Download citation
Download citation
link to html
In the title compound, [Fe(C5H4)2(CH3Si)]2O, the cyclo­penta­dienyl rings in both ferrocenophane moieties are tilted towards the bridging Si atoms, with tilt angles of 19.7 (2) and 20.7 (2)°; the central Si—O—Si angle is 143.25 (12)°.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802016690/ob6177sup1.cif
Contains datablocks k99163, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802016690/ob6177Isup2.hkl
Contains datablock I

CCDC reference: 198308

Key indicators

  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.029
  • wR factor = 0.069
  • Data-to-parameter ratio = 17.8

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry

General Notes

REFLT_03 From the CIF: _diffrn_reflns_theta_max 27.46 From the CIF: _reflns_number_total 4381 Count of symmetry unique reflns 2514 Completeness (_total/calc) 174.26% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 1867 Fraction of Friedel pairs measured 0.743 Are heavy atom types Z>Si present yes Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF.

Comment top

The title compound was isolated in trace amounts as an impurity from aged samples of the silicon-bridged [1]ferrocenophane, (II), (Zechel et al., 1996) which possesses a hydrolytically sensitive Si—Cl moiety. The bis(sila[1]ferrocenophane), (I), is of potential utility as a crosslinking agent in the polymerization of other sila[1]ferrocenophanes (MacLachlan et al., 1996, 2000; Kulbaba et al., 2001; Kulbaba & Manners, 2001); however, attempts to produce it on a large scale have been unsuccessful to date.

In (I), the cyclopentadienyl (Cp) rings of both of the ferrocenophane groups are tilted towards the bridging Si atoms. The angle between the least-squares planes of the Cp rings bonded to Fe1 is 19.7 (2)°, and the angle between the Cp rings bonded to Fe2 is 20.7 (2)°. The tilt of the Cp rings is also reflected in the variation of the Fe—C distances in each of the ferrocene groups. The Fe—C distances in the ferrocene group containing Fe1 range from 2.010 (2) to 2.082 (3) Å and in the ferrocene group containing Fe2, the Fe—C distances range from 2.009 (3) to 2.087 (3) Å. The shortest Fe—C distances are for the C atoms which are also bonded to the bridging Si atoms, namely C1, C6, C11 and C16 (see Table 1). The overall conformation of the molecule is twisted such that the ferrocene groups are rotated about the Si—O bonds so that the they are approximately perpendicular to each other (sse Fig. 1). The degree of rotation can be described by a torsion angle calculated using the non-bonded atoms Fe1—Si1—Si2—Fe2, which gives a value of 75.07 (5)°. The Si1—O1—Si2 angle is 143.25 (12)°.

Experimental top

Crystals of (I) were obtained at 243 K in trace amounts from the hexanes-soluble fraction of a reaction mixture which initially contained (II). No other hexanes-soluble products were formed in this reaction, and an investigation of the sample of (II) utilized in the synthesis revealed the presence of trace (< 5%) amounts of (I). For 1: 1H NMR (400 MHz, C6D6, 298 K): δ = 4.46–4.44 (m, 4 H, Cp), 4.42–4.39 (m, 8 H, Cp), 3.87–3.86 (m, 4 H, Cp), 0.58 (s, 6 H, Me); 13C{1H} NMR (100.4 MHz, C6D6, 298 K): δ = 78.4, 77.8, 75.9, 74.5 (Cp), 38.7 (ipso-Cp), −0.6 (Me); 29Si{1H} NMR (79.3 MHz, C6D6, 298 K): δ = −13.4.

Refinement top

All hydrogen atoms were included in calculated positions, with distances of 1.00 Å (for Cp C—H) and 0.98 Å (for methyl C—H). In the refinement hydrogen atoms were included in riding-motion approximation, with Uiso = 1.2Ueq (1.5eq for methyl) of the carrier atom.

