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In the title compound, C12H8Cl2N2OS, the dihedral angle between the two ring planes is 14.30 (3)°. The mol­ecules are linked via a weak inter­molecular N—H...O hydrogen bond, forming an extended supra­molecular structure.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807039694/at2371sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807039694/at2371Isup2.hkl
Contains datablock I

CCDC reference: 660294

Key indicators

  • Single-crystal X-ray study
  • T = 113 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.050
  • wR factor = 0.097
  • Data-to-parameter ratio = 17.4

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ?
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 1 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 0 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 structure of the title compound, (I).

In the structure of the title molecule, (I) (Fig. 1), the geometric parameters are normal. The thiophene ring system (C9—C12/S1) is planar, with an r.m.s. deviation for fitted atoms of 0.0032 (5) Å; the benzene group (C1—C6) is also planar, with an r.m.s. deviation of 0.0053 (2) Å. The dihedral angle between these planes is 14.30 (3)°.

The molecules are linked via weak intermolecular N—H···O hydrogen bond, forming an extended supramolecule (Table 1). The molecules associate to form a supramolecular structure, as illustrated 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-2-carbohydrazide (1.42 g, 10 mmol) was added to an anhydrous ethanol solution (50 ml) of 2,4-dichlorobenzaldehyde (1.75 g, 10 mmol), and the mixture was stirred at 350 K for 6 h under N2, whereupon a yellow precipitate appeared. The product was isolated, recrystallized from anhydrous ethanol and then dried in vacuo to give pure compound (I) in 85% yield. Yellow 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 freely. C-bound H atoms were included in calculated positions, with C—H = 0.95 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 structure of the title compound, (I).

In the structure of the title molecule, (I) (Fig. 1), the geometric parameters are normal. The thiophene ring system (C9—C12/S1) is planar, with an r.m.s. deviation for fitted atoms of 0.0032 (5) Å; the benzene group (C1—C6) is also planar, with an r.m.s. deviation of 0.0053 (2) Å. The dihedral angle between these planes is 14.30 (3)°.

The molecules are linked via weak intermolecular N—H···O hydrogen bond, forming an extended supramolecule (Table 1). The molecules associate to form a supramolecular structure, as illustrated 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: CrystalClear (Rigaku/MSC, 2005); cell refinement: CrystalClear (Rigaku/MSC, 2005); data reduction: CrystalClear (Rigaku/MSC, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: CrystalStructure (Rigaku/MSC, 2005); software used to prepare material for publication: CrystalStructure (Rigaku/MSC, 2005).

