Yong
Yu
a,
Andrew D.
Bond
b,
Philip W.
Leonard
a,
Ulrich J.
Lorenz
a,
Tatiana V.
Timofeeva
c,
K. Peter C.
Vollhardt
*a,
Glenn D.
Whitener
a and
Andrey A.
Yakovenko
c
aDepartment of Chemistry, University of California at Berkeley, and the Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720-1460, USA. E-mail: kpcv@berkeley.edu; Fax: ++1 510 643 5208; Tel: ++1 510 642 0286
bDepartment of Chemistry, University of Southern Denmark, Campusvej 55, 5230 Odense M, Denmark
cDepartment of Natural Sciences, New Mexico Highlands University, Las Vegas, NM 87701, USA
First published on 23rd May 2006
Hexaferrocenylbenzene has been synthesized by six-fold Negishi type ferrocenylation of hexabromo- or hexaiodobenzene.
Indeed, when hexaiodobenzene was treated with six equivalents of diferrocenylzinc,11,12 prepared from iodoferrocene13 by lithiation with BuLi followed by zincation with ZnBr2, complex 1 was obtained (4%), in addition to pentaferrocenylbenzene 2 (56%; Scheme 1, Fig. 1), separated by repeated chromatography on silica.‡ The observation of substantial quantities of 2 is evidence for the reluctance of the final system or its precursors to incorporate six bulky substituents around the benzene core, although the origin of the proton is obscure.14 Prolonged reaction times or using excess Fc2Zn did not improve yields. Switching the substrate to C6Br6 slowed conversion and allowed the isolation of 1 (1%), 2 (4%), and, in addition, products 3–5 (Fig. 1), as described in the Supplementary Information†. The structures of complexes 1–4 were ascertained by X-ray crystallographic analysis.§ HPLC of crude reaction mixtures showed a plethora of other compounds, presumably variously ferrocenylated benzenes bearing varying amounts of residual bromines, therefore the products reported are not representative of the entire spectrum of complexes generated.
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Fig. 1 Products of incomplete ferrocenylation of C6X6. |
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Scheme 1 Synthesis of hexaferrocenylbenzene 1. Reagents and conditions: (i) Pd2(dba)3 (30%), THF, 68 °C, 63 h. |
The title compound is remarkably stable, but sensitive to air, especially in solution. The crowded nature of the molecule notwithstanding, the NMR spectra indicate considerable flexibility and average symmetry at room temperature. However, VTNMR reveals decoalescence of the signals due to H3 and H4 at −60 °C to four peaks in the ratio 1 ∶ 1 ∶ 1 ∶ 1 at δ = 3.96 (C3), 4.26 (C4), 4.35 (C4′), and 4.57 (C3′) ppm, while the remote CpH absorptions remain as a singlet, signaling (at least local) chirality around C1–C4. Quantification of the data by EXSY provides ΔH‡ = 10.5 (±0.6) kcal mol−1 and ΔS‡ = −0.6 e.u (±3). Thus, as expected, symmetrization is more energetic than that in the pentaferrocenylcyclopentadienyl (Fc5Cp) scaffold,11 but not by much. On the basis of the X-ray structural features (vide infra), we propose a static, chiral, propeller-like structure with alternating “up–down” Fe atoms, all oriented in the same sense around the periphery, the NMR dynamics originating from enantiomerization by a presumably ungeared6 substituent motion that leaves the facial disposition of the metals unchanged. The 13C resonance for the central C6 fragment is surprisingly normal.15 Effective electronic communication is apparent in the UV spectrum, which displays bathochromic shifts relative to that of ferrocene (λmax = 325, 440 nm)16 and 1,3,5-triferrocenylbenzene (λmax = 330, 450 nm).1b Similarly, and in contrast to various Fcnbenzenes (n = 2–4),9,17 the voltammogram (see Supplementary Information†) exhibits clearly separated redox waves, E1/2 = −162.8 (1 e wave), −32.3 (2 e wave), and 222.4 (3 e wave) mV (CH2Cl2, NBu4PF6, versus [Cp2Fe]0/[Cp2Fe]+).
The extraordinary steric encumbrance in 1 is evident in its X-ray structural details (Fig. 2). The molecule has been characterized as two different solid-state solvates, and the conformation of 1 is indistinguishable in the two cases. In the following analysis, the corresponding geometric values found in the structure of the parent ferrocenylbenzene18 are given in italics. The molecule is arranged roughly as assumed above for the low-temperature NMR species, in this way minimizing steric and angle strain. The radial C5H4 substituents deviate substantially from coplanarity with the benzene frame. Thus, the dihedral angles of the respective benzene ring bonds with their proximal C5H4 counterparts (e.g., C1–C2–C17–C18, C2–C3–C27–C31, etc.) fall into two alternating groups averaging 30.8 and −81.9°, respectively (10.6°). As in Fc5CpMn(CO)3,11 but to a significantly attenuated degree, there appear to be elongated C5H4quat–Fe bonds in the direction of η1,η4-bonding [average bond lengths (long/short, Å): 2.09 (2.05)/2.04 (2.03)], and bent ferrocenyls, average value 177.2 (179.9)°. The quaternary C5H4 carbons are pyramidalized, such as to minimize interference of the appended CpFe unit with the neighboring Fc substituent, quantified by the nonlinear C5H4centroid–C5H4quat–Carom linkages, average value 170.1 (179.9)°. Further strain relief appears derived from elongated C5H4quat–Carom distances, average value 1.50 [1.469(5)] Å.
