




Supporting information
![]() | Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536813008398/qk2055sup1.cif |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S1600536813008398/qk2055Isup2.hkl |
![]() | Chemical Markup Language (CML) file https://doi.org/10.1107/S1600536813008398/qk2055Isup3.cml |
CCDC reference: 954231
Key indicators
- Single-crystal X-ray study
- T = 200 K
- Mean
(C-C) = 0.002 Å
- R factor = 0.037
- wR factor = 0.107
- Data-to-parameter ratio = 15.7
checkCIF/PLATON results
No syntax errors found
Alert level C PLAT230_ALERT_2_C Hirshfeld Test Diff for S1 -- C1 .. 6.0 su PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 2.4 PLAT480_ALERT_4_C Long H...A H-Bond Reported H1N1 .. O1 .. 2.66 Ang. PLAT910_ALERT_3_C Missing # of FCF Reflections Below Th(Min) ..... 1 PLAT911_ALERT_3_C Missing # FCF Refl Between THmin & STh/L= 0.600 29 PLAT913_ALERT_3_C Missing # of Very Strong Reflections in FCF .... 5
Alert level G PLAT005_ALERT_5_G No _iucr_refine_instructions_details in the CIF ? PLAT007_ALERT_5_G Note: Number of Unrefined D-H Atoms ............ 3 PLAT720_ALERT_4_G Number of Unusual/Non-Standard Labels .......... 3 PLAT912_ALERT_4_G Missing # of FCF Reflections Above STh/L= 0.600 2
0 ALERT level A = Most likely a serious problem - resolve or explain 0 ALERT level B = A potentially serious problem, consider carefully 6 ALERT level C = Check. Ensure it is not caused by an omission or oversight 4 ALERT level G = General information/check it is not something unexpected 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 ALERT type 3 Indicator that the structure quality may be low 3 ALERT type 4 Improvement, methodology, query or suggestion 2 ALERT type 5 Informative message, check
All starting materials are commercially available and were used without further purification. The synthesis was adapted from a procedure reported previously (de Oliveira et al., 2012). The hydrochloric acid catalyzed reaction of 3',4'-(methylenedioxy)acetophenone (10 mmol) and thiosemicarbazide (10 mmol) in a 3:1 mixture of ethanol and water (100 ml) was refluxed for 6 h. After cooling and filtering crystals suitable for X-ray diffraction were obtained.
Elemental analysis: Calc. 50.62% for C, 4.67% for H, 17.71% for N and 13.51% for S; found 50.72% for C, 4.66% for H, 17.70% for N and 13.47% for S. The melting point was determined by differential scanning calorimetry to 187° C and the enthalpy of fusion amount to 25.9 kJ/mol. After melting the compound decomposes.
All H atoms were located in a Fourier map. C-bonded H atoms were then geometrically placed (C—H = 0.95–0.99 Å) and refined as riding with Uiso(H) = 1.2Ueq(C(CH), C(CH2)) or 1.5Ueq(C) and AFIX 136 for the methyl group. The N-bonded H atoms were only adjusted to N—H = 0.88 Å and were then refined as riding with Uiso(H) = 1.2 Ueq(N).
Thiosemicarbazone derivatives have a wide range of pharmacological properties. For example, 3',4'-(methylenedioxy)acetophenone thiosemicarbazone derivatives show cytotoxic activity against KB cells (Silva et al., 1998). As part of our study on the synthesis of thiosemicarbazone derivatives, we report herein the crystal structure of a new 3',4'-(methylenedioxy)acetophenone thiosemicarbazone derivative.
In the crystal structure of the title compound, C10H11N3O2S, the molecules are twisted and consists of two nearly planar parts, a benzo[1,3]dioxole fragment and a hydrazinecarbothioamide fragment (mean deviations from planarity for non-H atoms 0.0325 (12) Å and 0.0707 (10) Å, respectively), which subtend a dihedral angle of 29.06 (5)° (Fig. 1). The molecule shows an E conformation for the atoms about the N3—N2 and N2—C1 bonds, which is also observed in the crystal structures of other thiosemicarbazone derivatives (de Oliveira et al., 2012).