Computing details top

Data collection: COLLECT (Nonius 1997-2001); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN; program(s) used to solve structure: SHELXTL (Sheldrick, 1999); program(s) used to refine structure: SHELXT; molecular graphics: SHELXT; software used to prepare material for publication: SHELXT.

Figures top
[Figure 1] Fig. 1. View of molecule (I), with displacement ellipsoids drawn at the 50% probability level.
(I) top
Crystal data top
[Fe(C5H4)2(CH3Si)]2OF(000) = 968
Mr = 470.28Dx = 1.631 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 19591 reflections
a = 7.5203 (1) Åθ = 2.9–27.5°
b = 11.4213 (3) ŵ = 1.65 mm1
c = 22.2986 (6) ÅT = 100 K
V = 1915.26 (8) Å3Plate, orange
Z = 40.35 × 0.32 × 0.10 mm
Data collection top
Nonius Kappa-CCD
diffractometer
4381 independent reflections
Radiation source: fine-focus sealed tube3810 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.075
Detector resolution: 9 pixels mm-1θmax = 27.5°, θmin = 2.9°
ϕ scans and ω scans with κ offsetsh = 99
Absorption correction: multi-scan
(DENZO-SMN; Otwinowski & Minor, 1997)
k = 1414
Tmin = 0.596, Tmax = 0.853l = 2828
19591 measured reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.029H-atom parameters constrained
wR(F2) = 0.069 w = 1/[σ2(Fo2) + (0.0359P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max = 0.001
4381 reflectionsΔρmax = 0.31 e Å3
246 parametersΔρmin = 0.48 e Å3
0 restraintsAbsolute structure: (Flack, 1983), 1871 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.009 (13)
Crystal data top
[Fe(C5H4)2(CH3Si)]2OV = 1915.26 (8) Å3
Mr = 470.28Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 7.5203 (1) ŵ = 1.65 mm1
b = 11.4213 (3) ÅT = 100 K
c = 22.2986 (6) Å0.35 × 0.32 × 0.10 mm
Data collection top
Nonius Kappa-CCD
diffractometer
4381 independent reflections
Absorption correction: multi-scan
(DENZO-SMN; Otwinowski & Minor, 1997)
3810 reflections with I > 2σ(I)
Tmin = 0.596, Tmax = 0.853Rint = 0.075
19591 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.029H-atom parameters constrained
wR(F2) = 0.069Δρmax = 0.31 e Å3
S = 1.00Δρmin = 0.48 e Å3
4381 reflectionsAbsolute structure: (Flack, 1983), 1871 Friedel pairs
246 parametersAbsolute structure parameter: 0.009 (13)
0 restraints
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Fe10.48696 (5)0.40794 (3)0.070092 (16)0.01818 (9)
Fe20.91547 (5)0.44410 (3)0.332136 (17)0.01771 (9)
