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The title compound, C13H10Cl2N2OS, was synthesized by mixing 2,4-di­chloro­benz­aldehyde, ethyl chloro­acetate and tetra­hydro­pyrimidine-2-thione in ethanol. The nearly planar thia­zoline ring is fused to a di­hydro­pyrimidine ring, which has a sofa conformation. The mol­ecules are connected through weak C—H...N, C—H...O and C—H...Cl interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680401654X/lh6239sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680401654X/lh6239Isup2.hkl
Contains datablock I

CCDC reference: 248797

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.038
  • wR factor = 0.094
  • Data-to-parameter ratio = 16.5

checkCIF/PLATON results

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No errors found in this datablock

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SMART; data reduction: SAINT (Bruker, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL.

(2E)-2-(2,4-Dichlorobenzylidene)-6,7-dihydro-2H-thiazolo[3,2-a]pyrimidin- 3(5H)-one top
Crystal data top
C13H10Cl2N2OSF(000) = 640
Mr = 313.19Dx = 1.555 Mg m3
Monoclinic, P21/cMelting point = 437–439 K
Hall symbol: -P 2ybcMo Kα radiation, λ = 0.71073 Å
a = 6.155 (2) ÅCell parameters from 791 reflections
b = 9.676 (4) Åθ = 3.6–26.5°
c = 22.507 (8) ŵ = 0.63 mm1
β = 93.543 (6)°T = 293 K
V = 1337.8 (8) Å3Block cut from needle, yellow
Z = 40.28 × 0.26 × 0.20 mm
Data collection top
Bruker SMART CCD
diffractometer
2841 independent reflections
Radiation source: fine-focus sealed tube2191 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.025
φ and ω scansθmax = 26.8°, θmin = 2.3°
Absorption correction: multi-scan
(SADABS; Bruker, 1997)
h = 77
Tmin = 0.820, Tmax = 0.881k = 1212
7749 measured reflectionsl = 1928
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.038 w = 1/[σ2(Fo2) + (0.0406P)2 + 0.4345P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.094(Δ/σ)max = 0.001
S = 1.06Δρmax = 0.27 e Å3
2841 reflectionsΔρmin = 0.20 e Å3
172 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
S10.14843 (10)0.52038 (6)0.40692 (2)0.04772 (18)
Cl10.90193 (10)0.15696 (7)0.41912 (3)0.0606 (2)
Cl20.59274 (12)0.05369 (7)0.63163 (3)0.0621 (2)
O10.5557 (3)0.48827 (17)0.28452 (7)0.0524 (4)
N10.2437 (3)0.60413 (17)0.30181 (7)0.0368 (4)
N20.0659 (3)0.7099 (2)0.34152 (9)0.0546 (5)
C10.2246 (4)0.6814 (2)0.24558 (9)0.0463 (5)
H1A0.27100.62400.21340.056*
H1B0.31690.76260.24840.056*
C20.0101 (4)0.7238 (3)0.23335 (11)0.0596 (7)
H2A0.02060.78720.19990.072*
H2B0.09670.64280.22250.072*
C30.1002 (4)0.7918 (3)0.28650 (11)0.0602 (7)
H3A0.03170.88140.29250.072*
H3B0.25510.80690.27850.072*
C40.0911 (3)0.6272 (2)0.34402 (9)0.0398 (5)
C50.4093 (3)0.5144 (2)0.31655 (9)0.0374 (5)
C60.3828 (3)0.4527 (2)0.37687 (9)0.0373 (5)
C70.5269 (4)0.3603 (2)0.39918 (9)0.0421 (5)
H70.63820.33960.37450.051*
C80.5390 (3)0.2865 (2)0.45577 (9)0.0392 (5)
C90.3883 (4)0.3042 (3)0.49957 (10)0.0513 (6)
H90.27460.36640.49230.062*
C100.4019 (4)0.2333 (3)0.55293 (10)0.0521 (6)
H100.29860.24700.58080.063*
C110.5701 (4)0.1424 (2)0.56408 (9)0.0443 (5)
C120.7249 (4)0.1199 (2)0.52314 (9)0.0464 (5)
H120.83880.05830.53120.056*
C130.7056 (3)0.1916 (2)0.46989 (9)0.0399 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0500 (3)0.0536 (4)0.0407 (3)0.0148 (3)0.0116 (2)0.0127 (3)
Cl10.0598 (4)0.0708 (4)0.0525 (4)0.0284 (3)0.0149 (3)0.0150 (3)
