organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoSTRUCTURAL
CHEMISTRY
ISSN: 2053-2296

2-Acet­amido-4-p-tolyl-1,3-thia­zole and 2-amino-4-p-tolyl-1,3-thia­zolium chloride dihydrate

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aSchool of Science and the Environment, Coventry University, Coventry CV1 5FB, England, and bKey Organics Ltd, Highfield Industrial Estate, Camelford, Cornwall PL32 9QZ, England
*Correspondence e-mail: apx106@coventry.ac.uk

(Received 23 August 2004; accepted 20 September 2004; online 22 October 2004)

The structures of 2-acet­amido-4-tolyl-1,3-thia­zole, C12H12N2OS, (I[link]), and 2-amino-4-tolyl-1,3-thia­zolium chloride dihydrate, C10H11N2S+·Cl·2H2O, (II[link]), reveal that both mol­ecules are essentially planar, with the respective dihedral angles between the benzene and thia­zole rings being 2.9 (1) and 10.39 (7)°. Compound (I[link]) associates via a single N—H⋯O interaction to form a flat alternate-facing hydrogen-bonded chain [graph-set C[{_2^2}](4)]. Compound (II[link]) packs with the hydrogen-bonding associations of the Cl atoms and the water mol­ecules creating a convoluted hydrogen-bonded ribbon made up of five-membered donor–acceptor rings, involving three water O atoms (with associated H atoms) and two Cl atoms. The thia­zolium rings form stacked columns, aligned in the same direction as the hydrogen-bonded ribbons, of alternate-facing mol­ecules that are also involved in the hydrogen-bonding network, linking to the Cl atoms and one of the water mol­ecules. Subsequently, each Cl atom is the hydrogen-bond acceptor for five separate O/N—H associations.

Comment

2-Amino-4-phenyl-1,3-thia­zole has both pharmaceutical and industrial applications (Au-Alvarez et al., 1999[Au-Alvarez, O., Peterson, R. C., Acosta Crespo, A., Rodríguez Esteva, Y., Marquez Alvarez, H., Plutín Stiven, A. M. & Pomés Hernández, R. (1999). Acta Cryst. C55, 821-823.]), including corrosion inhibition (Form et al., 1974[Form, G. R., Raper, E. S. & Downie, T. C. (1974). Acta Cryst. B30, 342-348.]); the structures of 2-amino-4-phenyl­thia­zole and its hydro­bromide hydrate salt are reported, respectively, in these two references. We have recently reviewed the structures of 2-amino-4-phenyl­thia­zole derivatives in terms of their hydrogen-bonding patterns, specifically highlighting any involvement of the thia­zole S atom (Lynch et al., 2002[Lynch, D. E., McClenaghan, I., Light, M. E. & Coles, S. J. (2002). Cryst. Eng. 5, 123-136.]). Since that paper, the structures of two more derivatives have been reported (Bernes et al., 2002[Bernès, S., Berros, M. I., Rodríguez de Barbarín, C. & Sánchez-Viesca, F. (2002). Acta Cryst. C58, o151-o153.]; Karanik et al., 2003[Karanik, M., Patzel, M. & Liebscher, J. (2003). Synthesis, pp. 1201-1208.]). Several of the analogues that we reported in 2002, such as 2-amino-4-tolyl-1,3-thia­zole, either packed quite simply as hydrogen-bonded R[{_2^2}](8) graph-set (Etter, 1990[Etter, M. C. (1990). Acc. Chem. Res. 23, 120-126.]) dimers through N—H⋯N interactions or displayed packing networks containing these dimers. In the cases where mol­ecules did not associate via N—H⋯N hydrogen bonds into dimers, and no other anions or water mol­ecules were present, N—H⋯S interactions were observed. The molecular arrangements in both the Bernes et al. and Karanik et al. structures also included N—H⋯N dimers. As a continuation of our 2002 study into the packing modes of 2-amino-4-phenyl-1,3-thia­zole derivatives, we have further determined the structures of 2-acet­amido-4-tolyl-1,3-thia­zole, (I[link]), and 2-amino-4-tolyl-1,3-thia­zolium chloride dihydrate, (II[link]), and report them here. As seen in two structures discussed in our 2002 paper, the packing modes of 2-­amino-4-phenyl-1,3-thia­zoles with additional anions and/or water mol­ecules differ from the structures of the thia­zole mol­ecules by themselves.

[Scheme 1]

The structure of (I[link]) consists of an essentially flat mol­ecule (Fig. 1[link]) which associates via a single N—H⋯O interaction, with alternate-facing mol­ecules, to form a C[{_2^2}](4) graph-set hydrogen-bonded chain (Fig. 2[link]). The N—H⋯O chain interaction (Table 1[link]) is one of two typical motifs displayed by amide linkages, with the other being an N—H⋯O hydrogen-bonded R[{_2^2}](8) graph-set dimer (Desiraju, 1995[Desiraju, G. R. (1995). Angew. Chem. Int. Ed. Engl. 34, 2311-2327.]). In other 2-acet­amido-1,3-thia­zole derivatives, of which there are four in the April 2004 version of the Cambridge Structural Database (CSD; Allen, 2002[Allen, F. H. (2002). Acta Cryst. B58, 380-388.]), none forms a hydrogen-bonded amide chain similar to (I[link]). Instead, one, namely N-(5-nitro-2-thia­zolyl)acet­amide (Peeters et al., 1985[Peeters, O. M., Blaton, N. M. & De Ranter, C. J. (1985). Acta Cryst. C41, 965-967.]), forms an R[{_2^2}](8) N—H⋯N hydrogen-bonded dimer, while the other three structures contain additional lattice elements, such as anions, cations and/or water mol­ecules. Furthermore, of 12 2-acet­amido-1,3,4-thia­diazole derivatives found in the CSD, only one, namely 2-acet­amido-4-benzoyl-5,5-di­methyl-4,5-di­hydro-1,3,4-thia­diazo­line (Kuban & Schulz, 1987[Kuban, R.-J. & Schulz, B. (1987). Cryst. Res. Technol. 22, 799-802.]), packs with a hydrogen-bonded amide chain. Interestingly, this mol­ecule contains a bulky substituent in the 4-position, similar to (I[link]), whereas those mol­ecules without such substituents predominantly pack as N—H⋯N dimers. In (I[link]), the dihedral angle between the thia­zole and phenyl rings is 2.9 (1)°. The comparative dihedral angle in 2-amino-4-tolyl­thia­zole is 12.80 (8)°.

