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Journal logoSTRUCTURAL
CHEMISTRY
ISSN: 2053-2296

2-Amino-3-hy­droxy-4-phenyl­thia­zol­ium chloride: π-stacked hydrogen-bonded chains of edge-fused R[_{\bf 4}^{\bf 2}](11) rings

CROSSMARK_Color_square_no_text.svg

aSchool of Chemistry, University of St Andrews, Fife KY16 9ST, Scotland, bDepartment of Chemistry, University of Aberdeen, Meston Walk, Old Aberdeen AB24 3UE, Scotland, and cInstituto de Química, Departamento de Química Inorgânica, Universidade Federal do Rio de Janeiro, 21945-970 Rio de Janeiro, RJ, Brazil
*Correspondence e-mail: cg@st-andrews.ac.uk

(Received 23 February 2004; accepted 2 March 2004; online 31 March 2004)

In the title compound, C9H9N2OS+·Cl, the cations exhibit amidinium-type delocalization of the positive charge. The ions are linked by one O—H⋯Cl hydrogen bond and two N—H⋯Cl hydrogen bonds into chains of edge-fused [R_4^2](11) rings. The chains are linked into sheets by a ππ stacking interaction.

Comment

Masaki et al. (1966[Masaki, M., Sugiyama, M., Tayama, M. & Ohta, M. (1966). Bull. Chem. Soc. Jpn, 39, 2745-2749.]) reported the preparation of 3-hydroxy-4-phenyl-2(3H)-thia­zol­imine, from the condensation reaction of the oxime of bromo­methyl phenyl ketone, BrCH2C(Ph)=NOH, with barium thio­cyanate, and these authors characterized the heterocycle as the picrate salt. The mass spectrum of the title compound, the hydro­chloride salt (I[link]), was reported by Entenmann (1975[Entenmann, G. (1975). Org. Mass Spectrom. 10, 831-835.]) as exhibiting a significant peak assigned to [M − 16]+, corresponding to the loss of an O atom, which suggested that the O atom was not protonated. In solution, the picrate salt was reported to give a positive phenol test with iron(III) chloride. However, in neither report was the constitution of the cation definitively established; in particular, neither report gave any indication of the solid-state structure, and hence the determination now reported was undertaken.

Compound (I[link]) consists of an ion pair containing a short O—H⋯Cl hydrogen bond (Fig. 1[link], and Tables 1[link] and 2[link]). In the cation, the heterocyclic ring is planar, as expected, and the dihedral angle between this plane and the plane of the benzene ring is 41.9 (2)°. There are considerable differences between the corresponding pairs of exocyclic angles at atoms C2, N3 and C4. The very small interbond angle at atom S1 is also notable. The C2—N2 and C2—N3 bonds are similar in length and both are significantly shorter than the N3—C4 bond. The bond orders, calculated using the recent recalibration by Kotelevskii & Prezhdo (2001[Kotelevskii, S. I. & Prezhdo, O. V. (2001). Tetrahedron, 57, 5715-5729.]) of the original equation relating bond order to bond length (Gordy, 1947[Gordy, W. (1947). J. Chem. Phys. 15, 305-310.]), for the C2—N2, C2—N3 and C3—N4 bonds are 1.77, 1.72 and 1.33, respectively, suggesting amidinium-type delocalization of the positive charge between atoms N2 and N3, as indicated in the scheme below.

[Scheme 1]