Figures top
[Figure 1] Fig. 1. The structure of the title molecule (I). Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2] Fig. 2. The crystal packing of (I), viewed down the c axis. Hydrogen bonds are indicated by dashed lines.
(E)-N'-(2,4-Dichlorobenzylidene)thiophene-2-carbohydrazide top
Crystal data top
C12H8Cl2N2OSF(000) = 608
Mr = 299.16Dx = 1.628 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 2966 reflections
a = 5.6320 (11) Åθ = 1.9–28.0°
b = 16.664 (3) ŵ = 0.69 mm1
c = 13.077 (3) ÅT = 113 K
β = 96.10 (3)°Block, yellow
V = 1220.3 (4) Å30.10 × 0.06 × 0.04 mm
Z = 4
Data collection top
Rigaku Saturn
diffractometer
2911 independent reflections
Radiation source: rotating anode2370 reflections with I > 2σ(I)
Confocal monochromatorRint = 0.064
Detector resolution: 7.31 pixels mm-1θmax = 27.9°, θmin = 2.0°
ω scansh = 76
Absorption correction: multi-scan
(CrystalClear, Rigaku/MSC, 2005)
k = 2121
Tmin = 0.934, Tmax = 0.973l = 1517
9849 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.050Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.097H atoms treated by a mixture of independent and constrained refinement
S = 1.10 w = 1/[σ2(Fo2) + (0.0332P)2 + 0.3458P]
where P = (Fo2 + 2Fc2)/3
2911 reflections(Δ/σ)max = 0.001
167 parametersΔρmax = 0.32 e Å3
0 restraintsΔρmin = 0.36 e Å3
Crystal data top
C12H8Cl2N2OSV = 1220.3 (4) Å3
Mr = 299.16Z = 4
Monoclinic, P21/nMo Kα radiation
a = 5.6320 (11) ŵ = 0.69 mm1
b = 16.664 (3) ÅT = 113 K
c = 13.077 (3) Å0.10 × 0.06 × 0.04 mm
β = 96.10 (3)°
Data collection top
Rigaku Saturn
diffractometer
2911 independent reflections
Absorption correction: multi-scan
(CrystalClear, Rigaku/MSC, 2005)
2370 reflections with I > 2σ(I)
Tmin = 0.934, Tmax = 0.973Rint = 0.064
9849 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0500 restraints
wR(F2) = 0.097H atoms treated by a mixture of independent and constrained refinement
S = 1.10Δρmax = 0.32 e Å3
2911 reflectionsΔρmin = 0.36 e Å3
167 parameters
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
Cl11.20133 (11)0.60285 (4)0.68221 (5)0.02104 (16)
Cl20.84737 (12)0.82985 (4)0.42176 (4)0.02250 (17)
S10.16921 (11)0.87926 (4)0.83555 (5)0.02168 (17)
O10.1664 (3)1.00868 (11)0.60854 (13)0.0212 (4)
N10.3309 (4)0.88243 (13)0.63613 (15)0.0168 (5)
N20.1711 (4)0.94002 (14)0.59904 (16)0.0187 (5)
H20.164 (5)0.956 (2)0.535 (2)0.042 (9)*
C10.6565 (4)0.75502 (16)0.69296 (18)0.0186 (5)
H10.54050.76710.73840.022*
C20.8196 (4)0.69461 (16)0.71835 (18)0.0189 (6)
H2A0.81390.66450.77970.023*
C30.9920 (4)0.67847 (16)0.65305 (18)0.0166 (5)
C41.0012 (4)0.72071 (16)0.56257 (18)0.0175 (5)
H41.12070.70940.51850.021*
C50.8331 (4)0.77977 (16)0.53762 (17)0.0164 (5)
C60.6578 (4)0.79905 (16)0.60175 (18)0.0167 (5)
C70.4807 (4)0.86188 (16)0.57394 (18)0.0173 (5)
H70.47710.88770.50900.021*
C80.0114 (4)0.96340 (16)0.65136 (18)0.0173 (5)
C90.0280 (4)0.93785 (15)0.75774 (18)0.0168 (5)
C100.2147 (4)0.96278 (17)0.80989 (18)0.0197 (6)
H100.34230.99530.78010.024*
C110.1964 (5)0.93495 (17)0.91240 (19)0.0227 (6)
H110.30990.94650.95910.027*
C120.0027 (5)0.88965 (17)0.9365 (2)0.0238 (6)
H120.04450.86641.00220.029*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0206 (3)0.0192 (4)0.0233 (3)0.0029 (3)0.0022 (2)0.0010 (3)
Cl20.0298 (4)0.0213 (4)0.0172 (3)0.0001 (3)0.0065 (3)0.0026 (3)
S10.0198 (3)0.0241 (4)0.0212 (3)0.0033 (3)0.0022 (3)0.0060 (3)
O10.0196 (9)0.0229 (11)0.0212 (9)0.0041 (8)0.0023 (7)0.0066 (8)
N10.0159 (11)0.0151 (12)0.0193 (10)0.0005 (9)0.0006 (8)0.0006 (9)
N20.0200 (11)0.0179 (12)0.0183 (11)0.0031 (9)0.0030 (9)0.0025 (9)
C10.0194 (13)0.0189 (14)0.0178 (12)0.0023 (11)0.0034 (10)0.0004 (10)
