metal-organic compounds
Bis[2-(ethoxycarbonylamino)ethanaminium] hexabromidostannate
aDepartment of Chemistry, University of Aberdeen, Old Aberdeen AB15 5NY, Scotland, bDepartamento de Quimica, ICEx, Universidade Federal de Minas Gerais, 31270-901 Belo Horizonte, MG, Brazil, cDepartment of Chemistry, University of Malaya, 50603 Kuala Lumpur, Malaysia, and dCHEMSOL, 1 Harcourt Road, Aberdeen AB15 5NY, Scotland
*Correspondence e-mail: edward.tiekink@gmail.com
In the title salt, (C5H13N2O2)2[SnBr6], the Sn atom (site symmetry ) exists in a slightly distorted octahedral geometry. The cation is non-planar as the terminal CH2NH3+ residue lies below the plane defined by the remaining non-H atoms. In the crystal, cations associate via N—H⋯O hydrogen bonds involving the ammonium and carbonyl residues, forming a 14-membered {⋯HNC2NCO}2 synthon. The cations and anions are arranged in alternating layers arranged along the a-axis direction, the major association between them being N—H⋯Br contacts.
Related literature
For background to the synthesis of the title salt, see: Duschinsky (1950); Kita et al. (1980); Smith et al. (1998); Tavridou et al. (1995); Wilson & Nowick (1998).
Experimental
Crystal data
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Refinement
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Data collection: COLLECT (Hooft, 1998); cell DENZO (Otwinowski & Minor, 1997) and COLLECT; data reduction: DENZO and COLLECT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: SHELXL97.
Supporting information
10.1107/S160053680904687X/hb5214sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S160053680904687X/hb5214Isup2.hkl
A solution of 2-imidazolidone (0.86 g) and SnBr4 (2.20 g) in EtOH (10 ml) was heated to 323 K for 15 minutes, cooled and maintained at room temperature to slowly form crystals of (I); m. pt. 459–463 K. IR(KBr) = 1692 cm-1.
All H atoms were located from a difference map but, were geometrically placed (C–H = 0.98–0.99 Å, and N–H = 0.88–0.91 Å) and refined as riding with Uiso(H) = 1.2–1.5Ueq(C, N). The maximum and minimum residual electron density peaks of 0.85 and 1.26 e Å-3, respectively, were located 1.81 Å and 0.82 Å from the S1 and Sn atoms, respectively.
Data collection: COLLECT (Hooft, 1998); cell
DENZO (Otwinowski & Minor, 1997) and COLLECT (Hooft, 1998); data reduction: DENZO (Otwinowski & Minor, 1997) and COLLECT (Hooft, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006; software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).(C5H13N2O2)2[SnBr6] | F(000) = 1624 |
Mr = 864.48 | Dx = 2.360 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71069 Å |
Hall symbol: -C 2yc | Cell parameters from 11507 reflections |
a = 21.8907 (5) Å | θ = 2.9–27.5° |
b = 7.4428 (2) Å | µ = 10.92 mm−1 |
c = 15.5318 (4) Å | T = 120 K |
β = 105.934 (2)° | Block, light-yellow |
V = 2433.34 (11) Å3 | 0.38 × 0.32 × 0.22 mm |
Z = 4 |
Bruker–Nonius 95mm CCD camera on κ-goniostat diffractometer | 2777 independent reflections |
Radiation source: Bruker-Nonius FR591 rotating anode | 2450 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.051 |
Detector resolution: 9.091 pixels mm-1 | θmax = 27.5°, θmin = 3.1° |
ϕ and ω scans | h = −28→28 |
Absorption correction: multi-scan (SADABS; Sheldrick, 2003) | k = −9→9 |
Tmin = 0.355, Tmax = 0.746 | l = −20→20 |
15137 measured reflections |
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)] = 0.034 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.070 | H-atom parameters constrained |
