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Spinel group

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(Redirected from Spinel structure) Mineral supergroup

The spinels are any of a class of minerals of general formulation AB
2X
4 which crystallise in the cubic (isometric) crystal system, with the X anions (typically chalcogens, like oxygen and sulfur) arranged in a cubic close-packed lattice and the cations A and B occupying some or all of the octahedral and tetrahedral sites in the lattice. Although the charges of A and B in the prototypical spinel structure are +2 and +3, respectively (A
B
2X
4), other combinations incorporating divalent, trivalent, or tetravalent cations, including magnesium, zinc, iron, manganese, aluminium, chromium, titanium, and silicon, are also possible. The anion is normally oxygen; when other chalcogenides constitute the anion sublattice the structure is referred to as a thiospinel.

A and B can also be the same metal with different valences, as is the case with magnetite, Fe3O4 (as Fe
Fe
2O
4), which is the most abundant member of the spinel group. Spinels are grouped in series by the B cation.

The group is named for spinel (MgAl
2O
4), which was once known as "spinel ruby". (Today the term ruby is used only for corundum.)

Spinel group members

Members of the spinel group include:

There are many more compounds with a spinel structure, e.g. the thiospinels and selenospinels, that can be synthesized in the lab or in some cases occur as minerals.

The heterogeneity of spinel group members varies based on composition with ferrous and magnesium based members varying greatly as in solid solution, which requires similarly sized cations. However, ferric and aluminium based spinels are almost entirely homogeneous due to their large size difference.

The spinel structure

Crystal structure of spinel

The space group for a spinel group mineral may be Fd3m (the same as for diamond), but in some cases (such as spinel itself, MgAl
2O
4, beyond 452.6 K) it is actually the tetrahedral F43m.

Normal spinel structures have oxygen ions closely approximating a cubic close-packed latice with eight tetrahedral and four octahedral sites per formula unit (but eight times as many per unit cell). The tetrahedral spaces are smaller than the octahedral spaces. B ions occupy half the octahedral holes, while A ions occupy one-eighth of the tetrahedral holes. The mineral spinel MgAl2O4 has a normal spinel structure.

In a normal spinel structure, the ions are in the following positions, where i, j, and k are arbitrary integers and δ, ε, and ζ are small real numbers (note that the unit cell can be chosen differently, giving different coordinates): 

X:
(1/4-δ,   δ,     δ  ) + ((i+j)/2, (j+k)/2, (i+k)/2)
( δ,     1/4-δ,  δ  ) + ((i+j)/2, (j+k)/2, (i+k)/2)
( δ,      δ,   1/4-δ) + ((i+j)/2, (j+k)/2, (i+k)/2)
(1/4-δ, 1/4-δ, 1/4-δ) + ((i+j)/2, (j+k)/2, (i+k)/2)
(3/4+ε, 1/2-ε, 1/2-ε) + ((i+j)/2, (j+k)/2, (i+k)/2)
(1-ε,   1/4+ε, 1/2-ε) + ((i+j)/2, (j+k)/2, (i+k)/2)
(1-ε,   1/2-ε, 1/4+ε) + ((i+j)/2, (j+k)/2, (i+k)/2)
(3/4+ε, 1/4+ε, 1/4+ε) + ((i+j)/2, (j+k)/2, (i+k)/2)
A:
(1/8, 1/8, 1/8) + ((i+j)/2, (j+k)/2, (i+k)/2)
(7/8, 3/8, 3/8) + ((i+j)/2, (j+k)/2, (i+k)/2)
B:
(1/2+ζ,   ζ,     ζ  ) + ((i+j)/2, (j+k)/2, (i+k)/2)
(1/2+ζ, 1/4-ζ, 1/4-ζ) + ((i+j)/2, (j+k)/2, (i+k)/2)
(3/4-ζ, 1/4-ζ,   ζ  ) + ((i+j)/2, (j+k)/2, (i+k)/2)
(3/4-ζ,   ζ,   1/4-ζ) + ((i+j)/2, (j+k)/2, (i+k)/2)

The first four X positions form a tetrahedron around the first A position, and the last four form one around the second A position. When the space group is Fd3m then δ=ε and ζ=0. In this case, a three-fold rotoinversion with axis in the 111 direction is centred on the point (0, 0, 0) (where there is no ion) and can also be centred on the B ion at (1/2, 1/2, 1/2), and in fact every B ion is the centre of a three-fold rotoinversion (point group D3d). Under this space group the two A positions are equivalent. If the space group is F43m then the three-fold rotoinversions become simple three-fold rotations (point group C3v) because the inversion disappears, and the two A positions are no longer equivalent.

Every ion is on at least three mirror planes and at least one three-fold rotation axis. The structure has tetrahedral symmetry around each A ion, and the A ions are arranged just like the carbon atoms in diamond. There are another eight tetrahedral sites per unit cell that are empty, each one surrounded by a tetrahedron of B as well as a tetrahedron of X ions.

Inverse spinel structures have a different cation distribution in that all of the A cations and half of the B cations occupy octahedral sites, while the other half of the B cations occupy tetrahedral sites. An example of an inverse spinel is Fe3O4, if the Fe (A) ions are d high-spin and the Fe (B) ions are d high-spin.

In addition, intermediate cases exist where the cation distribution can be described as (A1−xBx)2O4, where parentheses () and brackets are used to denote tetrahedral and octahedral sites, respectively. The so-called inversion degree, x, adopts values between 0 (normal) and 1 (inverse), and is equal to 2⁄3 for a completely random cation distribution.