The amine group acts as a double donor in N—H⋯Cl hydrogen bonds involving two different anions (Table 2[link]). In the shorter and more nearly linear of these two interactions, amine atom N2 acts as a hydrogen-bond donor, via atom H2A, to atom Cl1 at (x, y − 1, z), so generating by translation a C21(7) chain (Bernstein et al., 1995[Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl. 34, 1555-1573.]) running parallel to the [010] direction (Fig. 2[link]). Four chains of this type pass through each unit cell and these chains are linked into pairs by the second N—H⋯Cl hydrogen bond. In this interaction, atom N2 acts as a hydrogen-bond donor, this time via atom H2B, to atom Cl1 at ([{1 \over 2}] − x, y − [1\over 2], [{1 \over 2}] − z), so forming a C21(4) chain generated by the 21 screw axis along ([1\over 4], y, [1\over 4]) (Fig. 2[link]). The combination of the C21(4) and C21(7) motifs then produces a chain of edge-fused [R_4^2](11) rings. This chain of rings, containing the 21 axis along ([1\over 4], y, [1\over 4]), lies within the domain 0 < x < [1\over 2], and a second chain, related to the first by inversion and containing the 21 axis along ([3\over 4], y, [3\over 4]), lies in the domain [{1 \over 2}] < x < 1.

The only direction-specific interaction between adjacent chains of rings is a weak ππ stacking interaction between the heterocyclic rings of the cations related by a centre of symmetry. These rings are parallel, with an interplanar spacing of 3.631 (2) Å. The ring-centroid separation is 3.778 (2) Å, corresponding to a centroid offset of 1.044 (2) Å. These cations at (x, y, z) and (1 − x, 1 − y, 1 − z) lie, respectively, in the chains of rings along ([1\over 4], y, [1\over 4]) and ([3\over 4], −y, [3\over 4]), so that propagation of this stacking interaction links the chain into a (10[\overline 1]) sheet. However, there are no ππ stacking interactions involving the phenyl ring, nor are there any C—H⋯π(arene) hydrogen bonds.

As well as acting as a threefold acceptor of hydrogen bonds, the anion at (x, y, z) also forms a short contact with the S atom of the mol­ecule at (1 − x, 1 − y, 1 − z). This S⋯Cl distance is 3.3275 (7) Å, somewhat less than the sum of the van der Waals radii (3.50 Å; Bondi, 1964[Bondi, A. (1964). J. Phys. Chem. 68, 441-451.]). The overall coordination polyhedron at atom Cl1, including the secondary bond (Alcock, 1972[Alcock, N. W. (1972). Advances in Inorganic Radiochemistry, Vol. 15, edited by H. J. Emeléus & A. G. Sharpe, pp. 1-58. San Diego: Academic Press.]) involving the S atom, takes the form of a distorted trigonal bipyramid of VSEPR (valence-shell electron-pair repulsion) type MX4E (Gillespie, 1972[Gillespie, R. J. (1972). In Molecular Geometry. London: Van-Nostrand Rheinhold.]; Gillespie & Hargittai, 1991[Gillespie, R. J. & Hargittai, I. (1991). In The VSEPR Model of Molecular Geometry. Needham Heights, MA, USA: Allyn and Bacon.]; Burdett, 1997[Burdett, J. K. (1997). In Chemical Bonds. Chichester: John Wiley.]), where X represents a bonding pair of electrons at the central atom M (here M = Cl) and E ­represents the equatorial lone pair of non-bonding electrons (Fig. 3[link]). The angles at atom Cl1 are as follows: O3⋯Cl1⋯N2* = 110.79 (5)°, O3⋯Cl1⋯N2# = 78.64 (5)°, O3⋯Cl1⋯S1$ = 91.92 (3)°, N2*⋯Cl1⋯N2# = 92.69 (5)°, N2*⋯Cl1⋯S1$ = 109.99 (4)° and N2#⋯Cl1⋯S1$ = 157.30 (4)°, where atoms marked with an asterisk (*), a hash (#) or a dollar sign ($) are at the symmetry positions (x, y + 1, z), ([{1 \over 2}] − x, [{1 \over 2}] + y, [{1 \over 2}] − z) and (1 − x, 1 − y, 1 − z), respectively.

