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Hybrid materials, fabricated by the combination of inorganic and organic components, have potential applications in chemistry and are endowed with the advantages of both building elements. There are several types of inter­molecular inter­actions present in these hybrid compounds, including electrostatic forces, π–π stacking and hydrogen-bonding inter­actions, the latter playing an important role in the construction of three-dimensional architectures and stabilizing supra­molecular crystal structures. Analysis of the inter­molecular inter­actions and their influence on packing modes therefore requires focused scientific attention. Four new organic–inorganic salts, namely 2-amino-4-methyl-3-nitro­pyridinium hydrogen sulfate, C6H8N3O2+·HSO4, bis­(2-amino-4-methyl-3-nitro­pyridinium) sulfate, 2C6H8N3O2+·SO42−, 2-amino-3-methyl­pyridinium hydrogen sulfate, C6H9N2+·HSO4, and bis­(2-amino-3-methyl­pyridinium) sulfate monohydrate, 2C6H9N2+·SO42−·H2O, have been synthesized and characterized by X-ray diffraction. The crystal structures are stabilized by intra- and inter­molecular hydrogen bonds, as well as by weak π–π stacking and lp–π (lp is lone pair) inter­actions. Hirshfeld surface analysis was employed in order to study inter­molecular inter­actions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229616016004/ku3189sup1.cif
Contains datablocks I, II, III, IV

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229616016004/ku3189Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229616016004/ku3189IIsup3.hkl
Contains datablock II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229616016004/ku3189IIIsup4.hkl
Contains datablock III

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229616016004/ku3189IVsup5.hkl
Contains datablock IV

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2053229616016004/ku3189sup6.pdf
Hydrogen-bond tables and fingerprint plots

CCDC references: 1509129; 1509128; 1509127; 1509126

Computing details top

For all compounds, data collection: CrysAlis PRO (Rigaku Oxford Diffraction, 2015); cell refinement: CrysAlis PRO (Rigaku Oxford Diffraction, 2015); data reduction: CrysAlis PRO (Rigaku Oxford Diffraction, 2015); program(s) used to solve structure: SHELXT (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015b); molecular graphics: DIAMOND (Brandenburg, 1997); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).

