Crystal field splitting in octahedral vs tetrahedral complexes — color of transition metal compounds

hard CBSE JEE-MAIN JEE-ADVANCED JEE Advanced 2021 4 min read

Question

Using Crystal Field Theory, explain why the crystal field splitting energy (Δt\Delta_t) in a tetrahedral complex is approximately 49\frac{4}{9} of the octahedral splitting energy (Δo\Delta_o) for the same metal ion and ligand. How does this difference explain why tetrahedral complexes are rarely low-spin?

(JEE Advanced 2021, similar pattern)


Solution — Step by Step

In an octahedral complex, 6 ligands approach along the x, y, and z axes. The dz2d_{z^2} and dx2y2d_{x^2-y^2} orbitals (the ege_g set) point directly at the ligands, so they experience more repulsion and go up in energy. The dxyd_{xy}, dxzd_{xz}, dyzd_{yz} orbitals (the t2gt_{2g} set) point between the ligands, so they are lower in energy.

In a tetrahedral complex, 4 ligands approach from alternate corners of a cube. Now the t2t_2 set (dxyd_{xy}, dxzd_{xz}, dyzd_{yz}) points more toward the ligands, so they go up. The ee set (dz2d_{z^2}, dx2y2d_{x^2-y^2}) is lower. The splitting is inverted compared to octahedral.

Two reasons combine to make Δt<Δo\Delta_t < \Delta_o:

  1. Fewer ligands: Tetrahedral has 4 ligands vs 6 in octahedral. Fewer point charges means less total electrostatic interaction — splitting is weaker by a factor of roughly 4/6=2/34/6 = 2/3.

  2. No direct pointing: In a tetrahedron, none of the d-orbitals point directly at the ligands. The interaction is indirect (orbitals point between ligands, not at them), reducing splitting further by a factor of roughly 2/32/3.

Combined: Δt23×23×Δo=49Δo\Delta_t \approx \frac{2}{3} \times \frac{2}{3} \times \Delta_o = \frac{4}{9}\Delta_o

Since Δt49Δo\Delta_t \approx \frac{4}{9}\Delta_o, the crystal field splitting in tetrahedral complexes is usually too small to force electron pairing. The pairing energy PP exceeds Δt\Delta_t in almost all cases.

Result: electrons prefer to occupy higher-energy orbitals (high-spin) rather than pair up. That is why tetrahedral complexes are almost always high-spin. Low-spin tetrahedral complexes are extremely rare.

The color of transition metal complexes arises from d-d transitions — an electron absorbs visible light and jumps from a lower d-orbital set to a higher one. The energy of light absorbed equals the crystal field splitting energy.

Since Δt<Δo\Delta_t < \Delta_o, tetrahedral complexes absorb lower energy (longer wavelength) light compared to octahedral complexes of the same metal and ligand. This shifts the absorbed and transmitted colors differently.


Why This Works

Crystal Field Theory treats ligands as point charges that create an electrostatic field around the central metal ion. The five d-orbitals, which are degenerate in a free ion, split into groups based on how they orient relative to the ligand positions. The geometry dictates which orbitals face the ligands and therefore which ones go up in energy.

The 4/94/9 ratio is not just a qualitative argument — it falls out of the geometry of a tetrahedron inscribed in a cube and the angular dependence of d-orbital wavefunctions.

For JEE Advanced, remember the spectrochemical series: I<Br<Cl<F<OH<H2O<NH3<en<CN<CO\text{I}^- < \text{Br}^- < \text{Cl}^- < \text{F}^- < \text{OH}^- < \text{H}_2\text{O} < \text{NH}_3 < \text{en} < \text{CN}^- < \text{CO}. Strong-field ligands (right side) cause large Δ\Delta, leading to low-spin complexes in octahedral geometry.


Common Mistake

Students often state that “tetrahedral complexes have the same splitting pattern as octahedral but smaller.” This misses a crucial point — the splitting is inverted. In octahedral, ege_g is higher; in tetrahedral, t2t_2 is higher. Getting the energy level diagram wrong leads to incorrect electron configurations and wrong magnetic moment predictions.

Another error: assuming that color directly equals the absorbed wavelength. The color we see is the complementary color of the absorbed light. If a complex absorbs orange light, it appears blue — not orange.

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