supplementary materials


Acta Cryst. (2007). E63, m2068    [ doi:10.1107/S1600536807032023 ]

Bis(2-amino-2-thiazolinium) dichromate(VI)

L. Sieron

Abstract top

The crystal structure of the title compound, (C3H7N2S)2-[Cr2O7], consists of 2-amino-2-thiazolinium cations and discrete dichromate anions linked together by N-H...O hydrogen bonds to form a one-dimensional ribbon structure lying parallel to the (102) plane and running along the b axis. The dichromate anion is located on a twofold axis that passes through its central O atom.

Comment top

The title compound, (I), was investigated as part of a structural study on hydrogen-bonding patterns in 2-amino-2-thiazolinium salts (Sieroń, 2007).

In (I), the asymmetric unit is composed of one 2-amino-2-thiazolinium cation and half dichromate anion (Fig. 1). The cation occupies a general position whereas the anion is located on a twofold axis. The bond lengths and angles are within normal ranges (Allen et al., 1987).

The dichromate anion links the cation via intermolecular N—H···O hydrogen bonds forming eight-membered ring with graph-set descriptor R22(8) (Etter et al., 1990). The other N—H···O hydrogen bond associates adjacent cations via O1 atom into C22(6) chains. The combination of these motifs results in the formation of a one-dimensional ribbon structure lying parallel to the (102) plane and running along the b axis, as shown in Fig. 2. The same motifs are found in bis(2-amino-2-thiazolinium) tetra-µ-formato-κ8O:O'-bis[(formato-κO)copper(II)] structure (Sieroń, 2007).

Related literature top

For related structure, see: Sieroń (2007). For related literature, see: Allen et al. (1987); Etter et al. (1990).

Experimental top

The title compound was prepared by dissolving 2-amino-2-thiazoline (1 mmol) and chromic anhydride (1 mmol) in hot water (25 ml). After a few days, prism-shaped orange crystals were obtained at room temperature.

Refinement top

All H atoms were initially located in a difference Fourier map. C-bonded H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms, with C–H distances of 0.97 Å and Uiso(H) = 1.2Ueq(C). Amine H atoms were refined freely.

Computing details top

Data collection: CrysAlis CCD (Oxford Diffraction, 2007); cell refinement: CrysAlis RED (Oxford Diffraction, 2007); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXTL (Sheldrick, 2001); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL and Mercury (Macrae et al., 2006); software used to prepare material for publication: PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing the atom-numbering scheme. Displacement ellipsoids for non-H atoms are drawn at the 50% probability level. Unlabelled atoms are related to labelled atoms by symmetry code (−x + 3/2, y, −z + 3/2). Dotted lines indicate hydrogen bonds.
[Figure 2] Fig. 2. A packing view of (I), showing a ribbon of hydrogen-bonded (dashed lines) cations and anions running along the b axis.
Bis(2-amino-2-thiazolinium) dichromate(VI) top
Crystal data top
(C3H7N2S)2[Cr2O7]F(000) = 428
Mr = 422.35Dx = 1.903 Mg m3
Monoclinic, P2/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yacCell parameters from 8378 reflections
a = 8.0304 (1) Åθ = 2.5–30.0°
b = 6.5332 (1) ŵ = 1.79 mm1
c = 14.1019 (2) ÅT = 298 K
β = 95.065 (2)°Prism, orange
V = 736.96 (2) Å30.60 × 0.40 × 0.25 mm
Z = 2
Data collection top
Kuma KM-4 CCD
diffractometer
1708 independent reflections
Radiation source: CX-Mo12x0.4-S Seifert Mo tube1604 reflections with I > 2σ(I)
graphiteRint = 0.022
Detector resolution: 8.2356 pixels mm-1θmax = 27.5°, θmin = 2.8°
ω scansh = 1010
Absorption correction: multi-scan
(Oxford Diffraction, 2007)
k = 88
Tmin = 0.410, Tmax = 0.636l = 1818
9894 measured reflections
Refinement top
Refinement on F2Hydrogen site location: difference Fourier map
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.023 w = 1/[σ2(Fo2) + (0.0408P)2 + 0.3039P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.071(Δ/σ)max = 0.001
S = 1.12Δρmax = 0.39 e Å3
1708 reflectionsΔρmin = 0.31 e Å3
109 parametersExtinction correction: SHELXTL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0186 (18)
Primary atom site location: structure-invariant direct methods
Crystal data top
(C3H7N2S)2[Cr2O7]V = 736.96 (2) Å3
Mr = 422.35Z = 2
Monoclinic, P2/nMo Kα radiation
a = 8.0304 (1) ŵ = 1.79 mm1
b = 6.5332 (1) ÅT = 298 K
c = 14.1019 (2) Å0.60 × 0.40 × 0.25 mm
β = 95.065 (2)°
Data collection top
Kuma KM-4 CCD
diffractometer
1708 independent reflections
Absorption correction: multi-scan
(Oxford Diffraction, 2007)
1604 reflections with I > 2σ(I)
Tmin = 0.410, Tmax = 0.636Rint = 0.022
9894 measured reflectionsθmax = 27.5°
Refinement top
R[F2 > 2σ(F2)] = 0.023H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.071Δρmax = 0.39 e Å3
S = 1.12Δρmin = 0.31 e Å3
1708 reflectionsAbsolute structure: ?
109 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
Special details top