In the crystal structure the molecules are linked by pairs of N—H···S hydrogen bonds into inversion related dimers (Fig. 2 and Table 1). These dimers are further connected by centrosymmetric pairs of weak N—H···S interactions into chains extending along [101] (Fig. 2). Finally, there is one N—H···O contact between that NH2 hydrogen atom which is not involved in N—H···S bonding and the dioxole oxygen O1 (Table 1). If this contact is considered as an interaction the chains are additionally linked into a three-dimensional network (Fig. 2).
In the crystal structure the benzo[1,3]dioxole fragments are oriented nearly perpendicular to [001] and are stacked above each other along this direction by the c-glide plane with a repetition period of c/2 = 3.5645 (7) Å implying π-π stacking.
For the adapted synthesis of the title compound, see: de Oliveira et al. (2012). For the pharmacological activity of 3',4'-(methylenedioxy)acetophenone thiosimecarbazone derivatives, see: Silva et al. (1998).
Data collection: X-AREA (Stoe & Cie, 2008); cell refinement: X-AREA (Stoe & Cie, 2008); data reduction: X-RED32 (Stoe & Cie, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2011); software used to prepare material for publication: publCIF (Westrip, 2010).
C10H11N3O2S | F(000) = 496 |
Mr = 237.28 | Dx = 1.461 Mg m−3 |
Monoclinic, P21/c | Melting point: 460.2 K |
Hall symbol: -P 2ybc | Mo Kα radiation, λ = 0.71073 Å |
a = 6.1423 (12) Å | Cell parameters from 8000 reflections |
b = 26.065 (5) Å | θ = 3–27.9° |
c = 7.1289 (14) Å | µ = 0.29 mm−1 |
β = 109.07 (3)° | T = 200 K |
V = 1078.7 (4) Å3 | Block, yellow |
Z = 4 | 0.3 × 0.2 × 0.2 mm |
Stoe IPDS-1 diffractometer | 2018 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.046 |
Graphite monochromator | θmax = 27.0°, θmin = 3.1° |
φ scans | h = −7→7 |
12310 measured reflections | k = −33→33 |
2315 independent reflections | l = −9→9 |
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)] = 0.037 | H-atom parameters constrained |
wR(F2) = 0.107 | w = 1/[σ2(Fo2) + (0.0692P)2 + 0.2915P] where P = (Fo2 + 2Fc2)/3 |
S = 1.04 | (Δ/σ)max = 0.001 |
2315 reflections | Δρmax = 0.29 e Å−3 |
147 parameters | Δρmin = −0.32 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.047 (8) |
C10H11N3O2S | V = 1078.7 (4) Å3 |
Mr = 237.28 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 6.1423 (12) Å | µ = 0.29 mm−1 |
b = 26.065 (5) Å | T = 200 K |
c = 7.1289 (14) Å | 0.3 × 0.2 × 0.2 mm |
β = 109.07 (3)° |
Stoe IPDS-1 diffractometer | 2018 reflections with I > 2σ(I) |
12310 measured reflections | Rint = 0.046 |
2315 independent reflections |
R[F2 > 2σ(F2)] = 0.037 | 0 restraints |
wR(F2) = 0.107 | H-atom parameters constrained |
S = 1.04 | Δρmax = 0.29 e Å−3 |
2315 reflections | Δρmin = −0.32 e Å−3 |
147 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 | ||
