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In the title salt, C19H18NO2+·C7H7SO3, the C=C double bond in the cation has an E configuration. The cation is not planar as the dihedral angle between the quinolinium and benzene ring systems is 14.74 (8)°. The anion is aligned approximately perpendicularly to the cation, with the benzene ring of the anion making dihedral angles of 89.98 (8) and 75.36 (10)° with the quinolinium and benzene ring systems of the cation, respectively. An intra­molecular O—H...O hydrogen bond between the hydr­oxy and meth­oxy groups generates an S(5) ring motif. The cations link with anions through weak C—H...O inter­action into cation–anion pairs along the b direction, and the adjacent pairs are further linked by O—H...O hydrogen bonds and weak C—H...O inter­actions into a three-dimensional network. The crystal is further stabilized by C—H...π inter­actions, and π–π inter­actions [centroid–centroid distances of 3.5236 (12) and 3.5337 (12) Å] are also observed.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807061922/ng2386sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807061922/ng2386Isup2.hkl
Contains datablock I

CCDC reference: 674688

Key indicators

  • Single-crystal X-ray study
  • T = 297 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.030
  • wR factor = 0.078
  • Data-to-parameter ratio = 12.0

checkCIF/PLATON results

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Alert level C PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ? PLAT230_ALERT_2_C Hirshfeld Test Diff for C22 - C23 .. 6.09 su PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 2.01 PLAT720_ALERT_4_C Number of Unusual/Non-Standard Label(s) ........ 1
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 25.00 From the CIF: _reflns_number_total 3665 Count of symmetry unique reflns 1978 Completeness (_total/calc) 185.29% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 1687 Fraction of Friedel pairs measured 0.853 Are heavy atom types Z>Si present yes PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 2
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

We have previously reported some crystal structures of quinolinium derivatives salts (Jindawong et al., 2005; Chantrapromma et al., 2006; Chantrapromma, Jindawong & Fun 2007; Chantrapromma, Jindawong, Fun & Patil, 2007; Chantrapromma, Jindawong, Fun, Patil & Karalai, 2007), which were synthesized to study for their nonlinear optic (NLO) properties. At molecular level, a generally popular approach towards NLO materials is systhesis of compounds of extended conjugated systems with donor and acceptor groups. Since compounds which are likely to exhibit large values of molecular hyperpolarizability (β) have to have polarizable electrons (conjugated π system) spread over a large distance (Oudar & Chemla, 1977), the title compound which is a benzene-based π-conjugated system was synthesized. The single-crystal X-ray structural study of the title compound was carried out in order to obtain detailed information on its crystal structure. The tile compound crystallized in the non-centrosymmetric monoclinic Pc space group and therefore the title compound exhibits non-linear optical properties (Williams, 1984).

The asymmetric unit of the title compound consists of a C19H18NO2+ cation and a C7H7SO3- anion (Fig. 1). The cation is not planar as indicated by the dihedral angle between the quinolinium and benzene rings being 14.74 (8) °. The H atoms attached to C10 and C11 are trans to each other; thus the cation exists in an E configuration [the C9–C10–C11–C12 torsion angle is -179.49 (18) °]. The structure of cation shows intramolecular O—H···O hydrogen bond between the hydroxy and methoxy groups which generates a S(5) ring motif (Bernstein et al., 1995). The cation and anion are nearly perpendicular to each other which is indicated by the dihedral angles between the benzene ring of the 4-methylbenzenesulfonate anion with the quinolinium and benzene rings of the cation being 89.98 (8) ° and 75.36 (10) °, respectively.

