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   Size: 4291 
  
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   Size: 4293 
  
  Comment:  
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| Deletions are marked like this. | Additions are marked like this. | 
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| I added my own estimations for perfect hexagonally close packed tube density, Tubes/m² $ = \sqrt( 3 ) / 2 D^2 = 0.866 / D^2 $ The pullout pressure $ P = 866 F / D^2 $ KPa if F is nanonewtons and D is nanometers. Results: | I added my own estimations for perfect hexagonally close packed tube density,  tubes/m² $ = \sqrt( 3 ) / 2 D^2 = 0.866 / D^2 $  The pullout pressure $ P = 866 F / D^2 $ KPa if F is nanonewtons and D is nanometers.   Results: | 
CNTE
Pure carbon nanotubes exhibit superlubricity - approximately ZERO friction between neighboring tubes in a bundle. In 2013, Zhang et. al. published a paper on carbon nanotube superlubricity that measured the intershell sliding force of a 1 centimeter double-wall carbon nanotube (DWCNT). Three diameters were measured, and the tiny pullout force matched theory, pa function of outer tube diameter.
Zhang et. al.  | 
  
  | 
  Laurent et. al  | 
|||||
Diameter  | 
  Pullout  | 
  
  | 
  Inner  | 
  Density  | 
  Tubes  | 
  Pullout  | 
  Strength  | 
nm  | 
  Force nN  | 
  
  | 
  nm  | 
  Kg/m³  | 
  / m²  | 
  Pressure  | 
  Kyuri  | 
2.73  | 
  1.37  | 
  
  | 
  2.39  | 
  1951  | 
  1.16e17  | 
  159 MPa  | 
  81.5  | 
2.93  | 
  1.47  | 
  
  | 
  2.59  | 
  1835  | 
  1.01e17  | 
  148 MPa  | 
  80.7  | 
3.26  | 
  1.64  | 
  
  | 
  2.92  | 
  1672  | 
  8.10e16  | 
  134 MPa  | 
  80.1  | 
Laurent et. al. estimates that the inner tube diameter is 0.34 nM ( d_{s-s} ) less than the outer tube diameter, and that DWCNT density (g/cm³) is:
d_{MW} = 6084 { \Large { ( d_{out} ~ - ~ d_{s-s} ) \over { d_{out}^2 } } } with d_{out} and d_{s-s} in nanometers.
I added my own estimations for perfect hexagonally close packed tube density, tubes/m² = \sqrt( 3 ) / 2 D^2 = 0.866 / D^2 The pullout pressure P = 866 F / D^2 KPa if F is nanonewtons and D is nanometers. Results:
Zhang et. al.  | 
  
  | 
  Laurent et. al  | 
|||||
Diameter  | 
  Pullout  | 
  
  | 
  Inner  | 
  Density  | 
  Tubes  | 
  Pullout  | 
  Strength  | 
nm  | 
  Force nN  | 
  
  | 
  nm  | 
  kg/m³  | 
  / m²  | 
  Pressure  | 
  Kyuri  | 
2.73  | 
  1.37  | 
  
  | 
  2.39  | 
  1951  | 
  1.16e17  | 
  159 MPa  | 
  81.5  | 
2.93  | 
  1.47  | 
  
  | 
  2.59  | 
  1835  | 
  1.01e17  | 
  148 MPa  | 
  80.7  | 
3.26  | 
  1.64  | 
  
  | 
  2.92  | 
  1672  | 
  8.10e16  | 
  134 MPa  | 
  80.1  | 
These strengths for pure, perfect DWCNT are less than 0.2% of the minimum strength needed for a space elevator, and 2% of the strength of Torayca 1100G carbon fiber. Furthermore, given these pullout forces, which will be unevenly distributed in real atomically imperfect materials, the stretch will not recover; these are not spring forces, but disassembly forces. After the material slides apart, it will not go back together, the hysteresis is unity. This is weak taffy, not a strong elastic material like kevlar or carbon fiber, or even a .
The situation is grim but not completely hopeless. In CNT fibers - yarns between the extremes, Dr. Thurid Gspann et. al. suggests that defects create load-sharing crosslinks between tubes, but can reduce strength from the theoretical 100 GPa by 30% to 70%. Even with the theoretical "best defect" maximum of 70 GPa, and a density of 1700 kg/m, this theoretical atomic-precision macro-material will have a strength of 41 Myuri, less than the 48 Myuri (derated by 40% to 34 Myuri) material assumed by the 2013 Space Elevators assessment.
If ≈ 40 Myuri is potentially possible with perfect "precision-defect" CNT (based on current pessimistic knowledge), there may be an atomically-perfect 3D material structure with zero hysteresis and 40 Myuri strength. May be; in 2017, we do not have a scintilla of a clue how to do that. Indeed, these may be pseudo-life-like complex nanostructures that can repair and grow themselves under tension, but are far beyond our current understanding and technological imagination.
Space elevators have assumed diamond-like crystal tethers since the 1970s, and carbon nanotube tethers since the 1990s. The materials necessary have not yet been discovered, or even imagined in analyzable detail.
