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The mol­ecular and supra­molecular structures are reported of N-[2-(pyridin-2-yl)ethyl]methane­sulfonamide, C8H12N2O2S, (I), N-[2-(pyridin-2-yl)ethyl]benzene­sulfonamide, C13H14N2O2S, (II), and N-[2-(pyridin-2-yl)ethyl]toluene­sulfonamide, C14H16N2O2S, (III). Although (II) and (III) are almost structurally identical, the N(amide)-C(ethyl)-C(ethyl)-C(pyridinyl) torsion angles for (I) and (II) are more closely comparable, with magnitudes of 175.37 (15)° for (I) and 169.04 (19)° for (II). This angle decreases dramatically with an additional methyl group in the para position of the sulfonamide substituent, resulting in a value of 62.9 (2)° for (III). In each of the three compounds there is an N-H...N hydrogen bond between the sulfon­amide of one mol­ecule and the pyridine N atom of a neighbor. Compound (I) forms hydrogen-bonded dimers, (II) uses its hydrogen bonding to connect supra­molecular layers, and the hydrogen bonding of (III) connects linear chains to form layers. For arene-substituted (II) and (III), the different conformations afforded by the variable dihedral angles promote inter­molecular [pi]-[pi] stacking in the benzene-substituted structure (II), but distorted intra­molecular T-shaped [pi]-stacking in the toluene-substituted structure (III), with a centroid-to-centroid distance of 4.9296 (10) Å.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270113025341/yp3050sup1.cif
Contains datablocks I, II, III, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113025341/yp3050Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113025341/yp3050IIsup3.hkl
Contains datablock II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113025341/yp3050IIIsup4.hkl
Contains datablock III

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S0108270113025341/yp3050Isup5.cml
Supplementary material

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S0108270113025341/yp3050IIsup6.cml
Supplementary material

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S0108270113025341/yp3050IIIsup7.cml
Supplementary material

CCDC references: 960707; 960708; 960709

Computing details top

For all compounds, data collection: Instrument Service (Bruker, 2010); cell refinement: APEX2 (Bruker, 2009); data reduction: SAINT (Bruker, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: CrystalMaker (Palmer, 2009); software used to prepare material for publication: publCIF (Westrip, 2010).

(I) N-[2-(pyridin-2-yl)ethyl]methanesulfonamide top
Crystal data top
C8H12N2O2SF(000) = 424
Mr = 200.27Dx = 1.398 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 10.9122 (16) ÅCell parameters from 128 reflections
