Stereoisomers express different physiological properties; thus, stereocontrol is important in the synthesis of natural products and pharmaceuticals. The search for stereoselective reaction conditions [1, 2] and the development of stereoselective reducing agents [3], which are similarly required in the reduction of carbonyls, could be efficiently performed by a model that explains reduction selectivity. Cram pioneered the qualitative explanation of diastereoreductive selectivity by ranking the bulk of substituents for carbonyl compounds with a chiral point at the α-position [4] ; Cram's method was further developed by Felkin et al. to incorporate stereoelectronic effects. Given the qualitative nature of the prediction of reductive selectivity by these methods, we attempted to quantitatively predict the diastereoreductive selectivity of ketones by quantifying steric hindrance in this study.
Quantification of steric hindrance has been addressed from three aspects: experimental, quantum chemical, and geometric calculations. Taft et al. defined the parameter Es for substituent bulkiness based on esterification and hydrolysis rates [5]. Es has been developed by Hancock et al. and Duboi et al. into Esc, which accounts for the effect of superconjugation [6], and Es', which is evaluated from a single reaction, [7], respectively Fujita et al. devised a method to express the Esc of a substituent represented by CR1R2R3 by a linear combination of the Esc of R1, R2, and R3, respectively [8]. Kirilyuk et al. quantified the steric hindrance of substituents around the nitroxide radical by measuring the half-life of the radical [9]. In the reduction of carbonyls, Wigfiel calculated the steric hindrance of the reaction for each substituent of cyclohexanone analogues and predicted the selectivity of diastereoreduction with NaBH4 in iPrOH solvent [10]. In addition, Sun et al. quantified the relationship between ring size and steric hindrance in cycloalkanes by the reduction rate of cycloalkyl phenyl ketones with NaBH4 [11]. Murugan quantified the steric hindrance of cyclohexanone analogues by calculating constants for each substituent type and position [12]. These experimental methods are superior in that they reflect real systems; however, prediction is conducted based on experimental values of substrates with similar structures with minimal extrapolation.
We computationally calculated the activation enthalpies \({\Delta }{{H}_{1}}^{‡}\) and \({\Delta }{{H}_{2}}^{‡}\) of the reaction of radical addition to two olefins with different steric hindrance, respectively, and defined the difference in activation enthalpies as a dynamic parameter of steric hindrance (DPSH) and evaluate steric hindrance at the reaction point of radicals [13]. In the reduction of carbonyls, transition state calculations have been used to predict the selectivity of diastereoreduction with NaBH4 in MeOH solvent [14]. While experimental methods can only be applied to real molecules, quantum chemical calculations can be performed on virtual molecules, whereas experimental methods can only be applied to real molecules. However, quantum chemical methods for determining transition states are difficult to apply uniformly to a large number of systems because the increase in the number of atoms to be considered often causes problems in ensuring the validity of the initial configuration and the convergence of the calculations.
Tolman et al. evaluated steric hindrance in phosphorus ligands of metal complexes using the Tolman cone angle, which is the angle at the top of the cone circumscribed to the ligand [15]. Hirota et al. assumed a light source in a molecule and developed a method to calculate the shadow area created when light emitted from the light source is blocked by the surrounding atoms [16]. Tomilin et al. considered a virtual sphere centered on the reaction point of a radical and calculated the number of atoms inside the sphere [17]. Cavallo et al. used the volume occupied by atoms in the sphere to evaluate steric hindrance [18]. We quantified the volume occupied by atoms in the sphere for steric hindrance of 70 different nitroxide radicals [19]. These geometric methods are superior to transition state calculations because they are computationally less expensive and are more extrapolative than experimental methods. However, these methods are difficult to interpret chemically because they do not consider specific reaction directions.
In this study, we attempted to predict the diastereoreductive selectivity of ketones by developing a model that quantifies the difference in steric hindrance based on the difference in the common volume of a virtual sphere and a substrate atom moving in both reaction directions (Moving Sphere Model, MSM). Despite the existence of kinetic approaches to quantifying steric hindrance in the reduction of carbonyls [20–23], diastereoselectivity, which is the reaction selectivity at the same reaction point in the same molecule as those in Cram's method [4], was used as the target system in this study. In contrast to the method for determining the reaction rate between substrates, the diastereoselectivity method, which reflected the reaction rate at the same reaction point, was considered to be more capable of eliminating electronic factors at the reaction point. To properly evaluate steric hindrance, we targeted substrates without heteroatoms and aromatic rings, which contribute to electrostatic effects and coordination to counter cations in the diastereoreductive selectivity of carbonyls [24]. Here, the variables of the model were optimized with experimental values so that the direction of the reductant reaction can be inferred based on experiments.