[Figure 1]
Figure 1
The independent ions in (I[link]), showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2]
Figure 2
Part of the crystal structure of (I[link]), showing the formation of a chain of edge-fused [R_4^2](11) rings along the b axis. For clarity, H atoms bonded to C atoms have been omitted. Atoms marked with an asterisk (*), a hash (#), a dollar sign ($) or an ampersand (&) are at the symmetry positions (x, y − 1, z), ([{1 \over 2}] − x, y − [{1 \over 2}], [{1 \over 2}] − z), (x, y + 1, z) and ([{1 \over 2}] − x, [{1 \over 2}] + y, [{1 \over 2}] − z), respectively.
[Figure 3]
Figure 3
Part of the crystal structure of (I[link]), showing the coordination at the anion. For clarity, H atoms bonded to C atoms have been omitted. Atoms marked with an asterisk (*), a hash (#) or a dollar sign ($) are at the symmetry positions (x, y + 1, z), ([{1 \over 2}] − x, [{1 \over 2}] + y, [{1 \over 2}] − z) and (1 − x, 1 − y, 1 − z), respectively.

Experimental

The neutral heterocycle 3-hydroxy-2-imino-4-phenyl­thia­zole was prepared according to the method reported by Masaki et al. (1966[Masaki, M., Sugiyama, M., Tayama, M. & Ohta, M. (1966). Bull. Chem. Soc. Jpn, 39, 2745-2749.]). The hydro­chloride salt, (I[link]), was prepared by treating the neutral heterocycle in ethanol solution with aqueous HCl (6 mol dm−3) and was recrystallized from ethanol. Compound (I[link]) slowly darkened on heating and decomposed before melting.

Crystal data
  • C9H9N2OS+·Cl

  • Mr = 228.69

  • Monoclinic, P21/n

  • a = 9.2663 (5) Å

  • b = 7.0716 (4) Å

  • c = 15.461 (1) Å

  • β = 90.194 (2)°

  • V = 1013.12 (10) Å3

  • Z = 4

  • Dx = 1.499 Mg m−3

  • Mo Kα radiation

  • Cell parameters from 2247 reflections

  • θ = 3.2–27.4°

  • μ = 0.55 mm−1

  • T = 120 (2) K

  • Plate, colourless

  • 0.32 × 0.24 × 0.12 mm

Data collection
  • Nonius KappaCCD diffractometer

  • φ scans, and ω scans with κ offsets

  • Absorption correction: multi-scan (SORTAV; Blessing, 1995[Blessing, R. H. (1995). Acta Cryst. A51, 33-37.], 1997[Blessing, R. H. (1997). J. Appl. Cryst. 30, 421-426.]) Tmin = 0.827, Tmax = 0.934

  • 9736 measured reflections

  • 2247 independent reflections

  • 1751 reflections with I > 2σ(I)

  • Rint = 0.067

  • θmax = 27.4°

  • h = −11 → 11

  • k = −8 → 9

  • l = −19 → 19

Refinement
  • Refinement on F2

  • R[F2 > 2σ(F2)] = 0.045

  • wR(F2) = 0.119

  • S = 1.04

  • 2247 reflections

  • 128 parameters

  • H-atom parameters constrained

  • w = 1/[σ2(Fo2) + (0.0703P)2 + 0.159P] where P = (Fo2 + 2Fc2)/3

  • (Δ/σ)max = 0.001

  • Δρmax = 0.53 e Å−3

  • Δρmin = −0.41 e Å−3

Table 1
Selected geometric parameters (Å, °)

S1—C2 1.718 (2)
C2—N3 1.330 (3)
N3—C4 1.405 (3)
C4—C5 1.341 (3)
C5—S1 1.737 (2)
C2—N2 1.321 (3)
N3—O3 1.377 (2)
C4—C41 1.476 (3)
S1—C2—N3 110.64 (15)
C2—N3—C4 116.04 (18)
N3—C4—C5 110.03 (19)
C4—C5—S1 113.00 (17)
C5—S1—C2 90.29 (11)
S1—C2—N2 125.72 (17)
N2—C2—N3 123.58 (19)
C2—N3—O3 119.73 (17)
O3—N3—C4 124.22 (17)
N3—C4—C41 121.81 (19)
C5—C4—C41 128.2 (2)
N3—C4—C41—C42 −139.2 (2)
C5—C4—C41—C42 40.7 (3)
N3—C4—C41—C46 43.1 (3)
C5—C4—C41—C46 −136.9 (2)

Table 2
Hydrogen-bonding geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
O3—H3⋯Cl1 0.84 2.11 2.929 (2) 167
N2—H2A⋯Cl1i 0.88 2.30 3.131 (2) 157
N2—H2B⋯Cl1ii 0.88 2.46 3.217 (2) 145
Symmetry codes: (i) x,y-1,z; (ii) [{1\over 2}-x,y-{1\over 2},{1\over 2}-z].