S = 1.12 | w = 1/[σ2(Fo2) + (0.0263P)2 + 9.0406P] where P = (Fo2 + 2Fc2)/3 |
2777 reflections | (Δ/σ)max = 0.001 |
120 parameters | Δρmax = 0.87 e Å−3 |
1 restraint | Δρmin = −1.35 e Å−3 |
(C5H13N2O2)2[SnBr6] | V = 2433.34 (11) Å3 |
Mr = 864.48 | Z = 4 |
Monoclinic, C2/c | Mo Kα radiation |
a = 21.8907 (5) Å | µ = 10.92 mm−1 |
b = 7.4428 (2) Å | T = 120 K |
c = 15.5318 (4) Å | 0.38 × 0.32 × 0.22 mm |
β = 105.934 (2)° |
Bruker–Nonius 95mm CCD camera on κ-goniostat diffractometer | 2777 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 2003) | 2450 reflections with I > 2σ(I) |
Tmin = 0.355, Tmax = 0.746 | Rint = 0.051 |
15137 measured reflections |
R[F2 > 2σ(F2)] = 0.034 | 1 restraint |
wR(F2) = 0.070 | H-atom parameters constrained |
S = 1.12 | Δρmax = 0.87 e Å−3 |
2777 reflections | Δρmin = −1.35 e Å−3 |
120 parameters |
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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. |
x | y | z | Uiso*/Ueq | ||
Sn | 0.2500 | 0.2500 | 0.5000 | 0.01268 (10) | |
Br1 | 0.220893 (18) | 0.02595 (5) | 0.61162 (3) | 0.02190 (11) | |
Br2 | 0.135158 (17) | 0.22636 (5) | 0.39826 (3) | 0.02122 (11) | |
Br3 | 0.284421 (16) | −0.01941 (5) | 0.41692 (3) | 0.01712 (11) | |
O1 | −0.02161 (12) | 0.3062 (4) | 0.6285 (2) | 0.0235 (6) | |
O2 | 0.01221 (13) | 0.2554 (4) | 0.5051 (2) | 0.0224 (6) | |
N1 | 0.08208 (14) | 0.3322 (5) | 0.6316 (2) | 0.0200 (7) | |
H1N | 0.1073 | 0.3259 | 0.5963 | 0.024* | |
N2 | 0.14598 (16) | 0.2592 (4) | 0.8785 (2) | 0.0183 (7) | |
H2N | 0.1749 | 0.3501 | 0.8905 | 0.027* | |
H3N | 0.1627 | 0.1606 | 0.9111 | 0.027* | |
H4N | 0.1103 | 0.2942 | 0.8931 | 0.027* | |
C1 | −0.0502 (2) | 0.1802 (6) | 0.3600 (3) | 0.0277 (10) | |
H1A | −0.0323 | 0.2857 | 0.3379 | 0.042* | |
H1B | −0.0933 | 0.1584 | 0.3219 | 0.042* | |
H1C | −0.0235 | 0.0751 | 0.3584 | 0.042* | |
C2 | −0.05232 (18) | 0.2130 (6) | 0.4539 (3) | 0.0212 (9) | |
H2A | −0.0812 | 0.3143 | 0.4561 | 0.025* | |
H2B | −0.0677 | 0.1047 | 0.4785 | 0.025* | |
C3 | 0.02071 (18) | 0.2985 (5) | 0.5912 (3) | 0.0163 (8) | |
C4 | 0.10453 (17) | 0.3786 (5) | 0.7254 (3) | 0.0187 (8) | |
H4A | 0.0693 | 0.4315 | 0.7455 | 0.022* | |
H4B | 0.1387 | 0.4695 | 0.7339 | 0.022* | |
C5 | 0.1296 (2) | 0.2146 (6) | 0.7810 (3) | 0.0227 (9) | |
H5A | 0.0971 | 0.1185 | 0.7674 | 0.027* | |
H5B | 0.1679 | 0.1695 | 0.7657 | 0.027* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Sn | 0.01042 (17) | 0.01213 (17) | 0.0158 (2) | 0.00012 (12) | 0.00415 (14) | −0.00043 (13) |
Br1 | 0.0233 (2) | 0.01857 (19) | 0.0286 (2) | 0.00387 (15) | 0.01518 (17) | 0.00774 (16) |
Br2 | 0.01230 (18) | 0.0248 (2) | 0.0236 (2) | 0.00109 (15) | −0.00008 (16) | −0.00413 (16) |
Br3 | 0.01406 (18) | 0.01542 (18) | 0.0230 (2) | −0.00038 (14) | 0.00701 (15) | −0.00511 (15) |
O1 | 0.0150 (13) | 0.0372 (16) | 0.0200 (16) | −0.0028 (12) | 0.0075 (11) | −0.0051 (13) |
O2 | 0.0141 (13) | 0.0355 (17) | 0.0170 (15) | 0.0003 (11) | 0.0034 (12) | −0.0037 (12) |
N1 | 0.0116 (14) | 0.0328 (19) | 0.0161 (18) | −0.0009 (14) | 0.0046 (13) | 0.0002 (15) |
N2 | 0.0125 (14) | 0.0211 (16) | 0.0195 (18) | 0.0017 (12) | 0.0016 (13) | −0.0030 (13) |
C1 | 0.031 (2) | 0.026 (2) | 0.023 (2) | 0.0041 (19) | 0.0008 (18) | −0.0024 (18) |
C2 | 0.0159 (18) | 0.026 (2) | 0.017 (2) | 0.0009 (16) | −0.0038 (16) | −0.0016 (17) |
C3 | 0.0164 (18) | 0.0160 (17) | 0.016 (2) | 0.0001 (15) | 0.0044 (15) | −0.0005 (15) |