(I) 2-Amino-4-methyl-3-nitropyridinium hydrogen sulfate top
Crystal data top
C6H8N3O2+·HSO4Z = 4
Mr = 251.22F(000) = 520
Triclinic, P1Dx = 1.667 Mg m3
a = 7.835 (3) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.105 (3) ÅCell parameters from 5835 reflections
c = 15.881 (4) Åθ = 2.6–27.2°
α = 97.03 (3)°µ = 0.34 mm1
β = 90.21 (3)°T = 295 K
γ = 90.15 (3)°Block, colourless
V = 1000.9 (6) Å30.35 × 0.25 × 0.19 mm
Data collection top
Rigaku Oxford Diffraction Xcalibur Atlas
diffractometer
4903 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source3462 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.039
Detector resolution: 10.6249 pixels mm-1θmax = 29.5°, θmin = 2.6°
ω scansh = 1010
Absorption correction: analytical
[CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived Clark & Reid (1995)]
k = 1110
Tmin = 0.906, Tmax = 0.941l = 2022
15737 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.051 w = 1/[σ2(Fo2) + (0.057P)2 + 0.482P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.140(Δ/σ)max < 0.001
S = 1.03Δρmax = 0.36 e Å3
4903 reflectionsΔρmin = 0.26 e Å3
308 parametersExtinction correction: SHELXL2014 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.053 (3)
Primary atom site location: structure-invariant direct methods
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. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
S10.63763 (12)0.46573 (9)0.81181 (5)0.0458 (2)
S21.14346 (11)0.54496 (9)0.68721 (5)0.0445 (2)
O30.5457 (4)0.4259 (3)0.88454 (15)0.0636 (7)
O40.8158 (4)0.4193 (3)0.81129 (18)0.0691 (7)
O10.5657 (4)0.3578 (4)0.73207 (17)0.0721 (8)
H10.46480.38030.72580.108*
N210.3552 (4)0.8614 (3)0.84691 (15)0.0495 (7)
H210.39850.77220.82070.059*
O51.0629 (4)0.6246 (4)0.7708 (2)0.0870 (10)
H50.97960.56990.78190.131*
N220.3759 (4)0.7369 (3)0.96753 (17)0.0523 (7)
H22A0.41710.65080.93750.063*
H22B0.36300.73721.02130.063*
O23A0.3168 (4)0.9525 (4)1.10498 (15)0.0774 (9)
O20.6130 (4)0.6373 (3)0.79938 (18)0.0759 (9)
N230.2206 (4)1.0269 (4)1.06112 (18)0.0539 (7)
O13A0.8016 (5)0.0149 (4)0.39251 (16)0.0867 (10)
N110.8537 (4)0.1564 (3)0.64549 (17)0.0550 (7)
H110.89390.25230.66510.066*
C130.7522 (4)0.0329 (4)0.53327 (19)0.0410 (7)
N130.7042 (5)0.0655 (4)0.44409 (19)0.0594 (8)
C120.8215 (4)0.1255 (4)0.56154 (19)0.0425 (7)
C220.3323 (4)0.8688 (3)0.93097 (18)0.0394 (7)
N120.8551 (5)0.2460 (3)0.5147 (2)0.0617 (8)
H12A0.89570.33930.53810.074*
H12B0.83620.23110.46100.074*
C230.2562 (4)1.0166 (4)0.97069 (18)0.0405 (7)
O71.2457 (5)0.6765 (4)0.6604 (2)0.0708 (12)0.835 (7)
O13B0.5732 (4)0.1418 (5)0.4257 (2)0.1027 (12)
O23B0.0968 (4)1.1049 (4)1.0894 (2)0.0868 (10)
C240.2142 (4)1.1484 (4)0.9254 (2)0.0516 (8)
C140.7239 (4)0.1513 (4)0.5877 (2)0.0499 (8)
O61.0013 (6)0.4936 (6)0.6316 (2)0.0904 (14)0.835 (7)
O81.2358 (6)0.4042 (5)0.7044 (3)0.0940 (15)0.835 (7)
C250.2466 (5)1.1272 (4)0.8383 (2)0.0612 (10)
H250.22111.21200.80590.073*
C150.7664 (5)0.1061 (5)0.6734 (2)0.0633 (10)
H150.75240.18250.71200.076*
C260.3144 (6)0.9846 (5)0.8013 (2)0.0634 (11)
H260.33350.97110.74310.076*
C160.8265 (6)0.0453 (5)0.6998 (2)0.0660 (10)
H160.85000.07440.75720.079*
C410.6527 (6)0.3225 (4)0.5612 (3)0.0826 (14)
H41A0.53030.31770.56020.124*
H41B0.68880.39600.60080.124*