All H atoms were located from difference maps and subsequently treated as riding atoms, with C—H distances of 0.95 Å, N—H distances of 0.88 Å and an O—H distance of 0.84 Å.

Data collection: KappaCCD Server Software (Nonius, 1997[Nonius (1997). KappaCCD Server Software. Windows 3.11 Version. Nonius BV, Delft, The Netherlands.]); cell refinement: DENZO–SMN (Otwinowski & Minor, 1997[Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276, Macromolecular Crystallography, Part A, edited by C. W. Carter Jr & R. M. Sweet, pp. 307-326. New York: Academic Press.]); data reduction: DENZO–SMN; program(s) used to solve structure: OSCAIL (McArdle, 2003[McArdle, P. (2003). OSCAIL for Windows. Version 10. Crystallography Centre Chemistry Department, NUI Galway, Ireland.]) and SHELXS97 (Sheldrick, 1997[Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany.]); program(s) used to refine structure: OSCAIL and SHELXL97 (Sheldrick, 1997[Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany.]); molecular graphics: PLATON (Spek, 2003[Spek, A. L. (2003). J. Appl. Cryst. 36, 7-13.]); software used to prepare material for publication: SHELXL97 and PRPKAPPA (Ferguson, 1999[Ferguson, G. (1999). PRPKAPPA. University of Guelph, Canada.]).

Supporting information


Comment top

Masaki et al. (1966) reported the preparation of 3-hydroxy-4-phenyl-2(3H)-thiazolimine, from the condensation reaction of the oxime of bromomethyl phenyl ketone, BrCH2C(Ph)=NOH, with barium thiocyanate, and characterized the heterocycle as the picrate salt. The mass spectrum of the title compound, the hydrochloride salt (I), was reported by Entenmann (1975) as exhibiting a significant peak assigned to [M-16]+, corresponding to loss of an O atom, which suggested that the O atom was not protonated. In solution, the picrate salt was reported to give a positive phenol test with iron(III) chloride. However, in neither report was the constitution of the cation definitively established; in particular, neither report gave any indication of the solid-state structure, and hence the determination now reported was undertaken.

Compound (I) consists of an ion pair containing a short O—H···Cl hydrogen bond (Fig. 1, and Tables 1 and 2). In the cation, the heterocyclic ring is planar, as expected, and the dihedral angle between this plane and the Ph ring is 41.9 (2)°. There is considerable variation within the corresponding pairs of exocyclic angles at atoms C2, N3 and C4. The very small interbond angle at atom S1 is also notable. The C2—N2 and C2—N3 bonds are similar in length and both are significantly shorter than the N3—C4 bond. The bond orders, calculated using the recent recalibration by Kotelevskii & Prezhdo (2001) of the original equation relating bond order to bond length (Gordy, 1947), for the C2—N2, C2—N3 and C3—N4 bonds are 1.77, 1.72 and 1.33, respectively, suggesting amidinium-type delocalization of the positive charge between atoms N2 and N3, as indicated in the scheme.

