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Details of the structures of two conformational polymorphs of the title compound, C12H17N2OS+·Cl, are reported. In form (I) (space group P\overline{1}), the two N—H groups of the cation are in a trans conformation, while in form (II) (space group P21/c), they are in a cis arrangement. This results in different packing and hydrogen-bond arrangements in the two forms, both of which have extended chains lying along the a direction. In form (I), these chains are composed of centrosymmetric R42(18) (N—H...Cl and O—H...Cl) hydrogen-bonded rings and R22(18) (N—H...O) hydrogen-bonded rings. In form (II), the chains are formed by centrosymmetric R42(18) (N—H...Cl and O—H...Cl) hydrogen-bonded rings and by R42(12) (N—H...Cl) hydrogen-bonded rings.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270110045099/fg3203sup1.cif
Contains datablocks global, I, II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270110045099/fg3203Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270110045099/fg3203IIsup3.hkl
Contains datablock II

CCDC references: 810016; 810017

Comment top

Polymorphism, the phenomenon of a given molecule existing in more than one crystal structure, is a normal observation for organics (McCrone, 1965). Polymorphism is of great importance in pharmaceuticals as well as in materials science, because individual forms may have different physicochemical properties which can potentially lead to new formulations or new materials. Conformational polymorphism, a branch of polymorphism, is particularly interesting since it provides ideal cases for structure–property relationship studies (Bernstein, 2002, 1987). Conformational polymorphism arises from intrinsic molecular flexibility and is the result of a compromise between inter- and intramolecular interactions.

The free base of the title compound, (1), is the principal metabolite fragment recovered from equine urine after enzymatic hydrolysis of xylazine [N-(2,6-dimethylphenyl)-5,6-dihydro-4H-1,3-thiazin-2-amine], which is a relatively short-acting α-2 agonist tranquilizer widely used in equine medicine. Optimal regulatory control of the use of xylazine is dependent on the detection and quantification of urinary metabolites or metabolite fragments such as the free base of (1) (Mutlib et al., 1992). We report here the conformational polymorphism of (1), which occurs in two crystalline forms, viz. (I) and (II).

Our analysis establishes that form (I) is triclinic (space group P1) and form (II) monoclinic (space group P21/c), with one formula unit in the asymmetric unit in each case. Views of forms (I) and (II) are given in Figs. 1 and 2, respectively. In both forms, imine atom N3 is protonated, and in both forms the six-membered heterocyclic ring has a half-chair conformation, with atom C5 0.704 (2) Å from the S1/C2/N3/C4/C6 plane in form (I) and 0.699 (2) Å from the same plane in form (II). The C2—N2 and C2—N3 bond lengths in (I) are 1.3296 (16) and 1.3180 (16) Å, respectively, and the corresponding values in (II) are 1.328 (2) and 1.322 (2) Å. These dimensions are entirely consistent with delocalization of the C2C3 double bond over the C2—N2—C3 moiety, as shown in structures (1a) and (1b) in the scheme. Thus, the two cations could either be considered as configurational isomers (with C2—N2 considered as a double bond), with form (I) the E isomer and form (II) the Z isomer, or as conformational isomers (with C2—N3 considered as the double bond). As seen in Figs. 1 and 2 (which have been drawn to have similar orientations of the six-membered heterocyclic rings), the principal difference between the two forms is in the orientation of the 4-hydroxy-2,6-dimethylaniline moiety with respect to the heterocyclic ring. In form (I), the S1—C2—N2—C11 torsion angle is -176.54 (9)°, while in form (II) the corresponding value is 3.0 (2)°.

Due to the conformational difference between the cations in the two polymorphs, the packing patterns are dissimilar. In polymorph (I) (Fig. 3), hydrogen bonds between the protonated imine NH group and the phenol O atom (N3—H3···O4i; see Table 1 for details) link two cations to form an 18-membered ring dimer centred at (1/2, 1/2, 1/2), with the hydrogen-bonded ring graph-set descriptor R22(18) (Bernstein et al., 1995). This dimer is further connected through hydrogen bonds between the Cl- ion and the hydroxy O4—H4 and secondary N2–H2 groups (details in Table 1) to form a second set of 18-membered rings, but this time with hydrogen-bond descriptor R42(18), lying about inversion centres at (0, 1/2, 1/2), (1, 1/2, 1/2), etc. This gives rise to a one-dimensional chain along the a axis of the triclinic cell.

