5666
J . Org. Chem. 1998, 63, 5666-5667
Str u ctu r e a n d Sta bility of a n
Azoa lk a n e-Iod in e Com p lex
Paul S. Engel,* Shaoming Duan, and
Kenton H. Whitmire
Department of Chemistry, Rice University, P.O. Box 1892,
Houston, Texas 77251
Received February 13, 1998
Halogen complexes of aromatic hydrocarbons,1-3
olefins,4-6 amines,7,8 and other donors9,10 have been
known for many decades, but charge-transfer (CT) com-
plexes of azoalkanes were discovered more recently.11 In
the course of investigating the oxidation of 1,2-dialkyl-
hydrazines by halogens, we found that azoalkanes also
form CT complexes with halogens, which are xσ-type
acceptors.12 While earlier workers11 had mentioned the
color change that occurred on mixing of 2,3-diazabicyclo-
[2.2.2]oct-2-ene (DBO) with iodine, we were able to isolate
a single crystal of this complex and determine its X-ray
structure. Hydrazine also forms complexes with halo-
gens;13 hence, the halogen oxidation of hydrazines to
azoalkanes may be complicated by both hydrazine and
azo CT complexes.
F igu r e 1. UV-vis absorption spectrum in n-heptane of (a)
0.00406 M DBO, (b) 4.11 × 10-4 M I2, offset ) +0.5, (c) 0.00775
M DBO + 4.88 × 10-5 M I2, offset ) +1.2, and (d) 0.0205 M
DBO + 4.57 × 10-4 M I2, offset ) +1.2.
in 100-fold excess and used the Scott equation (7 points,
r ) 0.9998)19 to calculate the extinction coefficient and
the equilibrium constant. The value of ꢀ (18 500) is
similar to that of aliphatic amine-I2 complexes (ꢀ
∼25 000)20 but is smaller than that of pyridine-I2 (ꢀ )
51 700).16 Our ꢀ cannot be compared with that of
previously known DBO CT complexes because no short-
wavelength band was reported.11 The extinction coef-
ficient of our 424 nm band is ∼2000, comparable to that
of DBO-TCNE11 and to the 422 nm band of pyridine-
I2.16 The observed value of K (153 M-1) is far larger than
Mixing a heptane solution of I2 (4.88 × 10-5 M) with
one of DBO (0.00775-0.0493 M) gave immediate rise to
a light yellow color caused by a weak band at 424 nm
and to a stronger band at 266 nm, both attributed to the
CT complex (cf. Figure 1).14,15 The longer wavelength of
the of DBO-I2 CT band (266 nm) than of the analogous
pyridine-I2 band (236 nm)16 is in the direction expected
from the lower IP of DBO (8.19 eV)17 than pyridine (9.26
eV).18 We determined the absorbance of the 266 nm band
at 25 °C as a function of DBO concentration with DBO
that of other known DBO complexes: TCNE (1 M-1),
11
CBr4 (5 M-1), or AgNO3 (1 M-1
)
is smaller than the
highly structure-dependent values for amines (K ) 530-
21
12 100)20 but is very similar to that of R2S-I2
and
pyridine-I2 complexes.16 This last result is in accord
with the sp2 hydridization of nitrogen in both cases but
does not reflect the lower IP of DBO.9
(1) Hubig, S. M.; J ung, W.; Kochi, J . K. J . Org. Chem. 1994, 59,
6233.
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Kaul, P. J . Org. Chem. 1994, 59, 7335.
The enthalpy of complexation was calculated from the
266 nm absorbance of a sealed, degassed, and N2 back-
filled heptane solution of 0.0207 M DBO and 4.61 × 10-5
M I2 in a quartz cuvette at four temperatures from 8.8
to 30.6 °C. A plot of ln K vs 1/T yielded ∆H ) -6.2 kcal/
mol (r ) 0.9987), which was combined with our K(25 °C)
to yield ∆S ) -11 eu. These values are similar to those
for I2-ether complexes.15
A single crystal of the DBO-I2 complex was grown by
slow diffusion of ether into a MeCN solution of the
components at -5 °C. Because the crystal was unstable
to X-rays at room temperature, the data were acquired
at -100 °C. The refined structure (R ) 0.0382, cf. Figure
2) reveals that the geometry of the DBO moiety resembles
that of DBO itself.22 DBO is close to C2v symmetry, as
shown by the C3-N2-N1-C6 dihedral angle of 1.5° and
the nearly eclipsed conformation (5.3° deviation) about
the C4-C3 and C7-C8 bonds. Whereas the two C-Nd
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(5) Brown, R. S.; Nagorski, R. W.; Bennet, A. J .; McClung, R. E. D.;
Aarts, G. H. M.; Klobukowski, M.; McDonald, R.; Santarsiero, B. D. J .
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Chemistry; Holden Day: San Francisco, 1964.
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Press: London, 1969.
(11) Blackstock, S. C.; Kochi, J . K. J . Am. Chem. Soc. 1987, 109,
2484.
(12) Mulliken, R. S. J . Phys. Chem. 1952, 56, 801.
(13) Margerum, D. W.; J ia, Z.; Salaita, M.; Liu, R. M. In Abstracts
of the 213th ACS National Meeting, San Francisco, CA, Apr 13, 1997;
American Chemical Society: Washington, DC, 1997. paper no. 805.
Liu, R. M.; Margerum, D. W. Inorg. Chem. 1998, 37, 2531.
(14) Tamres, M.; Brandon, M. J . Am. Chem. Soc. 1960, 82, 2134.
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82, 2129.
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N.; Rozeboom, M. D.; Eaton, T. A.; Glass, R. S.; Broeker, J . L.
Tetrahedron 1988, 44, 6811.
(18) Franklin, J . L.; Dillard, J . G.; Rosenstock, H. M.; Herron, J . T.;
Draxl, K.; Field, F. H. Ionization Potentials, Appearance Potentials,
and Heats of Formation of Gaseous Positive Ions; Nat. Stand. Ref. Data
Ser. Nat. Bur. Stand.: Washington, D.C., 1969; Vol. NSRDS-NBS 26.
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S0022-3263(98)00265-5 CCC: $15.00 © 1998 American Chemical Society
Published on Web 07/17/1998