The structure of (II[link]) consists of an essentially flat 2-amino-4-tolyl-1,3-thia­zolium mol­ecule, a Cl anion and two water mol­ecules (Fig. 3[link]), associated in a hydrogen-bonded network. The CSD reveals that there are seven previously reported 2-amino-1,3-thia­zolium halide (either Cl or Br) structures, with three of these being monohydrates; thus, (II[link]) is unique in being the first reported dihydrate. In all of the reported structures, the halide anion associates with either N3 or N21, or both, although across these examples, all of the hydrate structures have N3+—H associating to a water O atom. Alternatively, in (II[link]), the same Cl atom (details of hydrogen-bonding interactions are given in Table 2[link]) associates with both N3 and N21, similar to the three non-hydrate structures, with the second H atom on N21 forming a hydrogen bond to a symmetry-equivalent water O atom [O1Wii, see Fig. 4[link]; symmetry code: (ii) 1 − x, y − [{1 \over 2}], −[{1 \over 2}] − z]. The Cl atom and the two water mol­ecules associate via hydrogen-bonding interactions to construct a convoluted hydrogen-bonded ribbon network which runs in the a cell direction. This ribbon network is made up of five-membered donor–acceptor rings, involving three water O atoms (with associated H atoms) and two Cl atoms [Cl1, O1W, O2Wiii, Cliii and O2W in Fig. 4[link]; R35(10) graph set; symmetry code: (iii) x − [{1 \over 2}], [{3 \over 2}] − y, −z], fused along the O2W—H⋯Cl hydrogen bond. In addition to the hydrogen-bonding associations to Cl1 and O1W, the thia­zolium mol­ecules stack in a column co-directional with the anion–water ribbon. The thia­zolium columns comprise alternate-facing mol­ecules, with the perpendicular distances between thia­zole–phenyl and phenyl–thia­zole ring centroids being 3.60 (1) and 3.67 (1) Å, respectively, and with the closest contact distance being 3.35 (1) Å from C4⋯C42(x + [{1 \over 2}], [{1 \over 2}] − y, −z).

For (II[link]), the dihedral angle between the thia­zole and phenyl rings is 10.39 (7)°, which compares with a value of 19 (1)° for 2-amino-4-phenyl-1,3-thia­zolium bromide hydrate (Form et al., 1974[Form, G. R., Raper, E. S. & Downie, T. C. (1974). Acta Cryst. B30, 342-348.]) and 7.3 (2)° for 2-amino-4-naphthyl-1,3-thia­zolium bromide (Lynch et al., 2002[Lynch, D. E., McClenaghan, I., Light, M. E. & Coles, S. J. (2002). Cryst. Eng. 5, 123-136.]). Also noteworthy in (II[link]) is the indication of a delocalized double bond across the N3—C2—N21 site, with distances of 1.322 (8) (C2—N21) and 1.342 (8) Å (C2—N3), compared with distances of 1.351 (2) and 1.309 (2) Å, respectively, for 2-amino-4-tolyl­thia­zole. Similar distances of 1.30 (2) and 1.33 (2) Å, respectively, for 2-­amino-4-phenyl-1,3-thia­zolium bromide hydrate, and 1.347 (5) and 1.298 (5) Å for 2-amino-4-phenyl-1,3-thia­zole itself [the dihedral angle in this mol­ecule is 6.2 (3)°] are also noted. The hydrogen-bonding coordination surrounding the Cl atom is interesting, because without the N21—H21⋯Cl1 association, the remaining four-coordinate motif is pseudo-tetrahedral, with the H⋯Cl⋯H angles from H3 being 94 (3), 118 (3) and 122 (3)°, and the three remaining angles being 105 (3), 105 (3) and 110 (3)°. The addition of the N21—H21⋯Cl1 association thus creates a five-coordinate pseudo-face-capped tetrahedral arrangement, not observed amongst the seven previously reported 2-amino-1,3-thia­zolium halide structures.

[Figure 1]
Figure 1
The molecular configuration and atom-numbering scheme for (I[link]). Displacement ellipsoids are drawn at the 50% probability level and H atoms are shown as small spheres of arbitrary radii.
[Figure 2]
Figure 2
A packing diagram for (I[link]), viewed down the a axis. [Symmetry code: (i) x + [{1 \over 2}], [{1 \over 2}] − y, z − [{1 \over 2}].]
[Figure 3]
Figure 3
The molecular configuration and atom-numbering scheme for (II[link]). Displacement ellipsoids are drawn at the 50% probability level and H atoms are shown as small spheres of arbitrary radii.
[Figure 4]
Figure 4
A packing diagram for (II[link]). [Symmetry codes: (ii) 1 − x, y − [{1 \over 2}], −[{1 \over 2}] − z; (iii) x − [{1 \over 2}], [{3 \over 2}] − y, −z.]

Experimental

Both title compounds were obtained from Key Organics Ltd and crystals were grown from ethanol solutions. Data for (I[link]) were collected at Station 9.8 of the Daresbury SRS (Cernik et al., 1997[Cernik, R. J., Clegg, W., Catlow, C. R. A., Bushnell-Wye, G., Flaherty, J. V., Greaves, G. N., Burrows, I., Taylor, D. J., Teat, S. J. & Hamichi, M. (1997). J. Synchotron Rad. 4, 279-286; erratum, 7, 40.]; Clegg, 2000[Clegg, W. (2000). J. Chem. Soc. Dalton Trans. pp. 3223-3232.]). Data for (II[link]) were collected at the EPSRC Crystallographic Service, Southampton.

Compound (I)[link]

Crystal data
  • C12H12N2OS

  • Mr = 232.30

  • Monoclinic, P21/n

  • a = 3.9541 (5) Å

  • b = 37.484 (5) Å

  • c = 7.7173 (9) Å

  • β = 99.338 (2)°

  • V = 1128.7 (2) Å3

  • Z = 4

  • Dx = 1.367 Mg m−3

  • Synchrotron radiation, λ = 0.6894 Å

  • Cell parameters from 1753 reflections

  • θ = 2.7–28.2°

  • μ = 0.27 mm−1

  • T = 120 (2) K

  • Plate, colourless

  • 0.050 × 0.030 × 0.002 mm

Data collection
  • Bruker SMART 1K CCD area-detector diffractometer

  • ω rotation scans with narrow frames

  • 6723 measured reflections

  • 2407 independent reflections

  • 1770 reflections with I > 2σ(I)

  • Rint = 0.040

  • θmax = 26.0°

  • h = −5 → 2

  • k = −44 → 47

  • l = −9 → 9

Refinement
  • Refinement on F2

  • R[F2 > 2σ(F2)] = 0.049

  • wR(F2) = 0.126

  • S = 1.08

  • 2407 reflections

  • 151 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • w = 1/[σ2(Fo2) + (0.0604P)2 + 0.4975P] where P = (Fo2 + 2Fc2)/3

  • (Δ/σ)max < 0.001

  • Δρmax = 0.32 e Å−3

  • Δρmin = −0.32 e Å−3

Table 1
Hydrogen-bonding geometry (Å, °) for (I)[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N21—H21⋯O22i 0.89 (3) 1.95 (3) 2.818 (3) 166 (3)
Symmetry code: (i) [{\script{1\over 2}}+x,{\script{1\over 2}}-y,z-{\script{1\over 2}}].