In form (II) (Fig. 4), the cations are interconnected through hydrogen bonds between the Cl- ion and all three hydrogen-bonding donors, viz. O4—H4, imine N3—H3 and amino N2—H2 (details in Table 2). There is a 12-membered ring [centred at (1/2, 1/2, 1/2)] involving the N2—H2 and N3—H3 groups and the Cl- ion, with descriptor R42(12) (details in Table 2). This dimer is then connected via N2—H2···Cl1 and O4—H4···Cl1ii hydrogen bonds (Table 2) to generate 18-membered rings [centred at (0, 1/2, 1/2), (1, 1/2, 1/2), etc.] with descriptor R42(18), the same as in form (I). In this way, a one-dimensional chain is developed along the a axis of this monoclinic cell.

Our work has thus shown that the two crystalline forms discovered for (1) can either be considered as configurational or conformational isomers, due to the delocalisation of the amine lone-pair electrons over three atoms. The configurational/conformational variation in the two forms gives rise to differences in packing and hydrogen-bond arrangements in the crystal structures.

Experimental top

3,5-Dimethyl-4-isothiocyanatophenol (1.70 g, 9.50 mmol) was dissolved in dry dichloromethane (20 ml) and 3-aminopropanol (1.70 ml, 22.18 mmol) was added. The reaction mixture was refluxed overnight with stirring. The solution was then cooled down to room temperature and the solvent removed under reduced pressure to give the crude product. Concentrated hydrochloric acid solution (8 ml) was added to the crude product and the resulting solution was refluxed overnight with stirring. The solution was poured into 10% NaOH (50 ml) and stirred for 3 h. The final product (2.0 g, yield 90.9%) was precipitated using Dowex resin H+ form (pH = 1) (Kai et al., 2007). Crystals from methanol and ethanol were found to be the same and were designated as form (I), and those from propan-2-ol were form (II).

Refinement top

All H atoms were found in difference Fourier maps and were subsequently placed in idealized positions, with O—H = 0.82 Å, N—H = 0.86 Å, Csp2—H = 0.93 Å, Csp3—H = 0.97 Å for CH2 H atoms and 0.96 Å for methyl H atoms. All H atoms were allowed for as riding, with Uiso(H) = 1.5Ueq(parent atom) for O—H and methyl H atoms, and 1.2Ueq(parent atom) for all others.

Computing details top

For both compounds, data collection: COLLECT (Nonius, 2002); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP in SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008) and local procedures.

