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The tetra­hydro­pyrimidine ring of the title mol­ecule, C10H10ClN3OS, adopts a half-chair conformation. In the crystal structure, mol­ecules are linked through N—H...S hydrogen bonding, forming a one-dimensional structure.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806049439/hg2131sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806049439/hg2131Isup2.hkl
Contains datablock I

CCDC reference: 633875

Key indicators

  • Single-crystal X-ray study
  • T = 294 K
  • R factor = 0.049
  • wR factor = 0.146
  • Data-to-parameter ratio = 14.6

checkCIF/PLATON results

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No errors found in this datablock

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SMART; data reduction: SAINT (Bruker, 1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1999); software used to prepare material for publication: SHELXTL.

3-[(6-Chloropyridin-3-yl)methyl]-2-thioxo-2,3,5,6-tetrahydropyrimidin-4(1H)-one top
Crystal data top
C10H10ClN3OSF(000) = 528
Mr = 255.72Dx = 1.408 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 1449 reflections
a = 10.131 (3) Åθ = 2.5–21.0°
b = 5.7977 (14) ŵ = 0.47 mm1
c = 20.957 (5) ÅT = 294 K
β = 101.562 (4)°Needle, colorless
V = 1205.9 (5) Å30.24 × 0.20 × 0.10 mm
Z = 4
Data collection top
Bruker SMART CCD area-detector
diffractometer
2470 independent reflections
Radiation source: fine-focus sealed tube1277 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.034
φ and ω scansθmax = 26.4°, θmin = 2.0°
Absorption correction: multi-scan
(SABABS; Sheldrick, 1996)
h = 1012
Tmin = 0.895, Tmax = 0.954k = 75
6496 measured reflectionsl = 2625
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.049H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.146 w = 1/[σ2(Fo2) + (0.0614P)2 + 0.3547P]
where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max = 0.001
2470 reflectionsΔρmax = 0.25 e Å3
169 parametersΔρmin = 0.24 e Å3
8 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0031 (19)
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*/UeqOcc. (<1)
S10.98460 (10)0.3609 (2)0.09604 (4)0.0982 (5)
Cl10.36045 (11)0.4397 (2)0.24228 (5)0.1150 (5)
O10.6241 (3)0.2187 (5)0.03536 (12)0.1079 (10)
N10.8558 (3)0.2570 (5)0.02128 (13)0.0744 (9)
H1A0.901 (3)0.360 (6)0.0349 (17)0.089*
N20.7897 (2)0.0472 (4)0.06012 (11)0.0587 (7)
C10.8710 (3)0.2151 (5)0.04145 (15)0.0598 (8)
C20.7853 (12)0.116 (3)0.0759 (7)0.078 (4)0.453 (14)
H2A0.83850.01800.08250.094*0.453 (14)
