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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 18;67(Pt 7):m949. doi: 10.1107/S1600536811022951

1,1′-Di-tert-butyl-2,2′,3,3′,4,4′,5,5′-octa­ethyl-1,1′-bis­tannole

Takuya Kuwabara a, Masaichi Saito a,*
PMCID: PMC3152095  PMID: 21836931

Abstract

The title compound, [Sn2(C4H9)2(C12H20)2], has two 1-stannacyclo­penta­diene skeletons related by inversion symmetry located at the mid-point of the Sn—Sn bond [2.7682 (2) Å]. Thus, the asymmetric unit comprises one half-mol­ecule. The planarity of the stannacyclo­penta­diene ring is illustrated by the dihedral angle of 0.3 (1)°, defined by the C4 and C—Sn—C planes. To avoid steric repulsion, the two stannole rings are oriented in an anti fashion through the Sn—Sn bond. These structural features are similar to those of other bis­tannoles.

Related literature

For the synthesis and X-ray diffraction analysis of bi(1,1-stannole)s whose carbon atoms of the five-membered rings have phenyl groups, see: Saito et al. (2002, 2005). For related literature on bi-, oligo- and poly-(1,1-metallole)s, see: Haga et al. (2008); Kanno et al. (1998); Kim & Woo (2002); Saito & Yoshioka (2005); Saito et al. (2010); Sohn et al. (1999, 2003); Yamaguchi & Tamao (1998); Yamaguchi et al. (1997, 1999).graphic file with name e-67-0m949-scheme1.jpg

Experimental

Crystal data

  • [Sn2(C4H9)2(C12H20)2]

  • M r = 680.20

  • Monoclinic, Inline graphic

  • a = 8.7161 (5) Å

  • b = 16.5999 (9) Å

  • c = 11.7913 (6) Å

  • β = 100.827 (1)°

  • V = 1675.67 (16) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 1.51 mm−1

  • T = 100 K

  • 0.25 × 0.10 × 0.05 mm

Data collection

  • Bruker APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (XPREP; Bruker, 2008) T min = 0.835, T max = 0.927

  • 9015 measured reflections

  • 3636 independent reflections

  • 3387 reflections with I > 2σ(I)

  • R int = 0.017

Refinement

  • R[F 2 > 2σ(F 2)] = 0.017

  • wR(F 2) = 0.043

  • S = 1.04

  • 3636 reflections

  • 161 parameters

  • H-atom parameters constrained

  • Δρmax = 0.43 e Å−3

  • Δρmin = −0.42 e Å−3

Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT and XPREP (Bruker, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XSHELL (Bruker, 2008); software used to prepare material for publication: XCIF (Bruker, 2008).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811022951/kp2332sup1.cif

e-67-0m949-sup1.cif (17.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811022951/kp2332Isup2.hkl

e-67-0m949-Isup2.hkl (177.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811022951/kp2332Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected geometric parameters (Å, °).

Sn1—C1 2.1416 (15)
Sn1—C4 2.1475 (16)
Sn1—C5 2.1906 (16)
C1—Sn1—C4 83.75 (6)

Symmetry code: (i) Inline graphic.

Acknowledgments

This work was partially supported by Grant-in-Aids for Scientific Research (B) (No. 22350015 to MS) from the Ministry of Education, Culture, Sports, Science, and Technology of Japan. MS acknowledges a research grant from Mitsubishi Foundation. TK acknowledges the Sasakawa Scientific Research Grant from the Japan Science Society

supplementary crystallographic information

Comment

The group 14 metalloles has received much attention as good precursors of their polymers that reveal interesting optical properties (Yamaguchi et al., 1998; Haga et al., 2008) as well as their anion species, which are heavier congeners of the cyclopentadienyl anion (Saito et al., 2005). After the synthesis of several oligo(1,1-silole)s and poly(1,1-silole)s (Yamaguchi et al., 1997, 1999); Kanno et al., 1998; Sohn et al., 1999), they have been used as building blocks of organic electroluminescent devices (Kim & Woo (2002)). Poly(1,1-germole)s have also been synthesized (Sohn et al., 2003). In contrast, as for tin analogues, only a few reports on the synthesis of oligo(1,1-stannole)s have appeared, so far (Haga et al., 2008). We report herein the molecular structure of the title compound, which is a novel bi(1,1-stannole) bearing ethyl groups on the carbon atoms of the five-membered rings.