The cation distribution in spinel structures are related to the crystal field stabilization energies (CFSE) of the constituent transition metals. Some ions may have a distinct preference for the octahedral site depending on the d-electron count. If the A ions have a strong preference for the octahedral site, they will displace half of the B ions from the octahedral sites to tetrahedral sites. Similarly, if the B ions have a low or zero octahedral site stabilization energy (OSSE), then they will occupy tetrahedral sites, leaving octahedral sites for the A ions.

Burdett and co-workers proposed an alternative treatment of the problem of spinel inversion, using the relative sizes of the s and p atomic orbitals of the two types of atom to determine their site preferences. This is because the dominant stabilizing interaction in the solids is not the crystal field stabilization energy generated by the interaction of the ligands with the d electrons, but the σ-type interactions between the metal cations and the oxide anions. This rationale can explain anomalies in the spinel structures that crystal-field theory cannot, such as the marked preference of Al cations for octahedral sites or of Zn for tetrahedral sites, which crystal field theory would predict neither has a site preference. Only in cases where this size-based approach indicates no preference for one structure over another do crystal field effects make any difference; in effect they are just a small perturbation that can sometimes affect the relative preferences, but which often do not.

Common uses in industry and technology

Spinels commonly form in high temperature processes. Either native oxide scales of metals, or intentional deposition of spinel coatings can be used to protect base metals from oxidation or corrosion. The presence of spinels may hereby serve as thin (few micrometer thick) functional layers, that prevent the diffusion of oxygen (or other atmospheric) ions or specific metal ions such as chromium, which otherwise exhibits a fast diffusion process at high temperatures.

Further reading

References

  1. Robert J. Naumann: Introduction to the Physics and Chemistry of Materials CRC Press, 2008, ISBN 978-1-4200-6134-5. Retrieved 15 April 2018.
  2. H-J Meyer: Festkörperchemie in: H-J Meyer (ed.), Riedel Moderne Anorganische Chemie, Walter de Gruyter, 2012, ISBN 978-3-11-024900-2. Retrieved 15 April 2018.
  3. Ernst, W. G. (1969). Earth Materials (Print ed.). Englewood Cliffs, NJ: Prentice-Hall. p. 58.
  4. "ruby spinel". Encyclopædia Britannica. Retrieved 2022-11-25.
  5. Spinel group at Mindat
  6. Rawat, Pankaj Singh; Srivastava, R. C.; Dixit, Gagan; Joshi, G. C.; Asokan, K. (2019). "Facile synthesis and temperature dependent dielectric properties of MnFe2O4 nanoparticles". Dae Solid State Physics Symposium 2018. Vol. 2115. p. 030104. doi:10.1063/1.5112943. S2CID 199183122.
  7. Vestal, Christy R.; Zhang, Z. John (2003). "Effects of Surface Coordination Chemistry on the Magnetic Properties of MnFe2O4 Spinel Ferrite Nanoparticles". Journal of the American Chemical Society. 125 (32): 9828–9833. doi:10.1021/ja035474n. PMID 12904049.
  8. American Elements, Manganese Cobalt Oxide, Spinel Powder.
  9. Ernst, W. G. (1969). Earth Materials (Print ed.). Englewood Cliffs, NJ: Prentice-Hall. p. 59.
  10. Zhang, Liang; Ji, Guang-Fu; Zhao, Feng; Meng, Chuan-Min; Wei, Dong-Qing (February 2011). "The first-principle studies of the crystal phase transitions: Fd3m-MgAl2O4→F4-3m-MgAl2O4". Physica B: Condensed Matter. 406 (3): 335–338. Bibcode:2011PhyB..406..335Z. doi:10.1016/j.physb.2010.10.054.
  11. Robert John Lancashire. "Normal Spinels". CHEM2101 (C 21J) Inorganic Chemistry - Chemistry of Transition Metal Complexes. University of the West Indies. Archived from the original on 2023-08-08.
  12. N. W. Grimes; et al. (Apr 8, 1983). "New Symmetry and Structure for Spinel". Proceedings of the Royal Society of London. Series A, Mathematical and Physical Sciences. 386 (1791): 333–345. Bibcode:1983RSPSA.386..333G. doi:10.1098/rspa.1983.0039. JSTOR 2397417. S2CID 96560029.
  13. L. Hwang; et al. (Jul 1973). "On the space group of MgAl
    2O
    4 spinel"    . Philosophical Magazine. doi:10.1080/14786437308217448.
  14. Assadi, M. Hussein N.; H., Katayama-Yoshida (2019). "Covalency a Pathway for Achieving High Magnetisation in TMFe2O4 Compounds". J. Phys. Soc. Jpn. 88 (4): 044706. arXiv:2004.10948. Bibcode:2019JPSJ...88d4706A. doi:10.7566/JPSJ.88.044706. S2CID 127456231.
  15. Sickafus, Kurt E.; Wills, John M.; Grimes, Norman W. (2004-12-21). "Structure of Spinel". Journal of the American Ceramic Society. 82 (12): 3279–3292. doi:10.1111/j.1151-2916.1999.tb02241.x.
  16. See Spinel Structure in the Encyclopedia of Crystallographic Prototypes, which gives coordinates for the Fd3m case.
  17. J.K. Burdett, G.L. Price and S.L. Price (1982). "Role of the crystal-field theory in determining the structures of spinels". J. Am. Chem. Soc. 104: 92–95. doi:10.1021/ja00365a019.
  18. Hyun Park, Joo (2007). "Formation Mechanism of Spinel-Type Inclusions in High-Alloyed Stainless Steel Melts". Metallurgical and Materials Transactions B. 38 (4): 657–663. Bibcode:2007MMTB...38..657P. doi:10.1007/s11663-007-9066-x. S2CID 135979316.
  19. Rose, L. (2011). On the degradation of porous stainless steel (Thesis). University of British Columbia. pp. 144–168. doi:10.14288/1.0071732.
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