In the crystal packing, O atoms of anion are involved in C—H···O weak interactions, (Table 1). The cations are linked with anions through weak C—H···O interaction [C3—H3A···O4; symmetry code x, 1 + y, z] (Table 1) into cation-anion pairs along the b direction and the adjacent pairs are further linked by O—H···O hydrogen bonds [O2—H1O2···O5; symmetry code 1 + x, y, 1 + z] and weak C—H···O interactions [C5—H5A···O2 symmetry code -1 + x, y, -1 + z] into a three dimension network. In addition, the cations are stacked along the a axis in such a way that the centroid–centroid distances between the N1/C1/C6–C9 ring (Cg1) and C12–C17 ring (Cg2) are 3.5236 (12) Å (symmetry code: x, 1 - y, -1/2 + z) and 3.5337 (12) Å (symmetry code: x, 1 - y, 1/2 + z), indicating π-π interactions. The crystal is further stabilized C—H···π interactions (Table 1); Cg3 and Cg4 are centroids of C1–C6 and C20–C25 benzene rings, respectively. Bond lengths and angles are in normal ranges and comparable with closely related structures (Chantrapromma, Jindawong & Fun, 2007; Chantrapromma, Jindawong, Fun & Patil, 2007; Chantrapromma, Jindawong, Fun, Patil & Karalai, 2007; Jindawong et al., 2005; Lakshmanaperumal et al., 2004).

Related literature top

For related structures, see, for example, Chantrapromma et al. (2006); Chantrapromma, Jindawong & Fun (2007); Chantrapromma, Jindawong, Fun & Patil (2007); Chantrapromma, Jindawong, Fun, Patil & Karalai, 2007); Jindawong et al. (2005); Lakshmanaperumal et al. (2004). For literature on nonlinear optical activity, see Oudar & Chemla (1977); Williams (1984).

For related literature, see: Bernstein et al. (1995).

Experimental top

A 0.30 g (0.72 mmol) solution of 2-[(E)-2-(4-hydroxy-3-methoxy- phenyl)ethenyl]-1-methylquinolinium iodide (Chantrapromma et al., 2007b) in hot methanol (150 ml) was mixed with 0.20 g (0.72 mmol) of silver (I) 4-methylbenzenesulfonate in hot methanol (30 ml). The mixture turned to dark-red and cloudy immediately. After stirring for 30 min, the precipitate of silver iodide was filtered and the filtrate was evaporated to give a brown solid (0.31 g, 92%yield). Brown single crystals of the title compound suitable for X-ray structure determination were recrystallized from methanol after several days at ambient temperature. (Mp. 536–537 K).

Refinement top

Hydroxy H atom was located in a difference map and isotropically refined. The remaining H atoms were positioned geometrically and allowed to ride on their parent atoms, with C—H distances in the range 0.93–0.97 Å. The Uiso values were constrained to be 1.5Ueq of the carrier atom for methyl H atoms and 1.2Ueq for the remaining H atoms. A rotating group model was used for the methyl groups. The highest residual electron density peak is located at 0.93 Å from O4 and the deepest hole is located at 0.68 Å from S1.

