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In the title compound, C10H8N2O2S, the dihedral angle between the thio­phene and furan planes is 12.3 (1)°. The mol­ecules are linked via weak inter­molecular N—H...O, C—H...S and C—H...O hydrogen bonds, forming a two-dimensional network parallel to the ab plane.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807041293/ci2444sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807041293/ci2444Isup2.hkl
Contains datablock I

CCDC reference: 660358

Key indicators

  • Single-crystal X-ray study
  • T = 294 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.023
  • wR factor = 0.065
  • Data-to-parameter ratio = 12.1

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ? PLAT230_ALERT_2_C Hirshfeld Test Diff for C9 - C10 .. 5.36 su
Alert level G REFLT03_ALERT_4_G 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. From the CIF: _diffrn_reflns_theta_max 25.01 From the CIF: _reflns_number_total 1694 Count of symmetry unique reflns 883 Completeness (_total/calc) 191.85% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 811 Fraction of Friedel pairs measured 0.918 Are heavy atom types Z>Si present yes PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 2
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

In order to establish control over the preparation of crystalline solid materials so that their architecture and properties are predictable (Belloni et al., 2005; Tynan et al., 2005; Parashar et al., 1988), the synthesis of new and designed crystal structures has become a major strand of modern chemistry. Metal complexes based on Schiff bases have attracted much attention because they can be utilized as model compounds of the active centres in various proteins and enzymes (Kahwa et al., 1986; Santos et al., 2001). As part of an investigation of the coordination properties of Schiff bases functioning as ligands, we report the synthesis and crystal structure of the title compound, (I).

In the molecular structure of the compound (I) (Fig. 1), the geometric parameters are normal. The thiophene ring (C1–C4/S1) is planar within ±0.002 (1) Å. The furan ring (C7–C10/O2) is essentially planar, with a maximum deviation from the mean plane of 0.004 (1) Å for atom C10. The dihedral angle between these planes is 12.3 (1)°.

The molecules are linked via weak intermolecular N—H···O, C—H···S and C—H···O type hydrogen bonds (Table 1), to form a two-dimensional network parallel to the ab plane, as illustraed in Fig.2.

Related literature top

For general background, see: Belloni et al. (2005); Kahwa et al. (1986); Parashar et al. (1988); Santos et al. (2001); Tynan et al. (2005).

Experimental top

An anhydrous ethanol solution (50 ml) of thiophene-3-carbaldehyde (1.12 g, 10 mmol) was added to an anhydrous ethanol solution (50 ml) of furan-2-carbohydrazide (1.26 g, 10 mmol), and the mixture was stirred at 350 K for 6 h under N2, whereupon a colourless precipitate appeared. The product was isolated, recrystallized from anhydrous ethanol and then dried in vacuo to give pure compound (I) in 79% yield. Colourless single crystals of (I) suitable for X-ray analysis were obtained by slow evaporation of an anhydrous ethanol solution.

Refinement top

The N-bound H atom was located in a difference Fourier map and refined with a N—H distance restraint of 0.90 (1) Å. C-bound H atoms were included in calculated positions [C—H = 0.93 Å] and refined using a riding model, with Uiso(H) = 1.2Ueq(C).

Structure description top

In order to establish control over the preparation of crystalline solid materials so that their architecture and properties are predictable (Belloni et al., 2005; Tynan et al., 2005; Parashar et al., 1988), the synthesis of new and designed crystal structures has become a major strand of modern chemistry. Metal complexes based on Schiff bases have attracted much attention because they can be utilized as model compounds of the active centres in various proteins and enzymes (Kahwa et al., 1986; Santos et al., 2001). As part of an investigation of the coordination properties of Schiff bases functioning as ligands, we report the synthesis and crystal structure of the title compound, (I).

In the molecular structure of the compound (I) (Fig. 1), the geometric parameters are normal. The thiophene ring (C1–C4/S1) is planar within ±0.002 (1) Å. The furan ring (C7–C10/O2) is essentially planar, with a maximum deviation from the mean plane of 0.004 (1) Å for atom C10. The dihedral angle between these planes is 12.3 (1)°.

The molecules are linked via weak intermolecular N—H···O, C—H···S and C—H···O type hydrogen bonds (Table 1), to form a two-dimensional network parallel to the ab plane, as illustraed in Fig.2.

For general background, see: Belloni et al. (2005); Kahwa et al. (1986); Parashar et al. (1988); Santos et al. (2001); Tynan et al. (2005).

