Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536814016407/tk5328sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536814016407/tk5328Isup2.hkl | |
Chemical Markup Language (CML) file https://doi.org/10.1107/S1600536814016407/tk5328Isup3.cml |
CCDC reference: 1014062
Key indicators
- Single-crystal X-ray study
- T = 296 K
- Mean (C-C) = 0.002 Å
- R factor = 0.034
- wR factor = 0.100
- Data-to-parameter ratio = 13.7
checkCIF/PLATON results
No syntax errors found
Alert level C PLAT230_ALERT_2_C Hirshfeld Test Diff for S1 -- C1 .. 5.9 su PLAT480_ALERT_4_C Long H...A H-Bond Reported H1 .. S1 .. 2.99 Ang. PLAT761_ALERT_1_C CIF Contains no X-H Bonds ...................... Please Check PLAT762_ALERT_1_C CIF Contains no X-Y-H or H-Y-H Angles .......... Please Check PLAT911_ALERT_3_C Missing # FCF Refl Between THmin & STh/L= 0.595 4 Why ?
Alert level G PLAT005_ALERT_5_G No _iucr_refine_instructions_details in the CIF Please Do ! PLAT909_ALERT_3_G Percentage of Observed Data at Theta(Max) still 78 %
0 ALERT level A = Most likely a serious problem - resolve or explain 0 ALERT level B = A potentially serious problem, consider carefully 5 ALERT level C = Check. Ensure it is not caused by an omission or oversight 2 ALERT level G = General information/check it is not something unexpected 2 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 2 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check
A solution of 4-methyl-3-thiosemicarbazide (392 mg, 3.72 mmol) in water (50 mL) was slowly added at 50°C to a solution of terephthaldicarboxaldehyde (500 mg, 3.73 mmol) in 100 mL water. Then the mixture was stirred at 50°C for 30 mins. Once cooled to room temperature, the yellow solid was filtered off and vacuum dried. Yellow single crystals suitable for X-ray diffraction were obtained by recrystallization from EtOH/H2O (1:1). Yield: 91%, M. pt: 213-216 °C. IR data (KBr, cm-1): 3368m, 3150m ν(N—H); 2838w, 2742w ν(C—H aldehyde); 1692 s ν(C═O); 1545 s, 1257m ν(C═N), 833m, 777w ν(C═S). 1H NMR data (DMSO-d6, ppm): 11.72 (s, 1H, N(2)—H); 10.03 (s, 1H, C(1)—H); 8.69 (s, 1H, N(2)—H); 8.11 (s, 1H, C(8)—H); 8.04 (d, 2H, J = 8.1 Hz, C(3,7)-H); 7.94 (d, 2H, J = 8.1 Hz, C(4,6)-H); 3.04 (s, 3H, C(10)—H).
Carbon-bound H-atoms were placed in calculated positions (C—H = 0.95–0.99 Å) and were included in the refinement in the riding model approximation, with Uiso(H) = 1.2Ueq(C). The N-bound H-atoms were located in a difference Fourier map but were refined with distance restraints N—H = 0.84 (1) and 0.90 (1) Å, and with Uiso(H) = 1.2Ueq(N).
Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007; data reduction: SAINT (Bruker, 2007; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Bruno et al., 2002); software used to prepare material for publication: publCIF (Westrip, 2010).