C4 | 0.0158 (17) | 0.0199 (18) | 0.019 (2) | −0.0042 (15) | 0.0034 (15) | −0.0015 (16) |
C5 | 0.0205 (19) | 0.028 (2) | 0.017 (2) | 0.0045 (17) | −0.0002 (16) | −0.0079 (17) |
Sn—Br2i | 2.5820 (4) | N2—H3N | 0.9100 |
Sn—Br2 | 2.5820 (4) | N2—H4N | 0.9100 |
Sn—Br3 | 2.6053 (4) | C1—C2 | 1.493 (6) |
Sn—Br3i | 2.6053 (4) | C1—H1A | 0.9800 |
Sn—Br1i | 2.6075 (4) | C1—H1B | 0.9800 |
Sn—Br1 | 2.6075 (4) | C1—H1C | 0.9800 |
O1—C3 | 1.222 (5) | C2—H2A | 0.9900 |
O2—C3 | 1.339 (5) | C2—H2B | 0.9900 |
O2—C2 | 1.453 (5) | C4—C5 | 1.509 (6) |
N1—C3 | 1.341 (5) | C4—H4A | 0.9900 |
N1—C4 | 1.445 (5) | C4—H4B | 0.9900 |
N1—H1N | 0.8800 | C5—H5A | 0.9900 |
N2—C5 | 1.494 (5) | C5—H5B | 0.9900 |
N2—H2N | 0.9100 | ||
Br2i—Sn—Br2 | 180.000 (10) | C2—C1—H1B | 109.5 |
Br2i—Sn—Br3 | 89.437 (12) | H1A—C1—H1B | 109.5 |
Br2—Sn—Br3 | 90.563 (12) | C2—C1—H1C | 109.5 |
Br2i—Sn—Br3i | 90.563 (12) | H1A—C1—H1C | 109.5 |
Br2—Sn—Br3i | 89.437 (12) | H1B—C1—H1C | 109.5 |
Br3—Sn—Br3i | 180.0 | O2—C2—C1 | 106.4 (3) |
Br2i—Sn—Br1i | 89.357 (13) | O2—C2—H2A | 110.4 |
Br2—Sn—Br1i | 90.643 (13) | C1—C2—H2A | 110.4 |
Br3—Sn—Br1i | 90.355 (12) | O2—C2—H2B | 110.4 |
Br3i—Sn—Br1i | 89.645 (12) | C1—C2—H2B | 110.4 |
Br2i—Sn—Br1 | 90.643 (13) | H2A—C2—H2B | 108.6 |
Br2—Sn—Br1 | 89.357 (13) | O1—C3—O2 | 124.8 (3) |
Br3—Sn—Br1 | 89.646 (12) | O1—C3—N1 | 124.2 (4) |
Br3i—Sn—Br1 | 90.354 (12) | O2—C3—N1 | 111.0 (3) |
Br1i—Sn—Br1 | 180.000 (16) | N1—C4—C5 | 110.7 (3) |
C3—O2—C2 | 116.5 (3) | N1—C4—H4A | 109.5 |
C3—N1—C4 | 122.4 (3) | C5—C4—H4A | 109.5 |
C3—N1—H1N | 114.7 | N1—C4—H4B | 109.5 |
C4—N1—H1N | 122.9 | C5—C4—H4B | 109.5 |
C5—N2—H2N | 109.5 | H4A—C4—H4B | 108.1 |
C5—N2—H3N | 109.5 | N2—C5—C4 | 110.4 (3) |
H2N—N2—H3N | 109.5 | N2—C5—H5A | 109.6 |
C5—N2—H4N | 109.5 | C4—C5—H5A | 109.6 |
H2N—N2—H4N | 109.5 | N2—C5—H5B | 109.6 |
H3N—N2—H4N | 109.5 | C4—C5—H5B | 109.6 |
C2—C1—H1A | 109.5 | H5A—C5—H5B | 108.1 |
C3—O2—C2—C1 | 176.8 (3) | C4—N1—C3—O2 | −178.8 (3) |
C2—O2—C3—O1 | −0.8 (6) | C3—N1—C4—C5 | 96.4 (4) |
C2—O2—C3—N1 | 179.1 (3) | N1—C4—C5—N2 | −173.7 (3) |
C4—N1—C3—O1 | 1.1 (6) |
Symmetry code: (i) −x+1/2, −y+1/2, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1n···Br3i | 0.88 | 2.83 | 3.501 (3) | 134 |
N2—H2n···Br1ii | 0.91 | 2.64 | 3.495 (3) | 157 |
N2—H3n···Br3iii | 0.91 | 2.84 | 3.425 (3) | 123 |
N2—H4n···O1iv | 0.91 | 1.88 | 2.717 (5) | 152 |
Symmetry codes: (i) −x+1/2, −y+1/2, −z+1; (ii) −x+1/2, y+1/2, −z+3/2; (iii) x, −y, z+1/2; (iv) −x, y, −z+3/2. |
Experimental details
Crystal data | |
Chemical formula | (C5H13N2O2)2[SnBr6] |
Mr | 864.48 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 120 |
a, b, c (Å) | 21.8907 (5), 7.4428 (2), 15.5318 (4) |
β (°) | 105.934 (2) |
V (Å3) | 2433.34 (11) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 10.92 |
Crystal size (mm) | 0.38 × 0.32 × 0.22 |
Data collection | |
Diffractometer | Bruker–Nonius 95mm CCD camera on κ-goniostat diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 2003) |
Tmin, Tmax | 0.355, 0.746 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 15137, 2777, 2450 |
Rint | 0.051 |
(sin θ/λ)max (Å−1) | 0.650 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.034, 0.070, 1.12 |
No. of reflections | 2777 |
No. of parameters | 120 |
No. of restraints | 1 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.87, −1.35 |
Computer programs: , DENZO (Otwinowski & Minor, 1997) and COLLECT (Hooft, 1998), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), DIAMOND (Brandenburg, 2006.