Compound (II)[link]

Crystal data
  • C10H11N2S+·Cl·2H2O

  • Mr = 262.75

  • Orthorhombic, P212121

  • a = 6.8815 (6) Å

  • b = 9.3072 (14) Å

  • c = 19.499 (3) Å

  • V = 1248.9 (3) Å3

  • Z = 4

  • Dx = 1.397 Mg m−3

  • Mo Kα radiation

  • Cell parameters from 2244 reflections

  • θ = 2.9–27.1°

  • μ = 0.46 mm−1

  • T = 120 (2) K

  • Needle, colourless

  • 0.35 × 0.02 × 0.02 mm

Data collection
  • Nonius KappaCCD area-detector diffractometer

  • φ and ω scans

  • 9123 measured reflections

  • 1441 independent reflections

  • 1048 reflections with I > 2σ(I)

  • Rint = 0.156

  • θmax = 26.0°

  • h = −8 → 8

  • k = −9 → 11

  • l = −23 → 24

Refinement
  • Refinement on F2

  • R[F2 > 2σ(F2)] = 0.063

  • wR(F2) = 0.152

  • S = 1.06

  • 1441 reflections

  • 159 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • w = 1/[σ2(Fo2) + (0.0775P)2 + 0.1085P] where P = (Fo2 + 2Fc2)/3

  • (Δ/σ)max < 0.001

  • Δρmax = 0.44 e Å−3

  • Δρmin = −0.47 e Å−3

Table 2
Hydrogen-bonding geometry (Å, °) for (II)[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N3—H3⋯Cl1 0.88 2.32 3.126 (5) 151
N21—H21⋯Cl1 0.88 2.58 3.337 (6) 144
N21—H22⋯O1Wii 0.88 1.86 2.726 (7) 166
O1W—H11W⋯Cl1 0.88 (6) 2.26 (6) 3.136 (5) 178 (7)
O1W—H12W⋯O2Wiii 0.88 (5) 1.83 (3) 2.700 (7) 169 (8)
O2W—H22W⋯Cl1 0.88 (2) 2.35 (2) 3.214 (5) 167 (6)
O2W—H21W⋯Cl1iii 0.88 (5) 2.29 (3) 3.151 (5) 166 (6)
Symmetry codes: (ii) [1-x,y-{\script{1\over 2}},-{\script{1\over 2}}-z]; (iii) [x-{\script{1\over 2}},{\script{3\over 2}}-y,-z].

All H atoms, except for the N—H atom in (I[link]) and the water H atoms in (II[link]), were included in the refinements at calculated positions in the riding-model approximation, with N—H distances of 0.88 Å and C—H distances of 0.95 (aromatic H atoms) and 0.98 Å (methyl H atoms), and with Uiso(H) = 1.25Ueq(C,N). The N—H atom in (I[link]) was located in Fourier syntheses and both its positional and displacement parameters were refined. The water H atoms in (II[link]) were also located in Fourier syntheses, but their positional and displacement parameters were refined with O—H distance restraints of 0.88 Å and H⋯H restraints of 1.4 Å. Uiso(H) values for the water H atoms were set equal to 1.25Ueq(O). Refinement of the absolute structure parameter (Flack, 1983[Flack, H. D. (1983). Acta Cryst. A39, 876-881.]) gave ambiguous results, indicating that the absolute structure of (II[link]) could not be accurately determined from the diffraction data, even with the presence of a Cl atom; thus Friedel opposites were merged. For (II[link]), the number of Friedel pairs is 837. The high Rint value was the result of weak high-angle data.

For compound (I[link]), data collection, cell refinement and data reduction: SMART (Bruker, 2001[Bruker (2001). SMART. Version 5.624. Bruker AXS Inc., Madison, Wisconsin, USA.]). For compound (II[link]), data collection and cell refinement: DENZO (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.]) and COLLECT (Nonius, 1998[Nonius (1998). COLLECT. Nonius BV, Delft, The Netherlands.]); data reduction: DENZO, SCALEPACK (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.]) and COLLECT. For both compounds, program(s) used to solve structure: SHELXS97 (Sheldrick, 1997[Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany.]); program(s) used to refine structure: 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.]).

Supporting information


Comment top

2-Amino-4-phenyl-1,3-thiazole has both pharmaceutical and industrial applications (Au-Alvarez et al., 1999), including corrosion inhibition (Form et al., 1974); the structures of 2-amino-4-phenylthiazole and its hydrobromide hydrate salt are reported, respectively, in these two references. We have recently reviewed the structures of 2-amino-4-phenylthiazole derivatives in terms of their hydrogen-bonding patterns, specifically highlighting any involvement of the thiazole S atom (Lynch et al., 2002). Since that paper, the structures of two more derivatives have been reported (Bernes et al., 2002; Karanik et al., 2003). Several of the analogues that we reported in 2002, such as 2-amino-4-tolyl-1,3-thiazole, either packed quite simply as hydrogen-bonded R22(8) graph set (Etter, 1990) dimers through N—H···N interactions, or displayed packing networks containing these dimers. In the cases where molecules did not associate via N—H···N dimers, and no other anions or water molecules were present, N—H···S interactions were observed. The molecular arrangements in both the Bernes et al. and Karanik et al. structures also included N—H···N dimers. As a continuation of our 2002 study into the packing modes of 2-amino-4-phenyl-1,3-thiazole derivatives, we have further determined the structures of 2-acetamido-4-tolyl-1,3-thiazole, (I), and 2-amino-4-tolyl-1,3-thiazolium chloride dihydrate, (II), and report them here. As seen in two structures discussed in our 2002 paper, the packing modes of 2-amino-4-phenyl-1,3-thiazoles with additional anions and/or water molecules differ from the structures of the thiazole molecules by themselves. \sch

The structure of (I) consists of an essentially flat molecule (Fig. 1) which associates via a single N—H···O interaction, with alternate-facing molecules, to form a C22(4) graph set hydrogen-bonded chain (Fig. 2). The N—H···O chain interaction (Table 1) is one of two typical motifs displayed by amide linkages, with the other being an N—H···O hydrogen-bonded R22(8) graph set dimer (Desiraju, 1995). In other 2-acetamido-1,3-thiazole derivatives, of which there are four in the April 2004 version of the Cambridge Structural Database (CSD; Allen, 2002), none forms a hydrogen-bonded amide chain similar to (I). Instead, one, N-(5-nitro-2-thiazolyl)-acetamide (Peeters et al., 1985), forms an R22(8) N—H···N hydrogen-bonded dimer, while the other three structures contain additional lattice elements, such as anions, cations and/or water molecules. Furthermore, of 12 2-acetamido-1,3,4-thiadiazole derivatives found in the CSD, only one, 2-acetamido-4-benzoyl-5,5-dimethyl-4,5-dihydro-1,3,4-thiadiazoline (Kuban & Schulz, 1987), packs with a hydrogen-bonded amide chain. Interestingly, this molecule contains a bulky substituent in the 4-position, similar to (I), whereas those molecules without such substituents predominantly pack as N—H···N dimers. In (I), the dihedral angle between the thiazole and phenyl rings is 2.9 (1)°. The comparative dihedral angle in 2-amino-4-tolylthiazole is 12.80 (8)°.