The amine group acts as a double donor in N—H···Cl hydrogen bonds involving two different anions (Table 2). In the shorter and more nearly linear of these two interactions, amine atom N2 acts as a hydrogen-bond donor, via atom H2A, to atom Cl at (x, y − 1, z), so generating by translation a C12(7) (Bernstein et al., 1995) chain running parallel to the [010] direction (Fig. 2). Four chains of this type pass through each unit cell and they are linked into pairs by the second N—H···Cl hydrogen bond. In this interaction, atom N2 acts as a hydrogen-bond donor, this type via atom H2B, to atom Cl at (1/2 − x, y − 1/2, 1/2 − z), so forming a C12(4) chain generated by the 21 screw axis along (1/4, y, 1/4) (Fig. 2). The combination of the C12(4) and C12(7) motifs then produces a chain of edge-fused R24(11) rings. This chain of rings, containing the 21 axis along (1/4, y, 1/4), lies within the domain 0 < x < 1/2, and a second chain, related to the first by inversion and containing the 21 axis along (3/4, y, 3/4), lies in the domain 1/2 < x < 1.

The only direction-specific interaction between adjacent chains of rings is a weak π···π stacking interaction between the heterocyclic rings of the cations related by a center of symmetry. These rings are parallel, with an interplanar spacing of 3.631 (2) Å. The ring-centroid separation is 3.778 (2) Å, corresponding to a centroid offset of 1.044 (2) Å. These cations at (x, y, z) and (1 − x, 1 − y, 1 − z) lie, respectively, in the chains of rings along (1/4, y, 1/4) and (3/4, −y, 3/4), so that propagation of this stacking interaction links the chain into a (10–1) sheet. However, there are no π···π stacking interactions involving the phenyl ring, nor are there any C—H···π(arene) hydrogen bonds.

As well as acting as a threefold acceptor of hydrogen bonds, the anion at (x, y, z) also forms a short contact with the S atom of the molecule at (1 − x, 1 − y, 1 − z). This S···Cl distance is 3.3275 (7) Å, somewhat below the sum of the van der Waals radii (3.50 Å; Bondi, 1964). The overall coordination polyhedron at atom Cl, including the secondary bond (Alcock, 1972) involving the S atom, takes the form of a distorted trigonal bipyramid of VSEPR (Gillespie, 1972; Gillespie & Hargittai, 1991; Burdett, 1997) type MX4E, where X represents a bonding pair of electrons at the central atom, M (here M = Cl), and E represents the equatorial lone pair of non-bonding electrons (Fig. 3). The angles at atom Cl1 are as follows: O3···Cl1···N2* = 110.79 (5)°, O3···Cl1···N2# = 78.64 (5)°, O3···Cl1···S1? = 91.92 (3)°, N2*···Cl1···N2# = 92.69 (5)°, N2*···Cl1···Si? = 109.99 (4)° and N2#···Cl1···S1? = 157.30 (4)°, where atoms marked with an asterisk (*), a hash (#) or a dollar sign () are at the symmetry positions (x, y + 1, z), (1/2 − x, 1/2 + y, 1/2 − z) and $ = (1 − x, 1 − y, 1 − z), resepctively.

Experimental top

The neutral heterocycle 2-imino-3-hydroxy-4-phenylthiazole was prepared according to the method reported by Masaki et al. (1966). The hydrochloride salt, (I), was prepared by treating the neutral heterocycle in ethanol solution with 6 mol dm−3 aqueous HCl, and (I) was recrystallized from ethanol. Compound (I) slowly darkened on heating and decomposed before melting.

Refinement top

All H atoms were located from difference maps and subsequently treated as riding atoms, with C—H distances of 0.95 Å, N—H distances of 0.88 Å and O—H distances of 0.84 Å.

Computing details top

Data collection: KappaCCD Server Software (Nonius, 1997); cell refinement: DENZO–SMN (Otwinowski & Minor, 1997); data reduction: DENZO–SMN; program(s) used to solve structure: OSCAIL (McArdle, 2003) and SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: OSCAIL and SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97 and PRPKAPPA (Ferguson, 1999).