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Fig. 2 Hexaferrocenylbenzene 1 in the solid 1·C6H6, showing displacement ellipsoids at 50% probability. The H atoms have been omitted for clarity. Selected bond distances (Å) and angles (°): C1–C2 1.413(6), C2–C3 1.431(5), C3–C4 1.409(5), C4–C5 1.431(5), C5–C6 1.415(5), C6–C1 1.419(5), C1–C7 1.498(5); C1–C2–C3 119.1(4), C5H4Fe1centroid–C7–C1 172.7, C1–C2–C3–C4 −13.7(6), C1–C2–C17–C18 −75.8(6), C7–C1–C2–C17 39.1(5). |
Most obvious are the distortions of the central ring caused by perferrocenylation. Thus, the benzene ring adopts a chair conformation, evidenced by alternating dihedral angles along the carbon sequence (e.g., C1–C2–C3–C4, etc.), average ± 14.0 (0.25)°, large torsion angles C5H4quat–Carom–Carom–C5H4quat, absolute values ranging from 37.5(5) to 40.5(6)° [average 38.9 (1.8 for C5H4quat–Carom–Carom–H)], and elongated bonds, average 1.42 (1.37) Å. In addition, there is noticeable bond alternation with long/short bonds averaging 1.427/1.411 Å. The bond angles deviate minimally from 120° (average 119.5°). Taking the plane C1–C2–C4–C5 (rms. deviation 0.001 Å) as a reference, C3 lies 0.148(6) Å above this plane and C6 lies 0.152(6) Å below it. These deformations are larger than those in the current record C6(SiMe3)6 (comparable deviations from the C1–C2–C4–C5 plane +0.13 and −0.08 Å)19 and other symmetrically hexasubstituted benzenes.20
Comparison of the structure of 1 with that of the pentaferrocenyl derivative 2 (Fig. 3) is revealing. Thus, the space supplied by removing one Fc substituent generates a much less ordered overall geometry, with Fc1 aligned roughly perpendicular to the benzene core [C6–C1–C7–C11 86.2(6)°], the remaining Fcs arranged in an up–down manner, but varying in the extent to which they are not coplanar and in their sense of direction [corresponding dihedral angles Fc2–Fc5: 31.1(7), −28.2(7), 15.8(6), 37.6(7)°]. As one might expect, the C6 core is more deformed from expected geometry around C6 than around C3. For example, the C1–C6 and C5–C6 bonds [both 1.392(6) Å] are close to that expected for a benzene ring, while the other four bonds (average 1.426 Å) are significantly elongated; the four Carom dihedrals incorporating C6 are smaller (average 8.6°) than the remaining two (average 27.0°); the C47–C5–C6–H6A–C1–C7 fragment is basically flat (rms deviation 0.002 Å), whereas the torsions C5H4quat–Carom–Carom–C5H4quat range from −14.0(6)° (C7–C1–C2–C17) to −47.9(5)° (C27–C3–C4–C37). Taking the near-plane C1–C2–C4–C5 (rms deviation 0.026 Å) as a reference, C6 is only slightly displaced from it [0.075(6) Å], but C3 acutely so [0.294(6) Å], and both in the same direction, thus describing a halfboat-like center ring.
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Fig. 3 Pentaferrocenylbenzene 2 in the solid, showing displacement ellipsoids at 50% probability. The H atoms have been omitted for clarity. For selected features, see text. |
Interestingly, in the structure of 3 (see Supplementary Information†), the sizeable Br atom serves to symmetrize the molecule substantially, with a pseudo-mirror plane passing through Br, C1, and C4 (for numbering, see Fig. 1), and the Fcs arranged in a regular up–down sequence. Taking the plane C2–C3–C5–C6 (rms deviation 0.006 Å) as a reference, C1 lies essentially in it [displacement 0.011(8) Å], while C4 is displaced substantially [0.272(7) Å] from it. The other features of 3 are similar to those of 2.
Finally, the structure of 4 deviates much less from expectation than the preceding molecules, most notable being a small dihedral angle of 3.8(6)° between the two ortho-ferrocenyls, and two elongated Carom–Carom bonds, one separating the two Fcs [1.439(6) Å], and one between one of these Fcs and the adjacent Br atom [1.431(6) Å]. The benzene ring is fairly flat (rms deviation of all six C atoms 0.025 Å, average Carom–Carom–Carom–Carom = 3.5°).
