The metal interacts with the extra in-plane bonding system of benzyne, not by replacing the ordinary out-of-plane aromatic pi system. Take the ring and metal to lie in the plane, with the metal-to-C–C-midpoint direction along and C1–C2 along . The carbon orbitals directed toward the metal form an occupied symmetric combination and an empty antisymmetric combination.
The occupied in-plane combination donates into an empty metal orbital of matching symmetry. An occupied metal -type orbital overlaps with the in-plane combination, providing back-donation. These are the same symmetry principles as alkene binding, rotated into the plane of the ring. The carbon orbitals perpendicular to the ring continue to participate in its aromatic system. The strained formal triple bond therefore does not supply two independent, ordinary out-of-plane alkene interactions.
Strong population of the in-plane acceptor can be described as reduction of the aryne to a dianionic, metallacyclopropene-like ligand. That description emphasizes two M–C sigma bonds and loss of the extra C–C pi bond. It is particularly useful for early-metal aryne complexes. The lower panels of the orbital schematic distinguish the interacting in-plane orbitals from the perpendicular aromatic set.
A useful strongly bound limit is Zr(IV), , and Ta(V), , with an aryne dianion in each complex. Charge balance uses two Cp ligands for zirconium, and Cp* plus two methyl ligands for tantalum:
Equivalently, an unreduced neutral-aryne description starts from Zr(II) and Ta(III), both , and transfers that pair strongly into the aryne acceptor. These are alternative bookkeeping limits for the same covalent interaction; saying that a formal assignment has no available electrons must not erase the strong metal–carbon bonds in the reduced-ligand description.
Both ligands have therefore lost much of the extra in-plane C–C bonding of free benzyne and approach the same reduced, approximately double-bond-length C1–C2 framework. Their identical C–C distances are consistent with similar aryne reduction in both complexes. The distance is intermediate in a delocalized ring, so it should not be converted into an exact integer bond order.
The M–C distances depend additionally on metal size, effective nuclear attraction and orbital overlap. The high formal charge of Ta(V), the size effects associated with the lanthanide contraction, and effective covalent bonding favour shorter Ta–C contacts than Zr–C contacts. This is consistent with versus . Different coordination envelopes and ancillary ligands also contribute, so this pair is not a controlled measurement of a radius or a metal–carbon bond energy. Similar internal ligand bond order can coexist with different metal–ligand distances.

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