C10H11N3OS | F(000) = 928 |
Mr = 221.28 | Dx = 1.306 Mg m−3 |
Orthorhombic, Pbca | Cu Kα radiation, λ = 1.54178 Å |
Hall symbol: -P 2ac 2ab | Cell parameters from 9894 reflections |
a = 13.1231 (3) Å | θ = 4.6–66.6° |
b = 8.8559 (2) Å | µ = 2.38 mm−1 |
c = 19.3702 (4) Å | T = 296 K |
V = 2251.14 (9) Å3 | Plate, yellow |
Z = 8 | 0.14 × 0.13 × 0.05 mm |
Bruker CCD SMART 6000 diffractometer | 1986 independent reflections |
Radiation source: fine-focus sealed tube | 1798 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.046 |
ϕ and ω scans | θmax = 66.6°, θmin = 4.6° |
Absorption correction: multi-scan (SADABS; Bruker, 2007) | h = −15→15 |
Tmin = 0.730, Tmax = 0.898 | k = −10→10 |
22698 measured reflections | l = −22→22 |
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)] = 0.034 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.100 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.08 | w = 1/[σ2(Fo2) + (0.0559P)2 + 0.3598P] where P = (Fo2 + 2Fc2)/3 |
1986 reflections | (Δ/σ)max < 0.001 |
145 parameters | Δρmax = 0.21 e Å−3 |
0 restraints | Δρmin = −0.16 e Å−3 |
C10H11N3OS | V = 2251.14 (9) Å3 |
Mr = 221.28 | Z = 8 |
Orthorhombic, Pbca | Cu Kα radiation |
a = 13.1231 (3) Å | µ = 2.38 mm−1 |
b = 8.8559 (2) Å | T = 296 K |
c = 19.3702 (4) Å | 0.14 × 0.13 × 0.05 mm |
Bruker CCD SMART 6000 diffractometer | 1986 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2007) | 1798 reflections with I > 2σ(I) |
Tmin = 0.730, Tmax = 0.898 | Rint = 0.046 |
22698 measured reflections |
R[F2 > 2σ(F2)] = 0.034 | 0 restraints |
wR(F2) = 0.100 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.08 | Δρmax = 0.21 e Å−3 |
1986 reflections | Δρmin = −0.16 e Å−3 |
145 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 | 0.90393 (3) | 1.04683 (4) | 0.40705 (2) | 0.06222 (18) | |
O1 | 0.88220 (12) | −0.01792 (18) | 0.72752 (8) | 0.0921 (5) | |
N1 | 0.81376 (12) | 0.78044 (16) | 0.39148 (7) | 0.0655 (4) | |
C1 | 0.87314 (11) | 0.86850 (16) | 0.42864 (8) | 0.0517 (3) | |
N2 | 0.90945 (10) | 0.81086 (15) | 0.48868 (7) | 0.0579 (3) | |
C2 | 0.92328 (12) | 0.62083 (19) | 0.56504 (9) | 0.0605 (4) | |
H2 | 0.9617 | 0.6879 | 0.5913 | 0.073* | |
N3 | 0.88781 (9) | 0.66473 (14) | 0.50704 (7) | 0.0542 (3) | |
C3 | 0.90556 (11) | 0.46928 (19) | 0.59137 (8) | 0.0536 (4) | |
C4 | 0.93836 (15) | 0.43343 (19) | 0.65777 (9) | 0.0678 (4) | |
H4 | 0.9707 | 0.5066 | 0.6844 | 0.081* | |
C5 | 0.92354 (14) | 0.2913 (2) | 0.68448 (9) | 0.0675 (4) | |
H5 | 0.9454 | 0.2692 | 0.7290 | 0.081* | |
C6 | 0.87602 (11) | 0.18070 (18) | 0.64526 (8) | 0.0554 (4) | |
C7 | 0.84324 (11) | 0.21631 (18) | 0.57902 (8) | 0.0558 (4) | |
H7 | 0.8112 | 0.1429 | 0.5524 | 0.067* | |
C8 | 0.85745 (11) | 0.35836 (17) | 0.55224 (8) | 0.0543 (4) | |
H8 | 0.8349 | 0.3805 | 0.5079 | 0.065* | |
C9 | 0.86069 (14) | 0.0265 (2) | 0.67155 (10) | 0.0678 (4) | |
H9 | 0.8313 | −0.0428 | 0.6415 | 0.081* | |
C10 | 0.76953 (19) | 0.8229 (2) | 0.32581 (10) | 0.0924 (7) | |
