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Diamond and graphite are two allotropes of carbon: pure forms of the same element that differ in crystalline structure.

Allotropy or allotropism (from Ancient Greek ἄλλος (allos), meaning 'other', and τρόπος (tropos), meaning 'manner, form') is the property of some chemical elements to exist in two or more different forms, in the same physical state, known as allotropes of the elements. Allotropes are different structural modifications of an element;[1] the atoms of the element are bonded together in a different manner. For example, the allotropes of carbon include diamond (the carbon atoms are bonded together in a tetrahedral lattice arrangement), graphite (the carbon atoms are bonded together in sheets of a hexagonal lattice), graphene (single sheets of graphite), and fullerenes (the carbon atoms are bonded together in spherical, tubular, or ellipsoidal formations). The term allotropy is used for elements only, not for compounds. The more general term, used for any crystalline material, is polymorphism. Allotropy refers only to different forms of an element within the same phase (i.e.: solid, liquid or gas states); differences in these states alone would not constitute examples of allotropy.

For some elements, allotropes have different molecular formulae despite difference in phase; for example, two allotropes of oxygen (dioxygen, O2, and ozone, O3) can both exist in the solid, liquid and gaseous states. Other elements do not maintain distinct allotropes in different phases; for example, phosphorus has numerous solid allotropes, which all revert to the same P4 form when melted to the liquid state.


The concept of allotropy was originally proposed in 1841 by the Swedish scientist Baron Jöns Jakob Berzelius (1779–1848).[2] The term is derived from Greek, Modern άλλοτροπἱα (allotropia), meaning 'variability, changeableness'.[3] After the acceptance of Avogadro's hypothesis in 1860, it was understood that elements could exist as polyatomic molecules, and two allotropes of oxygen were recognized as O2 and O3.[2] In the early 20th century, it was recognized that other cases such as carbon were due to differences in crystal structure.

By 1912, Ostwald noted that the allotropy of elements is just a special case of the phenomenon of polymorphism known for compounds, and proposed that the terms allotrope and allotropy be abandoned and replaced by polymorph and polymorphism.[2] Although many other chemists have repeated this advice, IUPAC and most chemistry texts still favour the usage of allotrope and allotropy for elements only.[4]

Differences in properties of an element's allotropes[edit]

Allotropes are different structural forms of the same element and can exhibit quite different physical properties and chemical behaviours. The change between allotropic forms is triggered by the same forces that affect other structures, i.e., pressure, light, and temperature. Therefore, the stability of the particular allotropes depends on particular conditions. For instance, iron changes from a body-centered cubic structure (ferrite) to a face-centered cubic structure (austenite) above 906 °C, and tin undergoes a modification known as tin pest from a metallic form to a semiconductor form below 13.2 °C (55.8 °F). As an example of allotropes having different chemical behaviour, ozone (O3) is a much stronger oxidizing agent than dioxygen (O2).

List of allotropes[edit]

Typically, elements capable of variable coordination number and/or oxidation states tend to exhibit greater numbers of allotropic forms. Another contributing factor is the ability of an element to catenate.

Examples of allotropes include:


Element Allotropes
  • Diamond – an extremely hard, transparent crystal, with the carbon atoms arranged in a tetrahedral lattice. A poor electrical conductor. An excellent thermal conductor.
  • Lonsdaleite – also called hexagonal diamond.
  • Graphene - is the basic structural element of other allotropes, nanotubes, charcoal, and fullerenes.
  • Q-carbon – a ferromagnetic, tough, and brilliant crystal structure that is harder and brighter than diamonds.[dubious ]
  • Graphite – a soft, black, flaky solid, a moderate electrical conductor. The C atoms are bonded in flat hexagonal lattices (graphene), which are then layered in sheets.
  • Linear acetylenic carbon (Carbyne)
  • Amorphous carbon
  • Fullerenes, including Buckminsterfullerene, a.k.a. "buckyballs", such as C60.
  • Carbon nanotubes – allotropes of carbon with a cylindrical nanostructure.
  • Sulfur has a large number of allotropes, second only to carbon
  • "Red selenium," cyclo-Se8
  • Gray selenium, polymeric Se
  • Black selenium, irregular polymeric rings up to 1000 atoms long
  • Monoclinic selenium, dark red transparent crystals