The structure of (II) consists of an essentially flat 2-amino-4-tolyl-1,3-thiazolium molecule, a Cl anion and two water molecules (Fig. 3), associated in a hydrogen-bonded network. The CSD reveals that there are seven previously reported 2-amino-1,3-thiazolium halide (either Cl or Br) structures, with three of these being monohydrates; thus (II) is unique in being the first reported dihydrate. In all of the reported structures, the halide anion associates with either N3 or N21, or both, although across these examples, all of the hydrate structures have N3+—H associating to a water O atom. Alternatively, in (II), the same Cl atom (details of hydrogen-bonding interactions in Table 2) associates to both N3 and N21, similar to three non-hydrate structures, with the second H atom from N21 forming a hydrogen bond to a symmetry-equivalent water O atom [O1Wii; Fig. 4; symmetry code: (ii) 1 − x, y − 1/2, 1/2 − z]. The Cl atom and the two water molecules associate, via hydrogen-bonding interactions, to construct a convoluted hydrogen-bonded ribbon network which runs in the a cell direction. This ribbon network is made up of five-membered donor-acceptor rings, involving three water O atoms (with associated H atoms) and two Cl atoms [Cl1, O1W, O2Wiii, Cliii and O2W in Fig. 4; R35(10) graph set; symmetry code: (iii) x − 1/2, 3/2 − y, −z], fused along the O2W—H···Cl hydrogen-bond. In addition to the hydrogen-bonding associations to Cl1 and O1W, the thiazolium molecules stack in a column co-directional with the anion-water ribbon. The thiazolium columns comprise alternate-facing molecules, with the perpendicular distances between thiazole-phenyl and phenyl-thiazole ring centroids being 3.60 (1) and 3.67 (1) Å, respectively, and with the closest contact distance being 3.35 (1) Å from C4 to C42(x + 1/2, 1/2 − y, −z).

For (II), the dihedral angle between the thiazole and phenyl rings is 10.39 (7)°, which compares with 19 (1)° for 2-amino-4-phenyl-1,3-thiazolium bromide hydrate (Form et al., 1974) and 7.3 (2)° for 2-amino-4-(naphthyl)-1,3-thiazolium bromide (Lynch et al., 2002). Also noteworthy in (II) is the indication of a delocalized double bond across the N3—C2—N21 site, with distances of 1.322 (8) (C2—N21) and 1.342 (8) Å (C2—N3), compared with distances of 1.351 (2) and 1.309 (2) Å, respectively, for 2-amino-4-tolylthiazole. Similar differences, of 1.30 (2) and 1.33 (2) Å, respectively, for 2-amino-4-phenyl-1,3-thiazolium bromide hydrate, and 1.347 (5) and 1.298 (5) Å, respectively, for 2-amino-4-phenyl-1,3-thiazole itself [dihedral angle in this molecule 6.2 (3)°], are also noted. The hydrogen-bonding coordination surrounding the Cl atom is interesting, because without the N21—H21···Cl1 association, the remaining four-coordinate motif is pseudo-tetrahedral, with H···Cl···H angles from H3 being 94 (3), 118 (3) and 122 (3)°, and the three remaining angles being 105 (3), 105 (3) and 110 (3)°. The addition of the N21—H21···Cl1 association thus creates a five-coordinate pseudo-face-capped tetrahedral arrangement, not observed amongst the seven previously reported 2-amino-1,3-thiazolium halide structures.

Experimental top

Both compounds were obtained from Key Organics Ltd., and crystals were grown from ethanol solutions.

Refinement top

All H atoms, except for the N—H atom and the water H atoms in (II), were included in the refinement at calculated positions, in the riding-model approximation, with N—H distances of 0.88 Å, and C—H distances of 0.95 (aromatic H atoms) and 0.98 Å (methyl H atoms), and with Uiso(H) = 1.25Ueq(C,N). The N—H atom in (II) was located in Fourier syntheses and both its positional and displacement parameters were refined. The water H atoms in (II) were also located in Fourier syntheses, but its positional and displacement parameters were refined with O—H distance restraints of 0.88 Å and H···H restraints of 1.4 Å. Uiso(H) values for the water H atoms were set equal to 1.25Ueq(O). Refinement of the absolute structure parameter (Flack, 1983) gave ambiguous results, indicating that the absolute structure of (II) could not be accurately determined from the diffraction data, even with the presence of a Cl atom; thus Friedel opposites were merged. For (II), the number of Friedel pairs is 837. The high Rint value was the result of weak high-angle data.