H41C0.69360.36310.50560.124*
C420.1419 (6)1.3117 (4)0.9643 (3)0.0803 (13)
H42A0.02241.29860.97500.120*
H42B0.15711.39350.92600.120*
H42C0.20011.34731.01670.120*
O8A1.120 (3)0.363 (2)0.6936 (11)0.065 (5)*0.165 (7)
O6A1.047 (2)0.578 (2)0.6174 (10)0.050 (4)*0.165 (7)
O7A1.319 (2)0.5916 (19)0.6971 (10)0.057 (5)*0.165 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0540 (5)0.0430 (4)0.0417 (4)0.0022 (4)0.0057 (4)0.0095 (3)
S20.0495 (5)0.0424 (4)0.0421 (4)0.0006 (4)0.0050 (4)0.0072 (3)
O30.0776 (19)0.0654 (15)0.0508 (14)0.0042 (14)0.0114 (13)0.0185 (12)
O40.0546 (16)0.0700 (16)0.0829 (19)0.0039 (13)0.0018 (14)0.0104 (14)
O10.0652 (18)0.0897 (19)0.0551 (16)0.0173 (15)0.0074 (14)0.0166 (13)
N210.070 (2)0.0436 (13)0.0343 (13)0.0065 (14)0.0001 (14)0.0025 (11)
O50.087 (2)0.088 (2)0.076 (2)0.0303 (17)0.0261 (17)0.0286 (16)
N220.074 (2)0.0421 (13)0.0422 (14)0.0050 (14)0.0018 (14)0.0110 (11)
O23A0.107 (2)0.0870 (19)0.0392 (14)0.0117 (18)0.0034 (15)0.0132 (13)
O20.099 (2)0.0501 (14)0.0839 (19)0.0085 (14)0.0216 (17)0.0275 (13)
N230.0526 (18)0.0587 (17)0.0476 (17)0.0117 (14)0.0067 (14)0.0042 (14)
O13A0.132 (3)0.094 (2)0.0352 (14)0.010 (2)0.0008 (17)0.0125 (13)
N110.069 (2)0.0509 (15)0.0436 (15)0.0042 (15)0.0005 (15)0.0021 (12)
C130.0392 (17)0.0456 (16)0.0374 (16)0.0098 (13)0.0006 (13)0.0014 (12)
N130.063 (2)0.0657 (18)0.0463 (17)0.0268 (16)0.0078 (16)0.0078 (14)
C120.0443 (18)0.0440 (16)0.0400 (17)0.0078 (14)0.0063 (14)0.0083 (13)
C220.0459 (18)0.0390 (15)0.0337 (15)0.0086 (13)0.0047 (14)0.0062 (12)
N120.080 (2)0.0476 (15)0.0604 (18)0.0003 (16)0.0094 (17)0.0191 (13)
C230.0449 (18)0.0400 (15)0.0364 (16)0.0066 (13)0.0018 (14)0.0046 (12)
O70.091 (3)0.0554 (19)0.070 (2)0.0150 (17)0.0039 (19)0.0236 (15)
O13B0.060 (2)0.141 (3)0.091 (2)0.015 (2)0.0280 (17)0.049 (2)
O23B0.063 (2)0.110 (2)0.079 (2)0.0046 (17)0.0191 (16)0.0205 (17)
C240.0443 (19)0.0438 (17)0.067 (2)0.0071 (14)0.0127 (17)0.0085 (15)
C140.0439 (19)0.0447 (17)0.062 (2)0.0098 (14)0.0115 (16)0.0109 (15)
O60.094 (3)0.105 (3)0.069 (2)0.028 (3)0.029 (2)0.002 (2)
O80.079 (3)0.075 (2)0.139 (4)0.022 (2)0.007 (3)0.057 (2)
C250.072 (3)0.0489 (19)0.067 (2)0.0049 (18)0.019 (2)0.0267 (18)
C150.075 (3)0.068 (2)0.052 (2)0.016 (2)0.017 (2)0.0278 (18)
C260.089 (3)0.065 (2)0.0392 (18)0.016 (2)0.0121 (19)0.0205 (16)
C160.084 (3)0.076 (2)0.0383 (19)0.010 (2)0.0017 (19)0.0088 (17)
C410.069 (3)0.0459 (19)0.131 (4)0.004 (2)0.013 (3)0.001 (2)
C420.070 (3)0.049 (2)0.120 (4)0.006 (2)0.007 (3)0.001 (2)
Geometric parameters (Å, º) top
S1—O31.433 (3)C13—N131.456 (4)
S1—O41.447 (3)C13—C121.414 (4)
S1—O11.552 (3)C13—C141.385 (4)
S1—O21.442 (2)N13—O13B1.213 (4)
S2—O51.542 (3)C12—N121.325 (4)
S2—O71.438 (3)C22—C231.417 (4)
S2—O61.447 (4)N12—H12A0.8600
S2—O81.407 (3)N12—H12B0.8600
S2—O8A1.500 (17)C23—C241.399 (4)
S2—O6A1.391 (15)C24—C251.397 (5)
S2—O7A1.428 (16)C24—C421.503 (5)
O1—H10.8200C14—C151.404 (5)
N21—H210.8600C14—C411.505 (5)
N21—C221.342 (4)C25—H250.9300
N21—C261.343 (4)C25—C261.342 (5)
O5—H50.8200C15—H150.9300
N22—H22A0.8600C15—C161.331 (6)
N22—H22B0.8600C26—H260.9300
N22—C221.323 (4)C16—H160.9300
O23A—N231.232 (4)C41—H41A0.9600
N23—C231.456 (4)C41—H41B0.9600
N23—O23B1.216 (4)C41—H41C0.9600
O13A—N131.227 (4)C42—H42A0.9600
N11—H110.8600C42—H42B0.9600