Figures top
[Figure 1] Fig. 1. The independent ions in (I), showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2] Fig. 2. Part of the crystal structure of (I), showing the formation of a chain of edge-fused R24(11) rings along the b axis. For clarity, H atoms bonded to C atoms have been omitted. Atoms marked with an asterisk (*), a hash (#), a dollar sign () or an ampersand (&) are at the symmetry positions (x, y − 1, z), (1/2 − x, y − 1/2, 1/2 − z), (x, y + 1, z) and (1/2 − x, 1/2 + y, 1/2 − z), respectively.
[Figure 3] Fig. 3. Part of the crystal structure of (I), showing the coordination at the anion. For clarity, H atoms bonded to C atoms have been omitted. Atoms marked with an asterisk (*), a hash (#) or a dollar sign () are at the symmetry positions (x, y + 1, z), (1/2 − x, 1/2 + y, 1/2 − z) and (1 − x, 1 − y, 1 − z), respectively.
2-Amino-3-hydroxy-4-phenylthiazolium chloride top
Crystal data top
C9H9N2OS+·ClF(000) = 472
Mr = 228.69Dx = 1.499 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 2247 reflections
a = 9.2663 (5) Åθ = 3.2–27.4°
b = 7.0716 (4) ŵ = 0.55 mm1
c = 15.461 (1) ÅT = 120 K
β = 90.194 (2)°Plate, colourless
V = 1013.12 (10) Å30.32 × 0.24 × 0.12 mm
Z = 4
Data collection top
KappaCCD
diffractometer
2247 independent reflections
Radiation source: rotating anode1751 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.067
ϕ scans, and ω scans with κ offsetsθmax = 27.4°, θmin = 3.2°
Absorption correction: multi-scan
(SORTAV; Blessing 1995, 1997)
h = 1111
Tmin = 0.827, Tmax = 0.934k = 89
9736 measured reflectionsl = 1919
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.045Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.119H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0703P)2 + 0.159P]
where P = (Fo2 + 2Fc2)/3
2247 reflections(Δ/σ)max = 0.001
128 parametersΔρmax = 0.53 e Å3
0 restraintsΔρmin = 0.41 e Å3
Crystal data top
C9H9N2OS+·ClV = 1013.12 (10) Å3
Mr = 228.69Z = 4
Monoclinic, P21/nMo Kα radiation
a = 9.2663 (5) ŵ = 0.55 mm1
b = 7.0716 (4) ÅT = 120 K
c = 15.461 (1) Å0.32 × 0.24 × 0.12 mm
β = 90.194 (2)°
Data collection top
KappaCCD
diffractometer
2247 independent reflections
Absorption correction: multi-scan
(SORTAV; Blessing 1995, 1997)
1751 reflections with I > 2σ(I)
Tmin = 0.827, Tmax = 0.934Rint = 0.067
9736 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0450 restraints
wR(F2) = 0.119H-atom parameters constrained
S = 1.04Δρmax = 0.53 e Å3
2247 reflectionsΔρmin = 0.41 e Å3
128 parameters
Special details top

