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The title compound, C6H7N3S, crystallizes with two essentially planar mol­ecules in the asymmetric unit (r.m.s. deviation for all non-H atoms = 0.055 and 0.006 Å), which are held together by two N—H...S hydrogen bonds. The two mol­ecules are almost identical (r.m.s. deviation for all non-H atoms = 0.066 Å). An intra­molecular N—H...N hydrogen bond stabilizes the synperiplanar conformations between the pyridine N atom and the thio­carbonyl C atom, as well as between the pivot C atom of the pyridine ring and the NH2 group [torsion angles: N—C—N—C = 7.3 (3) and −1.0 (3)°, C—N—C—N = −4.1 (3) and −0.4 (3)°].

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807057388/at2476sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807057388/at2476Isup2.hkl
Contains datablock I

CCDC reference: 672921

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](C-C)= 0.003 Å
  • R factor = 0.035
  • wR factor = 0.091
  • Data-to-parameter ratio = 13.1

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Comment top

1-(Pyridin-2-yl)thiourea crystallizes with two essentially planar molecules in the asymmetric unit (r.m.s. deviation for all non-H atoms 0.055 Å and 0.006 Å), which are held together by two N—H···S hydrogen bonds. The two molecules are almost identical (r.m.s. deviation for all non-H atoms 0.066 Å). An intramolecular N—H···N hydrogen bond stabilizes the syn-periplanar conformations between the pyridine N atom and the thiocarbonyl C atom, as well as between the C6 atom and the NH2 group [torsion angle N1—C6—N61—C62: 7.3 (3)°, N1'—C6'—N61'—C62': -1.0 (3)°, C6—N61—C62—N63: -4.1 (3)°, C6'—N61'—C62'—N63': -0.4 (3)°]. The crystal packing shows a network of intermolecular N—H···S hydrogen bonds resulting in corrugated layers.

Related literature top

At least one reference must be provided, to put the work in context.

Experimental top

Single crystals of title compound were obtained from recrystallization of the commercially available 1-(pPyridin-2-yl)thiourea from acetonitril at room temperature.

Refinement top

All H atoms were initially located by difference Fourier synthesis. Subsequently the positions of those bonded to C atoms were idealized and constrained to ride on their parent atoms with C—H = 0.95 Å and fixed individual displacement parameters [Uiso(H) = 1.2 Ueq(C)]. H atoms bonded to N were refined isotropically.

Computing details top

Data collection: X-AREA (Stoe & Cie, 2001); cell refinement: X-AREA (Stoe & Cie, 2001); data reduction: X-AREA (Stoe & Cie, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in SHELXTL-Plus (Sheldrick, 1991); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).

