Electron-transfer (ET) reactions are among the most fundamental chemical processes and are crucial in a number of important biological processes, such as photosynthesis and cell respiration. [1] Nature and chemists alike have been tuning electron-donor and -acceptor sites or their environments to obtain ET rates and relative donor-acceptor stabilities that are optimized for a particular task. Herein, we report an atomistic theoretical approach based on molecular-dynamics simulations and density functional theory to predict quantitatively the effects of such modifications on the parameters that control ET. This work confirms recent experiments [2] that highlight the role of hydrogen-bonding interactions in ET processes. We have investigated the redox properties of substituted quinones in methanol (MeOH) as a prototypical hydrogen-bonding solvent and in acetonitrile (MeCN) as a solvent with similar dielectric properties but without the specific hydrogen-bonding interactions. In view of their biological importance, it is not surprising that quinones are often employed in electrochemical experiments and that the effects of the solvent and substituents on the redox properties have been well characterized. [3][4][5][6][7][8][9][10] We employed 1,4-benzoquinone (BQ) and 2,3,5,6-tetramethylbenzoquinone (duroquinone, DQ) in this study.A key step in the understanding of ET reactions was the formulation by Marcus [11,12] of the rate of ET (k ET ) as a function of the reaction free energy DG and l, that is, the sum of the inner (l i ) and outer (l o ) sphere reorganization energies [Eq. (1)], in which k is a proportionality constant that depends on the donor and acceptor quantum coupling, T the temperature, and k B the Boltzmann constant. Furthermore, Marcus also derived an approximate expression for l o that provides insight into the nature of the reorganization energy for simple solutes in a homogeneous environment. Based on continuum theory, it provides the nonspecific solvent reorganization energy l s as a function of the effective radii of the donor and the acceptor (r D and r A ), their distance of separation r, the solvent refractive index n D , and the relative permittivity e r [Eq. (2)]. In this work, we obtain estimates for DG and l beyond the continuum approximation by using atomistic simulations.In simulation, the free-energy difference between the oxidized and reduced states of a system can be computed exactly from ensemble averages on the basis of the vertical ionization energy (DE). [13][14][15][16][17][18][19] Such an ensemble average can be computed by using molecular-dynamics (MD) simulations. Herein, we have employed a computationally straightforward, but approximate formula for the free-energy difference DA. This formula can be derived [13][14][15] if the atomistic equivalent of the parabolic functions derived from Marcus theory, which depict the assumed harmonic dependence of the free energy on the vertical energy gap, is introduced as an approximation. This atomistic equivalent is the premise that DE fl...