Element Allotropes
  • Amorphous boron – brown powder – B12 regular icosahedra
  • α-rhombohedral boron
  • β-rhombohedral boron
  • γ-orthorhombic boron
  • α-tetragonal boron
  • β-tetragonal boron
  • High-pressure superconducting phase
  • Yellow arsenic – molecular non-metallic As4, with the same structure as white phopshorus
  • Gray arsenic, polymeric As (metalloid)
  • Black arsenic – molecular and non-metallic, with the same structure as red phosphorus
  • α-germanium – semimetallic, with the same structure as diamond
  • β-germanium – metallic, with the same structure as beta-tin
  • Germanene - Buckled planar Germanium, similar to graphene
  • blue-white antimony – stable form (metalloid), with the same structure as gray arsenic
  • yellow antimony (non-metallic)
  • black antimony (non-metallic)
  • explosive antimony
  • amorphous tellurium - gray-black or brown powder[5]
  • crystalline tellurium - hexagonal crystalline structure (metalloid)


Among the metallic elements that occur in nature in significant quantities (56 up to U, without Tc and Pm), almost half (27) are allotropic at ambient pressure: Li, Be, Na, Ca, Ti, Mn, Fe, Co, Sr, Y, Zr, Sn, La, Ce, Pr, Nd, Sm, Gd, Tb, Dy, Yb, Hf, Tl, Th, Pa and U. Some phase transitions between allotropic forms of technologically relevant metals are those of Ti at 882 °C, Fe at 912 °C and 1394 °C, Co at 422 °C, Zr at 863 °C, Sn at 13 °C and U at 668 °C and 776 °C.

Element Allotropes
  • grey tin (alpha tin, Tin pest)
  • white tin (beta tin)
  • rhombic tin (gamma tin)
  • stanene
  • sigma tin (forms at very high pressure)[6]
  • ferrite (α-iron): the ferromagnetic form at T < 770 °C (the Curie point, TC); BCC crystal structure
  • β-iron: T = 770 – 912 °C; the paramagnetic form of α-iron; same structure as α
  • austenite (γ-iron): 912 – 1,394 °C; FCC crystal structure
  • δ-iron: 1,394 – 1,538 °C; forms from cooling down molten iron; same structure as α
  • ε-iron (also called hexaferrum): forms at high pressures; HCP crystal structure

Lanthanides and actinides[edit]

Phase diagram of the actinide elements.


In 2017, the concept of nanoallotropy was proposed by Prof. Rafal Klajn of the Organic Chemistry Department of the Weizmann Institute of Science.[8] Nanoallotropes, or allotropes of nanomaterials, are nanoporous materials that have the same chemical composition (e.g., Au), but differ in their architecture at the nanoscale (that is, on a scale 10 to 100 times the dimensions of individual atoms).[9] Such nanoallotropes may help create ultra-small electronic devices and find other industrial applications.[9] The different nanoscale architectures translate into different properties, as was demonstrated for surface-enhanced Raman scattering performed on several different nanoallotropes of gold.[8] A two-step method for generating nanoallotropes was also created.[9]

See also[edit]


  1. ^ IUPAC, Compendium of Chemical Terminology, 2nd ed. (the "Gold Book") (1997). Online corrected version:  (2006–) "Allotrope". doi:10.1351/goldbook.A00243
  2. ^ a b c Jensen, W. B. (2006), "The Origin of the Term Allotrope", J. Chem. Educ., 83 (6): 838–39, Bibcode:2006JChEd..83..838J, doi:10.1021/ed083p838.
  3. ^ "allotropy", A New English Dictionary on Historical Principles, 1, Oxford University Press, 1888, p. 238.
  4. ^ Jensen 2006, citing Addison, W. E. The Allotropy of the Elements (Elsevier 1964) that many have repeated this advice.
  5. ^ Raj, G. Advanced Inorganic Chemistry Vol-1. Krishna Prakashan. p. 1327. ISBN 9788187224037. Retrieved January 6, 2017.
  6. ^ Molodets, A. M.; Nabatov, S. S. (2000). "Thermodynamic Potentials, Diagram of State, and Phase Transitions of Tin on Shock Compression". High Temperature. 38 (5): 715–721. doi:10.1007/BF02755923.
  7. ^
  8. ^ a b Udayabhaskararao, Thumu; Altantzis, Thomas; Houben, Lothar; Coronado-Puchau, Marc; Langer, Judith; Popovitz-Biro, Ronit; Liz-Marzán, Luis M.; Vuković, Lela; Král, Petr (2017-10-27). "Tunable porous nanoallotropes prepared by post-assembly etching of binary nanoparticle superlattices". Science. 358 (6362): 514–518. Bibcode:2017Sci...358..514U. doi:10.1126/science.aan6046. ISSN 0036-8075. PMID 29074773.
  9. ^ a b c "Materials That Don't Exist in Nature Might Lead to New Fabrication Techniques". Retrieved 2017-12-08.


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