Conspectus
Interactions between sterically crowded hydrocarbon-substituted
ligands are widely considered to be repulsive because of the intrusion
of the electron clouds of the ligand atoms into each other’s
space, which results in Pauli repulsion. Nonetheless, there is another
interaction between the ligands which is less widely publicized but
is always present. This is the London dispersion (LD) interaction
which can occur between atoms or molecules in which dipoles can be
induced instantaneously, for example, between the H atoms from the
ligand C–H groups.
These LD interactions are always attractive,
but their effects
are not as widely recognized as those of the Pauli repulsion despite
their central role in the formation of condensed matter. Their relatively
poor recognition is probably due to the relative weakness (ca. 1 kcal
mol–1) of individual H···H interactions
owing to their especially strong distance dependence. In contrast,
where there are numerous H···H interactions, a collective
LD energy equaling several tens of kcal mol–1 may
ensue. As a result, in some molecules the latent importance of the
LD attraction energies emerges and assumes a prominence that can overshadow
the Pauli effects (e.g., in the stabilization of high-oxidation-state
transition-metal alkyls, inducing disproportionation reactions, or
in the stabilization of otherwise unstable bonds).
Despite being
known for over a century, the accurate quantification
of individual H···H LD effects in molecular species
is a relatively recent phenomenon and at present is based mainly on
modified DFT calculations. A few leading reviews summarized these
earlier studies of the C–H···H–C LD interactions
in organic molecules, and their effects on the structures and stabilities
were described. LD effects in sterically crowded inorganic and organometallic
molecules have been recognized.
The author’s interest
in these LD effects arose fortuitously
over a decade ago during research on sterically crowded heavier main-group
element carbene analogues and two-coordinate, open-shell (d1–d9) transition-metal complexes where counterintuitive
steric effects were observed. More detailed explanations of these
effects were provided by dispersion-corrected DFT calculations in
collaboration with the groups of Tuononen and Nagase (see below).
This Account describes our development of these initial results
for other inorganic molecular classes. More recently, the work has
led us to move to the planned inclusion of dispersion effects in ligands
to stabilize new molecular types with theoretical input from the groups
of Vasko and Grimme (see below). Our approach sought to use what Grimme
has described as dispersion effect donor (DED) groups (i.e., spatially
close-lying, densely packed substituents either as ligands (e.g.,
−C6H2-2,4,6-Cy3, Cy = cyclohexyl)
or as parts of ligands (e.g., a Cy substituent) that produce relatively
large dispersion energies to stabilize these new compounds.
We predict that the future design of sterically crowding hydrocarbon
ligands will include the ...