Cl20.0798 (5)0.0653 (4)0.0408 (3)0.0008 (3)0.0004 (3)0.0166 (3)
O10.0554 (10)0.0594 (10)0.0437 (9)0.0180 (8)0.0137 (7)0.0023 (8)
N10.0424 (10)0.0371 (9)0.0310 (9)0.0043 (8)0.0045 (7)0.0040 (7)
N20.0526 (12)0.0621 (13)0.0501 (12)0.0193 (10)0.0114 (9)0.0140 (10)
C10.0566 (14)0.0450 (13)0.0377 (12)0.0065 (11)0.0073 (10)0.0101 (10)
C20.0679 (17)0.0675 (17)0.0426 (13)0.0175 (14)0.0022 (12)0.0132 (12)
C30.0603 (16)0.0649 (17)0.0556 (15)0.0247 (13)0.0054 (12)0.0191 (13)
C40.0430 (12)0.0403 (12)0.0365 (11)0.0037 (9)0.0052 (9)0.0066 (9)
C50.0440 (12)0.0346 (11)0.0334 (11)0.0024 (9)0.0015 (9)0.0039 (8)
C60.0437 (12)0.0364 (11)0.0317 (10)0.0040 (9)0.0021 (8)0.0021 (8)
C70.0475 (13)0.0441 (12)0.0348 (11)0.0084 (10)0.0021 (9)0.0022 (9)
C80.0440 (12)0.0407 (12)0.0325 (11)0.0068 (10)0.0015 (8)0.0013 (9)
C90.0527 (14)0.0611 (15)0.0400 (12)0.0203 (12)0.0028 (10)0.0045 (11)
C100.0582 (15)0.0619 (16)0.0370 (12)0.0090 (12)0.0095 (10)0.0007 (11)
C110.0582 (14)0.0434 (12)0.0306 (11)0.0022 (11)0.0015 (9)0.0039 (9)
C120.0543 (14)0.0435 (13)0.0408 (12)0.0125 (10)0.0026 (10)0.0056 (10)
C130.0437 (12)0.0416 (12)0.0345 (11)0.0059 (9)0.0024 (9)0.0002 (9)
Geometric parameters (Å, º) top
S1—C61.757 (2)C3—H3A0.9700
S1—C41.771 (2)C3—H3B0.9700
Cl1—C131.746 (2)C5—C61.501 (3)
Cl2—C111.744 (2)C6—C71.336 (3)
O1—C51.215 (2)C7—C81.458 (3)
N1—C51.364 (3)C7—H70.9300
N1—C41.395 (3)C8—C131.398 (3)
N1—C11.468 (3)C8—C91.405 (3)
N2—C41.253 (3)C9—C101.381 (3)
N2—C31.474 (3)C9—H90.9300
C1—C21.511 (3)C10—C111.370 (3)
C1—H1A0.9700C10—H100.9300
C1—H1B0.9700C11—C121.383 (3)
C2—C31.501 (3)C12—C131.383 (3)
C2—H2A0.9700C12—H120.9300
C2—H2B0.9700
C6—S1—C492.16 (10)O1—C5—C6125.44 (19)
C5—N1—C4117.44 (17)N1—C5—C6110.60 (17)
C5—N1—C1123.53 (17)C7—C6—C5119.97 (19)
C4—N1—C1118.96 (17)C7—C6—S1130.31 (17)
C4—N2—C3116.79 (19)C5—C6—S1109.72 (14)
N1—C1—C2108.66 (18)C6—C7—C8130.8 (2)
N1—C1—H1A110.0C6—C7—H7114.6
C2—C1—H1A110.0C8—C7—H7114.6
N1—C1—H1B110.0C13—C8—C9115.29 (19)
C2—C1—H1B110.0C13—C8—C7121.14 (19)
H1A—C1—H1B108.3C9—C8—C7123.56 (19)
C3—C2—C1111.7 (2)C10—C9—C8122.9 (2)
C3—C2—H2A109.3C10—C9—H9118.6
C1—C2—H2A109.3C8—C9—H9118.6
C3—C2—H2B109.3C11—C10—C9118.8 (2)
C1—C2—H2B109.3C11—C10—H10120.6
H2A—C2—H2B107.9C9—C10—H10120.6
N2—C3—C2113.1 (2)C10—C11—C12121.5 (2)
N2—C3—H3A109.0C10—C11—Cl2119.62 (17)
C2—C3—H3A109.0C12—C11—Cl2118.84 (17)
N2—C3—H3B109.0C11—C12—C13118.2 (2)
C2—C3—H3B109.0C11—C12—H12120.9
H3A—C3—H3B107.8C13—C12—H12120.9
N2—C4—N1128.45 (19)C12—C13—C8123.25 (19)
N2—C4—S1121.57 (16)C12—C13—Cl1116.43 (16)
N1—C4—S1109.98 (15)C8—C13—Cl1120.31 (16)
O1—C5—N1123.96 (19)
C5—N1—C1—C2158.0 (2)N1—C5—C6—S10.6 (2)
C4—N1—C1—C225.0 (3)C4—S1—C6—C7179.3 (2)
N1—C1—C2—C349.8 (3)C4—S1—C6—C51.09 (16)
C4—N2—C3—C225.2 (3)C5—C6—C7—C8179.7 (2)
C1—C2—C3—N251.7 (3)S1—C6—C7—C80.7 (4)
C3—N2—C4—N11.8 (4)C6—C7—C8—C13179.3 (2)
C3—N2—C4—S1178.95 (18)C6—C7—C8—C90.8 (4)
C5—N1—C4—N2175.8 (2)C13—C8—C9—C100.1 (4)
C1—N1—C4—N21.4 (4)C7—C8—C9—C10179.9 (2)
C5—N1—C4—S13.6 (2)C8—C9—C10—C110.5 (4)
C1—N1—C4—S1179.28 (16)C9—C10—C11—C120.3 (4)
C6—S1—C4—N2176.9 (2)C9—C10—C11—Cl2179.04 (19)
C6—S1—C4—N12.52 (16)C10—C11—C12—C130.3 (4)
C4—N1—C5—O1177.9 (2)Cl2—C11—C12—C13179.63 (17)
C1—N1—C5—O10.9 (3)C11—C12—C13—C80.7 (3)
C4—N1—C5—C62.7 (3)C11—C12—C13—Cl1178.75 (17)
C1—N1—C5—C6179.77 (18)C9—C8—C13—C120.5 (3)
O1—C5—C6—C70.4 (3)C7—C8—C13—C12179.5 (2)
N1—C5—C6—C7179.00 (19)C9—C8—C13—Cl1178.93 (17)
O1—C5—C6—S1179.99 (19)C7—C8—C13—Cl11.1 (3)
 

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