Figures top
[Figure 1] Fig. 1. Perspective view of the title compound with the atom numbering; displacement ellipsoids are at the 50% probability level. Hydrogen bonds shown as dashed lines.
[Figure 2] Fig. 2. Partial packing diagram of the title compound. Hydrogen bonds are shown as dashed lines.
1-(Pyridin-2-yl)thiourea top
Crystal data top
C6H7N3SF(000) = 640
Mr = 153.21Dx = 1.403 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 11901 reflections
a = 14.0116 (13) Åθ = 3.5–25.9°
b = 6.1820 (4) ŵ = 0.37 mm1
c = 16.8726 (15) ÅT = 173 K
β = 97.140 (7)°Block, colourless
V = 1450.2 (2) Å30.52 × 0.40 × 0.28 mm
Z = 8
Data collection top
Stoe IPDS II two-circle
diffractometer
2700 independent reflections
Radiation source: fine-focus sealed tube2307 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.075
ω scansθmax = 25.6°, θmin = 3.5°
Absorption correction: multi-scan
[MULABS (Spek, 2003; Blessing, 1995)]
h = 1615
Tmin = 0.832, Tmax = 0.904k = 77
11661 measured reflectionsl = 2020
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)] = 0.035H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.091 w = 1/[σ2(Fo2) + (0.0536P)2 + 0.3005P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.001
2700 reflectionsΔρmax = 0.25 e Å3
206 parametersΔρmin = 0.21 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.019 (2)
Crystal data top
C6H7N3SV = 1450.2 (2) Å3
Mr = 153.21Z = 8
Monoclinic, P21/cMo Kα radiation
a = 14.0116 (13) ŵ = 0.37 mm1
b = 6.1820 (4) ÅT = 173 K
c = 16.8726 (15) Å0.52 × 0.40 × 0.28 mm
β = 97.140 (7)°
Data collection top
Stoe IPDS II two-circle
diffractometer
2700 independent reflections
Absorption correction: multi-scan
[MULABS (Spek, 2003; Blessing, 1995)]
2307 reflections with I > 2σ(I)
Tmin = 0.832, Tmax = 0.904Rint = 0.075
11661 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0350 restraints
wR(F2) = 0.091H atoms treated by a mixture of independent and constrained refinement
S = 1.03Δρmax = 0.25 e Å3
2700 reflectionsΔρmin = 0.21 e Å3
206 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
N10.13558 (11)0.0118 (2)0.67619 (8)0.0223 (3)
C20.12387 (15)0.1750 (3)0.71483 (11)0.0267 (4)
H20.17490.22260.75330.032*
C30.04226 (14)0.3015 (3)0.70201 (10)0.0256 (4)
H30.03750.43260.73060.031*
C40.03333 (14)0.2315 (3)0.64587 (10)0.0236 (4)
H40.09080.31400.63590.028*
C50.02313 (13)0.0402 (3)0.60495 (10)0.0210 (4)
H50.07350.01190.56680.025*
C60.06331 (13)0.0744 (2)0.62123 (9)0.0175 (3)
N610.07537 (11)0.2636 (2)0.57712 (8)0.0188 (3)
H610.0270 (16)0.303 (3)0.5476 (12)0.024 (5)*
C620.15552 (12)0.3890 (3)0.57543 (9)0.0169 (3)
S620.15173 (3)0.59971 (7)0.50991 (2)0.02136 (15)
N630.23412 (11)0.3401 (3)0.62421 (9)0.0239 (3)
H63A0.2874 (18)0.420 (4)0.6260 (13)0.034 (6)*
H63B0.2320 (16)0.220 (3)0.6586 (13)0.034 (6)*
N1'0.40042 (12)1.2425 (2)0.49260 (9)0.0287 (4)
C2'0.39561 (15)1.3748 (3)0.42865 (12)0.0338 (5)
H2'0.43041.50700.43420.041*
C3'0.34342 (15)1.3303 (3)0.35574 (11)0.0333 (5)
H3'0.34151.42960.31260.040*
C4'0.29375 (15)1.1354 (3)0.34738 (11)0.0323 (5)
H4'0.25801.09830.29770.039*
C5'0.29658 (14)0.9956 (3)0.41174 (10)0.0267 (4)
H5'0.26260.86240.40740.032*
C6'0.35137 (12)1.0571 (3)0.48370 (10)0.0212 (4)
N61'0.35356 (11)0.9141 (2)0.54900 (9)0.0220 (3)
H61'0.3152 (16)0.804 (4)0.5417 (12)0.027 (5)*
C62'0.40118 (12)0.9316 (3)0.62462 (10)0.0206 (4)
S62'0.38933 (3)0.72820 (7)0.69093 (3)0.02639 (16)
N63'0.45425 (12)1.1059 (3)0.64362 (11)0.0290 (4)
H63C0.4538 (17)1.207 (4)0.6090 (14)0.035 (6)*
H63D0.485 (2)1.118 (4)0.6931 (16)0.046 (7)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0221 (8)0.0209 (7)0.0232 (7)0.0018 (6)0.0004 (6)0.0045 (6)
C20.0319 (10)0.0243 (9)0.0239 (9)0.0054 (8)0.0037 (7)0.0066 (7)