Computing details top

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT (Siemens, 1996); program(s) used to solve structure: SHELXTL (Sheldrick, 1997); program(s) used to refine structure: SHELXTL (Sheldrick, 1997); molecular graphics: SHELXTL (Sheldrick, 1997); software used to prepare material for publication: SHELXTL and PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. The structure of (I) showing 50% probability displacement ellipsoids and the atom-numbering scheme. O—H···O hydrogen bond was drawn as a dash line.
[Figure 2] Fig. 2. The packing diagram of (I) viewd along the a axis. O—H···O hydrogen bonds and weak C—H···O interactions were drawn as dashed lines.
2-[(E)-2-(4-Hydroxy-3-methoxyphenyl)ethenyl]-1-methylquinolinium 4-methylbenzenesulfonate top
Crystal data top
C19H18NO2+·C7H7O3SF(000) = 488
Mr = 463.53Dx = 1.380 Mg m3
Monoclinic, PcMelting point = 536–537 K
Hall symbol: P -2ycMo Kα radiation, λ = 0.71073 Å
a = 6.9237 (5) ÅCell parameters from 3665 reflections
b = 11.1007 (7) Åθ = 1.8–25.0°
c = 15.1376 (9) ŵ = 0.18 mm1
β = 106.507 (3)°T = 297 K
V = 1115.49 (13) Å3Block, brown
Z = 20.58 × 0.23 × 0.13 mm
Data collection top
Siemens SMART CCD area detector
diffractometer
3665 independent reflections
Radiation source: medium-focus sealed tube3582 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.014
Detector resolution: 8.33 pixels mm-1θmax = 25.0°, θmin = 1.8°
ω scansh = 88
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
k = 913
Tmin = 0.901, Tmax = 0.976l = 1717
5512 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.030 w = 1/[σ2(Fo2) + (0.0454P)2 + 0.1204P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.078(Δ/σ)max = 0.001
S = 1.07Δρmax = 0.14 e Å3
3665 reflectionsΔρmin = 0.17 e Å3
306 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
2 restraintsExtinction coefficient: 0.014 (2)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (Flack, 1983) parameter from 1698 Friedel pairs
Secondary atom site location: difference Fourier mapAbsolute structure parameter: 0.03 (6)
Crystal data top
C19H18NO2+·C7H7O3SV = 1115.49 (13) Å3
Mr = 463.53Z = 2
Monoclinic, PcMo Kα radiation
a = 6.9237 (5) ŵ = 0.18 mm1
b = 11.1007 (7) ÅT = 297 K
c = 15.1376 (9) Å0.58 × 0.23 × 0.13 mm
β = 106.507 (3)°
Data collection top
Siemens SMART CCD area detector
diffractometer
3665 independent reflections
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
3582 reflections with I > 2σ(I)
Tmin = 0.901, Tmax = 0.976Rint = 0.014
5512 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.030H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.078Δρmax = 0.14 e Å3
S = 1.07Δρmin = 0.17 e Å3
3665 reflectionsAbsolute structure: Flack (Flack, 1983) parameter from 1698 Friedel pairs
306 parametersAbsolute structure parameter: 0.03 (6)
2 restraints
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.51215 (8)0.16189 (4)0.46563 (4)0.04787 (14)
O11.3315 (2)0.25370 (12)1.22793 (10)0.0551 (4)
O21.4831 (2)0.45553 (14)1.31606 (9)0.0548 (4)