H2B0.76580.20500.11590.094*0.453 (14)
C30.6566 (11)0.045 (3)0.0549 (6)0.081 (4)0.453 (14)
H3A0.60690.06310.08620.097*0.453 (14)
H3B0.60030.17890.05310.097*0.453 (14)
C2'0.7328 (13)0.1882 (16)0.0652 (5)0.078 (3)0.547 (14)
H2'A0.74330.20390.10990.093*0.547 (14)
H2'B0.65890.28620.05880.093*0.547 (14)
C3'0.7029 (13)0.0599 (16)0.0513 (5)0.075 (3)0.547 (14)
H3'A0.61860.10760.07890.090*0.547 (14)
H3'B0.77410.15940.06010.090*0.547 (14)
C40.6937 (4)0.0760 (6)0.01649 (17)0.0783 (10)
C50.7974 (3)0.0065 (5)0.12936 (14)0.0655 (9)
H5A0.88390.04460.15410.079*
H5B0.79240.17230.13450.079*
C60.6877 (3)0.1047 (5)0.15670 (12)0.0530 (7)
C70.6365 (3)0.3181 (5)0.13526 (14)0.0583 (8)
H70.66950.39360.10250.070*
C80.4871 (3)0.3105 (6)0.21018 (16)0.0674 (9)
C90.5360 (4)0.0967 (6)0.23275 (15)0.0886 (13)0.46 (3)
H90.50220.02100.26520.106*0.46 (3)
N30.5369 (3)0.4208 (5)0.16196 (16)0.0787 (12)0.46 (3)
N3'0.5360 (4)0.0967 (6)0.23275 (15)0.0886 (13)0.54 (3)
C9'0.5369 (3)0.4208 (5)0.16196 (16)0.0787 (12)0.54 (3)
H9'0.50350.56480.14730.094*0.54 (3)
C100.6369 (4)0.0019 (5)0.20568 (14)0.0653 (9)
H100.67150.14450.22100.078*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0945 (8)0.1388 (10)0.0629 (6)0.0603 (7)0.0195 (5)0.0257 (6)
Cl10.0950 (8)0.1483 (11)0.1073 (9)0.0031 (7)0.0338 (7)0.0253 (7)
O10.128 (2)0.0932 (19)0.0926 (18)0.0588 (17)0.0026 (16)0.0104 (15)
N10.071 (2)0.090 (2)0.0597 (18)0.0285 (15)0.0065 (14)0.0017 (15)
N20.0577 (15)0.0571 (15)0.0563 (15)0.0085 (12)0.0004 (12)0.0024 (12)
C10.0474 (17)0.070 (2)0.062 (2)0.0046 (15)0.0095 (15)0.0073 (16)
C20.060 (8)0.100 (8)0.070 (6)0.006 (6)0.002 (6)0.016 (6)
C30.084 (7)0.095 (8)0.054 (5)0.024 (6)0.007 (5)0.001 (6)
C2'0.054 (6)0.124 (9)0.049 (5)0.023 (5)0.004 (4)0.017 (5)
C3'0.074 (6)0.078 (6)0.067 (5)0.017 (5)0.000 (5)0.012 (5)
C40.083 (3)0.075 (2)0.072 (2)0.026 (2)0.0047 (19)0.0051 (19)
C50.068 (2)0.0597 (19)0.0608 (19)0.0009 (15)0.0055 (16)0.0143 (15)
C60.0631 (19)0.0440 (16)0.0441 (16)0.0130 (14)0.0083 (14)0.0066 (13)
C70.0612 (19)0.0519 (18)0.0601 (18)0.0095 (15)0.0078 (16)0.0152 (15)
C80.068 (2)0.072 (2)0.059 (2)0.0141 (17)0.0050 (17)0.0110 (17)
C90.108 (3)0.096 (3)0.059 (2)0.030 (2)0.0106 (19)0.0004 (19)
N30.076 (2)0.071 (2)0.081 (2)0.0124 (17)0.0027 (18)0.0050 (17)
N3'0.108 (3)0.096 (3)0.059 (2)0.030 (2)0.0106 (19)0.0004 (19)
C9'0.076 (2)0.071 (2)0.081 (2)0.0124 (17)0.0027 (18)0.0050 (17)
C100.090 (2)0.0513 (18)0.0477 (17)0.0117 (17)0.0032 (17)0.0074 (15)
Geometric parameters (Å, º) top
S1—C11.679 (3)C2'—H2'A0.9700
Cl1—C81.734 (4)C2'—H2'B0.9700