C30.0371 (11)0.0168 (8)0.0251 (9)0.0022 (8)0.0121 (8)0.0025 (7)
C40.0315 (10)0.0180 (8)0.0227 (9)0.0058 (7)0.0081 (7)0.0030 (6)
C50.0245 (9)0.0188 (8)0.0193 (8)0.0015 (7)0.0010 (7)0.0018 (6)
C60.0216 (9)0.0150 (8)0.0162 (7)0.0006 (7)0.0037 (6)0.0015 (6)
N610.0175 (8)0.0182 (7)0.0193 (7)0.0014 (6)0.0032 (6)0.0032 (5)
C620.0174 (8)0.0173 (8)0.0162 (7)0.0003 (6)0.0025 (6)0.0026 (6)
S620.0198 (2)0.0209 (2)0.0225 (2)0.00443 (16)0.00109 (17)0.00586 (15)
N630.0179 (8)0.0251 (8)0.0271 (8)0.0034 (7)0.0033 (6)0.0059 (6)
N1'0.0265 (9)0.0281 (8)0.0306 (8)0.0096 (7)0.0003 (7)0.0047 (6)
C2'0.0342 (12)0.0292 (10)0.0387 (11)0.0077 (9)0.0071 (9)0.0089 (8)
C3'0.0351 (11)0.0375 (11)0.0286 (10)0.0005 (9)0.0093 (8)0.0122 (8)
C4'0.0351 (11)0.0404 (11)0.0207 (9)0.0017 (9)0.0006 (8)0.0043 (8)
C5'0.0269 (10)0.0306 (10)0.0221 (9)0.0069 (8)0.0008 (7)0.0022 (7)
C6'0.0161 (9)0.0249 (9)0.0225 (9)0.0026 (7)0.0019 (7)0.0019 (7)
N61'0.0216 (8)0.0226 (8)0.0204 (7)0.0082 (6)0.0035 (6)0.0023 (6)
C62'0.0146 (8)0.0248 (9)0.0213 (8)0.0007 (7)0.0014 (6)0.0012 (6)
S62'0.0258 (3)0.0291 (3)0.0218 (2)0.00563 (19)0.00690 (18)0.00572 (17)
N63'0.0285 (9)0.0294 (9)0.0261 (8)0.0099 (7)0.0089 (7)0.0028 (7)
Geometric parameters (Å, º) top
N1—C61.342 (2)N1'—C6'1.335 (2)
N1—C21.346 (2)N1'—C2'1.349 (2)
C2—C31.380 (3)C2'—C3'1.379 (3)
C2—H20.9500C2'—H2'0.9500
C3—C41.399 (3)C3'—C4'1.390 (3)
C3—H30.9500C3'—H3'0.9500
C4—C51.386 (2)C4'—C5'1.385 (3)
C4—H40.9500C4'—H4'0.9500
C5—C61.401 (2)C5'—C6'1.406 (2)
C5—H50.9500C5'—H5'0.9500
C6—N611.408 (2)C6'—N61'1.410 (2)
N61—C621.368 (2)N61'—C62'1.369 (2)
N61—H610.83 (2)N61'—H61'0.87 (2)
C62—N631.325 (2)C62'—N63'1.326 (2)
C62—S621.7051 (16)C62'—S62'1.7047 (18)
N63—H63A0.89 (3)N63'—H63C0.86 (2)
N63—H63B0.95 (2)N63'—H63D0.89 (3)
C6—N1—C2117.08 (15)C6'—N1'—C2'117.17 (16)
N1—C2—C3123.97 (17)N1'—C2'—C3'124.12 (18)
N1—C2—H2118.0N1'—C2'—H2'117.9
C3—C2—H2118.0C3'—C2'—H2'117.9
C2—C3—C4118.29 (16)C2'—C3'—C4'117.84 (17)
C2—C3—H3120.9C2'—C3'—H3'121.1
C4—C3—H3120.9C4'—C3'—H3'121.1
C5—C4—C3119.01 (17)C5'—C4'—C3'119.77 (18)
C5—C4—H4120.5C5'—C4'—H4'120.1
C3—C4—H4120.5C3'—C4'—H4'120.1
C4—C5—C6118.31 (16)C4'—C5'—C6'117.90 (17)
C4—C5—H5120.8C4'—C5'—H5'121.1
C6—C5—H5120.8C6'—C5'—H5'121.1
N1—C6—C5123.31 (15)N1'—C6'—C5'123.19 (16)
N1—C6—N61118.37 (15)N1'—C6'—N61'119.29 (15)
C5—C6—N61118.32 (15)C5'—C6'—N61'117.52 (15)
C62—N61—C6129.40 (15)C62'—N61'—C6'129.79 (15)
C62—N61—H61115.7 (15)C62'—N61'—H61'114.5 (14)
C6—N61—H61114.9 (15)C6'—N61'—H61'115.4 (14)
N63—C62—N61118.61 (15)N63'—C62'—N61'118.90 (16)
N63—C62—S62122.24 (13)N63'—C62'—S62'122.56 (14)
N61—C62—S62119.14 (12)N61'—C62'—S62'118.55 (13)
C62—N63—H63A121.6 (14)C62'—N63'—H63C118.2 (15)
C62—N63—H63B118.2 (14)C62'—N63'—H63D118.9 (16)
H63A—N63—H63B120.2 (19)H63C—N63'—H63D123 (2)
C6—N1—C2—C31.0 (3)C6'—N1'—C2'—C3'0.2 (3)
N1—C2—C3—C40.4 (3)N1'—C2'—C3'—C4'0.9 (3)
C2—C3—C4—C50.6 (3)C2'—C3'—C4'—C5'1.1 (3)
C3—C4—C5—C60.6 (2)C3'—C4'—C5'—C6'0.7 (3)
C2—N1—C6—C52.3 (2)C2'—N1'—C6'—C5'0.3 (3)
C2—N1—C6—N61176.99 (15)C2'—N1'—C6'—N61'179.53 (17)
C4—C5—C6—N12.1 (3)C4'—C5'—C6'—N1'0.1 (3)
C4—C5—C6—N61177.19 (15)C4'—C5'—C6'—N61'179.78 (17)
N1—C6—N61—C627.3 (3)N1'—C6'—N61'—C62'1.0 (3)
C5—C6—N61—C62172.06 (16)C5'—C6'—N61'—C62'179.15 (18)
C6—N61—C62—N634.1 (3)C6'—N61'—C62'—N63'0.4 (3)
C6—N61—C62—S62174.97 (13)C6'—N61'—C62'—S62'179.88 (15)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N61—H61···S62i0.83 (2)2.64 (2)3.4401 (16)163.3 (19)
N63—H63A···S620.89 (3)2.55 (2)3.3383 (16)148.3 (19)
N63—H63B···N10.95 (2)1.91 (2)2.664 (2)134.4 (19)
N61—H61···S620.87 (2)2.61 (2)3.4273 (16)157.1 (18)
N63—H63C···N10.86 (2)2.02 (2)2.701 (2)135 (2)
N63—H63D···S62ii0.89 (3)2.56 (3)3.4127 (17)161 (2)
Symmetry codes: (i) x, y+1, z+1; (ii) x+1, y+1/2, z+3/2.

