organic compounds
(E)-2-[(E)-3-(Hydroxyimino)butan-2-ylidene]-N-methylhydrazinecarbothioamide
aSchool of Chemical Sciences, Universiti Sains Malaysia, Minden, Penang, Malaysia, bFaculty of Science, Sabha University, Libya, cDepartment of Chemistry, International University of Africa, Khartoum, Sudan, and dX-ray Crystallography Unit, School of Physics,Universiti Sains Malaysia, 11800 USM, Penang, Malaysia
*Correspondence e-mail: sgteoh@usm.my
In the title compound, C6H12N4OS, an intramolecular N—H⋯N hydrogen-bond is present giving rise to an S(5) ring motif. In the crystal, double-stranded chains propagating along [10] are formed via pairs of O—H⋯S and N—H⋯S hydrogen bonds. The chains are further stabilized by C—H⋯S interactions.
Related literature
For standard bond lengths, see: Allen et al. (1987). For graph-set analysis of hydrogen bonds, see: Bernstein et al. (1995). For related structures, see: Choi et al. (2008). For the biological activity and pharmacological properties of thiosemicarbazones and their metal complexes, see: Cowley et al. (2002); Ming (2003); Lobana et al. (2004, 2007).
Experimental
Crystal data
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Refinement
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Data collection: APEX2 (Bruker, 2005); cell SAINT (Bruker, 2005); 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
10.1107/S1600536811053621/mw2038sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811053621/mw2038Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536811053621/mw2038Isup3.cml
To a hot stirred solution of 2,3-butanedione monoxime (1.01 g, 10 mmole) in ethanol (20 ml) containing a few drops of glacial acetic acid was added 4-methyl-3-thiosemicarbazide (1.05 g, 10 mmole) dissolved in ethanol (20 ml). The reaction mixture was then heated under reflux for 3 h. The mixture was filtered and left to cool, the resulting white solid was collected by suction filtration and washed with cold EtOH. The white crystals were grown from ethanol soultion by slow evaporation at room temperature, yield, 78.8%, m.p., 487.5–490 K.
N and O bound H atoms were located in a difference Fourier map and were refined freely. The remaining H atoms were positioned geometrically and refined using a riding model with C—H = 0.98 and Uiso(H) = 1.5Ueq(C) for methyl groups. The highest residual electron density peak is located 0.63 Å from C2 and the deepest hole is located 0.68 Å from C4.
Data collection: APEX2 (Bruker, 2005); cell
SAINT (Bruker, 2005); data reduction: SAINT (Bruker, 2005); 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).Fig. 1. The molecular structure of the title compound with 50% probability displacement ellipsoids and the atom-numbering scheme. | |
Fig. 2. The crystal packing of the title compound viewed down the a axis. Hydrogen bonds are shown as dashed lines. |
C6H12N4OS | Z = 2 |
Mr = 188.26 | F(000) = 200 |
Triclinic, P1 | Dx = 1.403 Mg m−3 |
Hall symbol: -P 1 | Melting point = 487.5–490 K |
a = 5.5205 (1) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 8.6077 (2) Å | Cell parameters from 7387 reflections |
c = 9.5650 (2) Å | θ = 2.4–32.7° |
α = 79.750 (1)° | µ = 0.32 mm−1 |
β = 89.509 (1)° | T = 100 K |
γ = 85.083 (1)° | Plate, colourless |