H1O21.488 (4)0.389 (3)1.341 (2)0.075 (8)*
O30.3069 (2)0.15382 (15)0.46956 (12)0.0705 (5)
O40.5685 (3)0.06935 (13)0.41122 (11)0.0669 (5)
O50.5642 (3)0.28182 (14)0.44182 (11)0.0699 (5)
N10.8616 (2)0.68273 (13)0.74870 (10)0.0354 (3)
C10.7701 (2)0.68972 (16)0.65437 (12)0.0348 (4)
C20.7145 (3)0.80009 (17)0.60887 (14)0.0448 (4)
H2A0.73630.87180.64200.054*
C30.6282 (3)0.8017 (2)0.51536 (15)0.0538 (5)
H3A0.59420.87510.48540.065*
C40.5903 (3)0.6950 (2)0.46436 (14)0.0570 (6)
H4A0.52940.69770.40120.068*
C50.6423 (3)0.58759 (19)0.50710 (13)0.0478 (5)
H5A0.61610.51680.47290.057*
C60.7353 (3)0.58215 (16)0.60236 (12)0.0379 (4)
C70.8007 (3)0.47260 (16)0.64732 (13)0.0433 (4)
H7A0.77500.40070.61460.052*
C80.9009 (3)0.47140 (17)0.73804 (13)0.0447 (4)
H8A0.94990.39880.76630.054*
C90.9326 (3)0.57791 (15)0.79059 (13)0.0386 (4)
C101.0436 (3)0.57780 (17)0.88764 (12)0.0458 (4)
H10A1.10080.64990.91370.055*
C111.0685 (3)0.48202 (17)0.94132 (12)0.0424 (4)
H11A1.01120.41050.91400.051*
C121.1766 (3)0.47696 (16)1.03886 (12)0.0401 (4)
C131.1981 (3)0.36561 (16)1.08431 (13)0.0401 (4)
H13A1.14330.29681.05170.048*
C141.2991 (3)0.35693 (16)1.17639 (13)0.0396 (4)
C151.3805 (3)0.45985 (16)1.22647 (12)0.0395 (4)
C161.3588 (3)0.56993 (17)1.18148 (13)0.0442 (4)
H16A1.41270.63891.21420.053*
C171.2590 (3)0.57861 (16)1.08940 (13)0.0427 (4)
H17A1.24620.65331.06040.051*
C180.8755 (3)0.79311 (18)0.80513 (14)0.0514 (5)
H18A0.85290.77300.86310.077*
H18B0.77560.85000.77310.077*
H18C1.00710.82790.81580.077*
C191.2710 (4)0.14166 (19)1.18306 (17)0.0551 (6)
H19A1.30770.07751.22710.083*
H19B1.33670.13031.13570.083*
H19C1.12770.14161.15600.083*
C200.6664 (3)0.14174 (15)0.58113 (14)0.0414 (4)
C210.8739 (3)0.14691 (19)0.60100 (17)0.0559 (5)
H21A0.93420.15680.55390.067*
C220.9915 (4)0.1372 (2)0.69183 (19)0.0662 (7)
H22A1.13090.14230.70480.079*
C230.9079 (4)0.12039 (18)0.76303 (16)0.0612 (6)
C240.7022 (4)0.1133 (2)0.74191 (15)0.0611 (6)
H24A0.64200.10090.78880.073*
C250.5828 (3)0.12419 (18)0.65206 (14)0.0488 (5)
H25A0.44350.11950.63950.059*
C261.0397 (6)0.1097 (3)0.8620 (2)0.0979 (10)
H26A0.95990.08140.90030.147*
H26B1.09530.18720.88350.147*
H26C1.14700.05380.86480.147*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0664 (3)0.0345 (2)0.0378 (2)0.0055 (2)0.00683 (19)0.0028 (2)
O10.0824 (10)0.0344 (7)0.0428 (8)0.0006 (6)0.0085 (7)0.0082 (6)
O20.0805 (10)0.0435 (8)0.0325 (7)0.0048 (7)0.0031 (6)0.0053 (6)
O30.0577 (10)0.0778 (12)0.0635 (10)0.0028 (8)0.0028 (8)0.0065 (8)
O40.1095 (13)0.0449 (8)0.0466 (8)0.0111 (8)0.0226 (8)0.0011 (7)
O50.1107 (14)0.0400 (8)0.0472 (8)0.0014 (8)0.0036 (8)0.0130 (6)
N10.0400 (8)0.0322 (7)0.0329 (7)0.0018 (6)0.0085 (6)0.0010 (6)
C10.0334 (9)0.0375 (9)0.0330 (9)0.0000 (7)0.0087 (7)0.0003 (7)
C20.0540 (11)0.0348 (9)0.0436 (11)0.0034 (8)0.0105 (8)0.0025 (8)
C30.0640 (14)0.0507 (12)0.0425 (11)0.0050 (9)0.0084 (9)0.0127 (9)
C40.0638 (13)0.0696 (14)0.0312 (9)0.0039 (10)0.0031 (10)0.0048 (9)
C50.0520 (12)0.0528 (12)0.0360 (10)0.0028 (9)0.0084 (8)0.0076 (8)
