organic compounds
5,6-Di-2-thienyl-2,3-dihydropyrazine
aX-ray Crystallography Unit, School of Physics, Universiti Sains Malaysia, 11800 USM, Penang, Malaysia
*Correspondence e-mail: hkfun@usm.my
In the title compound, C12H10N2S2, which was synthesized by the reaction of 2,2′-thenil and ethylenediamine, the dihedral angle between the two thiophene rings is 66.33 (9)°. In the intermolecular C—H⋯N hydrogen bonds link the molecules into infinite chains along the b axis and weak C—H⋯π interactions may further stabilize the structure.
Related literature
For backgroud to thenils, see: Shimon et al. (1993). For related structures, see: Crundwell et al. (2002a,b, 2003); Linehan et al. (2003); Stacy et al. (2003). For bond-length data, see: Allen et al. (1987). For the stability of the temperature controller used in the data collection, see: Cosier & Glazer (1986).
Experimental
Crystal data
|
Data collection: APEX2 (Bruker, 2009); cell SAINT (Bruker, 2009); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009).
Supporting information
https://doi.org/10.1107/S1600536810012705/hb5396sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536810012705/hb5396Isup2.hkl
2,2'-thenil (55 mg) and ethylenediamine (15 mg) in ethanol/water (40 ml) were heated under reflux for 2 h with stirring. The resulting solution was then cooled to room temperature. After a few days of slow evaporation of the solvent, brown plates of (I) were obtained.
All H atoms were positioned geometrically (C—H = 0.93 or 0.97 Å) and were refined using a riding model, with Uiso(H) = 1.2 or 1.5Ueq(C). In the absence of significant
effects, 1899 Friedel pairs were merged.Thienyl-based guests have shown preferential inclusion into the host by keeping thienyl ring S atoms pointed away from the face of growing crystals, possibly to avoid unfavorable electrostatic interactions between sulfur lone pairs coplanar with the thiophene ring and molecules already incorporated into the growing crystal face (Shimon et al., 1993). The structural studies on thenoins (Crundwell et al., 2002a,b) and thenils (Crundwell et al., 2003), and other thiophene-containing molecules such as 2,5-diphenyl-3,4-dithien-3-ylcyclopentadien-1-one (Linehan et al., 2003) and 4-bromo-2-thiophenecarboxaldehyde (Stacy et al., 2003) have been reported in the literature. In continuation of this area of study, the
of the title compound, (I), is reported here.In the molecule of the title compound (Fig. 1), the bond lengths (Allen et al., 1987) and angles are within normal ranges. The dihedral angle between the two thiophene rings S1/C1–C4 and S2/C9–C12 is 66.33 (9)°. In the π interactions (Table 1), involving the S2/C9–C12 (centroid Cg2) ring.
intermolecular C—H···N hydrogen bonds (Table 1) link the molecules (Fig. 2) into infinite chains along the b axis, in which they may be effective in the stabilization of the structure. The is further stabilized by C—H···For backgroud to thenils, see: Shimon et al. (1993). For related structures, see: Crundwell et al. (2002a,b, 2003); Linehan et al. (2003); Stacy et al. (2003). For bond-length data, see: Allen et al. (1987). For the stability of the temperature controller used in the data collection, see: Cosier & Glazer (1986).