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles

Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating -R-factor-obs 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
S10.21595 (6)0.12790 (7)1.02709 (4)0.0414 (2)
N10.31040 (19)0.2021 (2)0.95161 (10)0.0331 (4)
N20.3482 (3)0.0856 (3)0.86045 (13)0.0426 (5)
C10.30017 (19)0.0056 (3)0.93613 (11)0.0294 (4)
C20.2114 (3)0.1018 (3)1.09950 (13)0.0393 (5)
C30.2295 (2)0.2811 (3)1.03239 (13)0.0366 (5)
Cr10.53421 (3)0.42057 (4)0.74127 (2)0.0263 (1)
O10.45721 (16)0.4958 (2)0.83802 (9)0.0373 (4)
O20.4996 (2)0.1793 (2)0.72715 (11)0.0523 (5)
O30.750000.4772 (4)0.750000.0558 (7)
O40.4462 (2)0.5453 (3)0.65261 (11)0.0542 (5)
H10.351 (3)0.280 (4)0.9131 (18)0.052 (7)*
H2A0.106700.111001.128600.0470*
H2B0.302600.100601.149400.0470*
H3A0.120600.337201.011400.0440*
H3B0.296900.388201.064200.0440*
H210.386 (3)0.014 (4)0.8192 (17)0.043 (6)*
H220.352 (3)0.205 (5)0.8556 (19)0.053 (7)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0513 (3)0.0294 (2)0.0450 (3)0.0049 (2)0.0127 (2)0.0094 (2)
N10.0397 (7)0.0273 (7)0.0336 (7)0.0038 (6)0.0102 (6)0.0044 (6)
N20.0566 (10)0.0313 (9)0.0418 (9)0.0075 (7)0.0150 (8)0.0013 (7)
C10.0263 (7)0.0287 (8)0.0330 (7)0.0022 (6)0.0019 (6)0.0053 (6)
C20.0429 (10)0.0434 (10)0.0322 (8)0.0022 (7)0.0065 (7)0.0038 (7)
C30.0441 (9)0.0314 (9)0.0350 (8)0.0036 (7)0.0072 (7)0.0029 (7)
Cr10.0251 (2)0.0267 (2)0.0280 (2)0.0017 (1)0.0076 (1)0.0007 (1)
O10.0405 (6)0.0331 (6)0.0409 (7)0.0021 (5)0.0190 (5)0.0040 (5)
O20.0727 (10)0.0310 (7)0.0556 (8)0.0064 (7)0.0197 (7)0.0111 (6)
O30.0263 (9)0.0703 (14)0.0725 (14)0.00000.0148 (9)0.0000
O40.0521 (9)0.0639 (10)0.0454 (8)0.0076 (7)0.0029 (6)0.0207 (7)
Geometric parameters (Å, °) top
Cr1—O11.6231 (13)N1—H10.83 (3)
Cr1—O21.6099 (13)N2—H210.83 (2)
Cr1—O31.7656 (6)N2—H220.78 (3)
Cr1—O41.6033 (17)C2—C31.521 (3)
S1—C11.7369 (17)C2—H2B0.97
S1—C21.817 (2)C2—H2A0.97
N1—C11.304 (2)C3—H3A0.97
N1—C31.455 (2)C3—H3B0.97
N2—C11.310 (3)
O1—Cr1—O2109.03 (7)S1—C1—N2122.36 (16)
O1—Cr1—O3108.80 (6)N1—C1—N2124.45 (17)