Refinement. The space group P21/n was uniquely assigned from the systematic absences.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.38910 (6)0.22878 (8)0.50432 (3)0.02526 (19)
C20.3016 (2)0.3484 (3)0.42286 (13)0.0216 (5)
N20.2959 (2)0.2964 (3)0.34083 (12)0.0264 (4)
N30.24406 (19)0.5079 (2)0.45261 (11)0.0217 (4)
O30.16664 (16)0.6230 (2)0.39757 (9)0.0265 (4)
C40.2658 (2)0.5452 (3)0.54098 (13)0.0229 (5)
C50.3437 (2)0.4061 (3)0.57711 (14)0.0256 (5)
C410.2075 (2)0.7165 (3)0.58266 (14)0.0221 (5)
C420.2927 (2)0.8124 (3)0.64260 (13)0.0251 (5)
C430.2390 (2)0.9687 (3)0.68564 (14)0.0274 (5)
C440.1001 (2)1.0312 (3)0.66872 (14)0.0301 (6)
C450.0152 (3)0.9379 (3)0.60891 (15)0.0307 (5)
C460.0680 (3)0.7809 (3)0.56603 (15)0.0272 (5)
Cl10.39250 (6)0.87277 (8)0.33083 (3)0.02775 (19)
H2A0.33580.18930.32450.032*
H2B0.25230.36890.30260.032*
H30.22070.70860.37850.040*
H50.37130.40460.63630.031*
H420.38820.77030.65400.030*
H430.29741.03310.72680.033*
H440.06321.13850.69830.036*
H450.07980.98150.59720.037*
H460.00900.71690.52510.033*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0326 (3)0.0234 (3)0.0197 (3)0.0063 (2)0.0034 (2)0.0027 (2)
C20.0218 (11)0.0206 (11)0.0225 (11)0.0007 (9)0.0049 (8)0.0026 (9)
N20.0360 (11)0.0237 (10)0.0195 (9)0.0058 (9)0.0073 (8)0.0002 (8)
N30.0254 (9)0.0196 (10)0.0201 (9)0.0030 (8)0.0068 (7)0.0033 (7)
O30.0310 (9)0.0235 (9)0.0247 (8)0.0042 (7)0.0097 (7)0.0051 (6)
C40.0243 (11)0.0245 (12)0.0199 (10)0.0007 (9)0.0013 (8)0.0022 (9)
C50.0303 (12)0.0262 (12)0.0204 (11)0.0038 (10)0.0012 (9)0.0004 (9)
C410.0260 (11)0.0199 (11)0.0203 (10)0.0001 (9)0.0009 (8)0.0022 (8)
C420.0273 (11)0.0282 (12)0.0196 (11)0.0009 (10)0.0017 (9)0.0041 (9)
C430.0336 (13)0.0292 (13)0.0196 (11)0.0032 (10)0.0022 (9)0.0013 (9)
C440.0398 (14)0.0238 (13)0.0267 (12)0.0028 (10)0.0052 (10)0.0012 (9)
C450.0296 (12)0.0283 (13)0.0342 (13)0.0059 (11)0.0001 (10)0.0008 (10)
C460.0271 (12)0.0257 (13)0.0289 (12)0.0014 (10)0.0037 (10)0.0006 (10)
Cl10.0331 (3)0.0245 (3)0.0255 (3)0.0016 (2)0.0097 (2)0.0011 (2)
Geometric parameters (Å, º) top
S1—C21.718 (2)C41—C421.392 (3)
C2—N31.330 (3)C41—C461.393 (3)
N3—C41.405 (3)C42—C431.383 (3)
C4—C51.341 (3)C42—H420.95
C5—S11.737 (2)C43—C441.385 (3)
C2—N21.321 (3)C43—H430.95
N3—O31.377 (2)C44—C451.380 (3)
C4—C411.476 (3)C44—H440.95
N2—H2A0.88C45—C461.383 (3)
N2—H2B0.88C45—H450.95
O3—H30.84C46—H460.95
C5—H50.95
S1—C2—N3110.64 (15)C42—C41—C4118.9 (2)
C2—N3—C4116.04 (18)C46—C41—C4121.9 (2)
N3—C4—C5110.03 (19)C43—C42—C41120.4 (2)
C4—C5—S1113.00 (17)C43—C42—H42119.8
C5—S1—C290.29 (11)C41—C42—H42119.8
S1—C2—N2125.72 (17)C42—C43—C44120.0 (2)
N2—C2—N3123.58 (19)C42—C43—H43120.0
C2—N3—O3119.73 (17)C44—C43—H43120.0
O3—N3—C4124.22 (17)C45—C44—C43120.1 (2)
N3—C4—C41121.81 (19)C45—C44—H44120.0
C5—C4—C41128.2 (2)C43—C44—H44120.0
C2—N2—H2A120.0C44—C45—C46120.2 (2)
C2—N2—H2B120.0C44—C45—H45119.9
H2A—N2—H2B120.0C46—C45—H45119.9
N3—O3—H3109.5C45—C46—C41120.2 (2)
C4—C5—H5123.5C45—C46—H46119.9
S1—C5—H5123.5C41—C46—H46119.9
C42—C41—C46119.2 (2)
C5—S1—C2—N2176.8 (2)N3—C4—C41—C42139.2 (2)
C5—S1—C2—N30.42 (16)C5—C4—C41—C4240.7 (3)
N2—C2—N3—O33.9 (3)N3—C4—C41—C4643.1 (3)
S1—C2—N3—O3178.81 (14)C5—C4—C41—C46136.9 (2)
N2—C2—N3—C4177.18 (19)C46—C41—C42—C430.6 (3)
S1—C2—N3—C40.2 (2)C4—C41—C42—C43177.19 (19)
C2—N3—C4—C50.3 (3)C41—C42—C43—C440.4 (3)
O3—N3—C4—C5179.21 (18)C42—C43—C44—C450.0 (3)
C2—N3—C4—C41179.73 (19)C43—C44—C45—C460.4 (4)
O3—N3—C4—C410.8 (3)C44—C45—C46—C410.2 (3)
N3—C4—C5—S10.6 (2)C42—C41—C46—C450.2 (3)
C41—C4—C5—S1179.41 (18)C4—C41—C46—C45177.46 (19)
C2—S1—C5—C40.61 (18)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O3—H3···Cl10.842.112.929 (2)167
N2—H2A···Cl1i0.882.303.131 (2)157
N2—H2B···Cl1ii0.882.463.217 (2)145
Symmetry codes: (i) x, y1, z; (ii) x+1/2, y1/2, z+1/2.

