Jump to content

Specific strength

From Wikipedia, the free encyclopedia
(Redirected from Breaking length)

The specific strength is a material's (or muscle's) strength (force per unit area at failure) divided by its density. It is also known as the strength-to-weight ratio or strength/weight ratio or strength-to-mass ratio. In fiber or textile applications, tenacity is the usual measure of specific strength. The SI unit for specific strength is Pam3/kg, or N⋅m/kg, which is dimensionally equivalent to m2/s2, though the latter form is rarely used. Specific strength has the same units as specific energy, and is related to the maximum specific energy of rotation that an object can have without flying apart due to centrifugal force.

Another way to describe specific strength is breaking length, also known as self support length: the maximum length of a vertical column of the material (assuming a fixed cross-section) that could suspend its own weight when supported only at the top. For this measurement, the definition of weight is the force of gravity at the Earth's surface (standard gravity, 9.80665 m/s2) applying to the entire length of the material, not diminishing with height. This usage is more common with certain specialty fiber or textile applications.

The materials with the highest specific strengths are typically fibers such as carbon fiber, glass fiber and various polymers, and these are frequently used to make composite materials (e.g. carbon fiber-epoxy). These materials and others such as titanium, aluminium, magnesium and high strength steel alloys are widely used in aerospace and other applications where weight savings are worth the higher material cost.

Note that strength and stiffness are distinct. Both are important in design of efficient and safe structures.

Calculations of breaking length

[edit]

where is the length, is the tensile strength, is the density and is the acceleration due to gravity ( m/s)

Examples

[edit]
Specific tensile strength of various materials
Material Tensile strength
(MPa)
Density
(g/cm3)
Specific strength
(kN·m/kg)
Breaking length
(km)
Source
Concrete 2–5 2.30 5.22 0.44 [citation needed]
Polyoxymethylene; POM 69 1.42 49 4.95 [1]
Rubber 15 0.92 16.3 1.66 [citation needed]
Copper 220 8.92 24.7 2.51 [citation needed]
Polypropylene; PP 25–40 0.90 28–44 2.8–4.5 [2]
(Poly)acrylonitrile-butadiene-styrene; ABS 41–45 1.05 39–43 [3]
Polyethylene terephthalate; polyester; PET 80 1.3–1.4 57–62 [4]
Piano wire; ASTM 228 Steel 1590–3340 7.8 204–428 [5]
Polylactic acid; polylactide; PLA 53 1.24 43 [6]
Low carbon steel (AISI 1010) 365 7.87 46.4 4.73 [7]
Stainless steel (304) 505 8.00 63.1 6.4 [8]
Maraging steel (18Ni(350)) 2450 8.2 298.78 29.7 [9]
Brass 580 8.55 67.8 6.91 [10]
Nylon 78 1.13 69.0 7.04 [11]
Titanium 344 4.51 76 7.75 [12]
CrMo Steel (4130) 560–670 7.85 71–85 7.27–8.70 [13][14]
Aluminium alloy (6061-T6) 310 2.70 115 11.70 [15]
Oak 90 0.78–0.69 115–130 12–13 [16]
Inconel (X-750) 1250 8.28 151 15.4 [17]
Magnesium alloy 275 1.74 158 16.1 [18]
Aluminium alloy (7075-T6) 572 2.81 204 20.8 [19]
Pine wood (American eastern white) 78 0.35 223 22.7 [20]
Titanium alloy (Beta C) 1250 4.81 260 26.5 [21]
Bainite 2500 7.87 321 32.4 [22]
Reversibly Assembled Cellular Composite Materials 0.073 0.0072 10,139 1035 [23][24]
Self-Reprogrammable Mechanical Metamaterials 0.01117 0.0103 1,084 111 [25]
Balsa 73 0.14 521 53.2 [26]
Carbon–epoxy composite 1240 1.58 785 80.0 [27]
Spider silk 1400 1.31 1,069 109 [citation needed]
Silicon carbide fiber 3440 3.16 1,088 110 [28]
Miralon carbon nanotube yarn C-series 1375 0.7–0.9 1,100 112 [29]
Glass fiber 3400 2.60 1,307 133 [30]
Basalt fiber 4840 2.70 1,790 183 [31]
1 μm iron whiskers 14000 7.87 1,800 183 [22]
Vectran 2900 1.40 2,071 211 [30]
Carbon fiber (AS4) 4300 1.75 2,457 250 [30]
Kevlar 3620 1.44 2,514 256 [32]
Dyneema (UHMWPE) 3600 0.97 3,711 378 [33]
Zylon 5800 1.54 3,766 384 [34]
Carbon fiber (Toray T1100G) 7000 1.79 3,911 399 [35]
Carbon nanotube (see note below) 62000 0.037–1.34 46,268–N/A 4716–N/A [36][37]
Colossal carbon tube 6900 0.116 59,483 6066 [38]
Graphene 130500 2.090 62,453 6366 [39]
Fundamental limit 9×1013 9.2×1012 [40]