O1—Cr1—O4109.10 (8)S1—C2—C3106.18 (13)
O2—Cr1—O3111.81 (10)N1—C3—C2106.73 (15)
O2—Cr1—O4109.99 (9)C3—C2—H2A110
O3—Cr1—O4108.07 (8)S1—C2—H2A111
C1—S1—C291.65 (9)S1—C2—H2B110
Cr1—O3—Cr1i155.81 (17)C3—C2—H2B110
C1—N1—C3117.04 (14)H2A—C2—H2B109
C3—N1—H1121.5 (18)N1—C3—H3A110
C1—N1—H1121.1 (18)N1—C3—H3B110
C1—N2—H21118.0 (18)C2—C3—H3A110
C1—N2—H22122.7 (19)C2—C3—H3B110
H21—N2—H22119 (3)H3A—C3—H3B109
S1—C1—N1113.19 (12)
Symmetry codes: (i) −x+3/2, y, −z+3/2.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O10.83 (3)2.00 (3)2.8233 (19)171 (2)
N2—H21···O20.83 (2)2.08 (2)2.900 (3)174 (2)
N2—H22···O1ii0.78 (3)2.15 (3)2.897 (2)159 (2)
Symmetry codes: (ii) x, y−1, z.
Table 1
Selected geometric parameters (Å, °)
top
Cr1—O11.6231 (13)S1—C21.817 (2)
Cr1—O21.6099 (13)N1—C11.304 (2)
Cr1—O31.7656 (6)N1—C31.455 (2)
Cr1—O41.6033 (17)N2—C11.310 (3)
S1—C11.7369 (17)C2—C31.521 (3)
O1—Cr1—O2109.03 (7)Cr1—O3—Cr1i155.81 (17)
O1—Cr1—O3108.80 (6)C1—N1—C3117.04 (14)
O1—Cr1—O4109.10 (8)S1—C1—N1113.19 (12)
O2—Cr1—O3111.81 (10)S1—C1—N2122.36 (16)
O2—Cr1—O4109.99 (9)N1—C1—N2124.45 (17)
O3—Cr1—O4108.07 (8)S1—C2—C3106.18 (13)
C1—S1—C291.65 (9)N1—C3—C2106.73 (15)
Symmetry codes: (i) −x+3/2, y, −z+3/2.
Table 2
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N1—H1···O10.83 (3)2.00 (3)2.8233 (19)171 (2)
N2—H21···O20.83 (2)2.08 (2)2.900 (3)174 (2)
N2—H22···O1ii0.78 (3)2.15 (3)2.897 (2)159 (2)
Symmetry codes: (ii) x, y−1, z.
Acknowledgements top

(No acknowledgements)

references
References top

Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.

Etter, M. C., MacDonald, J. C. & Bernstein, J. (1990). Acta Cryst. B46, 256–262.

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Oxford Diffraction (2007). CrysAlis CCD and CrysAlis RED. Versions 1.171. Oxford Diffraction Ltd, Abingdon, Oxfordshire, England.

Sheldrick, G. M. (2001). SHELXTL. Version 6.12. Bruker AXS Inc., Madison, Wisconsin, USA.

Sieroń, L. (2007). Acta Cryst. C63, m199–m200.

Spek, A. L. (2003). J. Appl. Cryst. 36, 7–13.