b = 5.0428 (7) Åθ = 4.3–29.0°
c = 17.279 (3) ŵ = 0.31 mm1
β = 93.284 (2)°T = 100 K
V = 949.3 (2) Å3Needle, colourless
Z = 40.51 × 0.10 × 0.09 mm
Data collection top
Bruker APEXII CCD area-detector
diffractometer
2277 independent reflections
Radiation source: fine-focus sealed tube1765 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.043
Detector resolution: 8.3333 pixels mm-1θmax = 28.6°, θmin = 1.9°
ω and φ scansh = 1313
Absorption correction: multi-scan
(SADABS; Bruker, 2009)
k = 66
Tmin = 0.822, Tmax = 1.00l = 2223
10388 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)] = 0.039Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.103H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0475P)2 + 0.4601P]
where P = (Fo2 + 2Fc2)/3
2277 reflections(Δ/σ)max = 0.001
122 parametersΔρmax = 0.30 e Å3
0 restraintsΔρmin = 0.38 e Å3
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 (isotroπc) 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
S10.65785 (4)0.90289 (9)0.34718 (2)0.01895 (14)
O10.76528 (11)1.0283 (3)0.38274 (7)0.0266 (3)
O20.56856 (12)1.0654 (2)0.30516 (7)0.0233 (3)
C80.70704 (17)0.6598 (4)0.28261 (11)0.0246 (4)
H8A0.63570.56270.26020.037*
H8B0.76280.53610.31060.037*
H8C0.750.74550.2410.037*
N10.59124 (14)0.7524 (3)0.41476 (9)0.0211 (3)
H10.6386 (19)0.690 (4)0.4470 (13)0.025*
C10.47383 (15)0.6144 (4)0.39803 (10)0.0199 (4)
H1A0.47560.44090.42490.024*
H1B0.46240.58120.34160.024*
C20.36621 (16)0.7782 (4)0.42458 (11)0.0228 (4)
H2A0.3810.82410.480.027*
H2B0.36040.94550.39460.027*
C30.24739 (16)0.6291 (4)0.41358 (10)0.0209 (4)
C40.16047 (17)0.6880 (4)0.35419 (11)0.0279 (4)
H40.17480.82740.31880.033*
C50.05307 (18)0.5430 (4)0.34681 (12)0.0311 (5)
H50.00730.58260.30670.037*
C60.03450 (17)0.3408 (4)0.39810 (12)0.0293 (5)
H60.03870.23860.39450.035*
C70.12578 (17)0.2904 (4)0.45532 (11)0.0269 (4)
H70.11370.14970.49060.032*
N20.23014 (14)0.4298 (3)0.46339 (9)0.0228 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0177 (2)0.0207 (2)0.0183 (2)0.00267 (17)0.00072 (16)0.00007 (17)
O10.0213 (7)0.0323 (8)0.0258 (7)0.0099 (6)0.0021 (5)0.0012 (6)
O20.0235 (7)0.0231 (7)0.0231 (6)0.0017 (5)0.0009 (5)0.0019 (5)
C80.0224 (9)0.0264 (10)0.0255 (9)0.0003 (8)0.0066 (7)0.0007 (8)
N10.0165 (7)0.0306 (9)0.0159 (7)0.0043 (7)0.0015 (6)0.0028 (6)
C10.0180 (8)0.0240 (9)0.0179 (8)0.0048 (7)0.0012 (7)0.0018 (7)
C20.0197 (9)0.0234 (9)0.0254 (9)0.0025 (8)0.0009 (7)0.0024 (8)
C30.0199 (9)0.0229 (9)0.0204 (8)0.0005 (7)0.0049 (7)0.0028 (7)
C40.0234 (10)0.0302 (11)0.0301 (10)0.0016 (8)0.0019 (8)0.0067 (8)
C50.0209 (10)0.0408 (12)0.0309 (10)0.0006 (9)0.0043 (8)0.0054 (9)
C60.0184 (9)0.0360 (11)0.0335 (11)0.0076 (8)0.0003 (8)0.0002 (9)