The data of this table is from best cases, and has been established for giving a rough figure.

Note: Multiwalled carbon nanotubes have the highest tensile strength of any material yet measured, with labs producing them at a tensile strength of 63 GPa,[36] still well below their theoretical limit of 300 GPa. The first nanotube ropes (20 mm long) whose tensile strength was published (in 2000) had a strength of 3.6 GPa, still well below their theoretical limit.[41] The density is different depending on the manufacturing method, and the lowest value is 0.037 or 0.55 (solid).[37]

The 'Yuri' and space tethers

[edit]

The International Space Elevator Consortium uses the "Yuri" as a name for the SI units describing specific strength. Specific strength is of fundamental importance in the description of space elevator cable materials. One Yuri is conceived to be the SI unit for yield stress (or breaking stress) per unit of density of a material under tension. One Yuri equals 1 Pa⋅m3/kg or 1 Nm/kg, which is the breaking/yielding force per linear density of the cable under tension.[42][43] A functional Earth space elevator would require a tether of 30–80 megaYuri (corresponding to 3100–8200 km of breaking length).[44]

Fundamental limit on specific strength

[edit]

The null energy condition places a fundamental limit on the specific strength of any material.[40] The specific strength is bounded to be no greater than c29×1013 kNm/kg, where c is the speed of light. This limit is achieved by electric and magnetic field lines, QCD flux tubes, and the fundamental strings hypothesized by string theory.[citation needed]

Tenacity (textile strength)

[edit]

Tenacity is the customary measure of strength of a fiber or yarn. It is usually defined as the ultimate (breaking) force of the fiber (in gram-force units) divided by the denier. Because denier is a measure of the linear density, the tenacity works out to be not a measure of force per unit area, but rather a quasi-dimensionless measure analogous to specific strength.[45] A tenacity of corresponds to:[citation needed] Mostly Tenacity expressed in report as cN/tex.

See also

[edit]

