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Exercises · 5.22

Q.Discuss the nature of bonding in metal carbonyls.

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Metal carbonyls use a synergistic bonding mechanism: a σ-dative bond from CO's lone pair to the metal, plus π-backbonding from filled metal d-orbitals to CO's empty π* orbitals. This dual interaction strengthens the metal–carbon bond while weakening the C≡O bond, shifting its IR stretching frequency to lower wavenumbers.

The Concept: Why CO Binds So Well to Metals

Carbon monoxide is a remarkable ligand. At first glance, it seems like a poor electron donor — the carbon atom carries a slight positive charge in the resonance structure C−≡O+\overset{-}{\mathrm{C}}\equiv\overset{+}{\mathrm{O}}. Yet CO forms exceptionally stable complexes with transition metals in low oxidation states. The secret lies in a beautifully cooperative bonding scheme that no single interaction could achieve alone.

Think of it as a handshake that turns into a mutual embrace. The metal and CO each give something, and each receive something back — creating a bond far stronger than either contribution alone would suggest.

Step-by-Step Bonding Analysis

1. The σ-dative bond: CO as a Lewis base

The carbon atom in CO has a lone pair in a sp-hybrid orbital. This lone pair donates electron density into an empty σ-acceptor orbital on the metal (typically a dz2_{z^2} or hybrid s-d orbital). This is a conventional coordinate covalent bond — the ligand gives, the metal receives.

But here's the puzzle: if this were the only interaction, CO would be a weak σ-donor compared to ligands like NH3_3 or H2_2O. The carbon's lone pair is in a relatively electronegative environment. Something else must be at work.

2. The π-backbond: Metal returns the favour

Transition metals in low oxidation states (0, +1, +2) have filled d-orbitals of π-symmetry (typically dxz_{xz}, dyz_{yz}). CO has empty π* antibonding orbitals of matching symmetry. The metal donates electron density from its filled d-orbitals into these empty π* orbitals on CO.

This is called π-backbonding or π-backdonation. It's the second half of the handshake.

3. The synergy: Each bond strengthens the other

Here's the elegant part — these two interactions are not independent. They reinforce each other:

  • The σ-donation makes the metal more electron-rich, which enhances its ability to π-backdonate.
  • The π-backdonation removes electron density from the metal, making it a better σ-acceptor for the next CO molecule.

This mutual reinforcement is called synergic bonding. It's why metal carbonyls are so stable and why CO can bind so strongly even to metals that are already electron-rich.

Tip

A quick way to remember: σ-donation flows from CO to metal; π-backdonation flows from metal to CO. The arrows point in opposite directions, but they work together.

4. Effect on the C≡O bond

The π* orbitals of CO are antibonding with respect to the C–O bond. When the metal fills these orbitals with electrons, it weakens the C≡O triple bond. The bond order drops from 3 towards something closer to 2.5 or 2, depending on the extent of backbonding.

This has a measurable consequence: the C≡O stretching frequency in the IR spectrum shifts to lower wavenumbers. Free CO absorbs at ~2143 cm−1^{-1}. In metal carbonyls, this drops to the range 2100–1800 cm−1^{-1}, with lower frequencies indicating stronger π-backbonding.

Watch out

A common mistake is to think that stronger metal–CO bonding always means a higher C≡O stretching frequency. In fact, the opposite is true: stronger backbonding lowers the C≡O frequency because it weakens the C–O bond. Don't confuse the metal–ligand bond strength with the internal ligand bond strength.

5. Factors that influence backbonding

FactorEffect on backbondingIR shift
Lower metal oxidation stateMore electron density on metal → stronger backbondingLower νCO\nu_{\mathrm{CO}}

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