C70.0246 (10)0.0299 (11)0.0263 (10)0.0058 (8)0.0028 (8)0.0031 (8)
N20.0202 (8)0.0266 (9)0.0217 (7)0.0017 (6)0.0014 (6)0.0002 (6)
Geometric parameters (Å, º) top
S1—O21.4377 (13)C2—H2A0.99
S1—O11.4384 (13)C2—H2B0.99
S1—N11.6016 (16)C3—N21.343 (2)
S1—C81.7618 (19)C3—C41.389 (3)
C8—H8A0.98C4—C51.381 (3)
C8—H8B0.98C4—H40.95
C8—H8C0.98C5—C61.373 (3)
N1—C11.472 (2)C5—H50.95
N1—H10.80 (2)C6—C71.386 (3)
C1—C21.528 (2)C6—H60.95
C1—H1A0.99C7—N21.339 (2)
C1—H1B0.99C7—H70.95
C2—C31.502 (2)
O2—S1—O1118.52 (8)C3—C2—H2A109.4
O2—S1—N1108.39 (8)C1—C2—H2A109.4
O1—S1—N1106.83 (8)C3—C2—H2B109.4
O2—S1—C8107.39 (8)C1—C2—H2B109.4
O1—S1—C8107.81 (9)H2A—C2—H2B108.0
N1—S1—C8107.43 (9)N2—C3—C4121.23 (17)
S1—C8—H8A109.5N2—C3—C2116.45 (16)
S1—C8—H8B109.5C4—C3—C2122.30 (17)
H8A—C8—H8B109.5C5—C4—C3119.66 (18)
S1—C8—H8C109.5C5—C4—H4120.2
H8A—C8—H8C109.5C3—C4—H4120.2
H8B—C8—H8C109.5C6—C5—C4119.29 (18)
C1—N1—S1120.46 (12)C6—C5—H5120.4
C1—N1—H1118.2 (16)C4—C5—H5120.4
S1—N1—H1112.9 (16)C5—C6—C7118.02 (18)
N1—C1—C2111.16 (15)C5—C6—H6121.0
N1—C1—H1A109.4C7—C6—H6121.0
C2—C1—H1A109.4N2—C7—C6123.39 (18)
N1—C1—H1B109.4N2—C7—H7118.3
C2—C1—H1B109.4C6—C7—H7118.3
H1A—C1—H1B108.0C7—N2—C3118.40 (16)
C3—C2—C1111.36 (15)
O2—S1—N1—C148.03 (16)C2—C3—C4—C5179.71 (18)
O1—S1—N1—C1176.81 (14)C3—C4—C5—C60.5 (3)
C8—S1—N1—C167.72 (16)C4—C5—C6—C70.3 (3)
S1—N1—C1—C2102.11 (16)C5—C6—C7—N20.6 (3)
N1—C1—C2—C3175.37 (15)C6—C7—N2—C30.1 (3)
C1—C2—C3—N273.6 (2)C4—C3—N2—C71.0 (3)
C1—C2—C3—C4105.0 (2)C2—C3—N2—C7179.55 (16)
N2—C3—C4—C51.3 (3)
(II) N-[2-(pyridin-2-yl)ethyl]benzenesulfonamide top
Crystal data top
C13H14N2O2SF(000) = 552
Mr = 262.32Dx = 1.376 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 5.4920 (7) ÅCell parameters from 2969 reflections
b = 9.4328 (11) Åθ = 2.3–26.2°
c = 24.569 (3) ŵ = 0.25 mm1
β = 95.651 (2)°T = 100 K
V = 1266.6 (3) Å3Needle, colourless
Z = 40.19 × 0.04 × 0.03 mm
Data collection top
Bruker APEXII CCD area-detector
diffractometer
2768 independent reflections
Radiation source: fine-focus sealed tube1800 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.094
Detector resolution: 8.3333 pixels mm-1θmax = 27.1°, θmin = 1.7°
ω and φ scansh = 77
Absorption correction: multi-scan
(SADABS; Bruker, 2009)
k = 1212
Tmin = 0.94, Tmax = 0.99l = 3131
13893 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)] = 0.046Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.090H atoms treated by a mixture of independent and constrained refinement
S = 1.08 w = 1/[σ2(Fo2) + (0.0297P)2]
where P = (Fo2 + 2Fc2)/3
2768 reflections(Δ/σ)max = 0.015
166 parametersΔρmax = 0.38 e Å3
0 restraintsΔρmin = 0.35 e Å3
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