Experimental details

Crystal data
Chemical formulaC9H9N2OS+·Cl
Mr228.69
Crystal system, space groupMonoclinic, P21/n
Temperature (K)120
a, b, c (Å)9.2663 (5), 7.0716 (4), 15.461 (1)
β (°) 90.194 (2)
V3)1013.12 (10)
Z4
Radiation typeMo Kα
µ (mm1)0.55
Crystal size (mm)0.32 × 0.24 × 0.12
Data collection
DiffractometerKappaCCD
diffractometer
Absorption correctionMulti-scan
(SORTAV; Blessing 1995, 1997)
Tmin, Tmax0.827, 0.934
No. of measured, independent and
observed [I > 2σ(I)] reflections
9736, 2247, 1751
Rint0.067
(sin θ/λ)max1)0.647
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.045, 0.119, 1.04
No. of reflections2247
No. of parameters128
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.53, 0.41

Computer programs: KappaCCD Server Software (Nonius, 1997), DENZO–SMN (Otwinowski & Minor, 1997), DENZO–SMN, OSCAIL (McArdle, 2003) and SHELXS97 (Sheldrick, 1997), OSCAIL and SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2003), SHELXL97 and PRPKAPPA (Ferguson, 1999).

Selected geometric parameters (Å, º) top
S1—C21.718 (2)C5—S11.737 (2)
C2—N31.330 (3)C2—N21.321 (3)
N3—C41.405 (3)N3—O31.377 (2)
C4—C51.341 (3)C4—C411.476 (3)
S1—C2—N3110.64 (15)N2—C2—N3123.58 (19)
C2—N3—C4116.04 (18)C2—N3—O3119.73 (17)
N3—C4—C5110.03 (19)O3—N3—C4124.22 (17)
C4—C5—S1113.00 (17)N3—C4—C41121.81 (19)
C5—S1—C290.29 (11)C5—C4—C41128.2 (2)
S1—C2—N2125.72 (17)
N3—C4—C41—C42139.2 (2)N3—C4—C41—C4643.1 (3)
C5—C4—C41—C4240.7 (3)C5—C4—C41—C46136.9 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O3—H3···Cl10.842.112.929 (2)167
N2—H2A···Cl1i0.882.303.131 (2)157
N2—H2B···Cl1ii0.882.463.217 (2)145
Symmetry codes: (i) x, y1, z; (ii) x+1/2, y1/2, z+1/2.
 

Acknowledgements

X-ray data were collected at the EPSRC X-ray Crystallographic Service, University of Southampton, England; the authors thank the staff for all their help and advice. JNL thanks NCR Self-Service, Dundee, for grants that have provided computing facilities for this work. JLW thanks CNPq and FAPERJ for financial support.

References

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