C20.0232 (14)0.0168 (14)0.0166 (12)0.0015 (11)0.0020 (10)0.0017 (10)
C30.0157 (12)0.0143 (14)0.0194 (12)0.0001 (10)0.0004 (10)0.0030 (10)
C40.0161 (12)0.0169 (14)0.0198 (12)0.0033 (11)0.0026 (10)0.0027 (10)
C50.0190 (13)0.0157 (14)0.0144 (11)0.0058 (11)0.0010 (10)0.0006 (10)
C60.0152 (12)0.0163 (14)0.0186 (12)0.0008 (10)0.0021 (10)0.0029 (10)
C70.0198 (13)0.0141 (13)0.0176 (12)0.0018 (11)0.0003 (10)0.0038 (10)
C80.0172 (12)0.0128 (13)0.0218 (12)0.0054 (10)0.0016 (10)0.0001 (10)
C90.0147 (12)0.0145 (14)0.0208 (12)0.0024 (10)0.0003 (10)0.0010 (10)
C100.0190 (13)0.0196 (15)0.0201 (12)0.0001 (11)0.0008 (10)0.0008 (11)
C110.0234 (14)0.0238 (16)0.0215 (13)0.0002 (12)0.0050 (11)0.0014 (11)
C120.0241 (14)0.0261 (16)0.0212 (13)0.0004 (12)0.0020 (11)0.0057 (11)
Geometric parameters (Å, º) top
Cl1—C31.740 (3)C3—C41.383 (3)
Cl2—C51.739 (2)C4—C51.381 (3)
S1—C121.707 (3)C4—H40.9500
S1—C91.727 (3)C5—C61.399 (3)
O1—C81.241 (3)C6—C71.465 (4)
N1—C71.279 (3)C7—H70.9500
N1—N21.369 (3)C8—C91.467 (3)
N2—C81.351 (3)C9—C101.377 (3)
N2—H20.88 (3)C10—C111.412 (3)
C1—C21.379 (4)C10—H100.9500
C1—C61.401 (3)C11—C121.361 (4)
C1—H10.9500C11—H110.9500
C2—C31.386 (3)C12—H120.9500
C2—H2A0.9500
C12—S1—C991.51 (13)C5—C6—C7121.4 (2)
C7—N1—N2114.6 (2)C1—C6—C7121.4 (2)
C8—N2—N1122.0 (2)N1—C7—C6120.7 (2)
C8—N2—H2116 (2)N1—C7—H7119.6
N1—N2—H2121 (2)C6—C7—H7119.6
C2—C1—C6121.6 (2)O1—C8—N2118.9 (2)
C2—C1—H1119.2O1—C8—C9119.4 (2)
C6—C1—H1119.2N2—C8—C9121.7 (2)
C1—C2—C3119.1 (2)C10—C9—C8120.7 (2)
C1—C2—H2A120.5C10—C9—S1110.85 (18)
C3—C2—H2A120.5C8—C9—S1128.38 (19)
C4—C3—C2121.4 (2)C9—C10—C11112.9 (2)
C4—C3—Cl1118.03 (19)C9—C10—H10123.6
C2—C3—Cl1120.56 (19)C11—C10—H10123.6
C5—C4—C3118.6 (2)C12—C11—C10112.1 (2)
C5—C4—H4120.7C12—C11—H11123.9
C3—C4—H4120.7C10—C11—H11123.9
C4—C5—C6122.1 (2)C11—C12—S1112.6 (2)
C4—C5—Cl2116.99 (19)C11—C12—H12123.7
C6—C5—Cl2120.9 (2)S1—C12—H12123.7
C5—C6—C1117.2 (2)
C7—N1—N2—C8174.2 (2)C5—C6—C7—N1175.6 (2)
C6—C1—C2—C31.5 (4)C1—C6—C7—N15.4 (4)
C1—C2—C3—C41.0 (4)N1—N2—C8—O1171.5 (2)
C1—C2—C3—Cl1179.94 (19)N1—N2—C8—C99.6 (4)
C2—C3—C4—C50.3 (4)O1—C8—C9—C100.8 (4)
Cl1—C3—C4—C5178.72 (18)N2—C8—C9—C10179.6 (2)
C3—C4—C5—C61.3 (4)O1—C8—C9—S1177.0 (2)
C3—C4—C5—Cl2178.62 (19)N2—C8—C9—S11.9 (4)
C4—C5—C6—C10.8 (4)C12—S1—C9—C100.6 (2)
Cl2—C5—C6—C1179.06 (19)C12—S1—C9—C8177.3 (2)
C4—C5—C6—C7180.0 (2)C8—C9—C10—C11177.7 (2)
Cl2—C5—C6—C70.1 (3)S1—C9—C10—C110.4 (3)
C2—C1—C6—C50.6 (4)C9—C10—C11—C120.1 (4)
C2—C1—C6—C7178.5 (2)C10—C11—C12—S10.5 (3)
N2—N1—C7—C6178.0 (2)C9—S1—C12—C110.7 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2···O1i0.88 (3)1.96 (3)2.843 (3)177 (3)
Symmetry code: (i) x, y+2, z+1.

Experimental details

Crystal data
Chemical formulaC12H8Cl2N2OS
Mr299.16
Crystal system, space groupMonoclinic, P21/n
Temperature (K)113
a, b, c (Å)5.6320 (11), 16.664 (3), 13.077 (3)
β (°) 96.10 (3)
V3)1220.3 (4)
Z4
Radiation typeMo Kα
µ (mm1)0.69
Crystal size (mm)0.10 × 0.06 × 0.04
Data collection
DiffractometerRigaku Saturn
Absorption correctionMulti-scan
(CrystalClear, Rigaku/MSC, 2005)
Tmin, Tmax0.934, 0.973
No. of measured, independent and
observed [I > 2σ(I)] reflections
9849, 2911, 2370
Rint0.064
(sin θ/λ)max1)0.659
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.050, 0.097, 1.10
No. of reflections2911
No. of parameters167
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.32, 0.36

Computer programs: CrystalClear (Rigaku/MSC, 2005), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), CrystalStructure (Rigaku/MSC, 2005).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2···O1i0.88 (3)1.96 (3)2.843 (3)177 (3)
Symmetry code: (i) x, y+2, z+1.
 

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