The X-ray diffraction analysis reveals that the title compound, bis(1-tert-butyl-2,3,4,5-tetraethylstannacyclopentadienyl) (I), has two planar five-membered rings with C–C bond alternations. The molecule is centrosymmetric with an inversion center in the middle of Sn–Sn bond, and hence a half moiety of the molecule was refined. The two stannole rings are oriented in an anti fashion through the Sn–Sn bond to avoid steric repulsion. The Sn–Sn bond length of 2.7689 (2) Å is in a normal range of the corresponding single bond, as was observed in other bi(1,1-stannole)s (2.7844 (7) and 2.7822 (7) Å (Saito et al., 2002, 2005). The structural features of the title compound are therefore quite similar to those of other bi(1,1-stannole)s that have electronically neutral tin centers, and substituents on the ring carbon atoms little affect the structural feartures of bi(1,1-stannole)s.

Experimental

A diethyl ether solution (0.55 mL) of tert-butyl chloride (0.94 M, 0.52 mmol) was added to a diethyl ether solution (7 mL) of 2,2',3,3',4,4',5,5'-octaethyl-1,1'-dilithiobistannole (Saito et al., 2010) (118.8 mg, 0.203 mmol) at room temperature, and the mixture was stirred for 3 h. After removal of volatile substances, the residue was degassed by freeze-pump-thaw cycles and sealed. In a glovebox, materials insoluble in hexane were removed by filtration and the filtrate was concentrated to provide a crude product. Recrystallisation of the crude product from diethyl ether afforded colourless crystals of bis(1-tert-butyl-2,3,4,5-tetraethylstannacyclopentadienyl) (107.7 mg, 0.154 mmol, 76%). (1) 1H NMR (C6D6, 400 MHz) δ 1.02 (t, J = 7 Hz, 12H), 1.19 (t, J = 7 Hz, 12H), 1.40(s, JSn–H = 73 Hz, 18H), 2.33(q, J = 7 Hz, 8H), 2.41–2.60(m, 8H); 13C NMR (101 MHz, C6D6) δ 18.44 (q, JSn–C = 13 Hz), 22.61 (t, JSn–C = 48 Hz), 26.85 (t, JSn–C = 54 Hz), 30.71 (s, JSn–C = 22, 314, 328 Hz), 32.54 (t), 145.74 (s, JSn–C = 26, 287, 301 Hz), 152.92 (s, JSn–C = 21, 63 Hz); 119Sn NMR (186 MHz, C6D6)δ -68.8 (JSn–C = 301 Hz, JSn–Sn = 948 Hz).

Refinement

All H atoms were positionated geometrically, with C–H 0.96 and 0.97 A for methyl and methylene H atoms, and constrated to ride on their parent atoms, with Uiso(H) = 1.5Ueq(C) and 1.2Ueq(C) for methyl and methylene H atoms, respectively.

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) with atom labels and 50% probability displacement ellipsoids for non-H atoms. H atoms are omitted for clarity. The complete molecule is generated by the symmetry operation: -x, -y+2, -z+1.

Fig. 2.

Fig. 2.

The side view of (I), with atom labels and 50% probability displacement ellipsoids for non-H atoms. H atoms are omitted for clarity.