S10.50738 (10)0.87372 (6)0.61471 (2)0.01712 (16)
O10.6283 (3)0.75088 (17)0.59572 (6)0.0232 (4)
O20.6496 (3)0.99878 (16)0.62970 (6)0.0213 (4)
N10.2960 (3)0.9214 (2)0.56934 (8)0.0183 (5)
H10.234 (4)1.010 (2)0.5719 (9)0.022*
N20.1253 (3)0.78632 (19)0.42114 (8)0.0185 (5)
C120.1863 (4)0.7532 (3)0.77132 (10)0.0246 (6)
H120.12410.73040.80410.03*
C110.0760 (4)0.8584 (3)0.73809 (10)0.0239 (6)
H110.06010.9060.74860.029*
C100.1676 (4)0.8928 (2)0.68938 (9)0.0197 (5)
H100.09330.9630.6670.024*
C90.3716 (4)0.8216 (2)0.67419 (9)0.0151 (5)
C10.1505 (4)0.8198 (2)0.53482 (9)0.0204 (5)
H1A0.01720.85290.52890.024*
H1B0.15010.7290.55340.024*
C20.2532 (4)0.8009 (3)0.47973 (9)0.0228 (6)
H2A0.28380.89350.46460.027*
H2B0.40830.75120.48530.027*
C30.0831 (4)0.7195 (3)0.43932 (9)0.0192 (5)
C70.2838 (4)0.7173 (2)0.38525 (9)0.0213 (6)
H70.42890.76250.37260.026*
C60.2417 (4)0.5828 (2)0.36626 (10)0.0228 (6)
H60.35550.53880.34130.027*
C140.4830 (4)0.7161 (2)0.70737 (9)0.0190 (5)
H140.61990.66910.6970.023*
C130.3895 (4)0.6816 (3)0.75580 (10)0.0234 (6)
H130.46240.61040.7780.028*
C50.0267 (4)0.5144 (2)0.38516 (10)0.0232 (6)
H50.0070.42370.37310.028*
C40.1360 (4)0.5836 (3)0.42218 (9)0.0220 (6)
H40.2810.53960.43570.026*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0160 (3)0.0196 (3)0.0158 (3)0.0019 (3)0.0019 (2)0.0009 (3)
O10.0268 (9)0.0233 (9)0.0205 (9)0.0102 (8)0.0069 (7)0.0017 (8)
O20.0182 (9)0.0243 (9)0.0208 (9)0.0032 (7)0.0005 (7)0.0028 (8)
N10.0200 (11)0.0156 (11)0.0180 (11)0.0033 (9)0.0043 (9)0.0016 (9)
N20.0182 (11)0.0188 (11)0.0184 (11)0.0004 (9)0.0016 (8)0.0021 (8)
C120.0278 (14)0.0300 (15)0.0171 (14)0.0074 (12)0.0072 (11)0.0014 (12)
C110.0187 (13)0.0299 (15)0.0237 (14)0.0014 (12)0.0055 (10)0.0031 (12)
C100.0155 (12)0.0221 (14)0.0210 (13)0.0018 (10)0.0010 (10)0.0002 (11)
C90.0146 (12)0.0167 (12)0.0136 (13)0.0024 (9)0.0004 (9)0.0022 (10)
C10.0205 (13)0.0230 (13)0.0177 (13)0.0010 (10)0.0019 (10)0.0021 (11)
C20.0175 (13)0.0304 (15)0.0207 (14)0.0002 (11)0.0023 (10)0.0028 (11)
C30.0169 (12)0.0266 (15)0.0148 (13)0.0005 (11)0.0045 (10)0.0022 (11)
C70.0194 (13)0.0246 (15)0.0194 (14)0.0004 (11)0.0004 (10)0.0009 (11)
C60.0251 (14)0.0212 (14)0.0223 (14)0.0056 (11)0.0034 (11)0.0049 (11)
C140.0168 (12)0.0192 (13)0.0208 (14)0.0017 (10)0.0007 (10)0.0014 (10)
C130.0297 (14)0.0201 (13)0.0196 (14)0.0005 (11)0.0016 (11)0.0027 (11)
C50.0293 (14)0.0147 (12)0.0276 (14)0.0002 (11)0.0119 (11)0.0021 (12)
C40.0228 (13)0.0248 (14)0.0189 (14)0.0064 (11)0.0046 (11)0.0043 (11)
Geometric parameters (Å, º) top
S1—O11.4363 (16)C1—H1A0.97
S1—O21.4426 (16)C1—H1B0.97
S1—N11.5931 (19)C2—C31.505 (3)
S1—C91.774 (2)C2—H2A0.97
N1—C11.464 (3)C2—H2B0.97
