modulus E, GPa || 70 || 210 || 3.0 :-) || ||<-4> Derived 5m²/kg || || Thickness t μm || 74.1 || 24.7 || || || 1000kg, 200 000 thinsats, m || 15 || 5 || 3.00 :-) || || Bending Stiffness (1) E t || 5.2e6 || 5.2e6 || 1.00 || || Bending Stiffness (2) E t³ || 28.4e-3 || 3.16e-4 || 0.111 :-( || || Resistance mΩ/□ || 0.38 || 7.32 || 0.019 :-( || || Thermal conduction mW/K || 17.6 || 0.63 || 0.036 :-( || |
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Thinsats will already "launch densely". Thinsats will be in multiple stacks, probably attached to the circumverence of the load bearing ring at the edge of the upper stage. India's PSLV has a 2.8 meter diameter second stage, 8.8 meters, so we can easily fit 50 stacks of thinsats onto an adapter around that ring. 15 meters of aluminum thinsats means 30 centimeter (1 foot high) stacks, 5 meters of thinsats means 10 centimeter stacks. A SpaceX Falcon 9 is 3.7 meters and 4 times the payload to LEO, 3x taller stacks. |
Maraging Steel Thinsat Substrates
The current thinsat design presumes a pure aluminum substrate. However, maraging steel (68% iron, 18% nickel, 8% cobalt, 5% molybdenum, other elements ) offers interesting advantages.
|
Aluminum |
Maraging Steel |
goodness |
density ρ kg/m³ |
2700 |
8100 |
|
rms. atomic number |
13 |
27.2 |
2.09 |
avg. atomic weight |
26 |
58.6 |
2.25 |
resistivity nΩ-m |
28.2 |
181 |
0.156 |
thermal conductance W/m-K |
237 |
24.8 |
0.105 |
thermal expansion μm/m-K |
23.1e-6 |
10.3e-6 |
2.24 |
Youngs modulus E, GPa |
70 |
210 |
3.0 |
Derived 5m²/kg |
|||
Thickness t μm |
74.1 |
24.7 |
|
1000kg, 200 000 thinsats, m |
15 |
5 |
3.00 |
Bending Stiffness (1) E t |
5.2e6 |
5.2e6 |
1.00 |
Bending Stiffness (2) E t³ |
28.4e-3 |
3.16e-4 |
0.111 |
Resistance mΩ/□ |
0.38 |
7.32 |
0.019 |
Thermal conduction mW/K |
17.6 |
0.63 |
0.036 |
http://www.matweb.com/search/DataSheet.aspx?MatGUID=adaadfebfb20417db13ce8d3683dbccc&ckck=1
The main advantages are launch stack density, thermal expansion, belt particle scattering, and magnetic properties. The main disadvantages are lower lateral thermal conduction and thin shell bending stiffness - the resistivity is higher, but not that important.
Thinsats will already "launch densely". Thinsats will be in multiple stacks, probably attached to the circumverence of the load bearing ring at the edge of the upper stage. India's PSLV has a 2.8 meter diameter second stage, 8.8 meters, so we can easily fit 50 stacks of thinsats onto an adapter around that ring. 15 meters of aluminum thinsats means 30 centimeter (1 foot high) stacks, 5 meters of thinsats means 10 centimeter stacks. A SpaceX Falcon 9 is 3.7 meters and 4 times the payload to LEO, 3x taller stacks.
Lateral thermal conduction helps cool chips, though they will be small and scattered and do not need to radiate over large areas.
Lower bending stiffness (2) makes area ripples in the curving surface slower and higher amplitude. However, slower is more easily corrected with the optical thrusters, and compensated by phasing of the emitters. Bending stiffness (1) is multiplied by thinsat shape factors, the same for both aluminum and maraging steel.
If the thinsats are magnetized on their north-south axis, then the earth's magnetic field will keep them aligned rotationally. Also, it will help the thinsats separate out of the launch stack. However, if a thinsat rotates 180 degrees in relation to a near neighbor, they may stick together inseparably. Shape tweaks to make them rotationally assymetric can reduce this effect.
Rutherford scattering is enhanced by higher nuclear weight and charge. Belt remediation will be faster, with less lattice displacement damage. Calculations should be scalable.
This requires more study.