Computing details top

Data collection: SMART (Bruker, 2001) for (I); DENZO (Otwinowski & Minor, 1997) and COLLECT (Nonius, 1998) for (II). Cell refinement: SMART for (I); DENZO and COLLECT for (II). Data reduction: SMART for (I); DENZO, SCALEPACK (Otwinowski & Minor, 1997) and COLLECT for (II). For both compounds, program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. The molecular configuration and atom-numbering scheme for (I). Displacement ellipsoids are drawn at the 50% probability level and H atoms are shown as small spheres of arbitrary radii.
[Figure 2] Fig. 2. A packing diagram for (I), viewed down the a axis. [Symmetry code: (i) x + 1/2, 1/2 − y, z − 1/2.]
[Figure 3] Fig. 3. The molecular configuration and atom-numbering scheme for (II). Displacement ellipsoids are drawn at the 50% probability level and H atoms are shown as small spheres of arbitrary radii.
[Figure 4] Fig. 4. A packing diagram for (II). [Symmetry codes: (ii) 1 − x, y − 1/2, 1/2 − z; (iii) x − 1/2, 3/2 − y, −z.]
(I) 2-Acetamido-4-p-tolyl-1,3-thiazole top
Crystal data top
C12H12N2OSF(000) = 488
Mr = 232.30Dx = 1.367 Mg m3
Monoclinic, P21/nSynchrotron radiation, λ = 0.6894 Å
Hall symbol: -P 2ynCell parameters from 1753 reflections
a = 3.9541 (5) Åθ = 2.7–28.2°
b = 37.484 (5) ŵ = 0.27 mm1
c = 7.7173 (9) ÅT = 120 K
β = 99.338 (2)°Plate, colourless
V = 1128.7 (2) Å30.05 × 0.03 × 0.002 mm
Z = 4
Data collection top
Bruker SMART 1K CCD area-detector
diffractometer
1770 reflections with I > 2σ(I)
Radiation source: Daresbury SRS Station 9.8 (Cernik et al., 1997; Clegg, 2000)Rint = 0.040
Silicon 111 monochromatorθmax = 26.0°, θmin = 2.1°
Detector resolution: 8.192 pixels mm-1h = 52
ω rotation with narrow frames scansk = 4447
6723 measured reflectionsl = 99
2407 independent reflections
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)] = 0.049Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.126H atoms treated by a mixture of independent and constrained refinement
S = 1.08 w = 1/[σ2(Fo2) + (0.0604P)2 + 0.4975P]
where P = (Fo2 + 2Fc2)/3
2407 reflections(Δ/σ)max < 0.001
151 parametersΔρmax = 0.32 e Å3
0 restraintsΔρmin = 0.32 e Å3
Crystal data top
C12H12N2OSV = 1128.7 (2) Å3
Mr = 232.30Z = 4
Monoclinic, P21/nSynchrotron radiation, λ = 0.6894 Å
a = 3.9541 (5) ŵ = 0.27 mm1
b = 37.484 (5) ÅT = 120 K
c = 7.7173 (9) Å0.05 × 0.03 × 0.002 mm
β = 99.338 (2)°
Data collection top
Bruker SMART 1K CCD area-detector
diffractometer
1770 reflections with I > 2σ(I)
6723 measured reflectionsRint = 0.040
2407 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0490 restraints
wR(F2) = 0.126H atoms treated by a mixture of independent and constrained refinement
S = 1.08Δρmax = 0.32 e Å3
2407 reflectionsΔρmin = 0.32 e Å3
151 parameters
Special details top

Geometry. Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane)

3.4460 (0.0017) x − 2.8824 (0.0477) y + 2.5969 (0.0060) z = 3.7007 (0.0085)

* −0.0014 (0.0011) S1 * −0.0004 (0.0014) C2 * 0.0025 (0.0015) N3 * −0.0039 (0.0016) C4 * 0.0032 (0.0015) C5

Rms deviation of fitted atoms = 0.0026

3.5389 (0.0021) x − 2.3368 (0.0465) y + 2.2430 (0.0086) z = 3.6065 (0.0047)

Angle to previous plane (with approximate e.s.d.) = 2.91 (0.13)

* −0.0026 (0.0019) C41 * 0.0006 (0.0020) C42 * 0.0028 (0.0021) C43 * −0.0043 (0.0021) C44 * 0.0023 (0.0022) C45 * 0.0011 (0.0021) C46

