{{Short description|Polymer with rubber-like elastic properties}} {{More citations needed|date=April 2015}}
thumb|upright|(A) is an unstressed polymer; (B) is the same polymer under stress. When the stress is removed, it will return to the A configuration. (The dots represent cross-links)
An '''elastomer''' is a polymer with viscoelasticity (i.e. both viscosity and elasticity) and with weak intermolecular forces, generally low Young's modulus (E) and high failure strain compared with other materials.<ref>{{cite book|last=De|first=Sadhan K.|title=Rubber Technologist's Handbook, Volume 1|date=31 December 1996|publisher=Smithers Rapra Press|isbn=978-1859572627|page=287|edition=1st|url=https://books.google.com/books?id=2rxFOm68Ui8C&q=elastomer+low+%22young%27s+modulus%22&pg=PA287|access-date=7 February 2017|archive-url=https://web.archive.org/web/20170207113815/https://books.google.ca/books?id=2rxFOm68Ui8C&pg=PA287&dq=elastomer+low+%22young%27s+modulus%22&hl=en&sa=X&ved=0ahUKEwjZoe3z8_zRAhVL1oMKHfl3DWoQ6AEIJDAC#v=onepage&q=elastomer%20low%20%22young's%20modulus%22&f=false#v=onepage&q=elastomer%20low%20%22young's%20modulus%22&f=false|archive-date=2017-02-07|url-status=live}}</ref> The term, a portmanteau of ''elastic polymer'',<ref>{{cite web |last=Gent |first=Alan N. |title=Elastomer Chemical Compound |url=https://www.britannica.com/science/elastomer |website=Encyclopædia Britannica |access-date=7 February 2017 |archive-url=https://web.archive.org/web/20170207114149/https://www.britannica.com/science/elastomer |archive-date=2017-02-07 |url-status=live }}</ref> is often used interchangeably with ''rubber'', although the latter is preferred when referring to vulcanisates.<ref>{{cite book |last=Alger |first=Mark |title=Polymer Science Dictionary |date=21 April 1989 |publisher=Springer |isbn=1851662200 |page=503 |url=https://books.google.com/books?id=OSAaRwBXGuEC&q=rubber+term+preferred+vulcanisates&pg=PA503 |archive-url=https://web.archive.org/web/20170207113813/https://books.google.ca/books?id=OSAaRwBXGuEC&pg=PA503&lpg=PA503&dq=rubber+term+preferred+vulcanisates&source=bl&ots=wVLr810pyp&sig=Ul09oC8mdMwqij3ILfDYqo7kl_g&hl=en&sa=X&ved=0ahUKEwjL1I629fzRAhVG64MKHeloC60Q6AEILTAE#v=onepage&q=rubber%20term%20preferred%20vulcanisates&f=false#v=onepage&q=rubber%20term%20preferred%20vulcanisates&f=false |archive-date=2017-02-07 |url-status=live |access-date=7 February 2017 }}</ref> Each of the monomers which link to form the polymer is usually a compound of several elements among carbon, hydrogen, oxygen and silicon.
{{Quote box |title =IUPAC definition |quote = '''Elastomer:''' Polymer that displays rubber-like elasticity<ref>{{cite journal |title=Definitions of Terms Relating to the Structure and Processing of Sols, Gels, Networks, and Inorganic–Organic Hybrid Materials (IUPAC Recommendations 2007) |journal=Pure and Applied Chemistry |date=2007 |volume=79 |issue=10 |pages=1801–1829 |doi=10.1351/pac200779101801 |url=http://www.iupac.org/publications/pac/pdf/2007/pdf/7910x1801.pdf |access-date=2017-07-14 |archive-url=https://web.archive.org/web/20180106173209/https://www.iupac.org/publications/pac/pdf/2007/pdf/7910x1801.pdf |archive-date=2018-01-06 |url-status=live |last1=Alemán |first1=J.V. |last2=Chadwick |first2=A.V. |last3=He |first3=J. |last4=Hess |first4=M. |last5=Horie |first5=K. |last6=Jones |first6=R.G. |last7=Kratochvíl |first7=P. |last8=Meisel |first8=I. |last9=Mita |first9=I. |last10=Moad |first10=G. |last11=Penczek |first11=S. |last12=Stepto |first12=R.F.T. |s2cid=97620232 }}</ref> | align = right | width = 30% }}
Rubber-like solids with elastic properties are called elastomers. Polymer chains are held together in these materials by relatively weak intermolecular bonds, which permit the polymers to stretch in response to macroscopic stresses.
Elastomers are usually thermosets (requiring vulcanization) but may also be thermoplastic (see thermoplastic elastomer). The long polymer chains cross-link during curing (i.e., vulcanizing). The molecular structure of elastomers can be imagined as a 'spaghetti and meatball' structure, with the meatballs signifying cross-links. The elasticity is derived from the ability of the long chains to reconfigure themselves to distribute an applied stress.