Si10.73986 (9)0.55859 (7)0.10626 (3)0.01936 (16)
Si20.77709 (10)0.57814 (6)0.24443 (3)0.01971 (16)
O10.8254 (2)0.55946 (16)0.17346 (8)0.0220 (4)
C10.4897 (4)0.5665 (2)0.10918 (11)0.0211 (5)
C20.3935 (4)0.4853 (2)0.14549 (13)0.0240 (6)
H2A0.42650.46230.18730.029*
C30.2454 (3)0.4395 (3)0.11270 (13)0.0251 (6)
H3A0.15930.37900.12710.030*
C40.2476 (4)0.4922 (2)0.05511 (13)0.0266 (7)
H4A0.16280.47470.02170.032*
C50.3937 (4)0.5711 (2)0.05198 (13)0.0233 (6)
H5A0.42670.62020.01650.028*
C60.7550 (3)0.4089 (2)0.07139 (12)0.0211 (5)
C70.6860 (4)0.3082 (2)0.10450 (12)0.0212 (6)
H7A0.70600.29230.14810.025*
C80.5825 (4)0.2377 (2)0.06505 (13)0.0238 (6)
H8A0.51540.16550.07650.029*
C90.5844 (4)0.2900 (2)0.00733 (12)0.0223 (6)
H9A0.51930.26090.02880.027*
C100.6909 (3)0.3940 (2)0.01038 (12)0.0219 (6)
H10A0.71420.44870.02370.026*
C110.9868 (4)0.5920 (2)0.28970 (12)0.0213 (5)
C120.9703 (4)0.6127 (2)0.35374 (12)0.0241 (6)
H12A0.88560.66870.37300.029*
C131.0925 (3)0.5392 (2)0.38468 (13)0.0243 (6)
H13A1.10570.53310.42920.029*
C141.1873 (4)0.4722 (3)0.34135 (13)0.0274 (7)
H14A1.27900.41110.35000.033*
C151.1240 (3)0.5050 (3)0.28363 (13)0.0261 (6)
H15A1.16630.47130.24480.031*
C160.6991 (3)0.4375 (2)0.27854 (12)0.0205 (5)
C170.6473 (3)0.4380 (2)0.34176 (12)0.0220 (6)
H17A0.57320.49960.36150.026*
C180.7214 (4)0.3389 (2)0.37108 (14)0.0260 (6)
H18A0.71080.32040.41480.031*
C190.8180 (4)0.2732 (2)0.32837 (13)0.0242 (6)
H19A0.88750.20030.33660.029*
C200.8060 (4)0.3321 (2)0.27218 (13)0.0223 (6)
H20A0.86380.30560.23420.027*
C210.8374 (4)0.6748 (2)0.05862 (13)0.0263 (6)
H21A0.83720.74910.08060.040*
H21B0.76680.68300.02190.040*
H21C0.95980.65370.04810.040*
C220.6212 (4)0.7006 (3)0.25725 (14)0.0319 (7)
H22A0.66980.77220.23950.048*
H22B0.60480.71200.30040.048*
H22C0.50640.68240.23860.048*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Fe10.01805 (18)0.01509 (18)0.02140 (19)0.00138 (14)0.00007 (16)0.00107 (15)
Fe20.01664 (17)0.01568 (18)0.02082 (19)0.00169 (14)0.00093 (15)0.00026 (15)
Si10.0212 (3)0.0165 (4)0.0204 (4)0.0003 (3)0.0010 (3)0.0006 (3)
Si20.0224 (3)0.0157 (4)0.0210 (4)0.0002 (3)0.0010 (3)0.0005 (3)
O10.0224 (8)0.0234 (10)0.0203 (9)0.0014 (8)0.0021 (8)0.0009 (9)
C10.0250 (12)0.0140 (12)0.0245 (13)0.0055 (11)0.0007 (12)0.0049 (11)
C20.0210 (13)0.0242 (14)0.0268 (15)0.0014 (11)0.0028 (12)0.0071 (11)
C30.0189 (12)0.0263 (15)0.0302 (15)0.0008 (11)0.0030 (11)0.0049 (12)
