˚
remarkable y0.46 A apical movement of the Fe atom in this solid-
state reaction of 1 with NO gas! Even more striking is that the
trans Fe–S bond length does not change in going from the five-
coordinate 1 to the six-coordinate 2, implying that there is no
significant structural trans effect of NO in this six-coordinate iron
nitrosyl thiolate porphyrin when prepared from the five-coordinate
crystals. This may be compared with the structural trans effect
observed in the {FeNO}7 compounds [Fe(por)(NO)(N-base)]
˚
which show a y0.2 A increase in the Fe–N(ax) distance upon
NO binding.15
Third, the FeNO and FeSC(thiolate) planes are essentially
mutually perpendicular, and these two planes straddle the Fe–N1
bond; C37–S1–Fe1–N1 torsion angle = 255.6(4)u, and O1–N5–
Fe1–N1 = 43(2)u. In addition, there is a slight opening of the Fe1–
S1–C37 angle (from 104u to 111u) upon NO binding and
subsequent movement of the S-atom toward the mean porphyrin
plane.
Fig. 2 Molecular structure of [Fe(oep)(NO){S-2,6-(CF3CONH)2C6H3}]
(2) with thermal ellipsoids drawn at 35%.
Whenplacedinabroadercontext,thecrystalstructureof2reveals
an intrinsic tilting (of the nitrosyl N-atom from the por-
phyrin normal) and bending of the NO group in this formally
{FeNO}6 species. We have previously reported that such a tilting
and bending feature represents a low energy conformation in the
related {FeNO}6 compound [Fe(oep)(NO)(C6H4F)].16 Our results
suggest that such a tilting and bending of the NO group may be a
common feature in the NO adducts of ferric heme thiolate proteins.
We are grateful to the US National Institutes of Health (GM
64476) for funding for this work.
the dark. However, attempted dissolution and crystallization of the
nitrosyl product 2 resulted only in the generation of the precursor
compound 1 and [Fe(oep)(NO)].
We then explored the possibility of a heterogeneous reaction of
crystals of 1 with NO gas with the hope that product formation
would not be accompanied by extensive crystal fragmentation.
The crystals used for the reaction were grown from CH2Cl2–
hexane (2 : 1) at room temperature.{{13 Several crystals of purple 1
were hand-picked and exposed to NO gas at room temperature for
several hours to allow for NO diffusion into the crystal lattice. The
molecular structure of the dark red nitrosyl product 2 is shown in
Fig. 2. Selected structural data of 2 are presented in Table 1, and
are compared with the related data from 1.
Notes and references
{ The crystal structure of 1 was reported previously by Ueyama et al.13
Their crystals were grown from toluene, and the Fe–S and Fe–Npor bond
˚
lengths in their structure were 2.356(3) and 2.048(avg) A, respectively.
{ Crystal data. Compound 1?1/2(hexane): C49H56F6FeN6O2S, M = 962.91,
There are several interesting features about the structure of 2.
First, the FeNO moiety in 2 is bent with an angle of 159.6(8)u in
this formally {FeNO}6 compound, and the nitrosyl N-atom is
tilted 9.1u from the normal to the 4N (and 24 atom) porphyrin
plane. The bent NO geometry is not the result of any close
intermolecular contacts; the shortest intermolecular distances are
between the nitrosyl O-atom and a thiolate F-atom of another
molecule, and between the nitrosyl N-atom and another porphyrin
¯
˚
˚
˚
triclinic, space group P1, a = 8.9881(14) A, b = 13.208(2) A, c = 19.879(3) A,
3
˚
a = 100.889(5)u, b = 91.761(5)u, c = 101.373(5)u, V = 2266.3(6) A , T =
100(2) K, Z = 2, Z9 = 1, Dc = 1.411 g cm23, m = 0.451 mm21, 18050
reflections measured, 8813 unique (Rint = 0.0260), F(000) = 1008, R1 (obs.
data) = 0.0563, wR2 (all data) = 0.1645. Compound 2?1/2(hexane):
¯
˚
C49H56F6FeN7O3S, M = 992.92, triclinic, space group P1, a = 9.181(5) A,
˚
˚
b = 12.455(7) A, c = 21.261(12) A, a = 98.573(9)u, b = 94.080(9)u,
3
˚
˚
ethyl carbon atom (both distances are ¢3.3 A).
Second, the Fe atom in 2 is situated almost in the 4N plane of
c = 99.425(9)u, V = 2360(2) A , T = 100(2) K, Z = 2, Z9 = 1, Dc
=
1.397 g cm23, m = 0.438 mm21, 9889 reflections measured, 4873 unique
(Rint = 0.0680), F(000) = 1038, R1 (obs. data) = 0.0833, wR2 (all data) =
0.2035. CCDC 298938 (2) and CCDC 298939 (1). For crystallographic
data in CIF or other electronic format see DOI: 10.1039/b602611g
˚
the porphyrin, with an upward displacement of 0.05 A towards the
NO ligand. Concurrent with this upward movement of the Fe
atom upon formation of 2 is the shortening of the Fe–Npor bond
˚
lengths by y0.05 A. Considering that the Fe atom was displaced
1 D. Mansuy and P. Battioni, in The Porphyrin Handbook, ed. K. M.
Kadish, K. M. Smith and R. Guilard, Academic Press, San Diego, 2000,
vol. 4, ch. 26, pp. 1–15.
˚
0.41 A towards the S atom in the precursor 1, this represents a
2 H. Shimizu, E. Obayashi, Y. Gomi, H. Arakawat, S.-Y. Park,
H. Nakamura, S.-I. Adachi, H. Shoun and Y. Shiro, J. Biol. Chem.,
2000, 275, 4816–4826.
3 T. L. Poulos and E. F. Johnson, in Cytochrome P450: Structure,
Mechanism, and Biochemistry, ed. P. R. Ortiz de Montellano, Plenum,
New York, 3rd edn, 2005, ch. 3, pp. 87–114.
˚
Table 1 Selected structural data (in A and u) for compounds 1 and 2
1
2
Fe1–N5
N5–O1
—
—
1.671(9)
1.187(9)
4 Y. Minamiyama, S. Takemura, S. Imaoka, Y. Funae, Y. Tanimoto and
M. Inoue, J. Pharmacol. Exp. Ther., 1997, 283, 1479–1485.
5 H. M. Abu-Soud, K. Ichimori, H. Nakazawa and D. J. Stuehr,
Biochemistry, 2001, 40, 6876–6881.
6 A. Weichsel, E. M. Maes, J. F. Andersen, J. G. Valenzuela, T. K.
Shokhireva, F. A. Walker and W. R. Montfort, Proc. Natl. Acad. Sci.
USA, 2005, 102, 594–599.
Fe1–Npor
Fe1–S1
/Fe1–N5–O1
/S1–Fe1–N5
/C37–S1–Fe1
S tilta
2.054(2)–2.064(2)
2.359(1)
—
—
104.22(11)
3.4 [4.3]
2.003(8)–2.017(7)
2.356(3)
159.6(8)
165.5(3)
110.6(3)
6.3 [6.7]
a
Tilt of the S atom from the normal to the porphyrin 4N [24 atom]
7 A. Franke, G. Stochel, N. Suzuki, T. Higuchi, K. Okuzono and R. van
Eldik, J. Am. Chem. Soc., 2005, 127, 5360–5375.
plane.
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Chem. Commun., 2006, 2030–2032 | 2031