C60.0384 (9)0.0390 (9)0.0360 (9)0.0015 (7)0.0099 (8)0.0024 (7)
C70.0505 (11)0.0319 (9)0.0469 (11)0.0026 (8)0.0131 (9)0.0069 (8)
C80.0537 (11)0.0336 (9)0.0435 (11)0.0026 (8)0.0086 (9)0.0050 (7)
C90.0397 (9)0.0368 (10)0.0385 (9)0.0004 (7)0.0100 (8)0.0038 (7)
C100.0540 (11)0.0396 (10)0.0385 (10)0.0020 (8)0.0043 (8)0.0028 (8)
C110.0446 (10)0.0409 (10)0.0394 (10)0.0013 (8)0.0084 (8)0.0012 (8)
C120.0415 (9)0.0412 (10)0.0385 (10)0.0021 (8)0.0125 (8)0.0051 (8)
C130.0434 (10)0.0373 (9)0.0388 (9)0.0029 (7)0.0103 (8)0.0002 (7)
C140.0454 (10)0.0348 (9)0.0389 (9)0.0027 (7)0.0125 (8)0.0058 (7)
C150.0437 (10)0.0417 (10)0.0331 (9)0.0023 (7)0.0110 (7)0.0033 (7)
C160.0556 (12)0.0347 (9)0.0414 (10)0.0028 (8)0.0122 (9)0.0004 (7)
C170.0492 (10)0.0389 (10)0.0402 (10)0.0001 (8)0.0129 (8)0.0083 (8)
C180.0726 (14)0.0388 (10)0.0381 (10)0.0047 (9)0.0081 (9)0.0078 (8)
C190.0617 (13)0.0368 (10)0.0652 (15)0.0009 (9)0.0158 (11)0.0056 (9)
C200.0516 (11)0.0288 (8)0.0417 (10)0.0040 (7)0.0097 (8)0.0044 (7)
C210.0552 (13)0.0509 (12)0.0642 (14)0.0031 (9)0.0212 (11)0.0116 (10)
C220.0509 (13)0.0510 (12)0.0849 (18)0.0051 (9)0.0001 (12)0.0059 (11)
C230.0856 (18)0.0351 (10)0.0506 (13)0.0081 (10)0.0006 (11)0.0001 (9)
C240.0904 (18)0.0496 (13)0.0446 (11)0.0080 (12)0.0215 (12)0.0033 (10)
C250.0569 (12)0.0443 (11)0.0459 (11)0.0037 (9)0.0160 (9)0.0041 (9)
C260.135 (3)0.0676 (17)0.0595 (15)0.0148 (17)0.0227 (16)0.0053 (14)
Geometric parameters (Å, º) top
S1—O41.4383 (16)C11—H11A0.9300
S1—O31.4421 (19)C12—C171.391 (3)
S1—O51.4511 (16)C12—C131.402 (2)
S1—C201.785 (2)C13—C141.374 (3)
O1—C141.369 (2)C13—H13A0.9300
O1—C191.422 (3)C14—C151.398 (3)
O2—C151.341 (2)C15—C161.386 (3)
O2—H1O20.83 (3)C16—C171.372 (3)
N1—C91.349 (2)C16—H16A0.9300
N1—C11.390 (2)C17—H17A0.9300
N1—C181.481 (2)C18—H18A0.9600
C1—C21.405 (3)C18—H18B0.9600
C1—C61.413 (2)C18—H18C0.9600
C2—C31.371 (3)C19—H19A0.9600
C2—H2A0.9300C19—H19B0.9600
C3—C41.397 (3)C19—H19C0.9600
C3—H3A0.9300C20—C251.371 (3)
C4—C51.356 (3)C20—C211.383 (3)
C4—H4A0.9300C21—C221.389 (3)
C5—C61.404 (3)C21—H21A0.9300
C5—H5A0.9300C22—C231.374 (4)
C6—C71.404 (3)C22—H22A0.9300
C7—C81.351 (3)C23—C241.370 (4)
C7—H7A0.9300C23—C261.522 (3)
C8—C91.407 (3)C24—C251.382 (3)
C8—H8A0.9300C24—H24A0.9300
C9—C101.452 (3)C25—H25A0.9300
C10—C111.319 (3)C26—H26A0.9600
C10—H10A0.9300C26—H26B0.9600
C11—C121.454 (2)C26—H26C0.9600
O4—S1—O3114.22 (10)C12—C13—H13A119.6
O4—S1—O5112.71 (10)O1—C14—C13126.22 (17)
O3—S1—O5112.61 (11)O1—C14—C15113.55 (15)
O4—S1—C20106.70 (9)C13—C14—C15120.23 (16)
O3—S1—C20105.91 (10)O2—C15—C16118.73 (17)
O5—S1—C20103.68 (9)O2—C15—C14122.36 (16)
C14—O1—C19118.80 (15)C16—C15—C14118.89 (16)
C15—O2—H1O2116 (2)C17—C16—C15120.93 (17)
C9—N1—C1121.99 (15)C17—C16—H16A119.5
C9—N1—C18119.15 (14)C15—C16—H16A119.5
C1—N1—C18118.83 (14)C16—C17—C12120.74 (17)
N1—C1—C2122.27 (16)C16—C17—H17A119.6
N1—C1—C6118.75 (15)C12—C17—H17A119.6
C2—C1—C6118.97 (16)N1—C18—H18A109.5
C3—C2—C1119.73 (19)N1—C18—H18B109.5
C3—C2—H2A120.1H18A—C18—H18B109.5
C1—C2—H2A120.1N1—C18—H18C109.5