C40.0223 (14)0.0244 (14)0.0332 (18)0.0068 (11)0.0054 (12)0.0074 (12)
C50.0264 (14)0.0146 (13)0.0288 (14)0.0068 (11)0.0051 (11)0.0002 (11)
C60.0194 (12)0.0214 (13)0.0224 (13)0.0044 (10)0.0023 (11)0.0034 (12)
C70.0249 (14)0.0175 (13)0.0211 (14)0.0035 (11)0.0036 (12)0.0020 (11)
C80.0276 (14)0.0136 (12)0.0303 (15)0.0017 (11)0.0005 (13)0.0011 (12)
C90.0218 (13)0.0200 (13)0.0250 (14)0.0028 (11)0.0014 (12)0.0053 (11)
C100.0212 (13)0.0199 (14)0.0245 (14)0.0027 (11)0.0016 (11)0.0028 (12)
C110.0258 (13)0.0175 (12)0.0208 (13)0.0066 (12)0.0002 (11)0.0017 (11)
C120.0263 (14)0.0182 (14)0.0279 (15)0.0086 (11)0.0040 (11)0.0018 (11)
C130.0236 (13)0.0254 (15)0.0239 (14)0.0083 (12)0.0035 (12)0.0017 (12)
C140.0144 (12)0.0377 (17)0.0302 (17)0.0023 (11)0.0004 (12)0.0038 (13)
C150.0209 (14)0.0347 (16)0.0227 (15)0.0069 (12)0.0039 (12)0.0022 (12)
C160.0160 (11)0.0196 (14)0.0259 (14)0.0023 (10)0.0021 (10)0.0014 (12)
C170.0152 (11)0.0216 (14)0.0291 (15)0.0034 (10)0.0047 (10)0.0008 (12)
C180.0258 (15)0.0242 (15)0.0282 (16)0.0090 (11)0.0009 (12)0.0038 (12)
C190.0264 (14)0.0156 (13)0.0306 (15)0.0033 (10)0.0060 (13)0.0031 (12)
C200.0237 (13)0.0177 (13)0.0256 (15)0.0010 (11)0.0021 (12)0.0010 (11)
C210.0315 (15)0.0230 (14)0.0246 (16)0.0024 (12)0.0029 (12)0.0004 (12)
C220.0442 (19)0.0212 (15)0.0304 (17)0.0072 (13)0.0059 (14)0.0027 (12)
Geometric parameters (Å, º) top
Fe1—C12.010 (2)C4—C51.423 (4)
Fe1—C62.016 (2)C4—H4A1.0000
Fe1—C22.025 (3)C5—H5A1.0000
Fe1—C72.032 (3)C6—C101.454 (4)
Fe1—C52.032 (3)C6—C71.462 (4)
Fe1—C102.037 (3)C7—C81.424 (4)
Fe1—C42.068 (3)C7—H7A1.0000
Fe1—C92.076 (3)C8—C91.419 (4)
Fe1—C82.076 (3)C8—H8A1.0000
Fe1—C32.082 (3)C9—C101.434 (4)
Fe1—Si12.6885 (8)C9—H9A1.0000
Fe2—C112.009 (3)C10—H10A1.0000
Fe2—C162.020 (3)C11—C151.439 (4)
Fe2—C202.025 (3)C11—C121.453 (4)
Fe2—C122.027 (3)C12—C131.423 (4)
Fe2—C152.028 (3)C12—H12A1.0000
Fe2—C172.030 (2)C13—C141.424 (4)
Fe2—C142.079 (3)C13—H13A1.0000
Fe2—C132.080 (3)C14—C151.422 (4)
Fe2—C182.080 (3)C14—H14A1.0000
Fe2—C192.087 (3)C15—H15A1.0000
Fe2—Si22.6929 (8)C16—C201.454 (4)
Si1—O11.6308 (18)C16—C171.463 (4)
Si1—C211.851 (3)C17—C181.421 (4)
Si1—C61.882 (3)C17—H17A1.0000
Si1—C11.885 (3)C18—C191.413 (4)
Si2—O11.6377 (19)C18—H18A1.0000
Si2—C221.847 (3)C19—C201.425 (4)
Si2—C161.871 (3)C19—H19A1.0000
Si2—C111.879 (3)C20—H20A1.0000
C1—C21.429 (4)C21—H21A0.9800
C1—C51.466 (4)C21—H21B0.9800
