In this study
ab initio Car–Parrinello molecular dynamics simulations, extended transition state (ETS)‐natural orbitals for chemical valence (NOCV) and QTAIM bonding analyses, were performed to characterize the ansa‐bridged molybdocene complexes [(C
5H
4)
2XMe
2MoH
3]
+ for X = C, Si, Ge, Sn, Pb, and nonbridged Cp
2MoH system. The results have shown that the [(C
5H
4)
2CMe
2MoH(H
2)]
+ complex exhibits nonclassical dihydrogen/hydride (H
2/H) conformation (97.6% of time of simulation), contrary to trihydride (H
3) structure noted for nonbridged Cp
2MoH (86.9%) and ansa‐bridged [(C
5H
4)
2SnMe
2MoH
3]
+ (84.8%), [(C
5H
4)
2PbMe
2MoH
3]
+ (84.9%) systems. Further, [(C
5H
4)
2SiMe
2MoH
3]
+ and [(C
5H
4)
2GeMe
2MoH
3]
+ complexes, appeared to exist in both conformations (H
2/H—55.4%, H
3—44.6% for Si‐based system and H
2/H—36.2%, H
3—63.8 % for germanium congener). It has been proven that the “steric availability” of the metal center, measured by the changes in the Cp? Mo? Cp angle (α), determines the existence of a given conformation—namely, the smaller value of the angle (molybdenum is sterically more accessible) the larger preference for the formation of dihydrogen/hydride structure. ETS‐NOCV method allowed to conclude that increase in the Cp? Mo? Cp angle (from α ca. 120° to α ca. 150°) leads to the enhancement of donation from H
2 and back‐donation from Mo to the σ*(H? H), what consequently leads to breaking of the H? H bond and formation of the trihydride structure. Systematical increase in the charge depletion from the σ‐bonding orbital of H
2 can be related to the reduction of the energy gap between the major orbitals involved in this contribution, namely highest occupied molecular orbital (HOMO) of H
2 with lowest unoccupied molecular orbital (LUMO) of [MoHL]
+; Δ
E = 0.0868 a.u. [for L =(C
5H
4)
2C], Δ
E = 0.0827a.u. [for L = (C
5H
4)
2Si] Δ
E = 0.0638 a.u. [for L = Cp
2]. Further, the relatively low energetic barrier to hydrogen exchange (Δ
E# = 3.3 kcal/mol) for carbon‐bridged complex, [(C
5H
4)
2CMe
2MoH
c(H
aH
b)]
+ → [(C
5H
4)
2 CMe
2MoH
a(H
bH
c)]
+, is related to strengthening of the Mo–H bonds when going from the substrate to the transition state (TS). Notably higher barrier to hydrogen rotation (Δ
E# = 10.1 kcal/mol) in [(C
5H
4)
2CMe
2MoH(H
2)]
+ is due to lowering in the electrostatic stabilization as well as weakening of the donation (H
2 → Mo charge transfer) and practically lack‐of back‐donation (Mo → H
2) in the rotated TS. © 2012 Wiley Periodicals, Inc.
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