==Examples== '''Unsaturated rubbers''' that can be cured by sulfur vulcanization: * Natural polyisoprene: cis-1,4-polyisoprene natural rubber (NR) and trans-1,4-polyisoprene gutta-percha * Synthetic polyisoprene (IR for isoprene rubber) * Polybutadiene (BR for butadiene rubber) * Chloroprene rubber (CR), polychloroprene, neoprene * Butyl rubber (copolymer of isobutene and isoprene, IIR) ** Halogenated butyl rubbers (chloro butyl rubber: CIIR; bromo butyl rubber: BIIR) * Styrene-butadiene rubber (copolymer of styrene and butadiene, SBR) * Nitrile rubber (copolymer of butadiene and acrylonitrile, NBR), also called Buna N rubbers ** Hydrogenated nitrile rubbers (HNBR) Therban and Zetpol
'''Saturated rubbers''' that cannot be cured by sulfur vulcanization: * EPM (ethylene propylene rubber, a copolymer of ethene and propene) and EPDM rubber (ethylene propylene diene rubber, a terpolymer of ethylene, propylene and a diene-component) * Epichlorohydrin rubber (ECO) * Acrylic rubber (ACM, ABR) * Silicone rubber (SI, Q, VMQ) * Fluorosilicone rubber (FVMQ) * Fluoroelastomers (FKM, and FEPM) Viton, Tecnoflon, Fluorel, Aflas and Dai-El * Perfluoroelastomers (FFKM) Tecnoflon PFR, Kalrez, Chemraz, Perlast * Polyether block amides (PEBA) * Chlorosulfonated polyethylene (CSM) * Ethylene-vinyl acetate (EVA)
'''Various other types of elastomers''': * Thermoplastic elastomers (TPE) * The proteins resilin and elastin * Polysulfide rubber * Elastolefin, elastic fiber used in fabric production * Poly(dichlorophosphazene), an "inorganic rubber" from hexachlorophosphazene polymerization
== Shear deformation == Crosslinking most likely occurs in an equilibrated polymer without any solvent. The free energy expression derived from the Neo-Hookean model of rubber elasticity is in terms of free energy change due to deformation per unit volume of the sample. The strand concentration, v, is the number of strands over the volume which does not depend on the overall size and shape of the elastomer.<ref>{{Cite journal |last1=Boczkowska |first1=Anna |last2=Awietjan |first2=Stefan F. |last3=Pietrzko |first3=Stanisław |last4=Kurzydłowski |first4=Krzysztof J. |date=2012-03-01 |title=Mechanical Properties of Magnetorheological Elastomers under Shear Deformation |url=https://www.sciencedirect.com/science/article/pii/S135983681100360X |journal=Composites Part B: Engineering |volume=43 |issue=2 |pages=636–640 |doi=10.1016/j.compositesb.2011.08.026 |issn=1359-8368 |url-access=subscription }}</ref> Beta relates the end-to-end distance of polymer strands across crosslinks over polymers that obey random walk statistics.
<math>\Delta f_d = \frac{\Delta F_d}{V} = \frac{K_BT\nu_{el}\beta\lambda_1p^2 + \lambda_2p + 2\lambda_3p^2 - 3}{2}</math>
<math>v_{el} = \frac{n_{el}}{V} , \beta = 1</math>
{{Clarify|reason=The parameters in the formulas above need explanation.|date=September 2024}}
In the specific case of shear deformation, the elastomer besides abiding to the simplest model of rubber elasticity is also incompressible. For pure shear we relate the shear strain, to the extension ratios lambdas. Pure shear is a two-dimensional stress state making lambda equal to 1, reducing the energy strain function above to:
<math>\Delta f_{d}= \frac{k_{B}T\nu_{s}\beta\gamma^2}{2}</math>
To get shear stress, then the energy strain function is differentiated with respect to shear strain to get the shear modulus, G, times the shear strain:
<math>\sigma_{12} = \frac{d(\Delta f_{d})}{d\gamma} = G\gamma</math>
Shear stress is then proportional to the shear strain even at large strains.<ref>{{Cite journal |last1=Liao |first1=Guojiang |last2=Gong |first2=Xinglong |last3=Xuan |first3=Shouhu |date=2013-09-01 |title=Influence of Shear Deformation on the Normal Force of Magnetorheological Elastomer |url=https://www.sciencedirect.com/science/article/pii/S0167577X13006836 |journal=Materials Letters |volume=106 |pages=270–272 |doi=10.1016/j.matlet.2013.05.035 |bibcode=2013MatL..106..270L |issn=0167-577X |url-access=subscription }}</ref> Notice how a low shear modulus correlates to a low deformation strain energy density and vice versa. Shearing deformation in elastomers, require less energy to change shape than volume.
<math>\Delta f_d = W = \frac{G(\lambda_{1p}^2+\lambda_{2p}^2+\lambda_{3p}^2-3)}{2}</math>
==See also== * Rubber elasticity
==References== {{Reflist}}
==External links== * [http://www.listdryprocessing.com/fileadmin/user_upload/download/publications/2014-9_Article___Ad_CPRJ-E.pdf Efficient and eco-friendly polymerization of elastomers, By Andreas Diener, Product Manager at List AG]
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Category:Elastomers Category:Materials science Category:Polymer physics