Abstract

We carried out ab initio molecular dynamic simulations in order to determine the free energy surfaces of two selected reactions including solvents, namely a rearrangement of a ruthenium oxoester in water and a carbon dioxide addition to a palladium complex in carbon dioxide. For the latter reaction we also investigated the gas phase reaction in order to take solvent effects into account. We used two techniques to reconstruct the free energy surfaces: thermodynamic integration and metadynamics. Furthermore, we gave a reasonable error estimation of the computed free energy surface. We calculated a reaction barrier of ΔF = 59.5 ± 8.5 kJ mol−1 for the rearrangement of a ruthenium oxoester in water from thermodynamic integration. For the carbon dioxide addition to the palladium complex in carbon dioxide we found a ΔF = 44.9 ± 3.3 kJ mol−1 from metadynamics simulations with one collective variable. The investigation of the same reactions in the gas phase resulted in ΔF = 24.9 ± 6.7 kJ mol−1 from thermodynamic integration, in ΔF = 26.7 ± 2.3 kJ mol−1 from metadynamics simulations with one collective variable, and in ΔF = 27.1 ± 5.9 kJ mol−1 from metadynamics simulations with two collective variables.

Highlights

  • The n-dimensional energy surface of a system with n degrees of freedom provides all information that are important for understanding the reactivity of a system

  • Helmholtz free energy surface (FES) corresponds to simulations carried out in the canonical ensemble (N,V,T), which is often applied in molecular dynamics simulations

  • In addition the auto-correlation function (ACF) of the constrained force was calculated to demonstrate the fast relaxation time compared to the simulation time

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Summary

Introduction

The n-dimensional energy surface of a system with n degrees of freedom provides all information that are important for understanding the reactivity of a system. In this work we selected two simple reactions of transition metal complexes (Figure 1) and carried out ab initio molecular dynamic simulations in order to explore their FES. To compare the order of magnitude of this barrier we carried out static quantum chemical calculations to determine the transition state of the ruthenium complex without any additional solvent molecule.

Results
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