References

[edit]
  1. ^ "Acetal Polyoxymethylene Homopolymer - POM". AZoM.com. August 30, 2001. Archived from the original on July 22, 2020. Retrieved July 22, 2020.
  2. ^ "Polypropylene - online catalogue source - supplier of research materials in small quantities - Goodfellow". www.goodfellow.com. Archived from the original on 2018-08-07. Retrieved 2017-04-24.
  3. ^ "Polyacrylonitrile-butadiene-styrene - online catalogue source - supplier of research materials in small quantities - Goodfellow". www.goodfellow.com. Archived from the original on 2018-12-20. Retrieved 2018-07-29.
  4. ^ "Polyethylene terephthalate - online catalogue source - supplier of research materials in small quantities - Goodfellow". www.goodfellow.com. Archived from the original on 2019-04-17. Retrieved 2018-07-29.
  5. ^ "ASTM A228 Steel (UNS K08500)". www.matweb.com. Archived from the original on 2019-01-19. Retrieved 2019-01-17.
  6. ^ "Polylactic acid - Biopolymer - online catalogue source - supplier of research materials in small quantities - Goodfellow". www.goodfellow.com. Archived from the original on 2018-07-29. Retrieved 2018-07-29.
  7. ^ "AISI 1010 Steel, cold drawn". matweb.com. Archived from the original on 2018-04-18. Retrieved 2015-10-20.
  8. ^ "ASM Material Data Sheet". asm.matweb.com. Archived from the original on 2018-10-01. Retrieved 2015-10-20.
  9. ^ "SSA Corp Maraging Data Sheet". matmatch.com/learn/material/maraging-steel.
  10. ^ "Properties of Copper Alloys". roymech.co.uk. Archived from the original on 2019-03-30. Retrieved 2006-04-17.
  11. ^ "Polyamide - Nylon 6 - online catalogue source - supplier of research materials in small quantities - Goodfellow". www.goodfellow.com. Archived from the original on 2019-04-17. Retrieved 2017-04-24.
  12. ^ "ASM Material Data Sheet". asm.matweb.com. Archived from the original on 2019-03-22. Retrieved 2016-11-14.
  13. ^ "ASM Material Data Sheet". asm.matweb.com. Archived from the original on 2019-04-06. Retrieved 2016-08-18.
  14. ^ "ASM Material Data Sheet". asm.matweb.com. Archived from the original on 2012-03-15. Retrieved 2016-08-18.
  15. ^ "ASM Material Data Sheet". asm.matweb.com. Archived from the original on 2018-10-22. Retrieved 2016-08-18.
  16. ^ "Environmental data: Oak wood". Archived from the original on 9 October 2007. Retrieved 2006-04-17.{{cite web}}: CS1 maint: bot: original URL status unknown (link)
  17. ^ "ASM Material Data Sheet". asm.matweb.com. Archived from the original on 2018-10-04. Retrieved 2015-10-20.
  18. ^ "eFunda: Typical Properties of Magnesium Alloys". www.efunda.com. Archived from the original on 2020-01-30. Retrieved 2021-10-01.
  19. ^ "ASM Material Data Sheet". asm.matweb.com. Archived from the original on 2018-10-16. Retrieved 2015-10-20.
  20. ^ "American Eastern White Pine Wood". www.matweb.com. Archived from the original on 2019-12-08. Retrieved 2019-12-08.
  21. ^ "AZo Materials Data Sheet". azom.com. 11 February 2003. Archived from the original on 2017-06-23. Retrieved 2016-11-14.
  22. ^ a b 52nd Hatfield Memorial Lecture: "Large Chunks of Very Strong Steel" by H. K. D. H. Bhadeshia 2005. on archive.is
  23. ^ "Toylike blocks make lightweight, strong structures". 2013-08-16. Retrieved 2024-03-21.
  24. ^ Schaedler, Tobias A.; Jacobsen, Alan J.; Carter, Wiliam B. (2013-09-13). "Toward Lighter, Stiffer Materials". Science. 341 (6151): 1181–1182. Bibcode:2013Sci...341.1181S. doi:10.1126/science.1243996. ISSN 0036-8075. PMID 24031005.
  25. ^ Krywko, Jacek (2024-02-08). "Building robots for "Zero Mass" space exploration". Ars Technica. Retrieved 2024-03-21.
