Fe(II)-polypyridines have limited applications as chromophores in dye-sensitized solar cells due to the short lifetimes (similar to 100 fs) of their photoactive metal-to-ligand charge transfer (MLCT) states formed upon photoexcitation. Recently, a 100-fold increase in the MLCT lifetime was observed in a [Fe(CNC)(2)](2+) complex (CNC = 2,6-bis(3-methylimidazole-1-ylidine)pyridine) which has strong sigma-donating N-heterocyclic carbene ligand in comparison to the weaker field parent [Fe(tpy)(2)](2+) complex (tpy = 2,2':6',2 ''-terpyridine). This study utilizes density functional theory (DFT), time-dependent DFT, and quantum dynamics simulations to investigate the interfacial electron transfer (IET) in [Fe(cCNC)(2)](2+) (cCNC = 4'-carboxy-2,6-bis(3-methylimidazole-1-ylidine)pyridine) and [Fe(ctpy)(2)](2+) (ctpy = 4'-carboxy2,2':6',2 ''-terpyridine) sensitized TiO2. Our results suggest that the replacement of tpy by CNC ligand does not significantly speed up the IET kinetics in the [Fe(cCNC)(2)](2+) TiO2 assembly in comparison to the [Fe(ctpy)(2)](2+) TiO2 analogue. The high IET efficiency in the [Fe(cCNC)(2)](2+) TiO2 assemblies is therefore due to longer lifetime of [Fe(cCNC)(2)](2+) photoactive (MLCT)-M-3 states rather than faster electron injection kinetics. It was also found that the inclusion of conformational sampling in the computational model is important for proper description of the IET processes in these systems, as the models relying on the use of only fully optimized structures may yield misleading results. The simulations presented in this work also illustrate various pitfalls of utilizing properties such as electronic coupling, number of available acceptor states, and driving force, as well as calculations based on Fermi's golden rule framework, to reach conclusions on the IET efficiency in dye-semiconductor systems.