C2—C3—C4121.17 (19)H18A—C18—H18C109.5
C2—C3—H3A119.4H18B—C18—H18C109.5
C4—C3—H3A119.4O1—C19—H19A109.5
C5—C4—C3119.95 (19)O1—C19—H19B109.5
C5—C4—H4A120.0H19A—C19—H19B109.5
C3—C4—H4A120.0O1—C19—H19C109.5
C4—C5—C6120.67 (19)H19A—C19—H19C109.5
C4—C5—H5A119.7H19B—C19—H19C109.5
C6—C5—H5A119.7C25—C20—C21118.64 (19)
C5—C6—C7121.72 (17)C25—C20—S1121.12 (15)
C5—C6—C1119.47 (17)C21—C20—S1120.22 (16)
C7—C6—C1118.78 (15)C20—C21—C22119.5 (2)
C8—C7—C6120.19 (16)C20—C21—H21A120.2
C8—C7—H7A119.9C22—C21—H21A120.2
C6—C7—H7A119.9C23—C22—C21121.9 (2)
C7—C8—C9121.25 (16)C23—C22—H22A119.1
C7—C8—H8A119.4C21—C22—H22A119.1
C9—C8—H8A119.4C24—C23—C22117.8 (2)
N1—C9—C8118.79 (16)C24—C23—C26121.2 (3)
N1—C9—C10119.58 (16)C22—C23—C26121.0 (3)
C8—C9—C10121.61 (16)C23—C24—C25121.1 (2)
C11—C10—C9124.26 (17)C23—C24—H24A119.5
C11—C10—H10A117.9C25—C24—H24A119.5
C9—C10—H10A117.9C20—C25—C24121.0 (2)
C10—C11—C12126.58 (17)C20—C25—H25A119.5
C10—C11—H11A116.7C24—C25—H25A119.5
C12—C11—H11A116.7C23—C26—H26A109.5
C17—C12—C13118.38 (16)C23—C26—H26B109.5
C17—C12—C11122.63 (16)H26A—C26—H26B109.5
C13—C12—C11118.99 (16)C23—C26—H26C109.5
C14—C13—C12120.82 (17)H26A—C26—H26C109.5
C14—C13—H13A119.6H26B—C26—H26C109.5
C9—N1—C1—C2173.31 (17)C11—C12—C13—C14179.98 (16)
C18—N1—C1—C28.7 (3)C19—O1—C14—C135.3 (3)
C9—N1—C1—C65.5 (2)C19—O1—C14—C15174.71 (18)
C18—N1—C1—C6172.56 (16)C12—C13—C14—O1179.36 (19)
N1—C1—C2—C3178.74 (18)C12—C13—C14—C150.7 (3)
C6—C1—C2—C30.0 (3)O1—C14—C15—O21.2 (3)
C1—C2—C3—C41.3 (3)C13—C14—C15—O2178.87 (17)
C2—C3—C4—C51.1 (3)O1—C14—C15—C16179.47 (17)
C3—C4—C5—C60.3 (3)C13—C14—C15—C160.6 (3)
C4—C5—C6—C7176.40 (19)O2—C15—C16—C17178.55 (17)
C4—C5—C6—C11.6 (3)C14—C15—C16—C170.2 (3)
N1—C1—C6—C5179.77 (16)C15—C16—C17—C120.1 (3)
C2—C1—C6—C51.4 (3)C13—C12—C17—C160.0 (3)
N1—C1—C6—C72.2 (2)C11—C12—C17—C16179.62 (18)
C2—C1—C6—C7176.66 (17)O4—S1—C20—C25122.65 (17)
C5—C6—C7—C8175.84 (18)O3—S1—C20—C250.58 (18)
C1—C6—C7—C82.2 (3)O5—S1—C20—C25118.16 (16)
C6—C7—C8—C93.5 (3)O4—S1—C20—C2159.14 (17)
C1—N1—C9—C84.3 (2)O3—S1—C20—C21178.80 (16)
C18—N1—C9—C8173.76 (18)O5—S1—C20—C2160.06 (18)
C1—N1—C9—C10174.23 (16)C25—C20—C21—C221.5 (3)
C18—N1—C9—C107.8 (2)S1—C20—C21—C22176.71 (16)
C7—C8—C9—N10.3 (3)C20—C21—C22—C231.2 (3)
C7—C8—C9—C10178.76 (18)C21—C22—C23—C240.0 (3)
N1—C9—C10—C11159.44 (19)C21—C22—C23—C26179.8 (2)
C8—C9—C10—C1122.1 (3)C22—C23—C24—C250.8 (3)
C9—C10—C11—C12179.49 (18)C26—C23—C24—C25179.4 (2)
C10—C11—C12—C174.0 (3)C21—C20—C25—C240.8 (3)
C10—C11—C12—C13176.44 (19)S1—C20—C25—C24177.46 (16)
C17—C12—C13—C140.4 (3)C23—C24—C25—C200.4 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H1O2···O10.83 (3)2.30 (3)2.666 (2)107 (2)
O2—H1O2···O5i0.83 (3)1.89 (3)2.655 (2)154 (3)
C3—H3A···O4ii0.932.413.334 (3)170
C5—H5A···O2iii0.932.393.149 (2)139
C25—H25A···O30.932.512.897 (3)106
C2—H2A···Cg4ii0.932.913.788 (2)157
C7—H7A···Cg40.933.123.818 (2)134
C8—H8A···Cg40.933.363.935 (2)123
C13—H13A···Cg3iv0.933.243.556 (2)102
Symmetry codes: (i) x+1, y, z+1; (ii) x, y+1, z; (iii) x1, y, z1; (iv) x, y+1, z+1/2.