N1 | 0.2311 (2) | 0.43475 (5) | 0.0548 (2) | 0.0326 (3) | |
H1N1 | 0.2765 | 0.4032 | 0.0431 | 0.049* | |
H2N1 | 0.0917 | 0.4461 | −0.0094 | 0.049* | |
C1 | 0.3775 (3) | 0.46661 (5) | 0.1778 (2) | 0.0229 (3) | |
S1 | 0.31425 (7) | 0.528178 (13) | 0.21371 (6) | 0.03093 (17) | |
N2 | 0.5891 (2) | 0.44885 (4) | 0.28111 (18) | 0.0252 (3) | |
H1N2 | 0.6685 | 0.4673 | 0.3840 | 0.030* | |
N3 | 0.6401 (2) | 0.39750 (4) | 0.26964 (18) | 0.0230 (3) | |
C2 | 0.8498 (2) | 0.38377 (5) | 0.3628 (2) | 0.0205 (3) | |
C3 | 1.0366 (3) | 0.42034 (6) | 0.4726 (3) | 0.0332 (4) | |
H3A | 1.0430 | 0.4489 | 0.3850 | 0.050* | |
H3B | 1.1849 | 0.4024 | 0.5151 | 0.050* | |
H3C | 1.0039 | 0.4336 | 0.5892 | 0.050* | |
C4 | 0.8967 (2) | 0.32787 (5) | 0.3605 (2) | 0.0201 (3) | |
C5 | 1.1206 (3) | 0.30922 (6) | 0.4082 (2) | 0.0276 (3) | |
H5 | 1.2450 | 0.3329 | 0.4394 | 0.033* | |
C6 | 1.1679 (3) | 0.25646 (6) | 0.4115 (3) | 0.0320 (4) | |
H6 | 1.3209 | 0.2440 | 0.4421 | 0.038* | |
C7 | 0.9848 (3) | 0.22397 (5) | 0.3689 (2) | 0.0250 (3) | |
O1 | 0.9848 (2) | 0.17122 (4) | 0.36822 (19) | 0.0362 (3) | |
C8 | 0.7485 (3) | 0.15623 (6) | 0.3202 (3) | 0.0329 (4) | |
H8A | 0.7026 | 0.1345 | 0.1997 | 0.039* | |
H8B | 0.7267 | 0.1362 | 0.4308 | 0.039* | |
O2 | 0.6109 (2) | 0.20154 (4) | 0.2866 (2) | 0.0409 (3) | |
C9 | 0.7615 (3) | 0.24196 (5) | 0.3209 (2) | 0.0241 (3) | |
C10 | 0.7108 (3) | 0.29321 (5) | 0.3141 (2) | 0.0242 (3) | |
H10 | 0.5562 | 0.3049 | 0.2795 | 0.029* |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1 | 0.0320 (7) | 0.0199 (6) | 0.0367 (8) | 0.0067 (5) | −0.0014 (6) | −0.0073 (5) |
C1 | 0.0269 (7) | 0.0175 (6) | 0.0227 (7) | 0.0036 (5) | 0.0060 (6) | 0.0011 (5) |
S1 | 0.0335 (3) | 0.0145 (2) | 0.0383 (3) | 0.00688 (13) | 0.00280 (18) | −0.00235 (13) |
N2 | 0.0285 (7) | 0.0133 (6) | 0.0287 (7) | 0.0050 (4) | 0.0022 (5) | −0.0034 (4) |
N3 | 0.0278 (6) | 0.0128 (5) | 0.0255 (6) | 0.0044 (4) | 0.0049 (5) | −0.0015 (4) |
C2 | 0.0231 (7) | 0.0162 (6) | 0.0226 (7) | 0.0011 (5) | 0.0079 (6) | −0.0007 (5) |
C3 | 0.0258 (8) | 0.0250 (7) | 0.0475 (10) | −0.0039 (6) | 0.0101 (7) | −0.0084 (6) |
C4 | 0.0220 (7) | 0.0168 (6) | 0.0204 (6) | 0.0039 (5) | 0.0056 (5) | 0.0008 (5) |
C5 | 0.0219 (7) | 0.0230 (7) | 0.0363 (8) | 0.0034 (5) | 0.0073 (6) | 0.0012 (6) |
C6 | 0.0251 (7) | 0.0269 (8) | 0.0429 (9) | 0.0116 (6) | 0.0095 (7) | 0.0044 (6) |
C7 | 0.0331 (8) | 0.0172 (7) | 0.0246 (7) | 0.0099 (5) | 0.0092 (6) | 0.0030 (5) |
O1 | 0.0434 (7) | 0.0165 (5) | 0.0473 (7) | 0.0112 (4) | 0.0129 (6) | 0.0045 (4) |
C8 | 0.0487 (10) | 0.0156 (7) | 0.0349 (9) | 0.0047 (6) | 0.0145 (8) | 0.0013 (6) |
O2 | 0.0333 (6) | 0.0141 (5) | 0.0703 (9) | −0.0002 (4) | 0.0100 (6) | −0.0022 (5) |
C9 | 0.0262 (7) | 0.0161 (6) | 0.0281 (7) | 0.0012 (5) | 0.0064 (6) | −0.0006 (5) |