Data collection: APEX2 (Bruker, 2009); cell
SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).C12H10N2S2 | F(000) = 256 |
Mr = 246.34 | Dx = 1.414 Mg m−3 |
Monoclinic, P21 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2yb | Cell parameters from 5014 reflections |
a = 5.5006 (9) Å | θ = 2.9–34.8° |
b = 7.5246 (12) Å | µ = 0.43 mm−1 |
c = 14.116 (2) Å | T = 100 K |
β = 97.902 (5)° | Plate, brown |
V = 578.73 (16) Å3 | 0.32 × 0.26 × 0.08 mm |
Z = 2 |
Bruker APEX DUO CCD area-detector diffractometer | 4603 independent reflections |
Radiation source: fine-focus sealed tube | 4295 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.022 |
φ and ω scans | θmax = 35.1°, θmin = 1.5° |
Absorption correction: multi-scan (SADABS; Bruker, 2009) | h = −8→8 |
Tmin = 0.875, Tmax = 0.965 | k = −12→12 |
9583 measured reflections | l = −22→22 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.032 | All H-atom parameters refined |
wR(F2) = 0.115 | w = 1/[σ2(Fo2) + (0.0632P)2 + 0.0559P] where P = (Fo2 + 2Fc2)/3 |
S = 1.20 | (Δ/σ)max < 0.001 |
4603 reflections | Δρmax = 0.62 e Å−3 |
145 parameters | Δρmin = −0.47 e Å−3 |
1 restraint | Absolute structure: Flack (1983), with 1899 Friedel pairs |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.07 (6) |
C12H10N2S2 | V = 578.73 (16) Å3 |
Mr = 246.34 | Z = 2 |
Monoclinic, P21 | Mo Kα radiation |
a = 5.5006 (9) Å | µ = 0.43 mm−1 |
b = 7.5246 (12) Å | T = 100 K |
c = 14.116 (2) Å | 0.32 × 0.26 × 0.08 mm |
β = 97.902 (5)° |
Bruker APEX DUO CCD area-detector diffractometer | 4603 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2009) | 4295 reflections with I > 2σ(I) |
Tmin = 0.875, Tmax = 0.965 | Rint = 0.022 |
9583 measured reflections |
R[F2 > 2σ(F2)] = 0.032 | All H-atom parameters refined |
wR(F2) = 0.115 | Δρmax = 0.62 e Å−3 |
S = 1.20 | Δρmin = −0.47 e Å−3 |
4603 reflections | Absolute structure: Flack (1983), with 1899 Friedel pairs |
145 parameters | Absolute structure parameter: 0.07 (6) |
1 restraint |
Experimental. The crystal was placed in the cold stream of an Oxford Cryosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K. |
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 | ||
S1 | 0.53730 (6) | 0.88379 (6) | 0.15567 (3) | 0.02249 (9) | |
S2 | −0.08370 (7) | 0.37500 (7) | 0.39261 (3) | 0.02435 (10) | |
N1 | −0.1511 (2) | 0.42753 (19) | 0.18646 (9) | 0.0176 (2) | |
N2 | 0.2016 (2) | 0.58341 (19) | 0.08083 (8) | 0.0167 (2) | |
C1 | 0.5372 (3) | 1.0745 (3) | 0.22117 (12) | 0.0256 (3) | |
H1A | 0.6518 | 1.1651 | 0.2206 | 0.031* | |
C2 | 0.3468 (3) | 1.0777 (2) | 0.27490 (12) | 0.0225 (3) | |
H2A | 0.3166 | 1.1719 | 0.3143 | 0.027* | |