Experimental details

Crystal data
Chemical formulaC19H18NO2+·C7H7O3S
Mr463.53
Crystal system, space groupMonoclinic, Pc
Temperature (K)297
a, b, c (Å)6.9237 (5), 11.1007 (7), 15.1376 (9)
β (°) 106.507 (3)
V3)1115.49 (13)
Z2
Radiation typeMo Kα
µ (mm1)0.18
Crystal size (mm)0.58 × 0.23 × 0.13
Data collection
DiffractometerSiemens SMART CCD area detector
diffractometer
Absorption correctionEmpirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.901, 0.976
No. of measured, independent and
observed [I > 2σ(I)] reflections
5512, 3665, 3582
Rint0.014
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.030, 0.078, 1.07
No. of reflections3665
No. of parameters306
No. of restraints2
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.14, 0.17
Absolute structureFlack (Flack, 1983) parameter from 1698 Friedel pairs
Absolute structure parameter0.03 (6)

Computer programs: SMART (Siemens, 1996), SAINT (Siemens, 1996), SHELXTL (Sheldrick, 1997), SHELXTL (Sheldrick, 1997), SHELXTL and PLATON (Spek, 2003).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H1O2···O10.83 (3)2.30 (3)2.666 (2)107 (2)
O2—H1O2···O5i0.83 (3)1.89 (3)2.655 (2)154 (3)
C3—H3A···O4ii0.932.41433.334 (3)170
C5—H5A···O2iii0.932.38853.149 (2)139
C25—H25A···O30.932.50492.897 (3)106
C2—H2A···Cg4ii0.932.91433.788 (2)157
C7—H7A···Cg40.933.11513.818 (2)134
C8—H8A···Cg40.933.35543.935 (2)123
C13—H13A···Cg3iv0.933.24093.556 (2)102
Symmetry codes: (i) x+1, y, z+1; (ii) x, y+1, z; (iii) x1, y, z1; (iv) x, y+1, z+1/2.
 

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