Tetrahedral Splitting and the 4/9 Relationship

Why Δt is roughly four-ninths of Δo for the same metal and ligand

Lesson 2692 of 4,500 · Coordination Chemistry and CFT

Learning objectives

Introduction

Four ligands at the corners of a tetrahedron approach the central metal along directions between the Cartesian axes. That changes which d orbitals experience the greatest repulsion. The tetrahedral order is opposite the octahedral order, and the gap is usually smaller. The frequently used Δ t≈4Δₒ/9 is a comparison for similar metal–ligand systems, not a universal physical constant.

Core explanation

In an octahedron, ligands lie on the x, y and z axes, so d(x²−y²) and d(z²) point most directly toward them and form a higher e g pair. In a tetrahedron, no ligand lies directly on an axis. The d(xy), d(xz) and d(yz) orbitals have lobes oriented more toward the between-axis ligand directions and form the higher t₂ triplet. The d(x²−y²) and d(z²) orbitals form the lower e pair. Tetrahedral labels omit the g subscript because a tetrahedron lacks a centre of inversion.

There are fewer ligands, and none points directly along a d-orbital lobe in the same way as octahedral axial approach. The ideal electrostatic model consequently predicts a smaller gap. Under comparable metal, oxidation state and ligand assumptions, the usual estimate is Δ t≈(4/9)Δₒ. If an analogous octahedral complex has Δₒ=18,000 cm⁻¹, a first estimate is Δ t≈8,000 cm⁻¹. Real bond lengths and covalency may differ between geometries, so this arithmetic is approximate.

The barycentre still supplies an orbital-energy reference. Two lower e orbitals and three upper t₂ orbitals have weighted mean zero. If the lower shift is −a and upper shift +b, then 2a=3b and a+b=Δ t. Solving gives a=0.6Δ t and b=0.4Δ t. Therefore tetrahedral e lies at −0.6Δ t and t₂ at +0.4Δ t. These coefficients look like the octahedral ones with the signs and degeneracies exchanged; using octahedral t₂g/eg energies for a tetrahedral ion gives a wrong CFSE.

Because Δ t is relatively small, pairing an electron in e rather than occupying a higher t₂ orbital usually costs more than the orbital saving. Familiar tetrahedral transition-metal complexes are therefore ordinarily high spin. This tendency helps interpret their magnetism but should follow from the actual geometry and d count. A four-coordinate metal can also be square planar, particularly for some d⁸ ions, with a very different energy pattern.

Do not use the 4/9 ratio to compare unrelated complexes such as a 3d chloride tetrahedron with a 5d cyanide octahedron. The relation assumes corresponding metal and ligand conditions; if metal, charge or ligand changes, those effects can outweigh the simple geometry factor. Spectroscopy provides the more reliable gap for a specific real compound.

Step-by-step reasoning

Identify four-coordinate tetrahedral geometry first. Draw two lower e boxes and three higher t₂ boxes, with a vertical gap Δ t. If a corresponding octahedral Δₒ is supplied, multiply it by 4/9 only as an estimate. Fill electrons using the small-gap/high-spin tendency, then compute CFSE with tetrahedral, not octahedral, level energies.

Visual explanation

Place a tetrahedron beside an octahedron. Mark six axial directions around the octahedral metal and four diagonal directions around the tetrahedral metal. Under each, draw energy shelves: octahedral three-low/two-high with a tall gap, tetrahedral two-low/three-high with a shorter gap.

Real-world analogy

A row of bright lamps aimed directly at a performer causes stronger glare than fewer lamps angled between the performer’s sight lines. Both number and direction matter. Octahedral versus tetrahedral ligands similarly change the directional interaction with d orbitals.

Real-world example

Tetrachlorocobaltate(II), [CoCl₄]²⁻, is a familiar tetrahedral complex. Co²⁺ is d⁷ and chloride is weak field, consistent with high-spin filling. Its blue colour differs from the pink octahedral aqua Co(II) environment because the geometry and ligand set change the electronic levels.

Why?

Why is the label e instead of e g in tetrahedral symmetry? The subscript g denotes even parity under inversion through the metal. A tetrahedron has no inversion centre, so that classification is unavailable, even though two orbitals still form the lower set.

Common misconception

“Δ t=4Δₒ/9 for every pair of tetrahedral and octahedral compounds.” It is an idealised same-metal, same-ligand comparison. Bond lengths, oxidation state, ligand identity and covalency can make real ratios differ.

Worked example

Estimate tetrahedral splitting if an analogous octahedral complex has Δₒ=22,500 cm⁻¹. Δ t≈(4/9)(22,500)=10,000 cm⁻¹. The tetrahedral lower e level is at −0.6Δ t≈−6,000 cm⁻¹ and upper t₂ at +0.4Δ t≈+4,000 cm⁻¹ relative to its own barycentre. Their separation is 10,000 cm⁻¹.

Quick check

1. Which tetrahedral d-orbital set lies lower? Answer: The twofold e set lies lower than the threefold t₂ set. 2. Is tetrahedral splitting usually larger than analogous octahedral splitting? Answer: No. It is usually smaller, often estimated as roughly four-ninths as large.

Exam focus

Use the correct e/t₂ labels and degeneracies. State the 4/9 relation as approximate, and do not compare gaps from unrelated metals or ligands as if only geometry changed.

Advanced insight

The 4/9 estimate arises from idealised angular and coordination-number effects in the simple point-charge picture. Actual ligand-field parameters reflect metal–ligand distances and orbital mixing; those details can shift Δ t/Δₒ away from the textbook ratio.

Summary

Tetrahedral ligands produce lower e and upper t₂ levels, with a usually smaller gap Δ t. For comparable systems, Δ t is often estimated as 4Δₒ/9. The reversed level order and small gap favour high-spin fillings.

Practice questions

1. A corresponding octahedral gap is 27,000 cm⁻¹. Estimate Δ t. Answer: Using the approximate relation, Δ t≈(4/9)(27,000)=12,000 cm⁻¹, provided metal and ligand conditions are comparable. 2. Derive the tetrahedral lower level shift from the barycentre rule. Answer: Let lower e be −a and upper t₂ be +b. Then 2a=3b and a+b=Δ t, giving a=0.6Δ t, so e is at −0.6Δ t. 3. Why are tetrahedral transition-metal complexes commonly high spin? Answer: Their relatively small Δ t usually makes promotion to an upper t₂ orbital less costly than adding a pair in the lower e set.