C2—C31.431 (4)C21—H21C0.9800
C2—H2A1.0000C22—H22A0.9800
C3—C41.418 (4)C22—H22B0.9800
C3—H3A1.0000C22—H22C0.9800
C1—Fe1—C688.78 (11)C4—C3—H3A126.3
C1—Fe1—C241.46 (11)C2—C3—H3A126.3
C6—Fe1—C2109.43 (11)Fe1—C3—H3A126.3
C1—Fe1—C7109.52 (11)C3—C4—C5108.8 (2)
C6—Fe1—C742.35 (10)C3—C4—Fe170.52 (15)
C2—Fe1—C7100.76 (11)C5—C4—Fe168.31 (15)
C1—Fe1—C542.54 (10)C3—C4—H4A125.6
C6—Fe1—C5110.06 (11)C5—C4—H4A125.6
C2—Fe1—C569.22 (11)Fe1—C4—H4A125.6
C7—Fe1—C5147.55 (11)C4—C5—C1108.4 (2)
C1—Fe1—C10110.26 (11)C4—C5—Fe171.09 (15)
C6—Fe1—C1042.03 (10)C1—C5—Fe167.95 (14)
C2—Fe1—C10146.94 (11)C4—C5—H5A125.8
C7—Fe1—C1069.41 (11)C1—C5—H5A125.8
C5—Fe1—C10101.64 (11)Fe1—C5—H5A125.8
C1—Fe1—C470.10 (11)C10—C6—C7105.2 (2)
C6—Fe1—C4150.46 (11)C10—C6—Si1118.24 (19)
C2—Fe1—C468.23 (11)C7—C6—Si1119.00 (19)
C7—Fe1—C4164.39 (12)C10—C6—Fe169.75 (14)
C5—Fe1—C440.60 (11)C7—C6—Fe169.38 (14)
C10—Fe1—C4125.88 (11)Si1—C6—Fe187.14 (10)
C1—Fe1—C9150.85 (11)C8—C7—C6109.1 (2)
C6—Fe1—C970.15 (11)C8—C7—Fe171.41 (15)
C2—Fe1—C9164.83 (11)C6—C7—Fe168.27 (14)
C7—Fe1—C968.32 (11)C8—C7—H7A125.4
C5—Fe1—C9125.66 (11)C6—C7—H7A125.4
C10—Fe1—C940.79 (11)Fe1—C7—H7A125.4
C4—Fe1—C9120.01 (11)C9—C8—C7108.5 (2)
C1—Fe1—C8149.76 (11)C9—C8—Fe170.01 (15)
C6—Fe1—C870.12 (11)C7—C8—Fe168.04 (14)
C2—Fe1—C8124.99 (12)C9—C8—H8A125.7
C7—Fe1—C840.55 (11)C7—C8—H8A125.7
C5—Fe1—C8165.43 (12)Fe1—C8—H8A125.7
C10—Fe1—C868.33 (11)C8—C9—C10108.1 (2)
C4—Fe1—C8136.73 (11)C8—C9—Fe170.02 (15)
C9—Fe1—C839.98 (10)C10—C9—Fe168.15 (15)
C1—Fe1—C369.81 (11)C8—C9—H9A125.9
C6—Fe1—C3149.89 (11)C10—C9—H9A125.9
C2—Fe1—C340.76 (10)Fe1—C9—H9A125.9
C7—Fe1—C3124.60 (11)C9—C10—C6109.1 (2)
C5—Fe1—C368.31 (12)C9—C10—Fe171.06 (15)
C10—Fe1—C3165.66 (11)C6—C10—Fe168.22 (14)
C4—Fe1—C339.96 (11)C9—C10—H10A125.4
C9—Fe1—C3136.73 (11)C6—C10—H10A125.4
C8—Fe1—C3119.28 (12)Fe1—C10—H10A125.4
C11—Fe2—C1688.15 (11)C15—C11—C12105.4 (2)
C11—Fe2—C20109.18 (11)C15—C11—Si2119.56 (19)
C16—Fe2—C2042.13 (11)C12—C11—Si2118.0 (2)
C11—Fe2—C1242.19 (11)C15—C11—Fe269.83 (15)
C16—Fe2—C12109.86 (11)C12—C11—Fe269.56 (14)
C20—Fe2—C12147.08 (11)Si2—C11—Fe287.59 (11)
C11—Fe2—C1541.75 (11)C13—C12—C11109.0 (2)
C16—Fe2—C15108.67 (11)C13—C12—Fe271.73 (15)
C20—Fe2—C15100.32 (12)C11—C12—Fe268.25 (15)
C12—Fe2—C1569.12 (12)C13—C12—H12A125.5
C11—Fe2—C17110.12 (12)C11—C12—H12A125.5
C16—Fe2—C1742.35 (10)Fe2—C12—H12A125.5
C20—Fe2—C1769.14 (11)C12—C13—C14108.1 (2)
C12—Fe2—C17102.09 (12)C12—C13—Fe267.75 (15)