V = 445.61 (2) Å3 | 0.51 × 0.25 × 0.07 mm |
Bruker APEXII CCD diffractometer | 3256 independent reflections |
Radiation source: fine-focus sealed tube | 2920 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.020 |
ϕ and ω scans | θmax = 32.7°, θmin = 2.2° |
Absorption correction: multi-scan (SADABS; Bruker, 2005) | h = −8→8 |
Tmin = 0.854, Tmax = 0.978 | k = −13→13 |
12035 measured reflections | l = −14→14 |
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)] = 0.031 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.081 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.08 | w = 1/[σ2(Fo2) + (0.0347P)2 + 0.1679P] where P = (Fo2 + 2Fc2)/3 |
3256 reflections | (Δ/σ)max = 0.001 |
124 parameters | Δρmax = 0.40 e Å−3 |
0 restraints | Δρmin = −0.39 e Å−3 |
C6H12N4OS | γ = 85.083 (1)° |
Mr = 188.26 | V = 445.61 (2) Å3 |
Triclinic, P1 | Z = 2 |
a = 5.5205 (1) Å | Mo Kα radiation |
b = 8.6077 (2) Å | µ = 0.32 mm−1 |
c = 9.5650 (2) Å | T = 100 K |
α = 79.750 (1)° | 0.51 × 0.25 × 0.07 mm |
β = 89.509 (1)° |
Bruker APEXII CCD diffractometer | 3256 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2005) | 2920 reflections with I > 2σ(I) |
Tmin = 0.854, Tmax = 0.978 | Rint = 0.020 |
12035 measured reflections |
R[F2 > 2σ(F2)] = 0.031 | 0 restraints |
wR(F2) = 0.081 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.08 | Δρmax = 0.40 e Å−3 |
3256 reflections | Δρmin = −0.39 e Å−3 |
124 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
S1 | 0.94334 (4) | 0.16073 (3) | 0.30007 (2) | 0.01590 (7) | |
O1 | −0.03857 (14) | 0.29827 (9) | 0.95645 (8) | 0.02032 (15) | |
N1 | 0.16712 (15) | 0.21630 (10) | 0.90822 (9) | 0.01569 (15) | |
N2 | 0.44402 (14) | 0.22893 (9) | 0.57941 (8) | 0.01351 (14) | |
N3 | 0.64505 (15) | 0.16555 (10) | 0.51705 (8) | 0.01452 (15) | |
N4 | 0.51169 (15) | 0.32555 (10) | 0.31045 (8) | 0.01554 (15) | |
C1 | 0.02246 (18) | 0.37515 (12) | 0.67902 (10) | 0.01835 (18) | |
H1A | −0.1458 | 0.3575 | 0.7064 | 0.028* | |
H1B | 0.0464 | 0.3628 | 0.5798 | 0.028* | |
H1C | 0.0556 | 0.4825 | 0.6895 | 0.028* | |
C2 | 0.19230 (17) | 0.25693 (11) | 0.77265 (10) | 0.01371 (16) | |
C3 | 0.40835 (17) | 0.17983 (11) | 0.71298 (10) | 0.01444 (16) | |
C4 | 0.5672 (2) | 0.05499 (14) | 0.80647 (11) | 0.0258 (2) | |
H4A | 0.6119 | −0.0328 | 0.7560 | 0.039* | |
H4B | 0.4791 | 0.0158 | 0.8932 | 0.039* | |
H4C | 0.7146 | 0.1001 | 0.8314 | 0.039* | |
C5 | 0.68449 (17) | 0.22272 (10) | 0.37711 (9) | 0.01296 (15) | |
C6 | 0.51377 (18) | 0.39340 (12) | 0.15976 (10) | 0.01718 (18) | |
H6A | 0.3703 | 0.4686 | 0.1362 | 0.026* | |
H6B | 0.5111 | 0.3086 | 0.1038 | 0.026* | |
H6C | 0.6612 | 0.4486 | 0.1379 | 0.026* | |
H1N3 | 0.754 (3) | 0.0948 (18) | 0.5626 (16) | 0.025 (4)* | |
H1N4 | 0.387 (3) | 0.3399 (18) | 0.3605 (17) | 0.026 (4)* | |
H1O1 | −0.040 (3) | 0.263 (2) | 1.046 (2) | 0.039 (4)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.01340 (11) | 0.02020 (11) | 0.01157 (10) | 0.00444 (8) | 0.00346 (7) | 0.00102 (7) |
O1 | 0.0191 (3) | 0.0277 (4) | 0.0116 (3) | 0.0092 (3) | 0.0044 (3) | −0.0022 (3) |
N1 | 0.0146 (4) | 0.0190 (3) | 0.0124 (3) | 0.0039 (3) | 0.0031 (3) | −0.0025 (3) |
N2 | 0.0128 (3) | 0.0160 (3) | 0.0112 (3) | 0.0009 (3) | 0.0029 (3) | −0.0020 (3) |