C10 | 0.0209 (7) | 0.0170 (7) | 0.0324 (8) | 0.0043 (5) | 0.0058 (6) | −0.0006 (5) |
N1—C1 | 1.324 (2) | C4—C10 | 1.408 (2) |
N1—H1N1 | 0.8802 | C5—C6 | 1.404 (2) |
N1—H2N1 | 0.8800 | C5—H5 | 0.9500 |
C1—N2 | 1.3494 (19) | C6—C7 | 1.361 (2) |
C1—S1 | 1.6901 (14) | C6—H6 | 0.9500 |
N2—N3 | 1.3831 (16) | C7—O1 | 1.3749 (17) |
N2—H1N2 | 0.8800 | C7—C9 | 1.382 (2) |
N3—C2 | 1.2921 (19) | O1—C8 | 1.432 (2) |
C2—C4 | 1.4864 (17) | C8—O2 | 1.4261 (19) |
C2—C3 | 1.500 (2) | C8—H8A | 0.9900 |
C3—H3A | 0.9800 | C8—H8B | 0.9900 |
C3—H3B | 0.9800 | O2—C9 | 1.3704 (18) |
C3—H3C | 0.9800 | C9—C10 | 1.3690 (19) |
C4—C5 | 1.392 (2) | C10—H10 | 0.9500 |
C1—N1—H1N1 | 118.7 | C4—C5—H5 | 119.0 |
C1—N1—H2N1 | 117.9 | C6—C5—H5 | 119.0 |
H1N1—N1—H2N1 | 123.4 | C7—C6—C5 | 117.03 (13) |
N1—C1—N2 | 118.10 (12) | C7—C6—H6 | 121.5 |
N1—C1—S1 | 123.79 (12) | C5—C6—H6 | 121.5 |
N2—C1—S1 | 118.11 (11) | C6—C7—O1 | 128.48 (14) |
C1—N2—N3 | 119.75 (12) | C6—C7—C9 | 121.67 (13) |
C1—N2—H1N2 | 116.1 | O1—C7—C9 | 109.84 (13) |
N3—N2—H1N2 | 120.3 | C7—O1—C8 | 105.81 (11) |
C2—N3—N2 | 116.40 (12) | O2—C8—O1 | 108.23 (12) |
N3—C2—C4 | 115.46 (12) | O2—C8—H8A | 110.1 |
N3—C2—C3 | 123.80 (13) | O1—C8—H8A | 110.1 |
C4—C2—C3 | 120.72 (13) | O2—C8—H8B | 110.1 |
C2—C3—H3A | 109.5 | O1—C8—H8B | 110.1 |
C2—C3—H3B | 109.5 | H8A—C8—H8B | 108.4 |
H3A—C3—H3B | 109.5 | C9—O2—C8 | 106.15 (13) |
C2—C3—H3C | 109.5 | C10—C9—O2 | 127.67 (14) |
H3A—C3—H3C | 109.5 | C10—C9—C7 | 122.40 (14) |
H3B—C3—H3C | 109.5 | O2—C9—C7 | 109.93 (12) |
C5—C4—C10 | 119.61 (13) | C9—C10—C4 | 117.38 (13) |
C5—C4—C2 | 121.26 (13) | C9—C10—H10 | 121.3 |
C10—C4—C2 | 119.12 (12) | C4—C10—H10 | 121.3 |
C4—C5—C6 | 121.91 (14) | ||
N1—C1—N2—N3 | −5.7 (2) | C6—C7—O1—C8 | 178.09 (16) |
S1—C1—N2—N3 | 174.06 (10) | C9—C7—O1—C8 | −0.96 (17) |
C1—N2—N3—C2 | 175.99 (13) | C7—O1—C8—O2 | 1.91 (17) |
N2—N3—C2—C4 | 175.80 (11) | O1—C8—O2—C9 | −2.14 (17) |
N2—N3—C2—C3 | −2.5 (2) | C8—O2—C9—C10 | −177.54 (15) |
N3—C2—C4—C5 | 163.15 (13) | C8—O2—C9—C7 | 1.57 (18) |
C3—C2—C4—C5 | −18.5 (2) | C6—C7—C9—C10 | −0.3 (2) |
N3—C2—C4—C10 | −18.52 (19) | O1—C7—C9—C10 | 178.77 (13) |
C3—C2—C4—C10 | 159.82 (14) | C6—C7—C9—O2 | −179.51 (15) |
C10—C4—C5—C6 | 0.0 (2) | O1—C7—C9—O2 | −0.39 (18) |
C2—C4—C5—C6 | 178.38 (14) | O2—C9—C10—C4 | 178.34 (15) |
C4—C5—C6—C7 | −1.0 (2) | C7—C9—C10—C4 | −0.7 (2) |
C5—C6—C7—O1 | −177.77 (15) | C5—C4—C10—C9 | 0.8 (2) |
C5—C6—C7—C9 | 1.2 (2) | C2—C4—C10—C9 | −177.57 (13) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N1···O1i | 0.88 | 2.66 | 3.2207 (17) | 123 |
N1—H2N1···S1ii | 0.88 | 2.53 | 3.4100 (18) | 175 |
N2—H1N2···S1iii | 0.88 | 2.84 | 3.5048 (15) | 134 |
Symmetry codes: (i) x−1, −y+1/2, z−1/2; (ii) −x, −y+1, −z; (iii) −x+1, −y+1, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C10H11N3O2S |