N1—H10.90 (2)C3—C41.389 (3)
N2—C31.343 (3)C7—C61.379 (3)
N2—C71.345 (3)C7—H70.93
C12—C111.386 (3)C6—C51.385 (3)
C12—C131.390 (3)C6—H60.93
C12—H120.93C14—C131.381 (3)
C11—C101.382 (3)C14—H140.93
C11—H110.93C13—H130.93
C10—C91.388 (3)C5—C41.375 (3)
C10—H100.93C5—H50.93
C9—C141.389 (3)C4—H40.93
C1—C21.527 (3)
O1—S1—O2119.11 (10)C3—C2—C1112.65 (19)
O1—S1—N1109.21 (10)C3—C2—H2A109.1
O2—S1—N1106.65 (10)C1—C2—H2A109.1
O1—S1—C9106.83 (10)C3—C2—H2B109.1
O2—S1—C9106.11 (10)C1—C2—H2B109.1
N1—S1—C9108.55 (11)H2A—C2—H2B107.8
C1—N1—S1122.59 (16)N2—C3—C4121.9 (2)
C1—N1—H1117.2 (14)N2—C3—C2115.7 (2)
S1—N1—H1117.7 (14)C4—C3—C2122.4 (2)
C3—N2—C7117.8 (2)N2—C7—C6123.2 (2)
C11—C12—C13120.2 (2)N2—C7—H7118.4
C11—C12—H12119.9C6—C7—H7118.4
C13—C12—H12119.9C7—C6—C5118.7 (2)
C10—C11—C12120.2 (2)C7—C6—H6120.6
C10—C11—H11119.9C5—C6—H6120.6
C12—C11—H11119.9C13—C14—C9119.7 (2)
C11—C10—C9119.5 (2)C13—C14—H14120.2
C11—C10—H10120.3C9—C14—H14120.2
C9—C10—H10120.3C14—C13—C12119.9 (2)
C10—C9—C14120.6 (2)C14—C13—H13120.0
C10—C9—S1120.21 (18)C12—C13—H13120.0
C14—C9—S1119.02 (17)C4—C5—C6118.5 (2)
N1—C1—C2111.22 (19)C4—C5—H5120.7
N1—C1—H1A109.4C6—C5—H5120.7
C2—C1—H1A109.4C5—C4—C3119.8 (2)
N1—C1—H1B109.4C5—C4—H4120.1
C2—C1—H1B109.4C3—C4—H4120.1
H1A—C1—H1B108.0
O1—S1—N1—C135.2 (2)C7—N2—C3—C40.2 (3)
O2—S1—N1—C1165.09 (17)C7—N2—C3—C2179.5 (2)
C9—S1—N1—C181.0 (2)C1—C2—C3—N268.6 (3)
C13—C12—C11—C100.1 (4)C1—C2—C3—C4110.8 (2)
C12—C11—C10—C90.3 (3)C3—N2—C7—C60.3 (3)
C11—C10—C9—C140.3 (3)N2—C7—C6—C50.4 (4)
C11—C10—C9—S1174.83 (17)C10—C9—C14—C130.2 (3)
O1—S1—C9—C10153.95 (17)S1—C9—C14—C13175.36 (17)
O2—S1—C9—C1078.00 (19)C9—C14—C13—C120.6 (3)
N1—S1—C9—C1036.3 (2)C11—C12—C13—C140.5 (4)
O1—S1—C9—C1430.9 (2)C7—C6—C5—C40.1 (3)
O2—S1—C9—C1497.18 (19)C6—C5—C4—C30.6 (3)
N1—S1—C9—C14148.52 (18)N2—C3—C4—C50.6 (3)
S1—N1—C1—C296.2 (2)C2—C3—C4—C5180.0 (2)
N1—C1—C2—C3169.04 (19)
(III) N-[2-(pyridin-2-yl)ethyl]toluenesulfonamide top
Crystal data top
C14H16N2O2SDx = 1.341 Mg m3
Mr = 276.35Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 129 reflections
a = 7.6869 (5) Åθ = 3.2–24.8°
b = 15.7109 (10) ŵ = 0.24 mm1
c = 22.6742 (14) ÅT = 100 K
V = 2738.3 (3) Å3Block, colourless
Z = 80.25 × 0.24 × 0.23 mm
F(000) = 1168
Data collection top
Bruker APEXII CCD area-detector
diffractometer
3221 independent reflections
Radiation source: fine-focus sealed tube2429 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.103
Detector resolution: 8.3333 pixels mm-1θmax = 27.8°, θmin = 1.8°
ω and φ scansh = 1010
Absorption correction: multi-scan
(SADABS; Bruker, 2009)
k = 2020
Tmin = 0.90, Tmax = 0.95l = 2929