Figures top
[Figure 1] Fig. 1. The molecular structure of form (I) of (1), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level.
[Figure 2] Fig. 2. The molecular structure of form (II) of (1), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level.
[Figure 3] Fig. 3. The crystal packing of form (I). (For details of symmetry operations, see Table 1.)
[Figure 4] Fig. 4. The crystal packing of form (II). [For details of symmetry operations, see Table 2. Additionally, symmetry code: (iii) 1 + x, y, z.]
(I) 2-(4-hydroxy-2,6-dimethylanilino)-5,6-dihydro-4H-1,3-thiazin-3-ium chloride top
Crystal data top
C12H17N2OS+·ClZ = 2
Mr = 272.79F(000) = 288
Triclinic, P1Dx = 1.376 Mg m3
a = 6.9961 (1) ÅMo Kα radiation, λ = 0.71073 Å
b = 7.9421 (1) ÅCell parameters from 2964 reflections
c = 13.0864 (2) Åθ = 1.0–27.5°
α = 73.3925 (6)°µ = 0.44 mm1
β = 84.1579 (6)°T = 90 K
γ = 70.8388 (6)°Block, colourless
V = 658.17 (2) Å30.30 × 0.20 × 0.10 mm
Data collection top
Nonius KappaCCD area-detector
diffractometer
2981 independent reflections
Radiation source: fine-focus sealed tube2762 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.017
Detector resolution: 18 pixels mm-1θmax = 27.5°, θmin = 1.6°
ω scans at fixed χ = 55°h = 99
Absorption correction: multi-scan
(SCALEPACK; Otwinowski & Minor, 1997)
k = 1010
Tmin = 0.881, Tmax = 0.958l = 1616
5923 measured 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)] = 0.028Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.072H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.028P)2 + 0.3783P]
where P = (Fo2 + 2Fc2)/3
2981 reflections(Δ/σ)max = 0.001
156 parametersΔρmax = 0.32 e Å3
0 restraintsΔρmin = 0.28 e Å3
Crystal data top
C12H17N2OS+·Clγ = 70.8388 (6)°
Mr = 272.79V = 658.17 (2) Å3
Triclinic, P1Z = 2
a = 6.9961 (1) ÅMo Kα radiation
b = 7.9421 (1) ŵ = 0.44 mm1
c = 13.0864 (2) ÅT = 90 K
α = 73.3925 (6)°0.30 × 0.20 × 0.10 mm
β = 84.1579 (6)°
Data collection top
Nonius KappaCCD area-detector
diffractometer
2981 independent reflections
Absorption correction: multi-scan
(SCALEPACK; Otwinowski & Minor, 1997)
2762 reflections with I > 2σ(I)
Tmin = 0.881, Tmax = 0.958Rint = 0.017
5923 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0280 restraints
wR(F2) = 0.072H-atom parameters constrained
S = 1.03Δρmax = 0.32 e Å3
2981 reflectionsΔρmin = 0.28 e Å3
156 parameters
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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
S10.33096 (5)0.11563 (4)0.90302 (2)0.01881 (9)
O40.24327 (13)0.72281 (12)0.36708 (7)0.01848 (19)
H40.23690.68700.31340.028*
N20.23495 (15)0.17820 (14)0.74414 (8)0.0162 (2)
H20.11710.19160.77730.019*
N30.57340 (15)0.01012 (14)0.74502 (8)0.0158 (2)
H30.58680.09090.68490.019*
C20.39103 (18)0.03369 (16)0.78804 (9)0.0143 (2)
C40.75611 (19)0.14085 (17)0.78973 (10)0.0198 (3)