C15—Fe2—C17146.79 (11)C14—C13—Fe269.98 (15)
C11—Fe2—C1469.77 (11)C12—C13—H13A125.9
C16—Fe2—C14148.86 (11)C14—C13—H13A125.9
C20—Fe2—C14124.23 (12)Fe2—C13—H13A125.9
C12—Fe2—C1468.28 (12)C15—C14—C13107.8 (3)
C15—Fe2—C1440.49 (11)C15—C14—Fe267.82 (15)
C17—Fe2—C14166.36 (11)C13—C14—Fe269.99 (15)
C11—Fe2—C1369.84 (11)C15—C14—H14A126.1
C16—Fe2—C13150.27 (11)C13—C14—H14A126.1
C20—Fe2—C13164.17 (11)Fe2—C14—H14A126.1
C12—Fe2—C1340.52 (11)C14—C15—C11109.7 (2)
C15—Fe2—C1368.05 (11)C14—C15—Fe271.69 (16)
C17—Fe2—C13126.48 (11)C11—C15—Fe268.42 (14)
C14—Fe2—C1340.04 (11)C14—C15—H15A125.2
C11—Fe2—C18150.40 (12)C11—C15—H15A125.2
C16—Fe2—C1870.15 (11)Fe2—C15—H15A125.2
C20—Fe2—C1868.02 (12)C20—C16—C17104.2 (2)
C12—Fe2—C18126.29 (11)C20—C16—Si2119.84 (19)
C15—Fe2—C18164.42 (12)C17—C16—Si2118.2 (2)
C17—Fe2—C1840.43 (11)C20—C16—Fe269.11 (15)
C14—Fe2—C18137.53 (12)C17—C16—Fe269.17 (14)
C13—Fe2—C18121.03 (11)Si2—C16—Fe287.48 (10)
C11—Fe2—C19149.46 (11)C18—C17—C16109.6 (2)
C16—Fe2—C1970.02 (11)C18—C17—Fe271.69 (15)
C20—Fe2—C1940.52 (11)C16—C17—Fe268.48 (13)
C12—Fe2—C19165.80 (11)C18—C17—H17A125.2
C15—Fe2—C19124.84 (12)C16—C17—H17A125.2
C17—Fe2—C1967.84 (11)Fe2—C17—H17A125.2
C14—Fe2—C19119.60 (12)C19—C18—C17108.3 (2)
C13—Fe2—C19137.40 (11)C19—C18—Fe270.43 (16)
C18—Fe2—C1939.65 (11)C17—C18—Fe267.88 (14)
O1—Si1—C21111.50 (12)C19—C18—H18A125.8
O1—Si1—C6111.18 (11)C17—C18—H18A125.8
C21—Si1—C6112.97 (13)Fe2—C18—H18A125.8
O1—Si1—C1111.21 (11)C18—C19—C20108.0 (2)
C21—Si1—C1112.39 (13)C18—C19—Fe269.92 (15)
C6—Si1—C196.82 (11)C20—C19—Fe267.41 (15)
O1—Si2—C22112.89 (12)C18—C19—H19A126.0
O1—Si2—C16110.51 (11)C20—C19—H19A126.0
C22—Si2—C16112.84 (13)Fe2—C19—H19A126.0
O1—Si2—C11110.11 (11)C19—C20—C16109.9 (2)
C22—Si2—C11112.69 (13)C19—C20—Fe272.06 (16)
C16—Si2—C1196.72 (11)C16—C20—Fe268.76 (15)
Si1—O1—Si2143.25 (12)C19—C20—H20A125.1
C2—C1—C5105.5 (2)C16—C20—H20A125.1
C2—C1—Si1119.59 (19)Fe2—C20—H20A125.1
C5—C1—Si1117.58 (19)Si1—C21—H21A109.5
C2—C1—Fe169.82 (15)Si1—C21—H21B109.5
C5—C1—Fe169.51 (14)H21A—C21—H21B109.5
Si1—C1—Fe187.24 (11)Si1—C21—H21C109.5
C1—C2—C3110.0 (2)H21A—C21—H21C109.5
C1—C2—Fe168.72 (15)H21B—C21—H21C109.5
C3—C2—Fe171.74 (15)Si2—C22—H22A109.5
C1—C2—H2A125.0Si2—C22—H22B109.5
C3—C2—H2A125.0H22A—C22—H22B109.5
Fe1—C2—H2A125.0Si2—C22—H22C109.5
C4—C3—C2107.4 (2)H22A—C22—H22C109.5
C4—C3—Fe169.52 (15)H22B—C22—H22C109.5
C2—C3—Fe167.50 (15)
Fe1—Si1—Si2—Fe275.07 (5)