  26. ^ "MatWeb – The Online Materials Information Resource". matweb.com. Archived from the original on 2015-04-02. Retrieved 2009-06-29.
  27. ^ McGRAW-HILL ENCYCLOPEDIA OF Science & Technology, 8th Edition, (c)1997, vol. 1 p 375
  28. ^ "Specialty Materials, Inc SCS Silicon Carbide Fibers". Archived from the original on 2018-04-04. Retrieved 2006-04-17.
  29. ^ NanoComp Technologies Inc. "Miralon Yarn" (PDF). Archived (PDF) from the original on 2018-12-20. Retrieved 2018-12-19.
  30. ^ a b c "Vectran". Vectran Fiber, Inc. Archived from the original on 2019-07-08. Retrieved 2017-06-12.
  31. ^ "RWcarbon.com – The Source for BMW & Mercedes Carbon Fiber Aero Parts". rwcarbon.com. Archived from the original on 2019-05-03. Retrieved 2021-10-01.
  32. ^ "Network Group for Composites in Construction: Introduction to Fibre Reinforced Polymer Composites". Archived from the original on January 18, 2006. Retrieved 2006-04-17.{{cite web}}: CS1 maint: bot: original URL status unknown (link)
  33. ^ "Dyneema Fact sheet". DSM. 1 January 2008. Archived from the original on 8 August 2019. Retrieved 23 May 2016.
  34. ^ Toyobo Co., Ltd. "ザイロン®(PBO 繊維)技術資料 (2005)" (PDF). Archived from the original (free download PDF) on 2012-04-26.
  35. ^ Toray Composites Materials America, Co., Ltd. "T1100S, INTERMEDIATE MODULUS CARBON FIBER" (free download PDF). Archived (PDF) from the original on 2021-07-13. Retrieved 2021-06-29.{{cite web}}: CS1 maint: multiple names: authors list (link)
  36. ^ a b Yu, Min-Feng; Lourie, Oleg; Dyer, Mark J.; Moloni, Katerina; Kelly, Thomas F.; Ruoff, Rodney S. (28 January 2000). "Strength and Breaking Mechanism of Multiwalled Carbon Nanotubes Under Tensile Load" (PDF). Science. 287 (5453): 637–640. Bibcode:2000Sci...287..637Y. doi:10.1126/science.287.5453.637. PMID 10649994. S2CID 10758240. Archived from the original (PDF) on 4 March 2011.
  37. ^ a b K.Hata (2007). "From highly efficient impurity-free CNT synthesis to DWNT forests, CNT solids, and super-capacitors" (PDF). In Razeghi, Manijeh; Brown, Gail J (eds.). From Highly Efficient Impurity-Free CNT Synthesis to DWNT forests, CNTsolids and Super-Capacitors. Quantum Sensing and Nanophotonic Devices IV. Vol. 6479. pp. 64791L. doi:10.1117/12.716279. S2CID 136421231. Archived from the original on 2014-12-14. Retrieved 2009-12-02.{{cite book}}: CS1 maint: unfit URL (link)
  38. ^ Peng, H.; Chen, D.; et al., Huang J.Y.; et al. (2008). "Strong and Ductile Colossal Carbon Tubes with Walls of Rectangular Macropores". Phys. Rev. Lett. 101 (14): 145501. Bibcode:2008PhRvL.101n5501P. doi:10.1103/PhysRevLett.101.145501. PMID 18851539.
  39. ^ "2010 Nobel Physics Laureates" (PDF). nobelprize.org. Archived (PDF) from the original on 2018-07-01. Retrieved 2019-03-28.
  40. ^ a b Brown, Adam R. (2013). "Tensile Strength and the Mining of Black Holes". Physical Review Letters. 111 (21): 211301. arXiv:1207.3342. Bibcode:2013PhRvL.111u1301B. doi:10.1103/PhysRevLett.111.211301. PMID 24313473. S2CID 16394667.
  41. ^ Li, F.; Cheng, H. M.; Bai, S.; Su, G.; Dresselhaus, M. S. (2000). "Tensile strength of single-walled carbon nanotubes directly measured from their macroscopic ropes". Applied Physics Letters. 77 (20): 3161–3163. Bibcode:2000ApPhL..77.3161L. doi:10.1063/1.1324984.
  42. ^ "Strong Tether Challenge 2013" (PDF). Archived from the original (PDF) on 2016-01-14.
  43. ^ "Terminology". isec.org. Archived from the original on 2012-05-27.
  44. ^ "Specific Strength in Yuris". keithcu.com. Archived from the original on 2019-02-09. Retrieved 2012-06-02.
  45. ^ Rodriguez, Ferdinand (1989). Principles of Polymer Systems (3rd ed.). New York: Hemisphere Publishing. p. 282. ISBN 9780891161769. OCLC 19122722.
[edit]