H4A0.87450.10240.76460.024*
H4B0.76710.24780.76510.024*
C50.7503 (2)0.1936 (2)0.91032 (11)0.0259 (3)
H5A0.73270.08530.93510.031*
H5B0.87790.28490.93750.031*
C60.5788 (2)0.2721 (2)0.95266 (11)0.0293 (3)
H6A0.57690.30141.02990.035*
H6B0.60430.38650.93310.035*
C110.24705 (17)0.31409 (16)0.64568 (9)0.0139 (2)
C120.24680 (17)0.27297 (16)0.54866 (10)0.0141 (2)
C130.24924 (17)0.40896 (16)0.45421 (9)0.0147 (2)
H130.25240.38330.38890.018*
C140.24696 (17)0.58294 (16)0.45753 (9)0.0148 (2)
C150.24651 (17)0.62147 (16)0.55438 (10)0.0158 (2)
H150.24510.73850.55530.019*
C160.24809 (17)0.48781 (16)0.65008 (10)0.0148 (2)
C170.23777 (19)0.08723 (16)0.54606 (10)0.0176 (2)
H17A0.23020.08610.47340.026*
H17B0.12030.06520.58470.026*
H17C0.35710.00790.57830.026*
C180.2548 (2)0.52859 (18)0.75508 (10)0.0201 (3)
H18A0.38470.45950.78720.030*
H18B0.15100.49380.80170.030*
H18C0.23310.65850.74320.030*
Cl10.18978 (4)0.32705 (4)0.84515 (2)0.02133 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.02351 (17)0.01550 (15)0.01458 (15)0.00706 (12)0.00309 (11)0.00028 (11)
O40.0215 (4)0.0158 (4)0.0162 (4)0.0084 (3)0.0005 (3)0.0015 (3)
N20.0154 (5)0.0150 (5)0.0146 (5)0.0034 (4)0.0035 (4)0.0012 (4)
N30.0164 (5)0.0125 (5)0.0146 (5)0.0031 (4)0.0008 (4)0.0003 (4)
C20.0190 (6)0.0121 (5)0.0127 (5)0.0056 (4)0.0008 (4)0.0040 (4)
C40.0166 (6)0.0165 (6)0.0202 (6)0.0009 (5)0.0007 (5)0.0011 (5)
C50.0250 (7)0.0256 (7)0.0191 (6)0.0020 (5)0.0049 (5)0.0040 (5)
C60.0304 (7)0.0217 (7)0.0187 (6)0.0035 (6)0.0048 (5)0.0054 (5)
C110.0118 (5)0.0124 (5)0.0144 (5)0.0026 (4)0.0007 (4)0.0004 (4)
C120.0111 (5)0.0123 (5)0.0175 (6)0.0032 (4)0.0016 (4)0.0031 (4)
C130.0130 (5)0.0162 (6)0.0143 (5)0.0042 (4)0.0013 (4)0.0043 (4)
C140.0106 (5)0.0141 (5)0.0167 (6)0.0044 (4)0.0007 (4)0.0007 (4)
C150.0134 (5)0.0117 (5)0.0222 (6)0.0041 (4)0.0016 (4)0.0037 (5)
C160.0110 (5)0.0155 (5)0.0172 (6)0.0023 (4)0.0008 (4)0.0050 (4)
C170.0199 (6)0.0140 (6)0.0194 (6)0.0064 (5)0.0024 (5)0.0049 (5)
C180.0206 (6)0.0204 (6)0.0195 (6)0.0042 (5)0.0022 (5)0.0077 (5)
Cl10.01833 (16)0.02361 (16)0.01703 (15)0.00342 (12)0.00454 (11)0.00310 (12)
Geometric parameters (Å, º) top
S1—C21.7394 (12)C6—H6B0.9700
S1—C61.8237 (15)C11—C121.3988 (17)
O4—C141.3680 (14)C11—C161.3997 (16)
O4—H40.8395C12—C131.3925 (16)
N2—C21.3296 (16)C12—C171.5071 (16)
N2—C111.4405 (14)C13—C141.3897 (16)
N2—H20.8803C13—H130.9300
N3—C21.3180 (16)C14—C151.3857 (17)
N3—C41.4693 (15)C15—C161.3895 (17)
N3—H30.8802C15—H150.9300
C4—C51.5125 (18)C16—C181.5076 (17)
C4—H4A0.9700C17—H17A0.9600
C4—H4B0.9700C17—H17B0.9600
C5—C61.515 (2)C17—H17C0.9600
C5—H5A0.9700C18—H18A0.9600
C5—H5B0.9700C18—H18B0.9600
C6—H6A0.9700C18—H18C0.9600
C2—S1—C6102.79 (6)C12—C11—N2119.48 (10)
C14—O4—H4109.5C16—C11—N2118.61 (10)
C2—N2—C11123.96 (10)C13—C12—C11118.70 (11)
C2—N2—H2118.0C13—C12—C17120.48 (11)
C11—N2—H2118.0C11—C12—C17120.80 (10)