Computing details top

Data collection: SMART (Bruker, 1999); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. The molecular structure of (I). Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2] Fig. 2. The crystal packing of (I), viwed down the a axis. Hydrogen bonds are indicated by dashed lines.
(E)-N'-(3-Thienylmethylene)furan-2-carbohydrazide top
Crystal data top
C10H8N2O2SF(000) = 456
Mr = 220.24Dx = 1.505 Mg m3
Orthorhombic, Pca21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2c -2acCell parameters from 3232 reflections
a = 10.1150 (15) Åθ = 4.0–26.2°
b = 4.7969 (7) ŵ = 0.31 mm1
c = 20.033 (3) ÅT = 294 K
V = 972.0 (2) Å3Block, colourless
Z = 40.24 × 0.20 × 0.18 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1694 independent reflections
Radiation source: fine-focus sealed tube1616 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.018
φ and ω scansθmax = 25.0°, θmin = 2.0°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1012
Tmin = 0.929, Tmax = 0.946k = 54
4486 measured reflectionsl = 2323
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)] = 0.023H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.065 w = 1/[σ2(Fo2) + (0.0391P)2 + 0.0578P]
where P = (Fo2 + 2Fc2)/3
S = 1.11(Δ/σ)max = 0.001
1694 reflectionsΔρmax = 0.14 e Å3
140 parametersΔρmin = 0.14 e Å3
2 restraintsAbsolute structure: Flack (1983), with 811 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.04 (7)
Crystal data top
C10H8N2O2SV = 972.0 (2) Å3
Mr = 220.24Z = 4
Orthorhombic, Pca21Mo Kα radiation
a = 10.1150 (15) ŵ = 0.31 mm1
b = 4.7969 (7) ÅT = 294 K
c = 20.033 (3) Å0.24 × 0.20 × 0.18 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1694 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1616 reflections with I > 2σ(I)
Tmin = 0.929, Tmax = 0.946Rint = 0.018
4486 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.023H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.065Δρmax = 0.14 e Å3
S = 1.11Δρmin = 0.14 e Å3
1694 reflectionsAbsolute structure: Flack (1983), with 811 Friedel pairs
140 parametersAbsolute structure parameter: 0.04 (7)
2 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
S10.22029 (5)1.02129 (9)0.32352 (3)0.04200 (14)
O10.15782 (12)0.0679 (3)0.10495 (7)0.0473 (4)
O20.11967 (13)0.2927 (3)0.00357 (7)0.0547 (4)
N10.04650 (14)0.3353 (3)0.16534 (7)0.0352 (3)
N20.06307 (14)0.1461 (3)0.11429 (8)0.0352 (3)
C10.05895 (18)0.9185 (4)0.32440 (11)0.0412 (4)
H10.00380.98540.35430.049*
C20.03343 (17)0.7284 (4)0.27648 (10)0.0398 (4)
H20.04930.64880.26960.048*
C30.14683 (17)0.6629 (4)0.23753 (9)0.0324 (4)
C40.2551 (2)0.8089 (4)0.25789 (10)0.0383 (4)
H40.33820.79400.23830.046*
C50.1512 (2)0.4638 (4)0.18335 (9)0.0360 (4)
H50.23070.42910.16150.043*
C60.04417 (19)0.0210 (4)0.08752 (9)0.0341 (4)
C70.01324 (16)0.1763 (4)0.03386 (9)0.0348 (4)
C80.0966 (2)0.2736 (5)0.00599 (11)0.0535 (6)
H80.18270.22670.01770.064*
C90.0584 (2)0.4613 (5)0.04464 (12)0.0536 (6)
H90.11390.56100.07290.064*
C100.0714 (3)0.4667 (5)0.04373 (12)0.0538 (5)
H100.12320.57560.07180.065*
H2A0.1439 (12)0.100 (5)0.1005 (10)0.043 (6)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0360 (2)0.0452 (3)0.0448 (2)0.00471 (19)0.0011 (2)0.0056 (2)
O10.0262 (7)0.0623 (9)0.0533 (8)0.0012 (6)0.0024 (6)0.0137 (7)
O20.0331 (7)0.0682 (10)0.0629 (9)0.0067 (6)0.0010 (7)0.0236 (8)
N10.0298 (7)0.0381 (9)0.0378 (8)0.0020 (6)0.0006 (6)0.0029 (7)
N20.0256 (7)0.0403 (9)0.0397 (8)0.0018 (7)0.0017 (6)0.0063 (7)
C10.0333 (10)0.0482 (10)0.0422 (9)0.0001 (7)0.0064 (10)0.0007 (11)
