Angewandte
Communications
Chemie
synthetically interesting contexts with electron-deficient qui-
nones is less unfavorable.[19] However, as noted above, these
quinones and their reduced counterparts are inherently weak
H-bond acceptors. As such, the success of the proposed HBD-
coupled ET strategy relies on finding the appropriate balance
between HBD strength and quinone reactivity.
Herein, we report a systematic evaluation of several
small-molecule hydrogen-bond donors, with the goal of
activating electron-deficient quinones (Figure 2). ortho-
Scheme 1. a) Square scheme describing pathways for HBD-coupled ET
to quinones and their associated equilibrium constants. b) Extended
square scheme accounting for two binding events.
concentration of the HBD results in a more positive DE1/2,
effectively creating a more potent oxidant by favoring the
reduced state through binding. As illustrated by the square
scheme in Scheme 1a, K’
specifically describes this stabi-
QCÀ
lizing interaction. The equilibrium constants that govern this
shift in the potential can be elucidated electrochemically
through cyclic voltammetry and provide a quantitative mea-
sure of the stabilization provided by the HBD to QCÀ.
Our investigations were carried out with a range of HBDs,
including the representative dual HBDs 1–3, with the aim of
understanding how H-bonding interactions affect DGassoc
[Eq. (3)] when electron-deficient quinones are used. Electro-
chemical titrations of Q were performed with each HBD,
using cyclic voltammetry to record the DE1/2 value as a func-
tion of HBD concentration (Figure 3a–c). Each of the HBDs
studied has a significant, measurable effect on the apparent
potential that corresponds to the first ET.[22] Furthermore, the
reversibility of the CVs recorded in all titration experiments
indicate that the effect on E1/2 is the result of H-bonding to
QCÀ and not protonation, which would manifest as irrever-
sibility in the CV traces.
To elucidate the equilibrium constants that describe the
binding of QCÀ to 1–3, the full set of electrochemical data for
these titrations was subjected to simulations.[23] This analysis
revealed that the experimental data are best described by
a mechanism in which two HBD molecules are involved in the
stabilization of QCÀ. This mechanistic interpretation provides
a good fit to the experimental data with respect to the overall
DE1/2 values, and also reproduces the distinct features of the
cyclic voltammogram at low HBD concentrations (e.g.,
Figure 3a, scan (c) and corresponding simulation
(a)).[24]
Figure 2. HBDs and additives examined in this study.
Chloranil (Q) was selected as the oxidant as it is an
electron-deficient quinone that nonetheless lacks the intrinsic
reactivity necessary to oxidize many organic substrates of
synthetic interest. Our examination of the influence of H-
bonding on the single-electron transfer chemistry of ortho-
chloranil has led to the discovery that dicationic bis(amidi-
nium) salts can exert a remarkable influence on the thermo-
dynamics and kinetics of ET. By taking advantage of this
effect, we demonstrate that these HBDs can also catalyze
a model oxidative transformation that is mediated by ortho-
chloranil.
In aprotic media, quinones undergo two sequential single-
electron transfers, proceeding via the semiquinone radical
anion QCÀ.[20] Protic and H-bonding molecules influence the
mechanism by which ET proceeds. This study is concerned
primarily with the effect of HBDs on the first ET step. To
quantify the ability of an HBD to modulate the thermody-
namics of ET, the association of the HBD with QCÀ must be
quantified; in other terms, we need to determine how strongly
the HBD favors the reduced state over the oxidized, neutral
state.
An HBD-coupled ET to Q that involves two binding
events requires the use of an expanded square scheme to
outline all mechanistic possibilities (Scheme 1b), wherein
K
K
provides a quantitative description of the stabili-
1QCÀ 2QCÀ
The mechanistic methods used to quantify HBD-coupled
ET are borrowed from the study of proton-coupled ET.[21]
Eq. (4), which is related to the Nernst equation, describes
HBD-coupled ET (Scheme 1a). The apparent potential of
a quinone involved in HBD-coupled ET will undergo a shift
(DE1/2) that is dependent on the HBD concentration and the
association constants for the binding of the quinone and
zation provided to QCÀ through binding, and a measure of the
oxidizing strength of Q in the presence of a given HBD.
The electrochemical simulations allow us to distinguish
between the pathways for HBD-coupled ET outlined in
Figure 1d and to determine the binding constants associated
with each individual step. The simulations for 1–3 reveal that
these HBDs all promote a mechanism in which binding of the
neutral quinone (K1Q) precedes ET (E2), and a second binding
semiquinone (KQ and K , respectively) to the HBD.
QCÀ
event follows (K ).[25] A simulation of this mechanism
explicitly determines values for these equilibrium constants,
2QCÀ
1 þ KQ ½HBD
CÀ
ð4Þ
DE1=2 ¼ 0:059V log
1 þ KQ½HBD
from which K
can be calculated. Independent determi-
1QCÀ
nation of K1Q using spectroscopic methods resulted in values
that were consistent with those obtained from the simulations
(Supporting Information, Figures S1–S4).
This relationship between DE1/2 and the association
constants shows that as long as K’ > K’Q, increasing the
QCÀ
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Angew. Chem. Int. Ed. 2016, 55, 539 –544