C2—N3—C4124.96 (10)C14—C13—C12120.01 (11)
C2—N3—H3117.5C14—C13—H13120.0
C4—N3—H3117.5C12—C13—H13120.0
N3—C2—N2121.02 (11)O4—C14—C15117.25 (10)
N3—C2—S1124.62 (9)O4—C14—C13122.26 (11)
N2—C2—S1114.37 (9)C15—C14—C13120.49 (11)
N3—C4—C5111.27 (10)C14—C15—C16120.96 (11)
N3—C4—H4A109.4C14—C15—H15119.5
C5—C4—H4A109.4C16—C15—H15119.5
N3—C4—H4B109.4C15—C16—C11117.99 (11)
C5—C4—H4B109.4C15—C16—C18120.68 (11)
H4A—C4—H4B108.0C11—C16—C18121.32 (11)
C4—C5—C6110.83 (12)C12—C17—H17A109.5
C4—C5—H5A109.5C12—C17—H17B109.5
C6—C5—H5A109.5H17A—C17—H17B109.5
C4—C5—H5B109.5C12—C17—H17C109.5
C6—C5—H5B109.5H17A—C17—H17C109.5
H5A—C5—H5B108.1H17B—C17—H17C109.5
C5—C6—S1113.60 (9)C16—C18—H18A109.5
C5—C6—H6A108.8C16—C18—H18B109.5
S1—C6—H6A108.8H18A—C18—H18B109.5
C5—C6—H6B108.8C16—C18—H18C109.5
S1—C6—H6B108.8H18A—C18—H18C109.5
H6A—C6—H6B107.7H18B—C18—H18C109.5
C12—C11—C16121.82 (11)
C4—N3—C2—N2177.58 (11)C16—C11—C12—C17177.69 (11)
C4—N3—C2—S12.90 (17)N2—C11—C12—C171.09 (16)
C11—N2—C2—N33.03 (18)C11—C12—C13—C141.54 (17)
C11—N2—C2—S1176.54 (9)C17—C12—C13—C14176.66 (11)
C6—S1—C2—N39.14 (12)C12—C13—C14—O4178.06 (10)
C6—S1—C2—N2171.30 (10)C12—C13—C14—C151.35 (17)
C2—N3—C4—C534.24 (17)O4—C14—C15—C16179.37 (10)
N3—C4—C5—C664.57 (14)C13—C14—C15—C160.07 (18)
C4—C5—C6—S157.07 (14)C14—C15—C16—C110.95 (17)
C2—S1—C6—C520.83 (12)C14—C15—C16—C18177.89 (11)
C2—N2—C11—C1278.84 (15)C12—C11—C16—C150.74 (17)
C2—N2—C11—C16104.46 (13)N2—C11—C16—C15175.89 (10)
C16—C11—C12—C130.50 (17)C12—C11—C16—C18178.09 (11)
N2—C11—C12—C13177.10 (10)N2—C11—C16—C185.28 (17)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2···Cl10.882.283.1244 (11)161
N3—H3···O4i0.882.122.8143 (13)136
O4—H4···Cl1ii0.842.172.9913 (10)165
Symmetry codes: (i) x+1, y+1, z+1; (ii) x, y+1, z+1.
(II) 2-(4-hydroxy-2,6-dimethylanilino)-5,6-dihydro-4H-1,3-thiazin-3-ium chloride top
Crystal data top
C12H17N2OS+·ClF(000) = 576
Mr = 272.79Dx = 1.323 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 11.8877 (2) ÅCell parameters from 3332 reflections
b = 9.2120 (2) Åθ = 1.0–27.5°
c = 12.6673 (3) ŵ = 0.42 mm1
β = 99.0242 (10)°T = 90 K
V = 1370.02 (5) Å3Rod, colourless
Z = 40.50 × 0.20 × 0.10 mm
Data collection top
Nonius KappaCCD area-detector
diffractometer
3141 independent reflections
Radiation source: fine-focus sealed tube2389 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.031
Detector resolution: 18 pixels mm-1θmax = 27.5°, θmin = 1.7°
ω scans at fixed χ = 55°h = 1515
Absorption correction: multi-scan
(SCALEPACK; Otwinowski & Minor, 1997)
k = 1111
Tmin = 0.818, Tmax = 0.959l = 1616
6046 measured 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)] = 0.042Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.112H-atom parameters constrained
S = 1.10 w = 1/[σ2(Fo2) + (0.0534P)2 + 0.5868P]
where P = (Fo2 + 2Fc2)/3
3141 reflections(Δ/σ)max = 0.001
157 parametersΔρmax = 0.50 e Å3