C3 | 0.2025 (3) | 0.9222 (2) | 0.26367 (10) | 0.0176 (2) | |
H3A | 0.0665 | 0.9026 | 0.2948 | 0.021* | |
C4 | 0.2854 (2) | 0.8021 (2) | 0.20133 (9) | 0.0141 (2) | |
C5 | 0.1765 (2) | 0.6334 (2) | 0.16622 (10) | 0.0141 (2) | |
C6 | 0.0602 (3) | 0.4259 (2) | 0.04601 (10) | 0.0199 (3) | |
H6A | 0.1494 | 0.3194 | 0.0686 | 0.024* | |
H6B | 0.0373 | 0.4245 | −0.0234 | 0.024* | |
C7 | −0.1875 (3) | 0.4280 (2) | 0.08163 (10) | 0.0192 (3) | |
H7A | −0.2783 | 0.5333 | 0.0582 | 0.023* | |
H7B | −0.2817 | 0.3244 | 0.0579 | 0.023* | |
C8 | 0.0286 (2) | 0.5231 (2) | 0.22635 (9) | 0.0136 (2) | |
C9 | 0.0980 (3) | 0.5061 (2) | 0.32993 (9) | 0.0148 (2) | |
C10 | 0.3080 (3) | 0.5582 (2) | 0.38767 (10) | 0.0199 (3) | |
H10A | 0.4286 | 0.6292 | 0.3670 | 0.024* | |
C11 | 0.3203 (4) | 0.4914 (3) | 0.48252 (11) | 0.0272 (3) | |
H11A | 0.4496 | 0.5144 | 0.5307 | 0.033* | |
C12 | 0.1220 (4) | 0.3904 (3) | 0.49497 (11) | 0.0296 (4) | |
H12A | 0.1007 | 0.3360 | 0.5524 | 0.036* |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.02124 (15) | 0.02353 (19) | 0.02375 (16) | −0.01080 (15) | 0.00690 (12) | −0.00227 (15) |
S2 | 0.02570 (17) | 0.0293 (2) | 0.01976 (15) | −0.00416 (17) | 0.00917 (12) | 0.00490 (16) |
N1 | 0.0195 (5) | 0.0164 (5) | 0.0168 (4) | −0.0061 (4) | 0.0022 (4) | −0.0014 (4) |
N2 | 0.0188 (5) | 0.0166 (5) | 0.0151 (5) | −0.0038 (4) | 0.0037 (4) | −0.0023 (4) |
C1 | 0.0311 (8) | 0.0176 (7) | 0.0264 (7) | −0.0130 (6) | −0.0022 (6) | 0.0022 (6) |
C2 | 0.0283 (7) | 0.0127 (6) | 0.0246 (6) | −0.0012 (6) | −0.0030 (5) | −0.0006 (5) |
C3 | 0.0178 (5) | 0.0161 (6) | 0.0186 (5) | −0.0030 (5) | 0.0010 (4) | −0.0018 (5) |
C4 | 0.0142 (5) | 0.0126 (6) | 0.0151 (5) | −0.0027 (4) | 0.0007 (4) | 0.0008 (4) |
C5 | 0.0138 (5) | 0.0131 (6) | 0.0154 (5) | −0.0023 (4) | 0.0019 (4) | 0.0006 (4) |
C6 | 0.0256 (6) | 0.0162 (6) | 0.0181 (5) | −0.0039 (5) | 0.0042 (5) | −0.0054 (5) |
C7 | 0.0203 (6) | 0.0200 (7) | 0.0164 (5) | −0.0066 (5) | 0.0001 (4) | −0.0024 (5) |
C8 | 0.0154 (5) | 0.0113 (5) | 0.0141 (5) | −0.0022 (4) | 0.0027 (4) | 0.0000 (4) |
C9 | 0.0180 (5) | 0.0129 (6) | 0.0140 (5) | −0.0001 (5) | 0.0036 (4) | 0.0004 (4) |
C10 | 0.0205 (6) | 0.0206 (7) | 0.0173 (5) | −0.0006 (5) | −0.0017 (5) | 0.0012 (5) |
C11 | 0.0331 (8) | 0.0304 (9) | 0.0163 (6) | 0.0034 (7) | −0.0030 (5) | 0.0006 (6) |
C12 | 0.0399 (8) | 0.0353 (10) | 0.0151 (5) | 0.0070 (9) | 0.0087 (5) | 0.0054 (7) |
S1—C1 | 1.707 (2) | C4—C5 | 1.461 (2) |
S1—C4 | 1.7201 (14) | C5—C8 | 1.5040 (19) |
S2—C12 | 1.7124 (19) | C6—C7 | 1.516 (2) |
S2—C9 | 1.7317 (14) | C6—H6A | 0.9700 |
N1—C8 | 1.2874 (18) | C6—H6B | 0.9700 |
N1—C7 | 1.4658 (19) | C7—H7A | 0.9700 |
N2—C5 | 1.2880 (18) | C7—H7B | 0.9700 |