Rms deviation of fitted atoms = 0.0026

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.49456 (18)0.165388 (17)0.95180 (8)0.02014 (19)
C20.6413 (6)0.18746 (6)0.7819 (3)0.0175 (5)
N30.7199 (5)0.16755 (5)0.6567 (2)0.0181 (4)
C40.6624 (7)0.13189 (6)0.6909 (3)0.0180 (5)
C50.5445 (7)0.12616 (7)0.8438 (3)0.0213 (6)
H50.49540.10330.88610.027*
N210.6790 (6)0.22419 (5)0.7745 (3)0.0180 (5)
H210.761 (7)0.2330 (7)0.682 (4)0.021 (7)*
C220.5850 (7)0.24777 (7)0.8913 (3)0.0182 (5)
O220.4597 (5)0.23738 (5)1.0180 (2)0.0229 (4)
C230.6423 (7)0.28629 (6)0.8541 (3)0.0205 (5)
H2310.56670.30100.94540.026*
H2320.51100.29260.73940.026*
H2330.88680.29040.85310.026*
C410.7322 (7)0.10513 (6)0.5611 (3)0.0200 (5)
C420.8383 (8)0.11578 (7)0.4062 (3)0.0261 (6)
H420.86810.14050.38520.033*
C430.9016 (8)0.09101 (8)0.2815 (4)0.0282 (6)
H430.97500.09900.17690.035*
C440.8595 (7)0.05489 (8)0.3072 (4)0.0284 (6)
C450.7557 (8)0.04429 (7)0.4627 (4)0.0341 (7)
H450.72770.01960.48370.043*
C460.6919 (8)0.06869 (7)0.5884 (4)0.0283 (6)
H460.62040.06060.69340.035*
C470.9250 (9)0.02808 (8)0.1707 (4)0.0402 (8)
H4711.17040.02260.18610.050*
H4720.85080.03800.05320.050*
H4730.79630.00620.18420.050*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0254 (4)0.0209 (3)0.0154 (3)0.0006 (3)0.0069 (2)0.0009 (2)
C20.0183 (13)0.0202 (12)0.0133 (11)0.0005 (10)0.0004 (9)0.0012 (9)
N30.0205 (11)0.0192 (10)0.0145 (9)0.0015 (9)0.0026 (8)0.0003 (8)
C40.0202 (13)0.0161 (12)0.0170 (11)0.0001 (10)0.0007 (10)0.0008 (9)
C50.0270 (15)0.0178 (12)0.0195 (12)0.0007 (11)0.0050 (11)0.0001 (10)
N210.0240 (12)0.0176 (10)0.0134 (10)0.0002 (9)0.0061 (9)0.0004 (8)
C220.0194 (13)0.0207 (12)0.0146 (11)0.0017 (10)0.0030 (10)0.0028 (9)
O220.0320 (11)0.0223 (9)0.0166 (9)0.0003 (8)0.0108 (8)0.0004 (7)
C230.0255 (14)0.0184 (12)0.0187 (12)0.0001 (10)0.0066 (10)0.0011 (10)
C410.0201 (13)0.0196 (13)0.0193 (12)0.0004 (10)0.0003 (10)0.0025 (10)
C420.0361 (16)0.0212 (13)0.0211 (13)0.0029 (12)0.0047 (12)0.0023 (10)
C430.0319 (16)0.0320 (15)0.0198 (13)0.0047 (12)0.0014 (12)0.0045 (11)
C440.0260 (15)0.0291 (15)0.0286 (15)0.0026 (12)0.0001 (12)0.0103 (11)
C450.0379 (18)0.0177 (14)0.0469 (18)0.0007 (13)0.0076 (15)0.0071 (12)
C460.0319 (16)0.0226 (14)0.0322 (15)0.0019 (12)0.0103 (13)0.0006 (11)
C470.046 (2)0.0356 (17)0.0393 (18)0.0028 (15)0.0092 (16)0.0163 (13)
Geometric parameters (Å, º) top
S1—C51.717 (3)C41—C421.388 (4)
S1—C21.728 (2)C41—C461.395 (4)
C2—N31.298 (3)C42—C431.389 (4)
C2—N211.387 (3)C42—H420.95
N3—C41.388 (3)C43—C441.382 (4)
C4—C51.354 (3)C43—H430.95
C4—C411.475 (3)C44—C451.388 (4)
C5—H50.95C44—C471.508 (4)
N21—C221.357 (3)C45—C461.386 (4)
N21—H210.89 (3)C45—H450.95
C22—O221.229 (3)C46—H460.95
C22—C231.496 (3)C47—H4710.98
C23—H2310.98C47—H4720.98
C23—H2320.98C47—H4730.98
C23—H2330.98
C5—S1—C287.86 (12)C42—C41—C4120.3 (2)
N3—C2—N21120.0 (2)C46—C41—C4121.6 (2)
N3—C2—S1116.09 (18)C43—C42—C41121.2 (3)
N21—C2—S1123.95 (18)C43—C42—H42119.4
C2—N3—C4110.2 (2)C41—C42—H42119.4
C5—C4—N3114.1 (2)C44—C43—C42121.1 (3)
C5—C4—C41127.8 (2)C44—C43—H43119.5
N3—C4—C41118.1 (2)C42—C43—H43119.5
C4—C5—S1111.72 (19)C43—C44—C45117.6 (2)
C4—C5—H5124.1C43—C44—C47121.0 (3)
S1—C5—H5124.1C45—C44—C47121.4 (3)
C22—N21—C2125.2 (2)C46—C45—C44122.0 (3)
C22—N21—H21117.7 (18)C46—C45—H45119.0
C2—N21—H21117.1 (18)C44—C45—H45119.0
O22—C22—N21120.7 (2)C45—C46—C41120.1 (3)
O22—C22—C23123.5 (2)C45—C46—H46119.9
N21—C22—C23115.8 (2)C41—C46—H46119.9
C22—C23—H231109.5C44—C47—H471109.5
C22—C23—H232109.5C44—C47—H472109.5
H231—C23—H232109.5H471—C47—H472109.5
C22—C23—H233109.5C44—C47—H473109.5
H231—C23—H233109.5H471—C47—H473109.5
H232—C23—H233109.5H472—C47—H473109.5
C42—C41—C46118.0 (2)
C5—S1—C2—N30.0 (2)N3—C4—C41—C422.7 (4)
C5—S1—C2—N21179.6 (2)C5—C4—C41—C462.5 (4)
N21—C2—N3—C4180.0 (2)N3—C4—C41—C46177.9 (2)
S1—C2—N3—C40.4 (3)C46—C41—C42—C430.2 (4)
C2—N3—C4—C50.7 (3)C4—C41—C42—C43179.3 (3)
C2—N3—C4—C41179.0 (2)C41—C42—C43—C440.3 (4)
N3—C4—C5—S10.7 (3)C42—C43—C44—C450.7 (4)
C41—C4—C5—S1179.0 (2)C42—C43—C44—C47179.4 (3)
C2—S1—C5—C40.4 (2)C43—C44—C45—C460.7 (5)
N3—C2—N21—C22175.6 (2)C47—C44—C45—C46179.4 (3)
S1—C2—N21—C224.8 (4)C44—C45—C46—C410.2 (5)
C2—N21—C22—O221.1 (4)C42—C41—C46—C450.3 (4)
C2—N21—C22—C23178.5 (2)C4—C41—C46—C45179.2 (3)
C5—C4—C41—C42177.0 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N21—H21···O22i0.89 (3)1.95 (3)2.818 (3)166 (3)
Symmetry code: (i) x+1/2, y+1/2, z1/2.
(II) 2-amino-4-tolyl-1,3-thiazolium chloride dihydrate top
Crystal data top
C10H11N2S+·Cl·2H2OF(000) = 552
Mr = 262.75Dx = 1.397 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 2244 reflections
a = 6.8815 (6) Åθ = 2.9–27.1°
b = 9.3072 (14) ŵ = 0.46 mm1
c = 19.499 (3) ÅT = 120 K
V = 1248.9 (3) Å3Needle, colourless
Z = 40.35 × 0.02 × 0.02 mm
Data collection top
Nonius KappaCCD area-detector
diffractometer
1048 reflections with I > 2σ(I)
Radiation source: Bruker Nonius FR591 rotating anodeRint = 0.156
Graphite monochromatorθmax = 26.0°, θmin = 3.0°
Detector resolution: 9.091 pixels mm-1h = 88
ϕ and ω scansk = 911
9123 measured reflectionsl = 2324
1441 independent reflections
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)] = 0.063Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.152H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.0775P)2 + 0.1085P]
where P = (Fo2 + 2Fc2)/3
1441 reflections(Δ/σ)max < 0.001
159 parametersΔρmax = 0.44 e Å3
6 restraintsΔρmin = 0.47 e Å3
Crystal data top
C10H11N2S+·Cl·2H2OV = 1248.9 (3) Å3
Mr = 262.75Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 6.8815 (6) ŵ = 0.46 mm1
b = 9.3072 (14) ÅT = 120 K
c = 19.499 (3) Å0.35 × 0.02 × 0.02 mm
Data collection top
Nonius KappaCCD area-detector
diffractometer
1048 reflections with I > 2σ(I)
9123 measured reflectionsRint = 0.156
1441 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0636 restraints
wR(F2) = 0.152H atoms treated by a mixture of independent and constrained refinement
S = 1.06Δρmax = 0.44 e Å3
1441 reflectionsΔρmin = 0.47 e Å3
159 parameters
Special details top

Geometry. Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane)

6.8444 (0.0021) x + 0.9623 (0.0236) y − 0.1571 (0.0462) z = 4.5106 (0.0062)

* 0.0027 (0.0047) C41 * −0.0022 (0.0049) C42 * 0.0001 (0.0049) C43 * 0.0015 (0.0043) C44 * −0.0010 (0.0047) C45 * −0.0011 (0.0050) C46

Rms deviation of fitted atoms = 0.0016

6.8599 (0.0018) x − 0.7208 (0.0273) y − 0.3258 (0.0468) z = 4.2195 (0.0099)

Angle to previous plane (with approximate e.s.d.) = 10.39 (0.07)