N3 | 0.0135 (3) | 0.0179 (3) | 0.0102 (3) | 0.0041 (3) | 0.0024 (3) | 0.0002 (3) |
N4 | 0.0135 (4) | 0.0203 (4) | 0.0103 (3) | 0.0044 (3) | 0.0026 (3) | 0.0012 (3) |
C1 | 0.0175 (4) | 0.0223 (4) | 0.0126 (4) | 0.0057 (3) | 0.0007 (3) | 0.0005 (3) |
C2 | 0.0134 (4) | 0.0154 (4) | 0.0113 (4) | 0.0017 (3) | 0.0009 (3) | −0.0013 (3) |
C3 | 0.0151 (4) | 0.0161 (4) | 0.0107 (4) | 0.0028 (3) | 0.0019 (3) | −0.0006 (3) |
C4 | 0.0265 (5) | 0.0314 (5) | 0.0129 (4) | 0.0159 (4) | 0.0054 (4) | 0.0048 (4) |
C5 | 0.0129 (4) | 0.0145 (4) | 0.0108 (4) | 0.0004 (3) | 0.0014 (3) | −0.0014 (3) |
C6 | 0.0180 (4) | 0.0202 (4) | 0.0106 (4) | 0.0046 (3) | 0.0013 (3) | 0.0017 (3) |
S1—C5 | 1.6914 (9) | C1—H1A | 0.9800 |
O1—N1 | 1.4034 (10) | C1—H1B | 0.9800 |
O1—H1O1 | 0.858 (19) | C1—H1C | 0.9800 |
N1—C2 | 1.2911 (12) | C2—C3 | 1.4752 (13) |
N2—C3 | 1.2912 (12) | C3—C4 | 1.4944 (13) |
N2—N3 | 1.3733 (11) | C4—H4A | 0.9800 |
N3—C5 | 1.3639 (12) | C4—H4B | 0.9800 |
N3—H1N3 | 0.876 (15) | C4—H4C | 0.9800 |
N4—C5 | 1.3285 (12) | C6—H6A | 0.9800 |
N4—C6 | 1.4560 (12) | C6—H6B | 0.9800 |
N4—H1N4 | 0.847 (16) | C6—H6C | 0.9800 |
C1—C2 | 1.4977 (13) | ||
N1—O1—H1O1 | 104.1 (12) | N2—C3—C2 | 115.15 (8) |
C2—N1—O1 | 111.22 (8) | N2—C3—C4 | 125.00 (9) |
C3—N2—N3 | 118.54 (8) | C2—C3—C4 | 119.84 (8) |
C5—N3—N2 | 117.75 (8) | C3—C4—H4A | 109.5 |
C5—N3—H1N3 | 118.0 (10) | C3—C4—H4B | 109.5 |
N2—N3—H1N3 | 124.1 (10) | H4A—C4—H4B | 109.5 |
C5—N4—C6 | 124.53 (8) | C3—C4—H4C | 109.5 |
C5—N4—H1N4 | 114.1 (11) | H4A—C4—H4C | 109.5 |
C6—N4—H1N4 | 120.9 (11) | H4B—C4—H4C | 109.5 |
C2—C1—H1A | 109.5 | N4—C5—N3 | 116.23 (8) |
C2—C1—H1B | 109.5 | N4—C5—S1 | 124.44 (7) |
H1A—C1—H1B | 109.5 | N3—C5—S1 | 119.33 (7) |
C2—C1—H1C | 109.5 | N4—C6—H6A | 109.5 |
H1A—C1—H1C | 109.5 | N4—C6—H6B | 109.5 |
H1B—C1—H1C | 109.5 | H6A—C6—H6B | 109.5 |
N1—C2—C3 | 115.02 (8) | N4—C6—H6C | 109.5 |
N1—C2—C1 | 124.30 (8) | H6A—C6—H6C | 109.5 |
C3—C2—C1 | 120.68 (8) | H6B—C6—H6C | 109.5 |
C3—N2—N3—C5 | −177.76 (8) | N1—C2—C3—C4 | 4.82 (14) |
O1—N1—C2—C3 | 178.35 (8) | C1—C2—C3—C4 | −176.26 (10) |
O1—N1—C2—C1 | −0.52 (13) | C6—N4—C5—N3 | −176.61 (9) |
N3—N2—C3—C2 | 178.38 (8) | C6—N4—C5—S1 | 3.43 (14) |
N3—N2—C3—C4 | −1.47 (15) | N2—N3—C5—N4 | −5.71 (13) |
N1—C2—C3—N2 | −175.03 (9) | N2—N3—C5—S1 | 174.25 (6) |
C1—C2—C3—N2 | 3.88 (13) |
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H1N3···S1i | 0.877 (16) | 2.781 (16) | 3.6519 (9) | 172.0 (14) |
N4—H1N4···N2 | 0.848 (16) | 2.155 (16) | 2.5932 (11) | 111.9 (13) |
O1—H1O1···S1ii | 0.857 (19) | 2.437 (19) | 3.2930 (8) | 178.3 (17) |
C1—H1B···N2 | 0.98 | 2.39 | 2.7919 (13) | 104 |
C4—H4A···S1i | 0.98 | 2.69 | 3.3991 (12) | 129 |
C4—H4B···N1 | 0.98 | 2.35 | 2.7698 (14) | 105 |
C4—H4C···O1iii | 0.98 | 2.71 | 3.6173 (16) | 154 |
C6—H6A···O1iv | 0.98 | 2.63 | 3.6011 (12) | 170 |
Symmetry codes: (i) −x+2, −y, −z+1; (ii) x−1, y, z+1; (iii) x+1, y, z; (iv) −x, −y+1, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C6H12N4OS |
Mr | 188.26 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 100 |
a, b, c (Å) | 5.5205 (1), 8.6077 (2), 9.5650 (2) |
α, β, γ (°) | 79.750 (1), 89.509 (1), 85.083 (1) |
V (Å3) | 445.61 (2) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.32 |