N2—C6 | 1.465 (2) | C8—C9 | 1.4652 (19) |
C1—C2 | 1.375 (3) | C9—C10 | 1.376 (2) |
C1—H1A | 0.9300 | C10—C11 | 1.423 (2) |
C2—C3 | 1.411 (2) | C10—H10A | 0.9300 |
C2—H2A | 0.9300 | C11—C12 | 1.361 (3) |
C3—C4 | 1.382 (2) | C11—H11A | 0.9300 |
C3—H3A | 0.9300 | C12—H12A | 0.9300 |
C1—S1—C4 | 92.13 (8) | C7—C6—H6B | 109.7 |
C12—S2—C9 | 91.82 (8) | H6A—C6—H6B | 108.2 |
C8—N1—C7 | 115.50 (12) | N1—C7—C6 | 109.29 (12) |
C5—N2—C6 | 115.48 (12) | N1—C7—H7A | 109.8 |
C2—C1—S1 | 111.76 (12) | C6—C7—H7A | 109.8 |
C2—C1—H1A | 124.1 | N1—C7—H7B | 109.8 |
S1—C1—H1A | 124.1 | C6—C7—H7B | 109.8 |
C1—C2—C3 | 112.51 (15) | H7A—C7—H7B | 108.3 |
C1—C2—H2A | 123.7 | N1—C8—C9 | 117.84 (12) |
C3—C2—H2A | 123.7 | N1—C8—C5 | 120.25 (12) |
C4—C3—C2 | 112.59 (13) | C9—C8—C5 | 121.61 (12) |
C4—C3—H3A | 123.7 | C10—C9—C8 | 130.47 (13) |
C2—C3—H3A | 123.7 | C10—C9—S2 | 110.85 (10) |
C3—C4—C5 | 128.94 (12) | C8—C9—S2 | 118.02 (10) |
C3—C4—S1 | 110.99 (11) | C9—C10—C11 | 112.61 (15) |
C5—C4—S1 | 119.83 (10) | C9—C10—H10A | 123.7 |
N2—C5—C4 | 118.67 (13) | C11—C10—H10A | 123.7 |
N2—C5—C8 | 120.18 (13) | C12—C11—C10 | 112.55 (15) |
C4—C5—C8 | 121.10 (11) | C12—C11—H11A | 123.7 |
N2—C6—C7 | 109.89 (12) | C10—C11—H11A | 123.7 |
N2—C6—H6A | 109.7 | C11—C12—S2 | 112.16 (12) |
C7—C6—H6A | 109.7 | C11—C12—H12A | 123.9 |
N2—C6—H6B | 109.7 | S2—C12—H12A | 123.9 |
C4—S1—C1—C2 | −1.31 (14) | C7—N1—C8—C5 | 3.3 (2) |
S1—C1—C2—C3 | 0.95 (19) | N2—C5—C8—N1 | −29.3 (2) |
C1—C2—C3—C4 | 0.1 (2) | C4—C5—C8—N1 | 148.07 (15) |
C2—C3—C4—C5 | −175.19 (14) | N2—C5—C8—C9 | 144.36 (15) |
C2—C3—C4—S1 | −1.03 (16) | C4—C5—C8—C9 | −38.3 (2) |
C1—S1—C4—C3 | 1.33 (12) | N1—C8—C9—C10 | 163.90 (16) |
C1—S1—C4—C5 | 176.10 (12) | C5—C8—C9—C10 | −9.9 (2) |
C6—N2—C5—C4 | −172.06 (13) | N1—C8—C9—S2 | −5.87 (19) |
C6—N2—C5—C8 | 5.4 (2) | C5—C8—C9—S2 | −179.66 (11) |
C3—C4—C5—N2 | 147.03 (16) | C12—S2—C9—C10 | −0.12 (14) |
S1—C4—C5—N2 | −26.69 (19) | C12—S2—C9—C8 | 171.56 (13) |
C3—C4—C5—C8 | −30.4 (2) | C8—C9—C10—C11 | −170.37 (16) |
S1—C4—C5—C8 | 155.92 (11) | S2—C9—C10—C11 | −0.03 (18) |
C5—N2—C6—C7 | 37.17 (19) | C9—C10—C11—C12 | 0.2 (2) |
C8—N1—C7—C6 | 38.97 (19) | C10—C11—C12—S2 | −0.3 (2) |
N2—C6—C7—N1 | −60.13 (17) | C9—S2—C12—C11 | 0.26 (17) |
C7—N1—C8—C9 | −170.61 (13) |
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1A···N1i | 0.93 | 2.33 | 3.235 (3) | 163 |
C2—H2A···Cg2ii | 0.93 | 2.85 | 3.7737 (18) | 171 |
Symmetry codes: (i) x+1, y+1, z; (ii) x, y+1, z. |
Experimental details
Crystal data | |
Chemical formula | C12H10N2S2 |
Mr | 246.34 |
Crystal system, space group | Monoclinic, P21 |
Temperature (K) | 100 |
a, b, c (Å) | 5.5006 (9), 7.5246 (12), 14.116 (2) |
