L. Juli a` , J. Rius and X. Torrelles
Figure 3. An ORTEP drawing of the molecular structure of bis(2,5-
dimethyl-1-pyrrolyl)-(1,3-phenylene) (4) (hydrogens have been removed
◦
for clarity). Selected interatomic distances (Å) and angles ( ): N1–C16
1
1
.387(2), N1–C13 1.390(2), N1–C6 1.428(2), N2–C10 1.379(2), N2–C7
.388(2), N2–C2 1.429(2), C1–C2 1.382(2), C1–C6 1.385(2), C2–C3 1.386(2),
C3–C4 1.375(2), C4–C5 1.370(2), C5–C6 1.386(2), C7–C8 1.351(2), C7–C12
1
1
1
1
1
1
1
1
1
.491(3), C8–C9 1.394(3), C9–C10 1.352(2), C10–C11 1.475(3), C13–C14
.353(2),C13–C181.488(2),C14–C151.406(2),C15–C161.361(2),C16–C17
.471(2); C16–N1–C13 109.56(12), C16–N1–C6 125.18(12), C13–N1–C6
25.16(12), C10–N2–C7 109.80(13), C10–N2–C2 125.99(12), C7–N2–C2
24.05(14), C2–C1–C6 120.04(12), C1–C2–C3 119.94(12), C1–C2–N2
20.31(12), C3–C2–N2 119.75(12), C4–C3–C2 119.57(13), C5–C4–C3
20.89(13), C4–C5–C6 119.86(13), C1–C6–C5 119.67(12), C1–C6–N1
20.19(11), C5–C6–N1 120.14(12), C8–C7–N2 106.4(2), C8–C7–C12
31.7(2), N2–C7–C12 121.9(2), C7–C8–C9 108.6(2), C10–C9–C8 109.0(2),
Figure 2. (a) EPR spectrum of a solution of bis(2,5-dimethyl-1-pyrrolyl)-
1,3-phenylene) (4) in TFA acid in the presence of thallium(III) trifluoroac-
etate at 298 K. (b) Computer simulation using the values given in the
text.
(
C9–C10–N2 106.3(2), C9–C10–C11 130.8(2), N2–C10–C11 122.85(14),
C14–C13–N1 106.76(14), C14–C13–C18 131.2(2), N1–C13–C18
1
21.92(13), C13–C14–C15 108.67(15), C16–C15–C14 108.40(14),
C15–C16–N1 106.62(14), C15–C16–C17 130.82(15), N1–C16–C17
22.54(13).
1
◦
◦
◦
3
α = 90.00(1) , β = 102.34(2) , γ = 90.00(1) , V = 1553.7(6) ꢀ ,
3
−1
Z = 4, F(000) = 568, Dc = 1.13 g/cm , µ = 0.067 mm , crystal
dimensions 0.72 mm × 0.38 mm × 0.14 mm. Data collection:
The diffractometer was an Enraf Nonius CAD4 with a graphite
monochromated MoKα radiation, λ = 0.71073 ꢀ. Cell parameters
were determined from refinement of 15 reflections using the
Inthiscontext,itisworthtosaythatabinitiocalculationsperformed
in 1 and its radical cation 1 predict that the minimum energy
conformation in both the structures correspond to a torsional
angle of 90 .
This case of β-dimerization in pyrrole radical cations, reported
in the literature in the case of electrochemical oxidation of 1,2,5-
trimethylpyrrole,[ confirms the reactivity of the β-carbon atoms
during the oxidative processes to polypyrroles and this is the
reason why chemical or electrochemical growing polypyrroles are
•+
◦
[5i]
[
11]
CAD4 Express software.
For thousand one hundred fifty-two
◦
reflections were measured with 2.28 ≤ θ ≤ 28.44 and index
4c]
ranges −12 ≤ H ≤ 0, 0 ≤ K ≤ 20, −14 ≤ L ≤ 15 in ω/2θ mode,
0
6
.55 + 0.65 tan(θ) scan width and maximum final scan time of
0 s. Three standard reflections were measured every 3600 s to
ꢁ
check for the intensity variation and three more standards were
measured every 55 reflections to check the crystal orientation.
Intensity gain was 0.00% and was not corrected. Absorption
correction was made using seven psi-scans, Tmax = 98.98% and
Tmin = 92.49%. Resolution and refinement: The structure was
not exclusively α,α -bonded, causing some crosslinking of the
polymers. These defects are practically eliminated by blocking the
β-positions with alkyl groups.
[
12]
2
solved by direct methods using the SumF-TF and refined on F
Experimental Section
with 4648 unique reflections and 316 parameters. Final R factors:
[
0
I > 2σ(I)] R1 = 0.0498 and wR2 = 0.1342; R factors (all data) R1 =
Melting points were obtained by using a K o¨ fler microscope
Reichert and are uncorrected. NMR spectra were determined
at 200 MHz with Varian Gemini 200 HC spectrometer. TFA acid was
distilled before use.
EPR spectra were recorded using a Varian E 109 spectrometer
working in the X band. To detect the radical cations, solutions of
substrates in TFA acid or in 1,1,1,3,3,3-hexafluoropropan-2-ol in a
quartz tube (internal diameter 2 mm) were degassed by passing a
stream of dry argon through the solutions to remove oxygen, and
then a small excess of thallium trifluoroacetate was added in the
same tube.
2
.1125 and wR2 = 0.1459. Goodness-of-fit on F = 0.985, where
2
2
2 2
2 2 1/2
R = ꢁ||F0| − |Fc||/ꢁ|F0|, wR = [ꢁw(F0 − Fc ) /ꢁw(F0 ) ]
,
2
2
2
2
2
w = 1/[ꢁδ(F0 ) +(0.0800P) +0.00P], P = [Max(F0 , 0)+2Fc ]/3,
2
2
1/2
GooF = [(ꢁw(F0 − Fc ))/(n − p)] (n, number of reflections; p,
number of parameters). Final shifts/esd were <0.000 in the last
cycle (with convergence to 0), and the maximum and minimum
residual electron density in the final Fourier difference was 0.12
−
3
[13]
and −0.18eꢀ , respectively. A SHELXL-93 program was used
[
14]
for refinement and plots were made with PLUTON programs ].
An ORTEP drawing of this molecule is shown in Fig. 3. The
dihedral angles between the pyrrolic rings and the benzene are
◦ ◦
6
7.25(0.05) and 61.56(0.05) . This torsion from planarity avoids
Acknowledgements
the steric interaction between methyl substituents and hydrogens
in benzene. It is reasonable to suggest that these angles will not
changeinagreatextensionongoingtotheradicalcationstructure.
Financial support from the MeI (Spain) through project AGL2009-
12374-C03-03/ALI is gratefully acknowledged. We also thank the
wileyonlinelibrary.com/journal/mrc
Copyright ꢀc 2011 John Wiley & Sons, Ltd.
Magn. Reson. Chem. 2011, 49, 164–167