Experimental details

Crystal data
Chemical formulaC6H7N3S
Mr153.21
Crystal system, space groupMonoclinic, P21/c
Temperature (K)173
a, b, c (Å)14.0116 (13), 6.1820 (4), 16.8726 (15)
β (°) 97.140 (7)
V3)1450.2 (2)
Z8
Radiation typeMo Kα
µ (mm1)0.37
Crystal size (mm)0.52 × 0.40 × 0.28
Data collection
DiffractometerStoe IPDS II two-circle
diffractometer
Absorption correctionMulti-scan
[MULABS (Spek, 2003; Blessing, 1995)]
Tmin, Tmax0.832, 0.904
No. of measured, independent and
observed [I > 2σ(I)] reflections
11661, 2700, 2307
Rint0.075
(sin θ/λ)max1)0.607
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.035, 0.091, 1.03
No. of reflections2700
No. of parameters206
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.25, 0.21

Computer programs: X-AREA (Stoe & Cie, 2001), SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), XP in SHELXTL-Plus (Sheldrick, 1991).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N61—H61···S62i0.83 (2)2.64 (2)3.4401 (16)163.3 (19)
N63—H63A···S62'0.89 (3)2.55 (2)3.3383 (16)148.3 (19)
N63—H63B···N10.95 (2)1.91 (2)2.664 (2)134.4 (19)
N61'—H61'···S620.87 (2)2.61 (2)3.4273 (16)157.1 (18)
N63'—H63C···N1'0.86 (2)2.02 (2)2.701 (2)135 (2)
N63'—H63D···S62'ii0.89 (3)2.56 (3)3.4127 (17)161 (2)
Symmetry codes: (i) x, y+1, z+1; (ii) x+1, y+1/2, z+3/2.
 

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