* −0.0004 (0.0030) S1 * −0.0028 (0.0037) C2 * 0.0053 (0.0042) N3 * −0.0057 (0.0043) C4 * 0.0035 (0.0038) C5

Rms deviation of fitted atoms = 0.0040

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.6173 (2)0.10019 (18)0.17494 (9)0.0381 (5)
N30.6432 (7)0.2996 (5)0.0877 (3)0.0312 (12)
H30.65470.38550.06930.039*
N210.6430 (7)0.3850 (6)0.2005 (3)0.0354 (12)
H210.65210.47420.18600.044*
H220.63830.36670.24470.044*
C20.6365 (9)0.2782 (7)0.1558 (3)0.0339 (15)
C40.6302 (9)0.1739 (6)0.0486 (3)0.0295 (14)
C50.6176 (10)0.0580 (7)0.0872 (3)0.0398 (16)
H50.60960.03700.06960.050*
C410.6339 (9)0.1855 (7)0.0270 (3)0.0309 (14)
C420.6516 (9)0.0617 (7)0.0679 (3)0.0349 (15)
H420.66330.03020.04710.044*
C430.6518 (9)0.0744 (7)0.1385 (3)0.0355 (16)
H430.66430.00970.16580.044*
C440.6342 (9)0.2060 (7)0.1704 (4)0.0347 (14)
C450.6158 (9)0.3280 (7)0.1304 (3)0.0327 (15)
H450.60310.41970.15140.041*
C460.6158 (9)0.3156 (7)0.0592 (3)0.0335 (15)
H460.60300.39990.03210.042*
C470.6348 (10)0.2194 (7)0.2479 (3)0.0392 (16)
H4710.58300.13110.26830.049*
H4720.55370.30110.26160.049*
H4730.76820.23470.26400.049*
Cl10.6618 (2)0.63450 (17)0.07781 (8)0.0390 (5)
O1W0.3448 (7)0.7854 (6)0.1681 (2)0.0447 (12)
H11W0.432 (7)0.741 (8)0.143 (3)0.056*
H12W0.240 (6)0.787 (8)0.142 (3)0.056*
O2W0.5451 (7)0.6804 (5)0.0803 (3)0.0437 (12)
H21W0.447 (7)0.739 (6)0.086 (3)0.055*
H22W0.556 (10)0.669 (8)0.0358 (12)0.055*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0377 (9)0.0418 (9)0.0347 (9)0.0028 (8)0.0041 (8)0.0082 (8)
N30.029 (3)0.040 (3)0.024 (3)0.002 (2)0.002 (2)0.003 (2)
N210.037 (3)0.042 (3)0.027 (3)0.002 (3)0.002 (2)0.003 (2)
C20.028 (3)0.046 (4)0.027 (4)0.002 (3)0.001 (3)0.009 (3)
C40.033 (3)0.027 (3)0.028 (3)0.003 (3)0.004 (3)0.000 (3)
C50.041 (4)0.043 (4)0.036 (4)0.005 (3)0.002 (3)0.006 (3)
C410.030 (3)0.035 (4)0.027 (3)0.000 (3)0.001 (3)0.000 (3)
C420.037 (4)0.036 (4)0.031 (4)0.003 (3)0.005 (3)0.005 (3)
C430.030 (3)0.037 (4)0.039 (4)0.004 (3)0.004 (3)0.010 (3)
C440.026 (3)0.049 (4)0.030 (3)0.001 (3)0.002 (3)0.004 (3)
C450.032 (3)0.036 (4)0.029 (3)0.001 (3)0.004 (3)0.007 (3)
C460.036 (4)0.037 (4)0.028 (3)0.005 (3)0.003 (3)0.006 (3)
C470.039 (4)0.051 (4)0.028 (4)0.002 (4)0.008 (3)0.005 (3)
Cl10.0406 (9)0.0407 (9)0.0357 (9)0.0016 (7)0.0011 (8)0.0008 (8)
O1W0.046 (3)0.062 (3)0.026 (3)0.000 (3)0.000 (2)0.008 (2)
O2W0.045 (3)0.054 (3)0.032 (3)0.009 (2)0.002 (2)0.007 (3)
Geometric parameters (Å, º) top
S1—C21.704 (7)C43—C441.379 (9)
S1—C51.755 (7)C43—H430.95
N3—C21.342 (8)C44—C451.383 (9)
N3—C41.400 (8)C44—C471.516 (9)
N3—H30.88C45—C461.395 (9)
N21—C21.322 (8)C45—H450.95
N21—H210.88C46—H460.95
N21—H220.88C47—H4710.98
C4—C51.318 (9)C47—H4720.98
C4—C411.479 (9)C47—H4730.98
C5—H50.95O1W—H11W0.88 (6)
C41—C461.369 (9)O1W—H12W0.88 (5)
C41—C421.407 (9)O2W—H21W0.88 (5)
C42—C431.382 (9)O2W—H22W0.88 (2)
C42—H420.95
C2—S1—C590.2 (3)C41—C42—H42120.2
C2—N3—C4114.4 (5)C42—C43—C44121.7 (6)
C2—N3—H3122.8C42—C43—H43119.2
C4—N3—H3122.8C44—C43—H43119.2
C2—N21—H21120.0C43—C44—C45118.9 (6)
C2—N21—H22120.0C43—C44—C47121.5 (6)
H21—N21—H22120.0C45—C44—C47119.6 (6)
N21—C2—N3122.6 (6)C44—C45—C46119.6 (6)
N21—C2—S1126.1 (5)C44—C45—H45120.2
N3—C2—S1111.3 (5)C46—C45—H45120.2
C5—C4—N3112.1 (5)C41—C46—C45121.9 (6)
C5—C4—C41129.1 (6)C41—C46—H46119.0
N3—C4—C41118.8 (5)C45—C46—H46119.0
C4—C5—S1111.9 (5)C44—C47—H471109.5
C4—C5—H5124.0C44—C47—H472109.5
S1—C5—H5124.0H471—C47—H472109.5
C46—C41—C42118.2 (6)C44—C47—H473109.5
C46—C41—C4121.3 (6)H471—C47—H473109.5
C42—C41—C4120.4 (5)H472—C47—H473109.5
C43—C42—C41119.6 (6)H11W—O1W—H12W104 (3)
C43—C42—H42120.2H21W—O2W—H22W105 (3)
C4—N3—C2—N21178.7 (6)N3—C4—C41—C42170.1 (6)
C4—N3—C2—S10.9 (8)C46—C41—C42—C430.5 (10)
C5—S1—C2—N21179.2 (7)C4—C41—C42—C43179.0 (6)
C5—S1—C2—N30.3 (5)C41—C42—C43—C440.3 (11)
C2—N3—C4—C51.2 (9)C42—C43—C44—C450.1 (10)
C2—N3—C4—C41179.3 (6)C42—C43—C44—C47179.9 (6)
N3—C4—C5—S11.0 (8)C43—C44—C45—C460.2 (10)
C41—C4—C5—S1179.6 (6)C47—C44—C45—C46179.8 (6)
C2—S1—C5—C40.4 (6)C42—C41—C46—C450.4 (10)
C5—C4—C41—C46169.2 (7)C4—C41—C46—C45178.9 (6)
N3—C4—C41—C4611.4 (10)C44—C45—C46—C410.1 (11)
C5—C4—C41—C429.2 (12)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3···Cl10.882.323.126 (5)151
N21—H21···Cl10.882.583.337 (6)144
N21—H22···O1Wi0.881.862.726 (7)166
O1W—H11W···Cl10.88 (6)2.26 (6)3.136 (5)178 (7)
O1W—H12W···O2Wii0.88 (5)1.83 (3)2.700 (7)169 (8)
O2W—H22W···Cl10.88 (2)2.35 (2)3.214 (5)167 (6)
O2W—H21W···Cl1ii0.88 (5)2.29 (3)3.151 (5)166 (6)
Symmetry codes: (i) x+1, y1/2, z1/2; (ii) x1/2, y+3/2, z.