H10A | 0.7165 | 0.8957 | 0.3332 | 0.139* | |
H10B | 0.7415 | 0.7351 | 0.3038 | 0.139* | |
H10C | 0.8213 | 0.8660 | 0.2968 | 0.139* | |
H2N | 0.9542 (15) | 0.865 (2) | 0.5138 (9) | 0.075 (5)* | |
H1 | 0.8010 (15) | 0.695 (2) | 0.4085 (9) | 0.073 (6)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0655 (3) | 0.0429 (3) | 0.0782 (3) | −0.00218 (15) | −0.01004 (18) | 0.00628 (16) |
O1 | 0.1022 (10) | 0.0890 (10) | 0.0851 (9) | 0.0013 (8) | −0.0037 (8) | 0.0320 (8) |
N1 | 0.0797 (9) | 0.0507 (8) | 0.0662 (8) | −0.0120 (7) | −0.0135 (7) | 0.0075 (6) |
C1 | 0.0458 (7) | 0.0469 (8) | 0.0622 (8) | 0.0028 (6) | 0.0023 (6) | 0.0008 (6) |
N2 | 0.0550 (7) | 0.0479 (7) | 0.0707 (8) | −0.0065 (5) | −0.0097 (6) | 0.0089 (6) |
C2 | 0.0566 (8) | 0.0555 (9) | 0.0693 (9) | −0.0066 (7) | −0.0097 (7) | 0.0047 (7) |
N3 | 0.0477 (6) | 0.0487 (7) | 0.0663 (8) | −0.0014 (5) | −0.0001 (5) | 0.0069 (6) |
C3 | 0.0468 (8) | 0.0555 (10) | 0.0585 (9) | 0.0000 (6) | −0.0032 (6) | 0.0047 (6) |
C4 | 0.0759 (11) | 0.0641 (10) | 0.0635 (9) | −0.0119 (8) | −0.0176 (8) | 0.0023 (7) |
C5 | 0.0763 (10) | 0.0707 (11) | 0.0555 (9) | −0.0044 (8) | −0.0131 (8) | 0.0106 (8) |
C6 | 0.0504 (8) | 0.0573 (9) | 0.0585 (8) | 0.0032 (6) | 0.0018 (6) | 0.0059 (7) |
C7 | 0.0539 (8) | 0.0544 (9) | 0.0590 (8) | −0.0013 (6) | −0.0037 (6) | −0.0017 (7) |
C8 | 0.0536 (8) | 0.0564 (9) | 0.0531 (7) | 0.0013 (6) | −0.0071 (6) | 0.0040 (6) |
C9 | 0.0656 (10) | 0.0653 (10) | 0.0724 (10) | 0.0035 (8) | 0.0001 (8) | 0.0122 (8) |
C10 | 0.1231 (18) | 0.0784 (12) | 0.0756 (11) | −0.0277 (12) | −0.0324 (12) | 0.0131 (10) |
S1—C1 | 1.6829 (15) | C3—C8 | 1.392 (2) |
O1—C9 | 1.187 (2) | C3—C4 | 1.393 (2) |
N1—C1 | 1.317 (2) | C4—C5 | 1.375 (2) |
N1—C10 | 1.448 (2) | C5—C6 | 1.388 (2) |
C1—N2 | 1.356 (2) | C6—C7 | 1.390 (2) |
N2—N3 | 1.3718 (18) | C6—C9 | 1.471 (2) |
C2—N3 | 1.277 (2) | C7—C8 | 1.373 (2) |
C2—C3 | 1.454 (2) | ||
C1—N1—C10 | 124.33 (15) | C4—C3—C2 | 118.99 (15) |
N1—C1—N2 | 116.98 (14) | C5—C4—C3 | 120.82 (15) |
N1—C1—S1 | 124.20 (12) | C4—C5—C6 | 120.26 (15) |
N2—C1—S1 | 118.81 (12) | C5—C6—C7 | 118.98 (15) |
C1—N2—N3 | 120.30 (13) | C5—C6—C9 | 121.80 (15) |
N3—C2—C3 | 122.09 (15) | C7—C6—C9 | 119.21 (15) |
C2—N3—N2 | 116.10 (13) | C8—C7—C6 | 120.97 (15) |
C8—C3—C4 | 118.82 (15) | C7—C8—C3 | 120.15 (14) |
C8—C3—C2 | 122.19 (14) | O1—C9—C6 | 126.24 (19) |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2N···S1i | 0.902 (19) | 2.53 (2) | 3.4154 (14) | 165.6 (16) |
N1—H1···N3 | 0.84 (2) | 2.238 (18) | 2.6467 (18) | 109.9 (15) |
N1—H1···S1ii | 0.84 (2) | 2.992 (19) | 3.5401 (15) | 124.6 (16) |
Symmetry codes: (i) −x+2, −y+2, −z+1; (ii) −x+3/2, y−1/2, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2N···S1i | 0.902 (19) | 2.53 (2) | 3.4154 (14) | 165.6 (16) |
N1—H1···N3 | 0.84 (2) | 2.238 (18) | 2.6467 (18) | 109.9 (15) |
N1—H1···S1ii | 0.84 (2) | 2.992 (19) | 3.5401 (15) | 124.6 (16) |
Symmetry codes: (i) −x+2, −y+2, −z+1; (ii) −x+3/2, y−1/2, z. |