Mr | 237.28 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 200 |
a, b, c (Å) | 6.1423 (12), 26.065 (5), 7.1289 (14) |
β (°) | 109.07 (3) |
V (Å3) | 1078.7 (4) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.29 |
Crystal size (mm) | 0.3 × 0.2 × 0.2 |
Data collection | |
Diffractometer | Stoe IPDS1 |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 12310, 2315, 2018 |
Rint | 0.046 |
(sin θ/λ)max (Å−1) | 0.639 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.037, 0.107, 1.04 |
No. of reflections | 2315 |
No. of parameters | 147 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.29, −0.32 |
Computer programs: X-AREA (Stoe & Cie, 2008), X-RED32 (Stoe & Cie, 2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), DIAMOND (Brandenburg, 2011), publCIF (Westrip, 2010).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N1···O1i | 0.88 | 2.66 | 3.2207 (17) | 122.7 |
N1—H2N1···S1ii | 0.88 | 2.53 | 3.4100 (18) | 174.8 |
N2—H1N2···S1iii | 0.88 | 2.84 | 3.5048 (15) | 133.8 |
Symmetry codes: (i) x−1, −y+1/2, z−1/2; (ii) −x, −y+1, −z; (iii) −x+1, −y+1, −z+1. |
Thiosemicarbazone derivatives have a wide range of pharmacological properties. For example, 3',4'-(methylenedioxy)acetophenone thiosemicarbazone derivatives show cytotoxic activity against KB cells (Silva et al., 1998). As part of our study on the synthesis of thiosemicarbazone derivatives, we report herein the crystal structure of a new 3',4'-(methylenedioxy)acetophenone thiosemicarbazone derivative.
In the crystal structure of the title compound, C10H11N3O2S, the molecules are twisted and consists of two nearly planar parts, a benzo[1,3]dioxole fragment and a hydrazinecarbothioamide fragment (mean deviations from planarity for non-H atoms 0.0325 (12) Å and 0.0707 (10) Å, respectively), which subtend a dihedral angle of 29.06 (5)° (Fig. 1). The molecule shows an E conformation for the atoms about the N3—N2 and N2—C1 bonds, which is also observed in the crystal structures of other thiosemicarbazone derivatives (de Oliveira et al., 2012).
In the crystal structure the molecules are linked by pairs of N—H···S hydrogen bonds into inversion related dimers (Fig. 2 and Table 1). These dimers are further connected by centrosymmetric pairs of weak N—H···S interactions into chains extending along [101] (Fig. 2). Finally, there is one N—H···O contact between that NH2 hydrogen atom which is not involved in N—H···S bonding and the dioxole oxygen O1 (Table 1). If this contact is considered as an interaction the chains are additionally linked into a three-dimensional network (Fig. 2).
In the crystal structure the benzo[1,3]dioxole fragments are oriented nearly perpendicular to [001] and are stacked above each other along this direction by the c-glide plane with a repetition period of c/2 = 3.5645 (7) Å implying π-π stacking.