In summary, we have shown that hexaferrocenylbenzene 1 can be made, despite its considerably encumbered structure, and that it shows remarkable conformational mobility in solution. Current efforts are directed at improving yields and exploring the chemistry of this molecule along the lines described in the introduction.
This work was supported by the Director, Office of Energy Research, Office of Basic Energy Sciences, Chemical Sciences Division, of the US Department of Energy, under Contract DE-AC02-05CH11231 (KPCV) and MRI/NSF 0420863 (TVT). PWL was an NSF Fellow, GDW was supported by NSF and Bayer-Miles predoctoral fellowships, and UL is grateful for a German National Academic Foundation Scholarship. We thank Dr Alex Shafir for expert assistance with the CV measurements and Professor J. Arnold for illuminating discussions.
Footnotes |
† Electronic supplementary information (ESI) available: Experimental and X-ray structural data. See DOI: 10.1039/b604844g |
‡ 1: Yellow-orange crystals. Mp: 270 °C (decomp.). Anal.: Calc. for C66H54Fe6: C, 67.05; H, 4.60%. Found: C, 66.99; H, 4.87%. HRMS (m/z): Calc. for C66H54Fe6: 1182.0322. Found: 1182.0345. 1H NMR (300 MHz, CD2Cl2, δ/ppm): 4.35 (BB'm, 12H, H4), 4.32 (AA'm, 12H, H3), 3.99 (s, 30H, CpH). 13C{1H} NMR (100 MHz, CD2Cl2, δ/ppm): 137.6 (C1), 93.0 (C2), 75.0 (C3), 70.0 (Cp), 67.8 (C4). IR (KBr, cm−1): 3100, 1655, 1638, 1459, 1108, 817. UV/VIS (CH2Cl2, nm/ε): 274sh (11400), 312 (11400), 370 (5850), 462 (1620). 2: Orange-red powder. Mp: 166-168 °C (decomp.). Anal.: Calc. for C56H46Fe5: C, 67.38; H, 4.64%. Found: C, 67.61; H, 4.89%. HRMS (m/z): Calc. for C56H46Fe5: 998.0346. Found: 998.0326. 1H NMR (300 MHz, CD2Cl2, δ/ppm): 8.29 (s, 1H), 4.85 (t, J = 1.8 Hz, 4H), 4.47 (t, J = 1.8 Hz, 4H), 4.38 (s, 10H), 4.32 (t, J = 1.8 Hz, 4H), 4.19 (t, J = 1.8 Hz, 4H), 3.90 (m, 4H), 3.88 (s, 5H), 3.85 (s, 10H). 13C{1H} NMR (100 MHz, CD2Cl2, δ/ppm): 143.3, 136.7, 133.0, 132.2 (CH), 92.8, 91.5, 88.9, 73.7, 72.2, 71.9, 69.9, 69.6 (2Cp), 69.5 (Cp), 67.4, 67.39, 67.30, 67.26. IR (KBr, cm−1): 3100, 1655, 1638, 1459, 1107, 817. UV/VIS (CH2Cl2, nm/ε): 296sh (18800), 354sh (11000), 466 (2840). |
§ Crystallographic data.1·C6H6
(from C6H6): C72H60Fe6, M
= 1260.3, T
= 100(2) K, crystal size 0.30 × 0.10 × 0.02 mm3, monoclinic, space group C2/c, a
= 39.8230(12), b
= 11.4629(3), c
= 22.8543(6)
Å, α
= 90, β
= 90.923(1), γ
= 90°, V
= 10431.3(5)
Å3, Z
= 8, Dcalc
= 1.605 g cm−3, μ(Mo Kα)
= 1.672 mm−1, 9210 unique reflections, of which 6409 were taken as observed [I > 2σ(I)], R1 = 0.041, wR2 = 0.104 (all data), S
= 1.01. 1·½C6H4Cl2
(from MeOH–C6H4Cl2): C69H56ClFe6, M
= 1255.7, T
= 220(2) K, crystal size 0.14 × 0.10 × 0.01 mm3, monoclinic, space group I2/a, a
= 44.218(11), b
= 11.535(2), c
= 22.898(5)
Å, α
= 90, μ
= 93.960(9), γ
= 90°, V
= 11651(4)
Å3, Z
= 8, Dcalc
= 1.432 g cm−3, μ(synchrotron, λ
= 0.6850 Å)
= 1.541 mm−1, 8218 unique reflections, of which 5820 were taken as observed [I > 2σ(I)], R1 = 0.105, wR2 = 0.291 (all data), S
= 1.04. 2
(from MeOH–CH2Cl2): C56H46Fe5, M
= 998.2, T
= 130(2) K, crystal size 0.50 × 0.20 × 0.18 mm3, triclinic, space group P![]() |
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