Experimental details

(I)(II)
Crystal data
Chemical formulaC12H12N2OSC10H11N2S+·Cl·2H2O
Mr232.30262.75
Crystal system, space groupMonoclinic, P21/nOrthorhombic, P212121
Temperature (K)120120
a, b, c (Å)3.9541 (5), 37.484 (5), 7.7173 (9)6.8815 (6), 9.3072 (14), 19.499 (3)
α, β, γ (°)90, 99.338 (2), 9090, 90, 90
V3)1128.7 (2)1248.9 (3)
Z44
Radiation typeSynchrotron, λ = 0.6894 ÅMo Kα
µ (mm1)0.270.46
Crystal size (mm)0.05 × 0.03 × 0.0020.35 × 0.02 × 0.02
Data collection
DiffractometerBruker SMART 1K CCD area-detector
diffractometer
Nonius KappaCCD area-detector
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
6723, 2407, 1770 9123, 1441, 1048
Rint0.0400.156
(sin θ/λ)max1)0.6360.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.049, 0.126, 1.08 0.063, 0.152, 1.06
No. of reflections24071441
No. of parameters151159
No. of restraints06
H-atom treatmentH atoms treated by a mixture of independent and constrained refinementH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.32, 0.320.44, 0.47

Computer programs: SMART (Bruker, 2001), DENZO (Otwinowski & Minor, 1997) and COLLECT (Nonius, 1998), SMART, DENZO and COLLECT, DENZO, SCALEPACK (Otwinowski & Minor, 1997) and COLLECT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2003), SHELXL97.

Hydrogen-bond geometry (Å, º) for (I) top
D—H···AD—HH···AD···AD—H···A
N21—H21···O22i0.89 (3)1.95 (3)2.818 (3)166 (3)
Symmetry code: (i) x+1/2, y+1/2, z1/2.
Hydrogen-bond geometry (Å, º) for (II) top
D—H···AD—HH···AD···AD—H···A
N3—H3···Cl10.882.323.126 (5)151
N21—H21···Cl10.882.583.337 (6)144
N21—H22···O1Wi0.881.862.726 (7)166
O1W—H11W···Cl10.88 (6)2.26 (6)3.136 (5)178 (7)
O1W—H12W···O2Wii0.88 (5)1.83 (3)2.700 (7)169 (8)
O2W—H22W···Cl10.88 (2)2.35 (2)3.214 (5)167 (6)
O2W—H21W···Cl1ii0.88 (5)2.29 (3)3.151 (5)166 (6)
Symmetry codes: (i) x+1, y1/2, z1/2; (ii) x1/2, y+3/2, z.
 

Acknowledgements

The authors thank the EPSRC National Crystallography Service, Southampton, and the EPSRC Chemical Database Service at Daresbury.

References

First citationAllen, F. H. (2002). Acta Cryst. B58, 380–388.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationAu-Alvarez, O., Peterson, R. C., Acosta Crespo, A., Rodríguez Esteva, Y., Marquez Alvarez, H., Plutín Stiven, A. M. & Pomés Hernández, R. (1999). Acta Cryst. C55, 821–823.  Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
First citationBernès, S., Berros, M. I., Rodríguez de Barbarín, C. & Sánchez-Viesca, F. (2002). Acta Cryst. C58, o151–o153.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationBruker (2001). SMART. Version 5.624. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationCernik, R. J., Clegg, W., Catlow, C. R. A., Bushnell-Wye, G., Flaherty, J. V., Greaves, G. N., Burrows, I., Taylor, D. J., Teat, S. J. & Hamichi, M. (1997). J. Synchotron Rad. 4, 279–286; erratum, 7, 40.  Google Scholar
First citationClegg, W. (2000). J. Chem. Soc. Dalton Trans. pp. 3223–3232.  Web of Science CrossRef Google Scholar
First citationDesiraju, G. R. (1995). Angew. Chem. Int. Ed. Engl. 34, 2311–2327.  CrossRef CAS Web of Science Google Scholar
First citationEtter, M. C. (1990). Acc. Chem. Res. 23, 120–126.  CrossRef CAS Web of Science Google Scholar
First citationFlack, H. D. (1983). Acta Cryst. A39, 876–881.  CrossRef CAS Web of Science IUCr Journals Google Scholar
First citationForm, G. R., Raper, E. S. & Downie, T. C. (1974). Acta Cryst. B30, 342–348.  CSD CrossRef CAS IUCr Journals Web of Science Google Scholar
First citationKaranik, M., Patzel, M. & Liebscher, J. (2003). Synthesis, pp. 1201–1208.  Google Scholar
First citationKuban, R.-J. & Schulz, B. (1987). Cryst. Res. Technol. 22, 799–802.  CrossRef CAS Web of Science Google Scholar
First citationLynch, D. E., McClenaghan, I., Light, M. E. & Coles, S. J. (2002). Cryst. Eng. 5, 123–136.  Web of Science CSD CrossRef CAS Google Scholar
First citationNonius (1998). COLLECT. Nonius BV, Delft, The Netherlands.  Google Scholar
First citationOtwinowski, 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.  Google Scholar
First citationPeeters, O. M., Blaton, N. M. & De Ranter, C. J. (1985). Acta Cryst. C41, 965–967.  CSD CrossRef CAS Web of Science IUCr Journals Google Scholar
First citationSheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany.  Google Scholar
First citationSpek, A. L. (2003). J. Appl. Cryst. 36, 7–13.  Web of Science CrossRef CAS IUCr Journals Google Scholar

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