C20.0291 (9)0.0429 (10)0.0475 (11)0.0016 (8)0.0014 (8)0.0022 (9)
C30.0268 (9)0.0334 (9)0.0372 (10)0.0013 (7)0.0002 (7)0.0042 (8)
C40.0299 (9)0.0403 (10)0.0445 (10)0.0010 (8)0.0047 (7)0.0001 (8)
C50.0293 (9)0.0382 (10)0.0407 (10)0.0023 (7)0.0016 (8)0.0021 (8)
C60.0294 (12)0.0367 (10)0.0362 (10)0.0005 (7)0.0005 (7)0.0035 (7)
C70.0309 (9)0.0367 (9)0.0367 (9)0.0035 (7)0.0036 (7)0.0029 (8)
C80.0283 (10)0.0697 (15)0.0624 (13)0.0015 (9)0.0026 (9)0.0237 (11)
C90.0418 (13)0.0604 (13)0.0585 (13)0.0018 (9)0.0065 (10)0.0197 (12)
C100.0513 (13)0.0544 (12)0.0558 (13)0.0036 (10)0.0070 (11)0.0190 (11)
Geometric parameters (Å, º) top
S1—C41.7003 (19)C2—H20.93
S1—C11.7050 (19)C3—C41.363 (3)
O1—C61.222 (2)C3—C51.446 (3)
O2—C101.354 (3)C4—H40.93
O2—C71.356 (2)C5—H50.93
N1—C51.277 (2)C6—C71.466 (3)
N1—N21.378 (2)C7—C81.328 (3)
N2—C61.351 (2)C8—C91.410 (3)
N2—H2A0.891 (9)C8—H80.93
C1—C21.349 (3)C9—C101.313 (3)
C1—H10.93C9—H90.93
C2—C31.423 (2)C10—H100.93
C4—S1—C191.90 (10)N1—C5—C3120.34 (18)
C10—O2—C7106.30 (16)N1—C5—H5119.8
C5—N1—N2115.26 (15)C3—C5—H5119.8
C6—N2—N1119.32 (15)O1—C6—N2124.07 (17)
C6—N2—H2A120.3 (15)O1—C6—C7121.93 (17)
N1—N2—H2A120.3 (15)N2—C6—C7113.98 (16)
C2—C1—S1111.79 (15)C8—C7—O2109.34 (17)
C2—C1—H1124.1C8—C7—C6135.53 (17)
S1—C1—H1124.1O2—C7—C6115.13 (15)
C1—C2—C3112.67 (17)C7—C8—C9107.30 (18)
C1—C2—H2123.7C7—C8—H8126.3
C3—C2—H2123.7C9—C8—H8126.3
C4—C3—C2111.75 (16)C10—C9—C8106.1 (2)
C4—C3—C5122.64 (18)C10—C9—H9127.0
C2—C3—C5125.60 (17)C8—C9—H9127.0
C3—C4—S1111.89 (15)C9—C10—O2111.0 (2)
C3—C4—H4124.1C9—C10—H10124.5
S1—C4—H4124.1O2—C10—H10124.5
C5—N1—N2—C6173.46 (17)N1—N2—C6—C7179.80 (14)
C4—S1—C1—C20.24 (17)C10—O2—C7—C80.4 (2)
S1—C1—C2—C30.1 (2)C10—O2—C7—C6179.86 (17)
C1—C2—C3—C40.1 (2)O1—C6—C7—C8177.7 (2)
C1—C2—C3—C5178.91 (18)N2—C6—C7—C83.3 (3)
C2—C3—C4—S10.3 (2)O1—C6—C7—O22.6 (3)
C5—C3—C4—S1178.77 (15)N2—C6—C7—O2176.41 (15)
C1—S1—C4—C30.29 (15)O2—C7—C8—C90.1 (3)
N2—N1—C5—C3178.56 (15)C6—C7—C8—C9179.7 (2)
C4—C3—C5—N1178.84 (17)C7—C8—C9—C100.5 (3)
C2—C3—C5—N12.3 (3)C8—C9—C10—O20.7 (3)
N1—N2—C6—O11.2 (3)C7—O2—C10—C90.7 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···O1i0.89 (1)2.16 (1)3.010 (2)158 (2)
C1—H1···S1ii0.932.863.438 (2)122
C8—H8···O1i0.932.503.328 (3)149
Symmetry codes: (i) x+1/2, y, z; (ii) x1/2, y+2, z.

Experimental details

Crystal data
Chemical formulaC10H8N2O2S
Mr220.24
Crystal system, space groupOrthorhombic, Pca21
Temperature (K)294
a, b, c (Å)10.1150 (15), 4.7969 (7), 20.033 (3)
V3)972.0 (2)
Z4
Radiation typeMo Kα
µ (mm1)0.31
Crystal size (mm)0.24 × 0.20 × 0.18
Data collection
DiffractometerBruker SMART CCD area-detector
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.929, 0.946
No. of measured, independent and
observed [I > 2σ(I)] reflections
4486, 1694, 1616
Rint0.018
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.023, 0.065, 1.11
No. of reflections1694
No. of parameters140
No. of restraints2
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.14, 0.14
Absolute structureFlack (1983), with 811 Friedel pairs
Absolute structure parameter0.04 (7)

Computer programs: SMART (Bruker, 1999), SAINT (Bruker, 1999), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1997), SHELXTL.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···O1i0.891 (9)2.163 (12)3.010 (2)158 (2)
C1—H1···S1ii0.932.863.438 (2)122
C8—H8···O1i0.932.503.328 (3)149
Symmetry codes: (i) x+1/2, y, z; (ii) x1/2, y+2, z.
 

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