29603 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)] = 0.040Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.109H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0511P)2 + 0.5958P]
where P = (Fo2 + 2Fc2)/3
3221 reflections(Δ/σ)max = 0.001
176 parametersΔρmax = 0.34 e Å3
0 restraintsΔρmin = 0.50 e Å3
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 (isotroπc) 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
S10.77568 (6)0.65729 (3)0.129057 (19)0.02024 (14)
O10.59894 (16)0.64405 (8)0.14735 (6)0.0296 (3)
O20.86748 (17)0.59037 (8)0.09914 (6)0.0294 (3)
N10.88519 (19)0.68080 (9)0.18739 (6)0.0198 (3)
H10.844 (2)0.7242 (13)0.2061 (8)0.024*
N21.2340 (2)0.82332 (9)0.24113 (7)0.0255 (4)
C210.7678 (3)0.97221 (12)0.02566 (8)0.0303 (4)
H21A0.6820.96490.05720.045*
H21B0.88330.98080.0430.045*
H21C0.73661.02190.00180.045*
C180.7699 (2)0.89408 (11)0.01265 (8)0.0227 (4)
C170.6633 (2)0.88763 (11)0.06214 (8)0.0220 (4)
H170.59010.9340.07240.026*
C160.6621 (2)0.81476 (11)0.09668 (8)0.0211 (4)
H160.5870.81090.12980.025*
C150.7716 (2)0.74731 (11)0.08245 (7)0.0185 (4)
C11.0717 (2)0.66184 (11)0.19239 (8)0.0234 (4)
H1A1.09240.60390.17670.028*
H1B1.10310.66120.23470.028*
C21.1935 (2)0.72375 (11)0.16050 (8)0.0257 (4)
H2A1.31450.70280.16410.031*
H2B1.16330.72460.11810.031*
C31.1844 (2)0.81310 (11)0.18431 (8)0.0222 (4)
C71.2255 (3)0.90199 (12)0.26408 (8)0.0287 (4)
H71.26020.90950.3040.034*
C61.1694 (3)0.97251 (12)0.23331 (8)0.0283 (4)
H61.16511.02690.25150.034*
C190.8759 (2)0.82484 (12)0.00155 (8)0.0254 (4)
H190.94770.82770.03560.031*
C200.8785 (2)0.75196 (12)0.03298 (7)0.0244 (4)
H200.95250.70570.0230.029*
C51.1196 (3)0.96181 (12)0.17525 (9)0.0295 (4)
H51.08061.0090.15270.035*
C41.1271 (2)0.88171 (12)0.15046 (8)0.0255 (4)
H41.09340.87330.11060.031*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0211 (2)0.0157 (2)0.0240 (2)0.00021 (16)0.00187 (17)0.00098 (16)
O10.0222 (7)0.0263 (7)0.0402 (8)0.0049 (5)0.0022 (6)0.0079 (6)
O20.0386 (8)0.0201 (7)0.0296 (7)0.0074 (6)0.0042 (6)0.0059 (5)
N10.0221 (8)0.0178 (7)0.0196 (7)0.0014 (6)0.0001 (6)0.0024 (6)
N20.0246 (8)0.0241 (8)0.0278 (8)0.0037 (6)0.0055 (6)0.0055 (6)
C210.0365 (11)0.0303 (11)0.0240 (9)0.0016 (8)0.0038 (8)0.0075 (8)
C180.0243 (9)0.0241 (9)0.0199 (9)0.0050 (7)0.0051 (7)0.0005 (7)
C170.0233 (9)0.0184 (9)0.0242 (9)0.0021 (7)0.0025 (7)0.0024 (7)
C160.0219 (9)0.0210 (9)0.0205 (9)0.0004 (7)0.0001 (7)0.0028 (7)
C150.0194 (9)0.0171 (8)0.0189 (8)0.0003 (7)0.0041 (7)0.0017 (7)
C10.0223 (9)0.0186 (9)0.0294 (10)0.0022 (7)0.0047 (7)0.0004 (7)
C20.0197 (9)0.0254 (10)0.0320 (10)0.0025 (7)0.0020 (7)0.0004 (8)
C30.0180 (9)0.0226 (9)0.0261 (9)0.0027 (7)0.0018 (7)0.0029 (7)
C70.0316 (11)0.0296 (10)0.0248 (10)0.0115 (8)0.0037 (8)0.0028 (8)