O1—C41.204 (4)C3'—C41.445 (11)
N1—C11.315 (4)C3'—H3'A0.9700
N1—C2'1.449 (11)C3'—H3'B0.9700
N1—C21.472 (14)C5—C61.495 (4)
N1—H1A0.83 (3)C5—H5A0.9700
N2—C11.381 (4)C5—H5B0.9700
N2—C41.391 (4)C6—C71.381 (4)
N2—C51.471 (4)C6—C101.383 (4)
C2—C31.515 (9)C7—N31.383 (4)
C2—H2A0.9700C7—H70.9300
C2—H2B0.9700C8—N31.374 (4)
C3—C41.626 (14)C8—C91.382 (5)
C3—H3A0.9700C9—C101.388 (5)
C3—H3B0.9700C9—H90.9300
C2'—C3'1.510 (8)C10—H100.9300
C1—N1—C2'119.8 (5)C2'—C3'—H3'A110.1
C1—N1—C2128.1 (6)C4—C3'—H3'B110.1
C2'—N1—C229.6 (4)C2'—C3'—H3'B110.1
C1—N1—H1A121 (2)H3'A—C3'—H3'B108.5
C2'—N1—H1A116 (2)O1—C4—N2121.0 (3)
C2—N1—H1A110 (2)O1—C4—C3'121.6 (4)
C1—N2—C4123.6 (3)N2—C4—C3'116.0 (5)
C1—N2—C5120.8 (2)O1—C4—C3123.7 (5)
C4—N2—C5115.6 (3)N2—C4—C3112.7 (6)
N1—C1—N2117.2 (3)C3'—C4—C327.9 (5)
N1—C1—S1121.0 (2)N2—C5—C6113.0 (2)
N2—C1—S1121.9 (2)N2—C5—H5A109.0
N1—C2—C3103.7 (10)C6—C5—H5A109.0
N1—C2—H2A111.0N2—C5—H5B109.0
C3—C2—H2A111.0C6—C5—H5B109.0
N1—C2—H2B111.0H5A—C5—H5B107.8
C3—C2—H2B111.0C7—C6—C10118.1 (3)
H2A—C2—H2B109.0C7—C6—C5121.4 (3)
C2—C3—C4109.3 (10)C10—C6—C5120.5 (3)
C2—C3—H3A109.8C6—C7—N3120.7 (3)
C4—C3—H3A109.8C6—C7—H7119.7
C2—C3—H3B109.8N3—C7—H7119.7
C4—C3—H3B109.8N3—C8—C9120.7 (3)
H3A—C3—H3B108.3N3—C8—Cl1119.5 (3)
N1—C2'—C3'108.7 (8)C9—C8—Cl1119.8 (3)
N1—C2'—H2'A109.9C8—C9—C10118.2 (3)
C3'—C2'—H2'A109.9C8—C9—H9120.9
N1—C2'—H2'B109.9C10—C9—H9120.9
C3'—C2'—H2'B109.9C8—N3—C7120.1 (3)
H2'A—C2'—H2'B108.3C6—C10—C9122.3 (3)
C4—C3'—C2'107.8 (8)C6—C10—H10118.9
C4—C3'—H3'A110.1C9—C10—H10118.9
C2'—N1—C1—N219.7 (7)C2'—C3'—C4—O1151.2 (8)
C2—N1—C1—N214.8 (9)C2'—C3'—C4—N241.8 (13)
C2'—N1—C1—S1160.2 (6)C2'—C3'—C4—C348.0 (11)
C2—N1—C1—S1165.3 (7)C2—C3—C4—O1152.1 (11)
C4—N2—C1—N10.5 (5)C2—C3—C4—N245.9 (15)
C5—N2—C1—N1178.4 (3)C2—C3—C4—C3'57.1 (13)
C4—N2—C1—S1179.4 (2)C1—N2—C5—C699.9 (3)
C5—N2—C1—S11.6 (4)C4—N2—C5—C678.1 (3)
C1—N1—C2—C343.7 (17)N2—C5—C6—C733.4 (4)
C2'—N1—C2—C340.5 (12)N2—C5—C6—C10148.3 (3)
N1—C2—C3—C453.7 (17)C10—C6—C7—N30.3 (4)
C1—N1—C2'—C3'49.0 (13)C5—C6—C7—N3178.7 (3)
C2—N1—C2'—C3'66.6 (16)N3—C8—C9—C100.4 (4)
N1—C2'—C3'—C457.3 (15)Cl1—C8—C9—C10179.7 (2)
C1—N2—C4—O1179.0 (3)C9—C8—N3—C70.2 (5)
C5—N2—C4—O11.0 (5)Cl1—C8—N3—C7179.1 (2)
C1—N2—C4—C3'14.0 (7)C6—C7—N3—C80.3 (4)
C5—N2—C4—C3'168.1 (6)C7—C6—C10—C91.0 (4)
C1—N2—C4—C316.5 (7)C5—C6—C10—C9179.4 (3)
C5—N2—C4—C3161.5 (6)C8—C9—C10—C61.0 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···S1i0.83 (3)2.49 (3)3.315 (3)169 (3)
Symmetry code: (i) x+2, y+1, z.
 

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