Crystal size (mm) | 0.51 × 0.25 × 0.07 |
Data collection | |
Diffractometer | Bruker APEXII CCD diffractometer |
Absorption correction | Multi-scan (SADABS; Bruker, 2005) |
Tmin, Tmax | 0.854, 0.978 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 12035, 3256, 2920 |
Rint | 0.020 |
(sin θ/λ)max (Å−1) | 0.761 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.031, 0.081, 1.08 |
No. of reflections | 3256 |
No. of parameters | 124 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.40, −0.39 |
Computer programs: APEX2 (Bruker, 2005), SAINT (Bruker, 2005), SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H1N3···S1i | 0.877 (16) | 2.781 (16) | 3.6519 (9) | 172.0 (14) |
N4—H1N4···N2 | 0.848 (16) | 2.155 (16) | 2.5932 (11) | 111.9 (13) |
O1—H1O1···S1ii | 0.857 (19) | 2.437 (19) | 3.2930 (8) | 178.3 (17) |
C1—H1B···N2 | 0.98 | 2.39 | 2.7919 (13) | 104 |
C4—H4A···S1i | 0.98 | 2.69 | 3.3991 (12) | 129 |
C4—H4B···N1 | 0.98 | 2.35 | 2.7698 (14) | 105 |
C4—H4C···O1iii | 0.98 | 2.71 | 3.6173 (16) | 154 |
C6—H6A···O1iv | 0.98 | 2.63 | 3.6011 (12) | 170 |
Symmetry codes: (i) −x+2, −y, −z+1; (ii) x−1, y, z+1; (iii) x+1, y, z; (iv) −x, −y+1, −z+1. |
Acknowledgements
The authors thank the Malaysian Government and Universiti Sains Malaysia for the RU research Grant (1001/PKIMIA/815067). NEE thanks Universiti Sains Malaysia for a post-doctoral fellowship and the International University of Africa (Sudan) for providing research leave. HAF and AQA each thank the Ministry of Higher Education and the University of Sabha (Libya) for a scholarship.
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
Thiosemicarbazones and their metal complexes have attracted significant attention because of their wide-ranging biological and pharmacological activities related to specific structures as well as chemical properties (Cowley et al., 2002; Ming, 2003; Lobana et al., 2007; Lobana et al., 2004). In this paper we report the crystal structure of (E)-2-((E)-3-(hydroxyimino)butan-2-ylidene)-N-methylhydrazinecarbothioamide (Fig. 1).
In the title compound, C6H12N4OS, butane is the longest carbon-carbon chain with the oxime group bound to C2 and the 4-methyl-3-thiosemicarbazide moiety bound to C3. The two methyl groups C1 and C4 are trans to each other. The torsion angles of the chains (O1/N1/C2/C3), (C1/C2/C3/C4) and (N2/N3/C5/N4) are 178.35 (8)°, -176.26 (10)° and -5.71 (13)°, respectively, indicating the near-planarity of the molecular backbone. All bond lengths and angles are normal (Allen et al., 1987).
Cyclic intramolecular N4—H1N4···N2, C1—H1B···N2 and C4—H4B···N1 hydrogen-bonding interactions [graph set S(5), (Bernstein et al., 1995)] are present (Table 1) with the latter two being notably weaker than the first. In the crystal molecules are connected through intermolecular O1—H1O1···S1 hydrogen bonds into infinite one-dimensional chains which propagate along [1 0 -1]. In addition, intermolecular N3—H1N3···S1, C4—H4A···S1 and C6—H6A···O1 hydrogen bonds associate these chains into sheets while the sheets are tied together via C4—H4C···O1 interactions (Fig. 2, Table 1). As a consequence of the C4—H4A···S1 and C4—H4C···O1 interactions, a rather short H4B-H4B contact is forced between adjacent molecules in the sheet.