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The complex with highest magnitude of crystal field splitting energy $$(\Delta_0)$$ is
The magnitude of Crystal Field Splitting Energy in octahedral complexes ($$Δ_o$$) depends on several key parameters:
Electronic Configuration Profiles
Let's inspect the 3d configurations for each +3 central metal ion:
| Complex Ion | Metal Ion | Outer Configuration | d-electron count | t2g vs eg Distribution |
|---|---|---|---|---|
| $$[Ti(H_2O)_6]^{3+}$$ | $$Ti^{3+}$$ | $$3d^1$$ | 1 | $$t_{2}g^{1} eg^0$$ |
| $$[Cr(OH_2)_6]^{3+}$$ | $$Cr^{3+}$$ | $$3d^3$$ | 3 | $$t_{2}g^{1} eg^0$$ (Half-filled t2g) |
| $$[Mn(OH_2)_6]^{3+}$$ | $$Mn^{3+}$$ | $$3d^4$$ | 4 | $$t_{2}g^{3} eg^1$$ |
| $$[Fe(OH_2)_6]^{3+}$$ | $$Fe^{3+}$$ | $$3d^5$$ | 5 | $$t_{2}g^{3} eg^2$$ |
Why Chromium ($$Cr^{3+}$$) possesses the Maximum $$Δ_o$$
As we move from left to right along the 3d period ($$Ti^{3+} → V^{3+} → Cr^{3+}$$), the effective nuclear charge (Zeff) increases steadily while the ionic radius decreases. This contraction pulls the $$H_2O$$ ligands closer to the metal nucleus, resulting in progressively stronger repulsions and a larger splitting value ($$Δ_o$$).
However, past $$Cr^{3+}$$ (d3), electrons begin entering the high-energy eg orbitals (as seen in $$Mn^{3+}$$ (d4) and $$Fe^{3+}$$ (d5)). Electrons in eg orbitals point directly along the axes toward the incoming ligands, providing shielding that increases the ionic radius and dampens ligand-metal proximity. Thus, $$Δ_o$$drops sharply after the d3 point.
Therefore, the d3 configuration of Cr3+ marks the absolute peak value for $$Δ_o$$among hexaaqua trivalent ions of the first transition series.
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