0 restraintsΔρmin = 0.31 e Å3
Crystal data top
C12H17N2OS+·ClV = 1370.02 (5) Å3
Mr = 272.79Z = 4
Monoclinic, P21/cMo Kα radiation
a = 11.8877 (2) ŵ = 0.42 mm1
b = 9.2120 (2) ÅT = 90 K
c = 12.6673 (3) Å0.50 × 0.20 × 0.10 mm
β = 99.0242 (10)°
Data collection top
Nonius KappaCCD area-detector
diffractometer
3141 independent reflections
Absorption correction: multi-scan
(SCALEPACK; Otwinowski & Minor, 1997)
2389 reflections with I > 2σ(I)
Tmin = 0.818, Tmax = 0.959Rint = 0.031
6046 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0420 restraints
wR(F2) = 0.112H-atom parameters constrained
S = 1.10Δρmax = 0.50 e Å3
3141 reflectionsΔρmin = 0.31 e Å3
157 parameters
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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
S10.26830 (4)0.87420 (5)0.70402 (4)0.01887 (15)
O40.19758 (11)0.58513 (17)0.64205 (11)0.0213 (3)
H40.23990.62190.59190.032*
N20.25741 (14)0.63610 (17)0.59182 (13)0.0177 (4)
H20.28450.56730.55740.021*
N30.43335 (13)0.74466 (18)0.61184 (13)0.0166 (4)
H30.45410.67680.57240.020*
C20.32677 (17)0.7434 (2)0.62978 (15)0.0160 (4)
C40.51844 (17)0.8530 (2)0.65420 (17)0.0177 (4)
H4A0.57970.85310.61180.021*
H4B0.55050.82800.72710.021*
C50.46578 (17)1.0029 (2)0.65208 (17)0.0194 (4)
H5A0.42801.02460.58030.023*
H5B0.52521.07460.67170.023*
C60.38039 (17)1.0115 (2)0.72899 (17)0.0213 (5)
H6A0.34561.10700.72360.026*
H6B0.42031.00010.80140.026*
C110.13924 (16)0.6285 (2)0.60511 (16)0.0153 (4)
C120.05724 (17)0.7029 (2)0.53393 (15)0.0170 (4)
C130.05634 (17)0.6893 (2)0.54664 (15)0.0172 (4)
H130.11230.73880.50090.021*
C140.08699 (16)0.6022 (2)0.62725 (15)0.0162 (4)
C150.00477 (17)0.5284 (2)0.69634 (15)0.0172 (4)
H150.02630.47040.74980.021*
C160.10955 (17)0.5402 (2)0.68661 (15)0.0164 (4)
C170.09010 (19)0.7947 (3)0.44518 (17)0.0247 (5)
H17A0.02300.82040.39630.037*
H17B0.14080.74080.40790.037*
H17C0.12740.88130.47470.037*
C180.19913 (17)0.4591 (2)0.76046 (17)0.0219 (5)
H18A0.16370.40400.81060.033*
H18B0.25210.52680.79840.033*
H18C0.23890.39450.71960.033*
Cl10.38915 (4)0.35624 (5)0.54403 (4)0.01989 (15)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0162 (3)0.0169 (3)0.0252 (3)0.00198 (19)0.0083 (2)0.0064 (2)
O40.0135 (7)0.0278 (8)0.0228 (8)0.0018 (6)0.0031 (6)0.0059 (6)
N20.0170 (9)0.0164 (9)0.0213 (9)0.0009 (7)0.0076 (7)0.0061 (7)
N30.0146 (9)0.0152 (8)0.0213 (9)0.0007 (7)0.0066 (7)0.0045 (7)
C20.0178 (10)0.0152 (10)0.0155 (10)0.0001 (8)0.0045 (8)0.0009 (8)
C40.0144 (10)0.0185 (10)0.0206 (10)0.0008 (8)0.0044 (8)0.0017 (8)
C50.0190 (10)0.0147 (10)0.0259 (11)0.0024 (8)0.0074 (9)0.0002 (8)
C60.0180 (10)0.0163 (10)0.0302 (12)0.0034 (8)0.0058 (9)0.0069 (9)
C110.0147 (10)0.0138 (10)0.0182 (10)0.0021 (7)0.0052 (8)0.0040 (8)
C120.0215 (10)0.0141 (10)0.0157 (10)0.0039 (8)0.0043 (8)0.0034 (8)
C130.0181 (10)0.0172 (10)0.0159 (10)0.0017 (8)0.0009 (8)0.0000 (8)
