Login / Signup

C-X Bond Activation by Palladium: Steric Shielding versus Steric Attraction.

Thomas HansenXiaobo SunMarco Dalla TiezzaWillem-Jan van ZeistJoost N P van StralenDaan P GeerkeLando P WoltersJordi PoaterTrevor A HamlinFriedrich Matthias Bickelhaupt
Published in: Chemistry (Weinheim an der Bergstrasse, Germany) (2022)
The C-X bond activation (X = H, C) of a series of substituted C(n°)-H and C(n°)-C(m°) bonds with C(n°) and C(m°) = H 3 C- (methyl, 0°), CH 3 H 2 C- (primary, 1°), (CH 3 ) 2 HC- (secondary, 2°), (CH 3 ) 3 C- (tertiary, 3°) by palladium were investigated using relativistic dispersion-corrected density functional theory at ZORA-BLYP-D3(BJ)/TZ2P. The effect of the stepwise introduction of substituents was pinpointed at the C-X bond on the bond activation process. The C(n°)-X bonds become substantially weaker going from C(0°)-X, to C(1°)-X, to C(2°)-X, to C(3°)-X because of the increasing steric repulsion between the C(n°)- and X-group. Interestingly, this often does not lead to a lower barrier for the C(n°)-X bond activation. The C-H activation barrier, for example, decreases from C(0°)-X, to C(1°)-X, to C(2°)-X and then increases again for the very crowded C(3°)-X bond. For the more congested C-C bond, in contrast, the activation barrier always increases as the degree of substitution is increased. Our activation strain and matching energy decomposition analyses reveal that these differences in C-H and C-C bond activation can be traced back to the opposing interplay between steric repulsion across the C-X bond versus that between the catalyst and substrate.
Keyphrases
  • density functional theory
  • transition metal
  • magnetic resonance
  • magnetic resonance imaging
  • room temperature
  • molecular dynamics
  • reduced graphene oxide
  • contrast enhanced