Crystal data

[Sn2(C4H9)2(C12H20)2] F(000) = 700
Mr = 680.20 Dx = 1.348 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 6469 reflections
a = 8.7161 (5) Å θ = 2.5–28.1°
b = 16.5999 (9) Å µ = 1.51 mm1
c = 11.7913 (6) Å T = 100 K
β = 100.827 (1)° Cube, colourless
V = 1675.67 (16) Å3 0.25 × 0.10 × 0.05 mm
Z = 2

Data collection

Bruker APEXII CCD area-detector diffractometer 3636 independent reflections
Radiation source: Bruker TXS fine-focus rotating anode 3387 reflections with I > 2σ(I)
Bruker Helios multilayer confocal mirror Rint = 0.017
Detector resolution: 8.333 pixels mm-1 θmax = 27.0°, θmin = 2.1°
φ and ω scans h = −11→9
Absorption correction: multi-scan (XPREP; Bruker, 2008) k = −21→21
Tmin = 0.835, Tmax = 0.927 l = −14→12
9015 measured reflections

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.017 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.043 H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.020P)2 + 0.7365P] where P = (Fo2 + 2Fc2)/3
3636 reflections (Δ/σ)max = 0.002
161 parameters Δρmax = 0.43 e Å3
0 restraints Δρmin = −0.42 e Å3

Special details

Experimental. (SADABS; Bruker, 2008)
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)

x y z Uiso*/Ueq
Sn1 0.025172 (11) 0.980800 (6) 0.390739 (8) 0.01472 (4)
C1 0.08418 (18) 1.07858 (9) 0.28847 (13) 0.0166 (3)
C2 −0.03317 (18) 1.08829 (9) 0.19728 (13) 0.0165 (3)
C3 −0.17491 (18) 1.03462 (9) 0.18331 (13) 0.0166 (3)
C4 −0.18366 (18) 0.97554 (9) 0.26111 (14) 0.0174 (3)
C5 0.20071 (18) 0.88519 (10) 0.40268 (14) 0.0207 (3)
C6 0.2344 (3) 0.86861 (15) 0.28284 (18) 0.0494 (6)
H6A 0.2631 0.9179 0.2498 0.074*
H6B 0.1428 0.8468 0.2347 0.074*
H6C 0.3187 0.8307 0.2884 0.074*
C7 0.3492 (2) 0.91665 (13) 0.47898 (19) 0.0412 (5)
H7A 0.4319 0.8783 0.4801 0.062*
H7B 0.3311 0.9245 0.5560 0.062*
H7C 0.3781 0.9670 0.4489 0.062*
C8 0.1474 (3) 0.80959 (13) 0.4556 (3) 0.0577 (7)
H8A 0.0592 0.7872 0.4042 0.087*
H8B 0.1182 0.8226 0.5280 0.087*
H8C 0.2310 0.7710 0.4681 0.087*
C9 0.23347 (19) 1.12690 (10) 0.31206 (14) 0.0207 (3)
H9A 0.2443 1.1562 0.2428 0.025*
H9B 0.3215 1.0904 0.3308 0.025*
C10 0.2376 (2) 1.18665 (11) 0.41124 (15) 0.0285 (4)
H10A 0.1539 1.2247 0.3915 0.043*