C140.0149 (10)0.0188 (10)0.0151 (9)0.0028 (8)0.0030 (8)0.0043 (8)
C150.0200 (10)0.0169 (10)0.0154 (9)0.0034 (8)0.0046 (8)0.0016 (8)
C160.0179 (10)0.0139 (10)0.0174 (10)0.0014 (8)0.0024 (8)0.0042 (8)
C170.0257 (12)0.0243 (12)0.0246 (11)0.0042 (9)0.0052 (9)0.0042 (9)
C180.0192 (11)0.0243 (12)0.0222 (11)0.0017 (9)0.0034 (8)0.0023 (9)
Cl10.0199 (3)0.0203 (3)0.0197 (3)0.00485 (19)0.0041 (2)0.00182 (19)
Geometric parameters (Å, º) top
S1—C21.739 (2)C6—H6B0.9700
S1—C61.828 (2)C11—C121.399 (3)
O4—C141.366 (2)C11—C161.403 (3)
O4—H40.8200C12—C131.390 (3)
N2—C21.328 (2)C12—C171.506 (3)
N2—C111.443 (2)C13—C141.392 (3)
N2—H20.8600C13—H130.9300
N3—C21.322 (2)C14—C151.384 (3)
N3—C41.462 (2)C15—C161.388 (3)
N3—H30.8600C15—H150.9300
C4—C51.514 (3)C16—C181.502 (3)
C4—H4A0.9700C17—H17A0.9600
C4—H4B0.9700C17—H17B0.9600
C5—C61.515 (3)C17—H17C0.9600
C5—H5A0.9700C18—H18A0.9600
C5—H5B0.9700C18—H18B0.9600
C6—H6A0.9700C18—H18C0.9600
C2—S1—C6103.33 (10)C12—C11—N2119.61 (17)
C14—O4—H4109.5C16—C11—N2118.43 (17)
C2—N2—C11123.66 (16)C13—C12—C11118.20 (18)
C2—N2—H2118.2C13—C12—C17120.48 (18)
C11—N2—H2118.2C11—C12—C17121.32 (18)
C2—N3—C4124.70 (16)C12—C13—C14120.51 (18)
C2—N3—H3117.6C12—C13—H13119.7
C4—N3—H3117.6C14—C13—H13119.7
N3—C2—N2120.09 (17)O4—C14—C15117.15 (17)
N3—C2—S1124.21 (15)O4—C14—C13122.38 (18)
N2—C2—S1115.69 (15)C15—C14—C13120.47 (18)
N3—C4—C5110.84 (16)C14—C15—C16120.66 (18)
N3—C4—H4A109.5C14—C15—H15119.7
C5—C4—H4A109.5C16—C15—H15119.7
N3—C4—H4B109.5C15—C16—C11118.26 (18)
C5—C4—H4B109.5C15—C16—C18120.96 (18)
H4A—C4—H4B108.1C11—C16—C18120.77 (18)
C4—C5—C6110.68 (17)C12—C17—H17A109.5
C4—C5—H5A109.5C12—C17—H17B109.5
C6—C5—H5A109.5H17A—C17—H17B109.5
C4—C5—H5B109.5C12—C17—H17C109.5
C6—C5—H5B109.5H17A—C17—H17C109.5
H5A—C5—H5B108.1H17B—C17—H17C109.5
C5—C6—S1113.33 (14)C16—C18—H18A109.5
C5—C6—H6A108.9C16—C18—H18B109.5
S1—C6—H6A108.9H18A—C18—H18B109.5
C5—C6—H6B108.9C16—C18—H18C109.5
S1—C6—H6B108.9H18A—C18—H18C109.5
H6A—C6—H6B107.7H18B—C18—H18C109.5
C12—C11—C16121.89 (18)
C4—N3—C2—N2176.75 (17)C16—C11—C12—C17178.56 (18)
C4—N3—C2—S12.0 (3)N2—C11—C12—C171.8 (3)
C11—N2—C2—N3178.18 (17)C11—C12—C13—C140.9 (3)
C11—N2—C2—S13.0 (2)C17—C12—C13—C14178.68 (18)
C6—S1—C2—N37.4 (2)C12—C13—C14—O4179.57 (18)
C6—S1—C2—N2173.80 (15)C12—C13—C14—C150.4 (3)
C2—N3—C4—C539.1 (3)O4—C14—C15—C16179.95 (17)
N3—C4—C5—C666.5 (2)C13—C14—C15—C160.1 (3)
C4—C5—C6—S156.1 (2)C14—C15—C16—C110.0 (3)
C2—S1—C6—C519.88 (18)C14—C15—C16—C18179.26 (18)
C2—N2—C11—C1284.1 (2)C12—C11—C16—C150.6 (3)
C2—N2—C11—C1699.1 (2)N2—C11—C16—C15177.36 (16)
C16—C11—C12—C131.0 (3)C12—C11—C16—C18178.68 (18)
N2—C11—C12—C13177.78 (17)N2—C11—C16—C181.9 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2···Cl10.862.333.1245 (17)154
N3—H3···Cl1i0.862.573.2437 (17)136
O4—H4···Cl1ii0.822.283.0579 (14)159
Symmetry codes: (i) x+1, y+1, z+1; (ii) x, y+1, z+1.