C60.0308 (11)0.0210 (9)0.0332 (11)0.0049 (8)0.0056 (8)0.0017 (8)
C190.0247 (10)0.0324 (10)0.0192 (9)0.0001 (8)0.0013 (7)0.0001 (8)
C200.0241 (9)0.0273 (10)0.0219 (9)0.0060 (7)0.0004 (7)0.0041 (7)
C50.0305 (11)0.0246 (10)0.0333 (11)0.0021 (8)0.0016 (8)0.0101 (8)
C40.0273 (10)0.0288 (10)0.0203 (9)0.0006 (8)0.0009 (7)0.0036 (8)
Geometric parameters (Å, º) top
S1—O11.4357 (13)C15—C201.393 (2)
S1—O21.4365 (13)C1—C21.531 (2)
S1—N11.6107 (15)C1—H1A0.99
S1—C151.7658 (17)C1—H1B0.99
N1—C11.469 (2)C2—C31.506 (2)
N1—H10.86 (2)C2—H2A0.99
N2—C71.343 (2)C2—H2B0.99
N2—C31.353 (2)C3—C41.394 (2)
C21—C181.504 (2)C7—C61.379 (3)
C21—H21A0.98C7—H70.95
C21—H21B0.98C6—C51.381 (3)
C21—H21C0.98C6—H60.95
C18—C171.393 (2)C19—C201.387 (3)
C18—C191.397 (3)C19—H190.95
C17—C161.387 (2)C20—H200.95
C17—H170.95C5—C41.379 (3)
C16—C151.391 (2)C5—H50.95
C16—H160.95C4—H40.95
O1—S1—O2119.68 (8)N1—C1—H1B108.4
O1—S1—N1106.89 (8)C2—C1—H1B108.4
O2—S1—N1107.39 (8)H1A—C1—H1B107.4
O1—S1—C15105.79 (8)C3—C2—C1113.22 (15)
O2—S1—C15108.20 (8)C3—C2—H2A108.9
N1—S1—C15108.49 (8)C1—C2—H2A108.9
C1—N1—S1121.81 (12)C3—C2—H2B108.9
C1—N1—H1118.7 (13)C1—C2—H2B108.9
S1—N1—H1113.2 (13)H2A—C2—H2B107.7
C7—N2—C3117.67 (15)N2—C3—C4121.42 (17)
C18—C21—H21A109.5N2—C3—C2116.02 (15)
C18—C21—H21B109.5C4—C3—C2122.56 (16)
H21A—C21—H21B109.5N2—C7—C6123.99 (17)
C18—C21—H21C109.5N2—C7—H7118.0
H21A—C21—H21C109.5C6—C7—H7118.0
H21B—C21—H21C109.5C7—C6—C5118.11 (17)
C17—C18—C19118.17 (16)C7—C6—H6120.9
C17—C18—C21121.21 (16)C5—C6—H6120.9
C19—C18—C21120.60 (17)C20—C19—C18121.41 (16)
C16—C17—C18121.25 (16)C20—C19—H19119.3
C16—C17—H17119.4C18—C19—H19119.3
C18—C17—H17119.4C19—C20—C15119.29 (16)
C17—C16—C15119.59 (16)C19—C20—H20120.4
C17—C16—H16120.2C15—C20—H20120.4
C15—C16—H16120.2C4—C5—C6119.20 (17)
C16—C15—C20120.26 (16)C4—C5—H5120.4
C16—C15—S1118.83 (13)C6—C5—H5120.4
C20—C15—S1120.89 (13)C5—C4—C3119.61 (17)
N1—C1—C2115.57 (14)C5—C4—H4120.2
N1—C1—H1A108.4C3—C4—H4120.2
C2—C1—H1A108.4
O1—S1—N1—C1152.14 (13)C7—N2—C3—C40.3 (3)
O2—S1—N1—C122.54 (15)C7—N2—C3—C2179.19 (15)
C15—S1—N1—C194.19 (14)C1—C2—C3—N263.0 (2)
C19—C18—C17—C160.2 (3)C1—C2—C3—C4116.49 (19)
C21—C18—C17—C16178.39 (16)C3—N2—C7—C60.0 (3)
C18—C17—C16—C151.2 (3)N2—C7—C6—C50.3 (3)
C17—C16—C15—C201.6 (3)C17—C18—C19—C201.2 (3)
C17—C16—C15—S1176.94 (13)C21—C18—C19—C20179.44 (16)
O1—S1—C15—C1638.47 (16)C18—C19—C20—C150.8 (3)
O2—S1—C15—C16167.86 (13)C16—C15—C20—C190.6 (3)
N1—S1—C15—C1675.92 (15)S1—C15—C20—C19177.91 (13)
O1—S1—C15—C20142.98 (14)C7—C6—C5—C40.2 (3)
O2—S1—C15—C2013.58 (16)C6—C5—C4—C30.1 (3)
N1—S1—C15—C20102.63 (15)N2—C3—C4—C50.4 (3)
S1—N1—C1—C278.71 (18)C2—C3—C4—C5179.09 (16)
N1—C1—C2—C362.9 (2)
 

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