H10B 0.3356 1.2147 0.4246 0.043*
H10C 0.2260 1.1581 0.4799 0.043*
C11 −0.02473 (19) 1.15157 (10) 0.10545 (13) 0.0213 (3)
H11A 0.0349 1.1974 0.1409 0.026*
H11B −0.1294 1.1701 0.0735 0.026*
C12 0.0514 (2) 1.11894 (11) 0.00763 (14) 0.0276 (4)
H12A 0.1557 1.1013 0.0387 0.041*
H12B 0.0547 1.1607 −0.0482 0.041*
H12C −0.0086 1.0744 −0.0289 0.041*
C13 −0.30873 (19) 1.05102 (10) 0.08346 (14) 0.0229 (3)
H13A −0.3647 1.0012 0.0615 0.027*
H13B −0.2668 1.0698 0.0176 0.027*
C14 −0.4225 (2) 1.11386 (11) 0.11409 (18) 0.0348 (4)
H14A −0.4702 1.0938 0.1755 0.052*
H14B −0.5018 1.1246 0.0475 0.052*
H14C −0.3669 1.1627 0.1385 0.052*
C15 −0.32148 (19) 0.92105 (10) 0.26192 (15) 0.0230 (3)
H15A −0.4082 0.9395 0.2037 0.028*
H15B −0.3527 0.9253 0.3364 0.028*
C16 −0.2897 (2) 0.83329 (11) 0.23913 (18) 0.0337 (4)
H16A −0.2663 0.8279 0.1631 0.051*
H16B −0.3802 0.8017 0.2446 0.051*
H16C −0.2024 0.8147 0.2952 0.051*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Sn1 0.01341 (6) 0.01614 (6) 0.01448 (6) 0.00001 (4) 0.00225 (4) 0.00191 (4)
C1 0.0176 (7) 0.0170 (7) 0.0159 (7) −0.0015 (6) 0.0052 (6) −0.0001 (6)
C2 0.0193 (7) 0.0139 (7) 0.0172 (7) 0.0008 (6) 0.0058 (6) −0.0002 (6)
C3 0.0149 (7) 0.0168 (7) 0.0175 (7) 0.0016 (6) 0.0014 (6) −0.0027 (6)
C4 0.0141 (7) 0.0185 (7) 0.0194 (8) −0.0002 (6) 0.0028 (6) −0.0020 (6)
C5 0.0170 (8) 0.0210 (8) 0.0232 (8) 0.0027 (6) 0.0013 (6) 0.0000 (6)
C6 0.0559 (14) 0.0607 (15) 0.0314 (11) 0.0330 (12) 0.0074 (10) −0.0069 (10)
C7 0.0230 (10) 0.0449 (12) 0.0498 (12) 0.0099 (8) −0.0082 (8) −0.0115 (10)
C8 0.0319 (12) 0.0326 (11) 0.112 (2) 0.0118 (9) 0.0221 (13) 0.0330 (13)
C9 0.0193 (8) 0.0216 (8) 0.0210 (8) −0.0044 (6) 0.0036 (6) 0.0011 (6)
C10 0.0302 (10) 0.0268 (9) 0.0270 (9) −0.0092 (7) 0.0015 (7) −0.0042 (7)
C11 0.0240 (8) 0.0190 (8) 0.0203 (8) −0.0009 (6) 0.0027 (6) 0.0041 (6)
C12 0.0343 (10) 0.0299 (9) 0.0195 (8) −0.0047 (7) 0.0075 (7) 0.0035 (7)
C13 0.0210 (8) 0.0226 (8) 0.0222 (8) −0.0001 (7) −0.0030 (6) 0.0014 (7)
C14 0.0234 (9) 0.0293 (9) 0.0472 (12) 0.0069 (7) −0.0054 (8) −0.0003 (8)
C15 0.0178 (8) 0.0241 (8) 0.0268 (8) −0.0037 (6) 0.0033 (6) 0.0017 (7)
C16 0.0355 (10) 0.0252 (9) 0.0433 (11) −0.0132 (8) 0.0146 (9) −0.0065 (8)

