Journal of the American Chemical Society
Although the computational and experimental studies above
indicate that the phenCF2H ligand engages in H-bond
interactions, quantifying the interaction strength is intrinsically
difficult. In contrast to classic H-bond donors (OH and NH)
that undergo a hypsochromic (blue) shift of the νE−H mode
upon the formation of an H-bond, H-bonds to C−H donors
may exhibit distinct shifts: the ν
may undergo a
C−H
hypsochromic (blue), no shift, or a bathochromic (red)
7
6
shift. As a result, it is difficult to identify ν
shifts for even
C−H
3
6
simple systems, and there are no reported correlations
between C−H H-bond energy and νC−H
.
To ascertain the influence of the −CR H group on the H-
2
bond interaction, the vibrational dependence (Δν ) of the
donor was analyzed computationally for 3-OArR′ and 5-
C−H
OArR′. We found that ν
for 3-OArR′ exhibits bath-
C−H
ochromic (red) shifts with increasing H-bond acceptor
7
7
strength. The important difference between the two modeled
complexes is that for R = CF H the Δν tracks with the H-
2
C−H
bond acceptor strength, while there is no systematic trend for
78
R = C(CH ) H (Figure 5B).
3
2
To experimentally establish the relative strength of the
CR H···X interaction (for CF H and C(CH ) H), we
2
2
3 2
interrogated the through-space H−F coupling interaction by
NMR spectroscopy. Despite efforts to prepare Pd difluoride
compounds (1-F, Figure 2), we found that they were generally
unstable toward further chemical manipulations, including
isolation and crystallization. To overcome this limitation, we
targeted the isolation of palladium aryl fluoride complexes
because they exhibit higher stability relative to palladium
Figure 7. (A) Synthesis of complexes 6-I, 7-I, 6-F, and 7-F. (B)
Crystal structure of 6-F (30% probability ellipsoids; for clarity, a
single molecule from the unit cell is shown and protons not involved
in H-bonds are removed). (C) H and selectively decoupled H{ F}
NMR of 6-F and 7-F.
1
1
19
5
4−59
CF2H
iPr
difluorides.
The addition of phen
or phen to
CF2H
Pd(Ph)I(Py) in CH Cl afforded Pd(Ph)I(phen
Pd(Ph)I(phen ) (7-I) in good yields (84 or 76%,
respectively) (Figure 7A). Sonication of 6-I and AgF in
) (6-I) or
2
2
2
−CF H(D) group. An NCI analysis of 6-F indicated a stronger
2
iPr
attractive interaction than found in 7-F (sign(λ )ρ for s = 0.5:
2
6
-F = −0.029; 7-F = −0.021), consistent with polarization
CH Cl while cooling in an ice bath facilitated halide exchange
2
2
serving as the dominant factor in forming unconventional H-
bonds (Table S13). Although preorganization can serve to
structurally enforce H-bonding interactions to unconventional
H-bond donors, the results of our combined experimental/
computational investigations indicate that, even with structur-
CF2H
to produce Pd(Ph)F(phen
) (6-F). The major isomer
observed (>95%) exhibited H···F H-bonding interactions, vide
infra.
1
H NMR spectra of 6-I and 6-F exhibit −CF H resonances
2
79
at 9.08 and 8.68 ppm, respectively. Similar to 1-F, the
CF H···F interaction in 6-F exhibits a through-space
ally similar environments, the −CF H group imparts
2
i
−
2
significantly stronger interactions when compared to an − Pr
1
coupling interaction: | J | = 23 Hz. This value is smaller
FH
group.
1
than | J | coupling to stronger H-bond donors (−OH = 50
FH
Determination of −CF H Hydrogen Bond Strength.
2
4
3
80
Hz; −NH = 50−64 Hz ). To examine a direct comparison
2
To determine the strength of the unconventional −CF H···X
2
using stronger H-bond donors within this system, we targeted
H-bonds for the strongest H-bond acceptor (F), we applied
OH
82
bpy as a related bidentate ligand. In contrast to the stable
computational methods. We approximated the H-bond
CF2H
complex obtained using phen
, we found that metalation of
enthalpy (ΔH ) of the −CR H···F−Pd bond of 1-F as the
H−F
2
this ligand under analogous conditions produced benzene (via
protonation of Pd-Ph) as a primary product, which is a
reaction liability introduced by acidic H-bond donors (−OH).
To further interrogate the electronic requirements needed to
difference between the formation enthalpy of the Pd−F bond
(ΔH
) of 1-F and a reference compound that cannot H-
Pd−F
8
3
bond. The −CF H substituent, when placed in the para
2
4
‑CF2H
position of the pyridine ring (phen
), removes the
1
3
visualize a through-space J coupling to C sp −H units, we
attractive H-bond interaction for enthalpy analysis but also
imparts a geometric distortion relative to the para substitution
FH
iPr
1
analyzed the isostructural complex with phen . The H NMR
spectrum of the analogously prepared Pd(Ph)F(phen ) (7-F)
complex does not feature detectable through-space JFH
iPr
(overlay RMS = 0.111; SI page S82). As such, the ΔH
Pd−F
1
difference between ortho and para does not simply reflect the
H-bond contribution of the group but also a primary-sphere
perturbation (2-CF H vs 4-CF H; ΔPd−N = 0.095 Å; ΔPd−F
8
1
coupling but is broadened. Selective Pd−F decoupling
1
19
H{ F} NMR collapses the broadened resonance to a sharp
septet, which is consistent with a very weak through-space H···
2
2
< 0.011 Å; ΔH
< 1.8 kcal/mol). To minimize the primary-
Pd−F
1
1
F interaction of | J | ≤ 3 Hz. The contrast between the J of
sphere distortion and assess the electronic effect of the −CF H
FH
FH
2
4
‑CF2H
6
-F and 7-F provides further support that the C−H bond in
group, we compared isostructural pair PdF (phen
) and
2
−
CF H is uniquely polarized and capable of stronger attractive
PdF (phen) (overlay RMS = 0.006). The minimal structural
2
2
interactions and electronic communication via H-bonding.
changes and small enthalpic differences between −H and
−CF H (4-H vs 4-CF H; ΔPd−N = 0.002 Å; ΔPd−F < 0.002
Similar to 1-X and 3-OAr, the −CF H vibrations of 6-I/F were
2
2
2
unable to be identified even with isotopic labeling of the
Å; ΔH
< 0.8 kcal/mol) demonstrate that the −CF H
Pd−F
2
E
J. Am. Chem. Soc. XXXX, XXX, XXX−XXX