STRUCTURAL MATERIALS
Slings, elevators, and many other orbital structures must be
made of materials having high specific strength (strength-to-mass
ratio). The specific strength of composites is only half of the
specific strength of the reinforcing fibers. High-strength
plastics, e.g., PBO, become brittle when exposed to thermal fatigue
and space radiation. Atomic oxygen erosion, space junk, and
meteoroids also damage orbital contraptions and towers.
Contraptions protected by the atmosphere or a pile of rubble, can
be made of plastic.
- For details on atomic oxygen erosion see:
- -John N. Stevens, "Method for Estimating Atomic Oxygen Surface
Erosion in Space Environments," Journal of Spacecraft and
Rockets, Vol. 27, No. 1, 1990, pp. 93-95.
- -G. E. Caledonia and R. H. Krech, "Studies of the Interaction
of 8 km/s Oxygen Atoms," in Materials Degradation in Low Earth
Orbit (LEO), edited by V. Srinivasan and B. A. Banks, Minerals,
Metals, and Materials Society, Warendale, PA, 1990, pp.
145-153.
- -R. C. Tennyson, "Atomic Oxygen and Its Effects on Materials,"
in The Behavior of Systems in the Space Environment, edited
by R. N. DeWitt, Kluwer Academic, Amsterdam, 1993, pp.
233-357.
-
- For details on space junk and meteoroids see:
- -William. A. Bacarat and C. L. Butner,
- Tethers in Space Handbook
, NASA, 1986, page 4-32.
- -Nicholas L. Johnson and D. S. McKnight, Artificial Space
Debris, Orbit Books, 1991.
- - Interagency
Report on Orbital Debris, Office of Science and Technology Policy,
National Science Technology Council, November 1995.
- - http://elses1.msfc.nasa.gov/nee/meteo.html
- - http://www.animatedsoftware.com/spacedeb/index.htm
- - http://members.aol.com/earth2039/index.html
- -Nicholas L. Johnson, "Monitoring and Controlling Debris in
Space," Scientific
American, Vol. 279, No. 2, August 1998, pp. 42-47.
- Glass ribbons are cheap and resistant to oxygen erosion but
fragile. For details see:
- John V. Milewski (ed.), Handbook of Reinforcements for
Plastics, Van Nostrand, New York, 1987, pp. 76-97.
- Polycrystalline diamond has a tensile strength of about 700
megapascals. A small device using plasma chemical vapor deposition
technique can deposit 25 micrometers of polycrystalline diamond per
hour. The same device can deposit graphite at the rate of several
millimeters per hour. A protective coating is needed to prevent
erosion of carbon by atomic oxygen. Details:
- J. J. Beulens, A. J. M. Buuron, and D. C. Schram, "Carbon
Deposition Using an Expanding Cascaded Arc D.C. Plasma," Surface
& Coatings Technology, Vol. 47, No. 1-3, 1991, pp.
401-417.
- A carbon matrix produced by a chemical vapor deposition
technique and reinforced with carbon fibers has a tensile strength
of at least 1.5 GPa. Details:
- John V. Milewski (ed.), Handbook of Reinforcements for
Plastics," Van Nostrand, New York, 1987, p. 376.
-
- A glass matrix reinforced with carbon fibers is fairly strong
and resistant to oxygen erosion. Details:
- -Brian C. Hoskins and Alan A. Baker, (eds.) Composite
Materials for Aircraft Structures, AIAA, 1986, ISBN
0-930403-11-8.
- -William K. Tredway and Karl M. Prewo, "Fiber Reinforced Glass
Matrix Composites for Space Structures," in 23rd International
SAMPE Technical Conference, Vol. 23, ed. Robert L. Carri, 1991,
pp. 762-776.
- Piano wire is cheap and has a tensile strength of about 3 GPa,
while the strongest commercial steel wire attains 5 GPa.
Details:
- H. K. D. H. Bhadeshia and H. Harada, "High-strength (5 GPa)
steel wire: an atom-probe study" Applied Surface Science, Vol. 67,
1993, pp. 328-333.
- Buckytubes are microscopic carbon tubes. They are also known as
carbon nanotubes. Their specific strength is 2 orders of magnitude
greater than that of steel! Buckytubes are still too expensive to
be used as a structural material, but fabrication techniques have
been improving rapidly. Cheap buckytubes would make
- skyhook
practicable. Professor Richard E.
Smalley of Rice University is the leading buckytube expert.
(Richard Smalley, Robert Curl and Harold Kroto received 1996 Nobel
prize for chemistry for the discovery of a similar carbon structure
called buckyball.) You can learn more about buckytubes from:
- -David
Tomanek's Nanotube Site.
- -Web article:
"From Fullerenes to Nanotubes".
- -Associated
Press article: "Carbon material could be used for space
elevator".
- -Smalley speech:
"From Balls to Tubes to Ropes: New Materials from Carbon".
longitudinal speed of sound =
(Y/R)0.5
- where:
- Y is the Young's modulus
- R is the density of the solid
substance |
tensile
strength
[GPa] |
Y
(Young's
modulus)
[GPa] |
R
(density)
[kgm-3] |
longitudinal
speed of sound
in thin rods
[m/s] |
steel |
1-5 |
200 |
7900 |
5000 |
berylium fiber |
3.3 |
310 |
1870 |
12870 |
boron fiber |
3.5 |
400 |
2450 |
12778 |
fused silica |
n. a. |
73 |
2200 |
5760 |
pyrex glass |
n. a. |
62 |
2320 |
5170 |
E-glass fiber |
2.4 |
72.4 |
2540 |
5339 |
S-glass fiber |
4.5 |
85.5 |
2490 |
5860 |
Kevlar 49 (aramid fiber) |
3.6 |
130 |
1440 |
9502 |
Spectra fiber (gel-spun polyethylene) |
3.0 |
170 |
970 |
13239 |
PBO (poly-paraphenylene benzobisthiazole, plastic fiber) |
5.8 |
365 |
1580 |
15199 |
carbon fiber |
2-5 |
250-830 |
1850 |
11600-21200 |
buckytube cable (theoretical data) |
150 |
630 |
1300 |
22014 |
- Table data compiled from:
- -Dominic V. Rosato, Rosato's Plastics Encyclopedia and
Dictionary, Hanser Publishers, Munich, 1993, p. 638.
- -Alan S. Brown, "Spreading Spectrum of Reinforcing Fibers"
Aerospace America, January 1989, pp. 14-18.
- -CRC Handbook of Chemistry and Physics, 66th edition, page
E-43.
- -Theoretical buckytube cable data provided by
- Boris I. Yakobson
(North Carolina State University, Department of Physics).
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