Experimental details

Crystal data
Chemical formula[Fe(C5H4)2(CH3Si)]2O
Mr470.28
Crystal system, space groupOrthorhombic, P212121
Temperature (K)100
a, b, c (Å)7.5203 (1), 11.4213 (3), 22.2986 (6)
V3)1915.26 (8)
Z4
Radiation typeMo Kα
µ (mm1)1.65
Crystal size (mm)0.35 × 0.32 × 0.10
Data collection
DiffractometerNonius Kappa-CCD
diffractometer
Absorption correctionMulti-scan
(DENZO-SMN; Otwinowski & Minor, 1997)
Tmin, Tmax0.596, 0.853
No. of measured, independent and
observed [I > 2σ(I)] reflections
19591, 4381, 3810
Rint0.075
(sin θ/λ)max1)0.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.029, 0.069, 1.00
No. of reflections4381
No. of parameters246
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.31, 0.48
Absolute structure(Flack, 1983), 1871 Friedel pairs
Absolute structure parameter0.009 (13)

Computer programs: COLLECT (Nonius 1997-2001), DENZO-SMN (Otwinowski & Minor, 1997), DENZO-SMN, SHELXTL (Sheldrick, 1999), SHELXT.

Selected geometric parameters (Å, º) top
Fe1—C12.010 (2)Fe2—C152.028 (3)
Fe1—C62.016 (2)Fe2—C172.030 (2)
Fe1—C22.025 (3)Fe2—C142.079 (3)
Fe1—C72.032 (3)Fe2—C132.080 (3)
Fe1—C52.032 (3)Fe2—C182.080 (3)
Fe1—C102.037 (3)Fe2—C192.087 (3)
Fe1—C42.068 (3)Si1—O11.6308 (18)
Fe1—C92.076 (3)Si1—C211.851 (3)
Fe1—C82.076 (3)Si1—C61.882 (3)
Fe1—C32.082 (3)Si1—C11.885 (3)
Fe2—C112.009 (3)Si2—O11.6377 (19)
Fe2—C162.020 (3)Si2—C221.847 (3)
Fe2—C202.025 (3)Si2—C161.871 (3)
Fe2—C122.027 (3)Si2—C111.879 (3)
O1—Si1—C6111.18 (11)O1—Si2—C11110.11 (11)
O1—Si1—C1111.21 (11)C16—Si2—C1196.72 (11)
C6—Si1—C196.82 (11)Si1—O1—Si2143.25 (12)
O1—Si2—C16110.51 (11)
Fe1—Si1—Si2—Fe275.07 (5)
 

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds