Inorganic VII

Chapters / Chapter 1 · Solid state / Topic 14 of 14

Normal and inverse spinel: CFSE

Chapter 1 · Solid state and crystal structures

Octahedraleg (+0.6 Delt_o)t2g (-0.4 Delt_o)Delt_od3: t2g3, CFSE = 1.2 Delt_od5 high spin: CFSE = 0Tetrahedralt2 (+0.4 Delt_t)e (-0.6 Delt_t)Delt_t = 4/9 Delt_oSplitting is invertedand smaller than oct.
Octahedral splitting is larger and inverted relative to tetrahedral splitting.

This is the page in the photograph you sent. It is the last page of the notes, and it states the rule that decides normal against inverse spinel.

From the notes, transcribed: “This generally takes place [in] transition metal oxide. Generally the site selection is governed by the relative change of CFSE (Crystal Field Stabilization Energy) in occupying the Oct and Td holes.”

The crossed-out words in the photograph are “crystal” (before CFSE) and “octa” (before “oct”). The sentence is about spinel oxides, AB2O4.

Normal spinel

Named after the mineral spinel, MgAl2O4. It consists of a ccp array of oxide ions in which the divalent metal ion (Mg2+) occupies 1/8 of the tetrahedral holes and the trivalent metal ion (Al3+) occupies 1/2 of the octahedral holes. In a ccp anion sublattice there is one octahedral hole and two tetrahedral holes per anion. There are four oxides per formula unit, and consequently four octahedral holes and eight tetrahedral holes.

Normal: (AII)tet (BIII)2oct O4

Inverse spinel

In an inverse spinel, half of the B ions occupy 1/8 of the tetrahedral holes, and A and the other half of B occupy 1/2 of the octahedral holes in the ccp array of O2−.

Inverse: BIII tet [ AII BIII ]oct O4
Normal spinel (A)tet(B)2oct O4A2+B3+B3+Td hole (1/8 filled) - Oct holes (1/2 filled)MgAl2O4, ZnFe2O4, Mn3O4Inverse spinel B(AB)O4B3+A2+B3+Td: B3+ - Oct: A2+ + B3+Fe3O4, CoFe2O4, NiFe2O4O2- forms a ccp / fcc array in both cases.
Normal against inverse: which cation sits in which hole.

Why CFSE decides it

For transition-metal oxide spinels, O2− is a weak-field ligand, so the ions are usually high spin. The structure that forms is the one with the larger total CFSE. The octahedral site preference energy (OSPE) is CFSE(oct) − CFSE(tet), with Δt = 4/9 Δo. Its size depends on the d-electron count:

d count (high spin)CFSE oct (Δo)CFSE tet (Δo)OSPE (Δo)
d0, d5, d10000
d1, d60.400.270.13
d2, d70.800.530.27
d3, d81.200.360.84
d4, d90.600.180.42

So d3 and d8 have the strongest octahedral preference, d0, d5 and d10 have none, and the rest fall in between.

Worked examples from the notes

SpinelDistributionWhy
MgAl2O4NormalBoth non-transition metals; CFSE = 0. The more highly charged Al3+ prefers the octahedral site.
ZnFe2O4NormalZn2+ is d10 and Fe3+ is d5; both have zero CFSE, and small Zn2+ fits the tetrahedral site.
Mn3O4NormalMn2+ is high-spin d5 (CFSE 0); Mn3+ is d4 and takes the octahedral site.
Fe3O4Inverse: Fe3+[Fe2+Fe3+]O4Fe3+ is d5 (CFSE 0 in either site); Fe2+ is d6 and prefers octahedral.
CoFe2O4, NiFe2O4InverseCo2+ (d7) and Ni2+ (d8) have a strong octahedral preference over Fe3+ (d5).
FeCr2O4NormalCr3+ is d3, with the largest octahedral preference (0.84 Δo).
Co3O4NormalCo3+ is low-spin d6 with very high CFSE in the octahedral site.

Verified

The rule on this page is correct and is the standard explanation: for transition-metal oxide spinels, normal against inverse is driven primarily by the CFSE of the ions in tetrahedral and octahedral sites. The worked examples above follow the same rule, with the OSPE values taken from the standard high-spin table.