Experimental details

(I)(II)
Crystal data
Chemical formulaC12H17N2OS+·ClC12H17N2OS+·Cl
Mr272.79272.79
Crystal system, space groupTriclinic, P1Monoclinic, P21/c
Temperature (K)9090
a, b, c (Å)6.9961 (1), 7.9421 (1), 13.0864 (2)11.8877 (2), 9.2120 (2), 12.6673 (3)
α, β, γ (°)73.3925 (6), 84.1579 (6), 70.8388 (6)90, 99.0242 (10), 90
V3)658.17 (2)1370.02 (5)
Z24
Radiation typeMo KαMo Kα
µ (mm1)0.440.42
Crystal size (mm)0.30 × 0.20 × 0.100.50 × 0.20 × 0.10
Data collection
DiffractometerNonius KappaCCD area-detector
diffractometer
Nonius KappaCCD area-detector
diffractometer
Absorption correctionMulti-scan
(SCALEPACK; Otwinowski & Minor, 1997)
Multi-scan
(SCALEPACK; Otwinowski & Minor, 1997)
Tmin, Tmax0.881, 0.9580.818, 0.959
No. of measured, independent and
observed [I > 2σ(I)] reflections
5923, 2981, 2762 6046, 3141, 2389
Rint0.0170.031
(sin θ/λ)max1)0.6490.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.028, 0.072, 1.03 0.042, 0.112, 1.10
No. of reflections29813141
No. of parameters156157
H-atom treatmentH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.32, 0.280.50, 0.31

Computer programs: COLLECT (Nonius, 2002), DENZO-SMN (Otwinowski & Minor, 1997), SHELXS97 (Sheldrick, 2008), XP in SHELXTL (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008) and local procedures.

Hydrogen-bond geometry (Å, º) for (I) top
D—H···AD—HH···AD···AD—H···A
N2—H2···Cl10.882.283.1244 (11)161
N3—H3···O4i0.882.122.8143 (13)136
O4—H4···Cl1ii0.842.172.9913 (10)165
Symmetry codes: (i) x+1, y+1, z+1; (ii) x, y+1, z+1.
Hydrogen-bond geometry (Å, º) for (II) top
D—H···AD—HH···AD···AD—H···A
N2—H2···Cl10.862.333.1245 (17)154
N3—H3···Cl1i0.862.573.2437 (17)136
O4—H4···Cl1ii0.822.283.0579 (14)159
Symmetry codes: (i) x+1, y+1, z+1; (ii) x, y+1, z+1.
 

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