β (°) | 97.902 (5) |
V (Å3) | 578.73 (16) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.43 |
Crystal size (mm) | 0.32 × 0.26 × 0.08 |
Data collection | |
Diffractometer | Bruker APEX DUO CCD area-detector |
Absorption correction | Multi-scan (SADABS; Bruker, 2009) |
Tmin, Tmax | 0.875, 0.965 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 9583, 4603, 4295 |
Rint | 0.022 |
(sin θ/λ)max (Å−1) | 0.810 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.032, 0.115, 1.20 |
No. of reflections | 4603 |
No. of parameters | 145 |
No. of restraints | 1 |
H-atom treatment | All H-atom parameters refined |
Δρmax, Δρmin (e Å−3) | 0.62, −0.47 |
Absolute structure | Flack (1983), with 1899 Friedel pairs |
Absolute structure parameter | 0.07 (6) |
Computer programs: APEX2 (Bruker, 2009), SAINT (Bruker, 2009), SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1A···N1i | 0.93 | 2.33 | 3.235 (3) | 163 |
C2—H2A···Cg2ii | 0.93 | 2.85 | 3.7737 (18) | 171 |
Symmetry codes: (i) x+1, y+1, z; (ii) x, y+1, z. |
Acknowledgements
The authors thank the Malaysian Government and Universiti Sains Malaysia for Research University Golden Goose grant No. 1001/PFIZIK/811012. MH thanks Universiti Sains Malaysia for a postdoctoral research fellowship.
References
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Thienyl-based guests have shown preferential inclusion into the host by keeping thienyl ring S atoms pointed away from the face of growing crystals, possibly to avoid unfavorable electrostatic interactions between sulfur lone pairs coplanar with the thiophene ring and molecules already incorporated into the growing crystal face (Shimon et al., 1993). The structural studies on thenoins (Crundwell et al., 2002a,b) and thenils (Crundwell et al., 2003), and other thiophene-containing molecules such as 2,5-diphenyl-3,4-dithien-3-ylcyclopentadien-1-one (Linehan et al., 2003) and 4-bromo-2-thiophenecarboxaldehyde (Stacy et al., 2003) have been reported in the literature. In continuation of this area of study, the crystal structure of the title compound, (I), is reported here.
In the molecule of the title compound (Fig. 1), the bond lengths (Allen et al., 1987) and angles are within normal ranges. The dihedral angle between the two thiophene rings S1/C1–C4 and S2/C9–C12 is 66.33 (9)°. In the crystal structure, intermolecular C—H···N hydrogen bonds (Table 1) link the molecules (Fig. 2) into infinite chains along the b axis, in which they may be effective in the stabilization of the structure. The crystal structure is further stabilized by C—H···π interactions (Table 1), involving the S2/C9–C12 (centroid Cg2) ring.