metal-organic compounds
adopts a distorted half-chair conformation, in which atoms O1
Ê
and C15 are 0.426 (1) and 0.348 (2) A from the plane of the
ferrocene derivatives we have reported previously (Cetina et
al., 2002, 2003). The main conformational difference was
observed in the orientation of the Cp rings. In (I), the rings are
twisted from an eclipsed conformation by 19.4 (2)ꢀ (mean
value). The values of the corresponding CÐCg3ÐCg2ÐC
pseudo-torsion angles (Cg3 and Cg2 are the centroids of the
C1±C5 and C6±C10 rings, respectively), de®ned by joining two
eclipsing Cp C atoms through the ring centroids, range from
19.0 (2) to 19.7 (2)ꢀ. The conformation is almost exactly
halfway between eclipsed and staggered, as demonstrated by
the C1ÐCg3ÐCg2ÐC9 torsion angle of 163.4 (1)ꢀ. This angle
would be 180ꢀ for a staggered conformation and 144ꢀ for a
fully eclipsed conformation. The centroids of the Cp rings are
almost equidistant from the Fe atom; the FeÐCg3 and FeÐ
other ring atoms (C11±C14); the C11ÐC12ÐC13ÐC14
torsion angle is 2.4 (2)ꢀ. The bond lengths in the heterocyclic
and fused phenyl rings (Table 1) mostly agree with the
equivalent bond lengths in the structures of 1,10-oxybis(iso-
chromane) (Eikawa et al., 1999) and (S)-1-(phenyl)ethyl-
ammonium (S)-isochromane-1-carboxylate (Unterhalt et al.,
1994). The exception is the C12ÐC13 bond, which is shorter
Ê
(ꢁ0.04 A) in the latter structure. Heterocyclic ring atoms O1,
C11 and C15 and cyclopentadienyl (Cp) ring atom C1 lie in the
same plane, the C15ÐO1ÐC11ÐC1 torsion angle being
178.95 (14)ꢀ. The dihedral angle between the mean plane of
these four atoms and the C1±C5 Cp ring is 47.8 (1)ꢀ.
Furthermore, the plane of the heterocyclic ring is almost
perpendicular to the plane of the C1±C5 ring and is parallel to
the plane of the fused phenyl ring. The corresponding dihedral
angles are 87.3 (1) and 4.0 (1)ꢀ.
Ê
Cg2 distances are 1.647 (1) and 1.650 (1) A, respectively, while
the Cg3ÐFeÐCg2 angle is 178.2 (1)ꢀ.
There are a number of CÐHÁ Á Áꢀ interactions (Table 2 and
Fig. 2). Atom H14A of the heterocyclic ring is positioned
almost perpendicularly above the phenyl-ring centroid (Cg1)
of the adjacent molecule. The six relevant HÁ Á ÁC distances fall
The exocyclic C2ÐC1ÐC11 bond angle is larger than the
C5ÐC1ÐC11 angle (Table 1). The Cp rings are planar and
almost parallel to each other [the dihedral angle between their
planes is 2.7 (1)ꢀ], and the FeÐC distances are in the range
i
Ê
in the narrow range 3.06±3.28 A, and the HÁ Á ÁCg distance is
signi®cantly shorter than any of the HÁ Á ÁC distances
1
2.034 (2)±2.051 (2) A for the substituted (C1±C5) and
[symmetry code: (i) x,
y, z 12; Table 2]. The CÐHÁ Á Áꢀ
Ê
2
Ê
2.029 (2)±2.049 (2) A for the unsubstituted (C6±C10) ring, the
Ê
average values being 2.042 (2) and 2.038 (2) A, respectively.
The CÐC bonds are slightly longer in the substituted ring than
in the unsubstituted ring [1.410 (3)±1.429 (2) versus 1.397 (3)±
interaction between phenyl atom H18 and the unsubstituted
Cp ring exhibits a completely different geometry. The
H18Á Á ÁC7ii distance is shorter than the HÁ Á ÁCgii distance
[symmetry code: (ii) 1 + x, y, 1 + z]. The second shortest
HÁ Á ÁC contact is that to atom C6, and the CÐH bond points
towards the C6ÐC7 bond of the Cp ring rather than towards
the ring centroid (Cg2). Similarly, the longest interaction,
C5ÐH5Á Á ÁCg1iii [symmetry code: (iii) 1 x, y, 2 z], points
towards the C12ÐC13 bond. Both the H5Á Á ÁC12iii and the
H5Á Á ÁC13iii contacts are shorter than the HÁ Á ÁCgiii distance.
The molecules linked by these CÐHÁ Á Áꢀ interactions build a
three-dimensional framework (Fig. 3).
Ê
1.414 (3) A], and the bond angles in both rings range from
107.52 (15) to 108.33 (18)ꢀ.
The geometry of the ferrocenyl moiety agrees well with the
structures of ferrocene (Seiler & Dunitz, 1979) and of the
Experimental
NaBH4 (253 mg, 6.7 mmol) was added gradually to a solution of
methyl 2-(ferrocenoyl)benzeneacetate (326 mg, 0.9 mmol) in a
mixture of EtOH and Et2O (1:1 v/v; 5 ml). The mixture was re¯uxed
for 2 h and worked up in the usual manner. Separation by preparative
thin-layer chromatography on silica gel (Merck, Kieselgel 60 HF254
)
yielded 2-(ꢁ-hydroxyferrocenyl)benzeneethanol (237 mg; yield 78%)
and orange crystals of 1-ferrocenylisochromane (57 mg; yield 20%;
m.p. 365±366 K). Single crystals of the title compound were obtained
by slow evaporation from a cyclohexane solution at room tempera-
ture. IR (CH2Cl2, cm 1): ꢂ 3081 (w) and 3020 (w) (CÐH, ferrocene),
2942 (m) (CÐH, aliphatic), 1278 (m) (CÐOÐC); 1H NMR (DMSO,
p.p.m.): ꢃ 7.18 (d, 1H, H16), 7.12 (d, 1H, H17), 7.14 (d, 1H, H18), 7.16
(d, 1H, H19), 4.23 (s, 5H, unsubstituted ferrocene ring), 4.13±4.20 (m,
4H, substituted ferrocene ring), 3.97 (m, 1H, H15A), 3.77 (m, 1H,
H15B), 2.78 (m, 2H, H14), 5.58 (s, 1H, H11); 13C NMR (DMSO,
p.p.m.): ꢃ 137.29 (C12), 132.91 (C13), 128.5 (C17), 126.25 (C18),
125.98 (C16), 125.36 (C19), 90.21 (C1), 73.63 (C11), 68.62 (unsub-
stituted ferrocene ring), 68.56±66.31 (substituted ferrocene ring),
61.55 (C15), 27.99 (C14).
Figure 3
Part of the crystal structure of (I), showing the cyclic motif generated by
the C5ÐH5Á Á ÁCg1iii interaction (Cg1 is the centroid of ring C12/C13/
C16±C19), which links the (010) sheets into a three-dimensional
framework. CÐHÁ Á Áꢀ interactions are indicated by dashed lines, and
the unit-cell box has been omitted for clarity. [Symmetry code: (iii) 1 x,
y, 2 z.]
ꢂ
Acta Cryst. (2003). C59, m328±m330
Mario Cetina et al. [Fe(C5H5)(C14H13O)] m329