Geometric parameters (Å, °)

Sn1—C1 2.1416 (15) C9—H9A 0.9700
Sn1—C4 2.1475 (16) C9—H9B 0.9700
Sn1—C5 2.1906 (16) C10—H10A 0.9600
Sn1—Sn1i 2.7682 (2) C10—H10B 0.9600
C1—C2 1.347 (2) C10—H10C 0.9600
C1—C9 1.509 (2) C11—C12 1.534 (2)
C2—C3 1.507 (2) C11—H11A 0.9700
C2—C11 1.520 (2) C11—H11B 0.9700
C3—C4 1.355 (2) C12—H12A 0.9600
C3—C13 1.518 (2) C12—H12B 0.9600
C4—C15 1.505 (2) C12—H12C 0.9600
C5—C8 1.513 (3) C13—C14 1.529 (2)
C5—C6 1.521 (3) C13—H13A 0.9700
C5—C7 1.523 (2) C13—H13B 0.9700
C6—H6A 0.9600 C14—H14A 0.9600
C6—H6B 0.9600 C14—H14B 0.9600
C6—H6C 0.9600 C14—H14C 0.9600
C7—H7A 0.9600 C15—C16 1.516 (2)
C7—H7B 0.9600 C15—H15A 0.9700
C7—H7C 0.9600 C15—H15B 0.9700
C8—H8A 0.9600 C16—H16A 0.9600
C8—H8B 0.9600 C16—H16B 0.9600
C8—H8C 0.9600 C16—H16C 0.9600
C9—C10 1.529 (2)
C1—Sn1—C4 83.75 (6) C1—C9—H9B 109.1
C1—Sn1—C5 110.28 (6) C10—C9—H9B 109.1
C4—Sn1—C5 120.31 (6) H9A—C9—H9B 107.9
C1—Sn1—Sn1i 116.51 (4) C9—C10—H10A 109.5
C4—Sn1—Sn1i 114.24 (4) C9—C10—H10B 109.5
C5—Sn1—Sn1i 109.75 (4) H10A—C10—H10B 109.5
C2—C1—C9 125.63 (14) C9—C10—H10C 109.5
C2—C1—Sn1 108.27 (11) H10A—C10—H10C 109.5
C9—C1—Sn1 126.08 (11) H10B—C10—H10C 109.5
C1—C2—C3 120.03 (13) C2—C11—C12 112.17 (14)
C1—C2—C11 121.33 (14) C2—C11—H11A 109.2
C3—C2—C11 118.62 (13) C12—C11—H11A 109.2
C4—C3—C2 120.22 (14) C2—C11—H11B 109.2
C4—C3—C13 121.47 (14) C12—C11—H11B 109.2
C2—C3—C13 118.26 (13) H11A—C11—H11B 107.9
C3—C4—C15 125.86 (15) C11—C12—H12A 109.5
C3—C4—Sn1 107.73 (11) C11—C12—H12B 109.5
C15—C4—Sn1 126.20 (11) H12A—C12—H12B 109.5
C8—C5—C6 111.14 (18) C11—C12—H12C 109.5
C8—C5—C7 109.49 (17) H12A—C12—H12C 109.5
C6—C5—C7 108.65 (17) H12B—C12—H12C 109.5
C8—C5—Sn1 111.26 (12) C3—C13—C14 112.16 (14)
C6—C5—Sn1 109.01 (12) C3—C13—H13A 109.2
C7—C5—Sn1 107.17 (11) C14—C13—H13A 109.2
C5—C6—H6A 109.5 C3—C13—H13B 109.2
C5—C6—H6B 109.5 C14—C13—H13B 109.2
H6A—C6—H6B 109.5 H13A—C13—H13B 107.9
C5—C6—H6C 109.5 C13—C14—H14A 109.5
H6A—C6—H6C 109.5 C13—C14—H14B 109.5
H6B—C6—H6C 109.5 H14A—C14—H14B 109.5
C5—C7—H7A 109.5 C13—C14—H14C 109.5
C5—C7—H7B 109.5 H14A—C14—H14C 109.5
H7A—C7—H7B 109.5 H14B—C14—H14C 109.5
C5—C7—H7C 109.5 C4—C15—C16 113.80 (14)
H7A—C7—H7C 109.5 C4—C15—H15A 108.8
H7B—C7—H7C 109.5 C16—C15—H15A 108.8
C5—C8—H8A 109.5 C4—C15—H15B 108.8
C5—C8—H8B 109.5 C16—C15—H15B 108.8
H8A—C8—H8B 109.5 H15A—C15—H15B 107.7
C5—C8—H8C 109.5 C15—C16—H16A 109.5
H8A—C8—H8C 109.5 C15—C16—H16B 109.5
H8B—C8—H8C 109.5 H16A—C16—H16B 109.5
C1—C9—C10 112.43 (13) C15—C16—H16C 109.5
C1—C9—H9A 109.1 H16A—C16—H16C 109.5
C10—C9—H9A 109.1 H16B—C16—H16C 109.5

Symmetry codes: (i) −x, −y+2, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: KP2332).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811022951/kp2332sup1.cif

e-67-0m949-sup1.cif (17.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811022951/kp2332Isup2.hkl

e-67-0m949-Isup2.hkl (177.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811022951/kp2332Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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