Kinetics of the p-Aminodiphenylamine Radical
J. Phys. Chem., Vol. 100, No. 12, 1996 4869
•+
AH2 + H+ a AH3
(2)
(3)
(4)
(5)
(6)
AH+3 a AH2•+ + e- + H+
•+
AH+3 + H+ a AH4
AH42+ a AH2•+ + e-1 + 2H+
AH2•+ a QH+ + e- + H+
Q + H+ a QH+
(7)
(8)
•+
AH+3 + QH+ a 2AH2
with AH2 ) unprotonated ADPA, AH+ ) single-protonated
3
ADPA, AH24+ ) double-protonated ADPA, AH2 ) radical
•+
cation of ADPA, and Q ) PQDI. It meets all results mentioned
in the present paper and is based on three one-electron transfer
reactions of three different protonated ADPA species forming
the corresponding cation radicals. These cation radicals undergo
quick protonation/deprotonation reactions and are oxidized to
PQDI, which also undergoes protonation/deprotonation. With
this mechanism we were also able to fit the experimental cyclic
voltammograms. The following parameter set was found to be
representative but probably overvalues the amount of the double-
protonated ADPA: formal potentials according to eq 1, E )
-0.15 eV; eq 2, E ) 0.49 V; eq 5, E ) 0.66 V; eq 6, E ) 0.06
V, and equilibrium constants for eq 2, K ) 2 × 105 L/mol; eq
4, K ) 10 L/mol; eq 7, K ) 105 L/mol.
Figure 2. (a) Cyclic voltammogram of ADPA measured at a Pt
working electrode in 0.5 M H2SO4/DMSO with an Ag/AgCl wire as a
reference electrode. Potentials are referred to the potential of the
ferrocene couple; sweep rate was 150 mV/s; concentration of ADPA
was 10-3 M. (b) Simulated cyclic voltammogram of ADPA with E1
) 0.15 V, E2 ) 0.49 V, E3 ) 0.66 V, and E4 ) 0.06 V. For
explanation, see text; for mechanism see eqs 1-8.
3. Results
A cyclic voltammogram of ADPA in acidic DMSO solution
is shown in Figure 2, curve a. The peak separation of the
oxidation and the re-reduction peak is 320 mV. This result is
quite different from that in neutral and HClO4-acidic acetonitrile
(MeCN).5,14 The H2SO4/DMSO solution gives a quite different
protonation equilibrium of ADPA and PQDI from that in HClO4/
MeCN, resulting in different cyclic voltammograms. The
current increase at potentials higher than 800 mV is due to the
starting formation of an oxide layer on the platinum electrode
in DMSO. This effect is not as significant as it is in sulfuric
acid solution where it has been known for a long time from
potentiodynamic measurements.15 The current increase is also
due to the beginning decomposition of the electrolyte. The weak
voltammetric wave at the foot of the anodic peak increases and
results in an additional peak at lower sweep rates.
It is known from in situ UV-vis electrochemical measure-
ments16 that within the time scale of our measurements PQDI
is the only product formed during oxidation of ADPA. In the
same study it is shown that the amount of the starting material
is re-formed during re-reduction.
For the simulation of the cyclic voltammograms, we tried
different reaction mechanisms like deprotonation before and
after oxidation or the electron transfer reaction of only the
protonated ADPA, but the simulations of the voltammograms
failed.
The equilibrium constant for the symproportionation reaction
(eq 8) is not determined by simulation but by our independent
measurement to be K ) 0.027 as described later. On the basis
of these simulations we can interpret the measured cyclic
voltammograms as follows:
The weak voltammetric wave at the foot of the anodic peak
is due to the oxidation of the nonprotonated ADPA. Its
concentration is low because the equilibrium according to eq 2
is shifted to the right side. This wave becomes the most intense
peak at very slow sweep rates due to the back reaction (eq 2).
The main oxidation peak at 0.49 V is due to the oxidation of
the single-protonated ADPA, while the small amount of twice-
protonated ADPA is oxidized at 0.66 V where the electrolyte
starts to decompose. As it can be concluded from the proto-
nation constants resulting from the simulation, nearly the whole
amount of the cation radicals is present in the nonprotonated
form which has a low formal potential for their oxidation. This
causes the immediate oxidation to PCDI and the large volta-
mmetric peak separation.
At the very beginning of this study of ESR spectroscopy of
ADPA, it turned out that neither the lifetime of the radical nor
the low radical concentration was the main problem in the ESR
measurements, but it was the formation of an adhering polymer
layer at the electrode surface. This polymer itself gives a strong
single ESR line (Figure 3a) well-known for polyaniline and other
conducting polymers which interferes with the highly resolved
ESR spectra of the low molecular structures. Especially, the
quantitative determination of the ADPA•+ radical concentration
is impossible. Therefore, DMSO was used as the solvent. Thus,
the polymer layer formation is suppressed, and no single ESR
line of the polymer observed by making sensitive ESR measure-
ments of the monomeric radical structures is possible. It was
found furthermore that the addition of DMSO in a small amount
of an aqueous electrolyte of 0.5 mM ADPA is the reason for
the suppression of the polymer layer formation. Figure 3b
Furthermore, we simulated the cyclic voltammograms on the
basis of three two-electron transfer reactions at three different
potentials according to three different protonated species of
ADPA. With this mechanism a good fit was possible, but the
fitted constants for the protonation equilibria showed that the
PQDI should be unprotonated. This fact is contradictory to our
in situ UV-vis measurements, where only the spectra of the
protonated PQDI were found. All our attempts to find a data
set with protonation constants which meet these facts failed.
We propose the following mechanism
AH2 a AH2•+ + e-
(1)