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1n···Br3i | 0.88 | 2.83 | 3.501 (3) | 134 |
N2—H2n···Br1ii | 0.91 | 2.64 | 3.495 (3) | 157 |
N2—H3n···Br3iii | 0.91 | 2.84 | 3.425 (3) | 123 |
N2—H4n···O1iv | 0.91 | 1.88 | 2.717 (5) | 152 |
Symmetry codes: (i) −x+1/2, −y+1/2, −z+1; (ii) −x+1/2, y+1/2, −z+3/2; (iii) x, −y, z+1/2; (iv) −x, y, −z+3/2. |
Footnotes
‡Additional correspondence author, e-mail: j.wardell@abdn.ac.uk.
Acknowledgements
The use of the EPSRC X-ray crystallographic service at the University of Southampton, England and the valuable assistance of the staff there is gratefully acknowledged. JLW acknowledges support from FAPEMIG (Brazil).
References
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Tin halides react with 2-imidazolidone, 1 (Scheme 2), in non-protic solvents such as dichloromethane, to form solid complexes [R2SnCl2(1-O)2] (R = Me, Bu or Ph), [MeSnCl3(1-O)2] and [SnX4(1-O)2] (X = Cl, Br or I) (Tavridou et al., 1995); 1-O is the O-bound form of 1. As reported herein, 2-imidazolidone reacts with SnBr4 in EtOH to form ethyl (2-ammonioethyl)carbamate hexabromostannate, (I), Fig. 4. The combination of SnBr4 and EtOH proved to have sufficient Brønsted acidity to open the 2-imidazidone ring. Ring opening reactions of 2-imidazolidone derivatives have been variously reported using bases, e.g. N-(2-nitrobenzenesulfonyl)-2-imidazolidon by a secondary amine, R R'NH (Wilson & Nowick, 1998) and acids, e.g., ring opening of 1-methyl-3–3-hydroxyphenyl-2-imidaxolidone by concentrated HCl to give MeNHCH2CH2NHC6H4OH-m (Duschinsky, 1950). With reduced acidity, co-crystallization can occur instead as shown by the isolation of a 1:1 adduct of 2-imidazolidone and 5-nitrosalicylic acid (Smith et al., 1998). The free base of 2 has been reported from the reaction of H2NCH2CH2NH2 with EtO2CO(MeO)CCH2 (Kita et al., 1980).
The structure of (I) comprises ethyl (2-ammonioethyl)carbamate cations and SnBr6 dianions in the ratio 2:1; the Sn atom is located on a crystallographic centre of inversion so that the asymmetric unit is defined by one cation and half an anion, Fig. 1. The cation is not planar. While the RMS deviation of the O1, O2, N1 and C1—C4 atoms is 0.019 Å, the C5 atom lies 1.410 (5) Å out of this plane; the C3/N1/C4/C5 torsion angle of 96.4 (4)°. In the anion, the Sn—Br2 bond distance of 2.5820 (4) Å is significantly shorter than the Sn–Br1 and Sn–Br3 bond distances of 2.6075 (4) and 2.6053 (4) Å, respectively, an observation rationalized in terms of the pattern of intermolecular interactions,see below. The carbonyl-O1 atom forms a hydrogen bond with an ammonium-H atom to form a dimeric aggregate, Table 1 and Fig. 2. The resulting 14-membered {···HNC2NCO}2 synthon has twofold symmetry. The remaining acidic H atoms form contacts to the Br1 and Br3 atoms, Table 1, explaining the variation of the Sn–Br bond distances, whereby the Br2 atom not engaged in a significant intermolecular contact forms the shorter of the Sn–Br bonds. Globally, the crystal packing comprises alternating layers of cations and anions stacking along the a direction.