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The title compound {alternatively, 3-methyl-2-[oxido(oxo)hydrazono]-2,3-dihydro-1,3-thiazole}, C
4H
5N
3O
2S, was obtained by methylation of
N-(2-thiazolyl)nitramine. The molecule lies on a mirror plane and the thiazole ring is planar, regular in shape and aromatic. The S atom participates in the aromatic sextet
via an electron pair on the 3
pz orbital. In the crystal, the molecules are arranged in parallel layers, bound to each other by weak C—H
O and C—H
N hydrogen bonds and by S
O dipolar interactions, with an interlayer separation of 3.23 Å.
Supporting information
CCDC reference: 153923
Cell refinement: Kuma Diffraction Software (Kuma, 1997); data reduction: Kuma Diffraction Software; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Sheldrick, 1990); software used to prepare material for publication: SHELXL97.
2,3-Dihydro-3-methyl-2-nitriminothiazole
top
Crystal data top
C4H5N3O2S | F(000) = 164 |
Mr = 159.17 | Dx = 1.679 Mg m−3 |
Monoclinic, P21/m | Mo Kα radiation, λ = 0.71073 Å |
a = 6.947 (2) Å | Cell parameters from 27 reflections |
b = 6.469 (3) Å | θ = 9–14° |
c = 7.478 (3) Å | µ = 0.45 mm−1 |
β = 110.51 (3)° | T = 295 K |
V = 314.8 (2) Å3 | Translucent, light orange |
Z = 2 | 0.7 × 0.5 × 0.5 mm |
Data collection top
Kuma KM4 diffractometer | Rint = 0.031 |
Radiation source: fine-focus sealed tube | θmax = 30.1°, θmin = 2.9° |
Graphite monochromator | h = −9→9 |
ω scans | k = −9→0 |
1958 measured reflections | l = −9→10 |
994 independent reflections | 2 standard reflections every 50 reflections |
940 reflections with I > 2σ(I) | intensity decay: 0.3% |
Refinement top
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) = 0.097 | All H-atom parameters refined |
S = 1.11 | Calculated w = 1/[σ2(Fo2) + (0.0563P)2 + 0.0468P] where P = (Fo2 + 2Fc2)/3 |
994 reflections | (Δ/σ)max < 0.001 |
74 parameters | Δρmax = 0.44 e Å−3 |
0 restraints | Δρmin = −0.26 e Å−3 |
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 | x | y | z | Uiso*/Ueq | |
S1 | 0.15659 (6) | 1/4 | 0.01599 (5) | 0.03453 (17) | |
C2 | 0.3189 (2) | 1/4 | −0.11204 (19) | 0.0265 (3) | |
N3 | 0.2129 (2) | 1/4 | −0.30017 (17) | 0.0305 (3) | |
C4 | 0.0023 (3) | 1/4 | −0.3449 (2) | 0.0374 (4) | |
C5 | −0.0536 (3) | 1/4 | −0.1916 (3) | 0.0402 (4) | |
N6 | 0.5259 (2) | 1/4 | −0.05619 (18) | 0.0299 (3) | |
N7 | 0.6240 (2) | 1/4 | 0.13224 (17) | 0.0306 (3) | |
O9 | 0.5327 (2) | 1/4 | 0.24842 (17) | 0.0425 (3) | |
O8 | 0.81546 (19) | 1/4 | 0.18608 (19) | 0.0466 (4) | |
C31 | 0.3109 (3) | 1/4 | −0.4439 (2) | 0.0427 (4) | |
H4 | −0.078 (4) | 1/4 | −0.471 (4) | 0.044 (6)* | |
H5 | −0.191 (4) | 1/4 | −0.199 (3) | 0.040 (6)* | |
H31A | 0.214 (5) | 1/4 | −0.557 (4) | 0.069 (9)* | |
H31B | 0.402 (2) | 0.140 (3) | −0.421 (2) | 0.056 (5)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
S1 | 0.0291 (2) | 0.0483 (3) | 0.0284 (2) | 0 | 0.01276 (18) | 0 |
C2 | 0.0257 (6) | 0.0296 (6) | 0.0235 (6) | 0 | 0.0079 (5) | 0 |
N3 | 0.0273 (6) | 0.0402 (7) | 0.0224 (5) | 0 | 0.0068 (5) | 0 |
C4 | 0.0276 (7) | 0.0478 (9) | 0.0316 (7) | 0 | 0.0037 (6) | 0 |
C5 | 0.0250 (7) | 0.0539 (10) | 0.0398 (8) | 0 | 0.0090 (6) | 0 |
N6 | 0.0258 (6) | 0.0388 (7) | 0.0239 (6) | 0 | 0.0073 (5) | 0 |
N7 | 0.0289 (6) | 0.0346 (6) | 0.0252 (5) | 0 | 0.0056 (5) | 0 |
O9 | 0.0385 (6) | 0.0632 (8) | 0.0255 (5) | 0 | 0.0108 (5) | 0 |
O8 | 0.0262 (6) | 0.0709 (10) | 0.0361 (6) | 0 | 0.0026 (5) | 0 |
C31 | 0.0411 (9) | 0.0632 (12) | 0.0258 (7) | 0 | 0.0142 (7) | 0 |
Geometric parameters (Å, º) top
S1—C2 | 1.716 (2) | N3—C31 | 1.460 (2) |
S1—C5 | 1.718 (2) | C4—C5 | 1.333 (2) |
C2—N3 | 1.340 (2) | N6—N7 | 1.333 (2) |
C2—N6 | 1.349 (2) | N7—O9 | 1.242 (2) |
N3—C4 | 1.382 (2) | N7—O8 | 1.247 (2) |
| | | |
C2—S1—C5 | 90.7 (1) | C5—C4—N3 | 113.2 (1) |
N3—C2—N6 | 117.3 (1) | C4—C5—S1 | 111.5 (1) |
N3—C2—S1 | 111.0 (1) | N7—N6—C2 | 115.0 (1) |
N6—C2—S1 | 131.6 (1) | O9—N7—O8 | 121.5 (1) |
C2—N3—C4 | 113.6 (1) | O9—N7—N6 | 122.8 (1) |
C2—N3—C31 | 123.1 (1) | O8—N7—N6 | 115.7 (1) |
C4—N3—C31 | 123.3 (1) | | |
| | | |
C5—S1—C2—N3 | 0.0 | C31—N3—C4—C5 | 180.0 |
C5—S1—C2—N6 | 180.0 | N3—C4—C5—S1 | 0.0 |
N6—C2—N3—C4 | 180.0 | C2—S1—C5—C4 | 0.0 |
S1—C2—N3—C4 | 0.0 | N3—C2—N6—N7 | 180.0 |
N6—C2—N3—C31 | 0.0 | S1—C2—N6—N7 | 0.0 |
S1—C2—N3—C31 | 180.0 | C2—N6—N7—O9 | 0.0 |
C2—N3—C4—C5 | 0.0 | C2—N6—N7—O8 | 180.0 |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
C4—H4···O8i | 0.91 (3) | 2.41 (3) | 3.286 (3) | 162 (2) |
C5—H5···N6ii | 0.94 (2) | 2.55 (2) | 3.411 (2) | 154 (2) |
Symmetry codes: (i) x−1, y, z−1; (ii) x−1, y, z. |
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