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Auxetics are materials that have a negative Poisson's ratio. When stretched, they become thicker perpendicular to the applied force. This occurs due to their particular internal structure and the way this deforms when the sample is uniaxially loaded. Auxetics can be single molecules, crystals, or a particular structure of macroscopic matter. Such materials and structures are expected to have mechanical properties such as high energy absorption and fracture resistance. Auxetics may be useful in applications such as body armor,[1] packing material, knee and elbow pads, robust shock absorbing material, and sponge mops.

The term auxetic derives from the Greek word αὐξητικός (auxetikos) which means "that which tends to increase" and has its root in the word αὔξησις, or auxesis, meaning "increase" (noun). This terminology was coined by Professor Ken Evans of the University of Exeter.[2]

The earliest published example of a synthetic auxetic material was in Science in 1987, entitled "Foam structures with a Negative Poisson's Ratio" [3] by R.S. Lakes from the University of Iowa. The use of the word auxetic to refer to this property probably began in 1991.[4]

Designs of composites with inverted hexagonal periodicity cell (auxetic hexagon), possessing negative Poisson's ratio, were published in 1985,[5] [6] ,[7] ,[8] ,[9] [10]

Typically, auxetic materials have low density, which is what allows the hinge-like areas of the auxetic microstructures to flex.[11]

At the macroscale, auxetic behaviour can be illustrated with an inelastic string wound around an elastic cord. When the ends of the structure are pulled apart, the inelastic string straightens while the elastic cord stretches and winds around it, increasing the structure's effective volume.

Examples of auxetic materials include:

  • Certain rocks and minerals[12]
  • Graphene, which can be made auxetic through the introduction of vacancy defects[13]
  • Folded sheet materials such as zigzag-based folded sheets.[14]
  • Living bone tissue (although this is only suspected)[12]
  • Tendons within their normal range of motion.[15]
  • Specific variants of polytetrafluorethylene polymers such as Gore-Tex[16]
  • Paper, all types. If a paper is stretched in an in-plane direction it will expand in its thickness direction due to its network structure.[17]
  • Tailored structures designed to exhibit special designed Poisson's ratios.[18]
  • Chain organic molecules. Recent researches revealed that organic crystals like n-paraffins and similar to them may demonstrate an auxetic behavior.[19]

See also[edit]


  1. ^ "Hook's law". The Economist. 1 December 2012. Retrieved 1 March 2013. 
  2. ^ Quinion, Michael (1996-11-09), Auxetic, retrieved 2009-01-02 .
  3. ^ Lakes, R.S. (1987-02-27), "Foam structures with a negative Poisson's ratio", Science 235 (4792): 1038, Bibcode:1987Sci...235.1038L, doi:10.1126/science.235.4792.1038, PMID 17782252. 
  4. ^ Evans, Ken (1991), Auxetic polymers: a new range of materials, doi:10.1016/0160-9327(91)90123-S .
  5. ^ Kolpakov, A.G. "Determination of the average characteristics of elastic frameworks". Journal of Applied Mathematics and Mechanics 49 (6): 739–745. Bibcode:1985JApMM..49..739K. doi:10.1016/0021-8928(85)90011-5. 
  6. ^ Almgren, R.F. (1985). "An isotropic three-dimensional structure with Poisson's ratio=-1". J. Elasticity 15: 427–430. doi:10.1007/bf00042531. 
  7. ^ Theocaris, P.S.; Stavroulakis, G.E.; Panagiotopoulos, P.D. (1997). "Negative Poisson's ratio in composites with star-shaped inclusions: a numerical homogenization approach .". Archive of Applied Mechanics (former Ingenieur Archiv) 67 (4): 274–286. Bibcode:1997AAM....67..274T. doi:10.1007/s004190050117. 
  8. ^ Theocaris, P.S.; Stavroulakis, G.E. "The homogenization method for the study of variation of Poisson's ratio in fiber composites". Archive of Applied Mechanics (former Ingenieur Archiv) 69 (3-4): 281–295. 
  9. ^ Stavroulakis, G.E. "Auxetic behaviour: Appearance and engineering applications". Physica Status Solidi (b) 242 (3): 710–720. Bibcode:2005PSSBR.242..710S. doi:10.1002/pssb.200460388. 
  10. ^ Kaminakis, N.T.; Stavroulakis, G.E. "Topology optimization for compliant mechanisms, using evolutionary-hybrid algorithms and application to the design of auxetic materials". Composites Part B: Engineering 43 (6): 2655–2668. doi:10.1016/j.compositesb.2012.03.018. 
  11. ^ A stretch of the imagination - 7 June 1997 - New Scientist Space
  12. ^ a b Burke, Maria (1997-06-07), "A stretch of the imagination", New Scientist 154 (2085): 36 
  13. ^ Grima, J. N.; Winczewski, S.; Mizzi, L.; Grech, M. C.; Cauchi, R.; Gatt, R.; Attard, D.; Wojciechowski, K.W.; Rybicki, J. (2014). "Tailoring Graphene to Achieve Negative Poisson's Ratio Properties". Advanced Materials 27: 1455–1459. doi:10.1002/adma.201404106. 
  14. ^ Eidini, Maryam; Paulino, Glaucio H. (2015). "Unraveling metamaterial properties in zigzag-base folded sheets". Science Advances 1 (8): e1500224. doi:10.1126/sciadv.1500224. ISSN 2375-2548. 
  15. ^ Gatt R, Vella Wood M, Gatt A, Zarb F, Formosa C, Azzopardi KM, Casha A, Agius TP, Schembri-Wismayer P, Attard L, Chockalingam N, Grima JN (2015). "Negative Poisson's ratios in tendons: An unexpected mechanical response". Acta Biomater. doi:10.1016/j.actbio.2015.06.018. 
  16. ^ Auxetic materials, retrieved 2009-01-02 .
  17. ^ Baum et al. 1984, Tappi journal, Öhrn, O. E. (1965): Thickness variations of paper on stretching, Svensk Papperstidn. 68(5), 141.
  18. ^ Tiemo Bückmann; et al. "Tailored 3D Mechanical Metamaterials Made by Dip-in Direct-Laser-Writing Optical Lithography". Advanced Materials 24: 2710–2714. doi:10.1002/adma.201200584. Retrieved 10 May 2012. 
  19. ^ Stetsenko, M (2015). "Determining the elastic constants of hydrocarbons of heavy oil products using molecular dynamics simulation approach". Journal of Petroleum Science and Engineering 126: 124–130. doi:10.1016/j.petrol.2014.12.021. 

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