N11—C121.349 (4)C42—H42C0.9600
N11—C161.338 (4)
O3—S1—O4114.08 (18)N12—C12—C13127.0 (3)
O3—S1—O1108.45 (18)N21—C22—C23115.7 (3)
O3—S1—O2110.97 (16)N22—C22—N21117.4 (3)
O4—S1—O1102.80 (16)N22—C22—C23126.8 (3)
O2—S1—O4112.66 (18)C12—N12—H12A120.0
O2—S1—O1107.25 (18)C12—N12—H12B120.0
O7—S2—O5103.72 (18)H12A—N12—H12B120.0
O7—S2—O6114.5 (2)C22—C23—N23117.7 (3)
O6—S2—O5105.5 (2)C24—C23—N23120.4 (3)
O8—S2—O5108.1 (2)C24—C23—C22121.9 (3)
O8—S2—O7114.8 (2)C23—C24—C42124.6 (4)
O8—S2—O6109.6 (3)C25—C24—C23117.2 (3)
O8A—S2—O5101.7 (7)C25—C24—C42118.3 (3)
O6A—S2—O5111.3 (7)C13—C14—C15116.7 (3)
O6A—S2—O8A105.8 (10)C13—C14—C41124.7 (4)
O6A—S2—O7A122.2 (9)C15—C14—C41118.6 (3)
O7A—S2—O5103.1 (6)C24—C25—H25119.9
O7A—S2—O8A111.0 (10)C26—C25—C24120.2 (3)
S1—O1—H1109.5C26—C25—H25119.9
C22—N21—H21118.0C14—C15—H15119.7
C22—N21—C26123.9 (3)C16—C15—C14120.6 (3)
C26—N21—H21118.0C16—C15—H15119.7
S2—O5—H5109.5N21—C26—H26119.5
H22A—N22—H22B120.0C25—C26—N21121.1 (3)
C22—N22—H22A120.0C25—C26—H26119.5
C22—N22—H22B120.0N11—C16—H16119.4
O23A—N23—C23117.7 (3)C15—C16—N11121.3 (3)
O23B—N23—O23A123.3 (3)C15—C16—H16119.4
O23B—N23—C23119.0 (3)C14—C41—H41A109.5
C12—N11—H11118.3C14—C41—H41B109.5
C16—N11—H11118.3C14—C41—H41C109.5
C16—N11—C12123.4 (3)H41A—C41—H41B109.5
C12—C13—N13117.1 (3)H41A—C41—H41C109.5
C14—C13—N13120.6 (3)H41B—C41—H41C109.5
C14—C13—C12122.3 (3)C24—C42—H42A109.5
O13A—N13—C13117.1 (3)C24—C42—H42B109.5
O13B—N13—O13A124.6 (4)C24—C42—H42C109.5
O13B—N13—C13118.3 (4)H42A—C42—H42B109.5
N11—C12—C13115.8 (3)H42A—C42—H42C109.5
N12—C12—N11117.2 (3)H42B—C42—H42C109.5
N21—C22—C23—N23176.9 (3)C22—N21—C26—C250.1 (6)
N21—C22—C23—C242.4 (5)C22—C23—C24—C251.5 (5)
N22—C22—C23—N230.2 (5)C22—C23—C24—C42176.6 (3)
N22—C22—C23—C24179.5 (3)C23—C24—C25—C260.3 (5)
O23A—N23—C23—C2231.3 (4)O23B—N23—C23—C22147.2 (3)
O23A—N23—C23—C24149.4 (3)O23B—N23—C23—C2432.1 (5)
N23—C23—C24—C25177.8 (3)C24—C25—C26—N211.2 (6)
N23—C23—C24—C424.1 (5)C14—C13—N13—O13A141.3 (3)
C13—C14—C15—C161.7 (6)C14—C13—N13—O13B37.9 (4)
N13—C13—C12—N11175.6 (3)C14—C13—C12—N111.9 (5)
N13—C13—C12—N123.3 (5)C14—C13—C12—N12179.2 (3)
N13—C13—C14—C15177.0 (3)C14—C15—C16—N112.3 (7)
N13—C13—C14—C413.3 (5)C26—N21—C22—N22179.0 (4)
C12—N11—C16—C150.8 (6)C26—N21—C22—C231.6 (5)
C12—C13—N13—O13A41.2 (4)C16—N11—C12—C131.3 (5)
C12—C13—N13—O13B139.7 (3)C16—N11—C12—N12179.6 (4)
C12—C13—C14—C150.5 (5)C41—C14—C15—C16178.6 (4)
C12—C13—C14—C41179.2 (3)C42—C24—C25—C26178.6 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O8i0.821.842.655 (5)173
O1—H1···O7Ai0.822.152.812 (17)137
N21—H21···O20.862.012.764 (4)145
N21—H21···O7Ai0.862.383.040 (15)134
O5—H5···O40.821.872.680 (4)171
N22—H22A···O30.862.163.013 (4)169
N22—H22B···O3ii0.862.232.897 (4)134
N22—H22B···O23A0.862.092.667 (4)124
N11—H11···O60.862.252.998 (6)145
N11—H11···O8A0.862.012.72 (2)139
N12—H12A···O60.862.002.801 (5)155
N12—H12B···O13A0.862.172.721 (4)122
N12—H12B···O7iii0.862.243.028 (5)152
C25—H25···O8iv0.932.383.276 (5)163
C25—H25···O8Aiv0.932.423.316 (17)163
C15—H15···O2v0.932.403.286 (4)160
C26—H26···O13Avi0.932.463.244 (4)142
C16—H16···O23Aii0.932.593.299 (4)134
Symmetry codes: (i) x1, y, z; (ii) x+1, y+1, z+2; (iii) x+2, y+1, z+1; (iv) x1, y+1, z; (v) x, y1, z; (vi) x+1, y+1, z+1.
(II) Bis(2-amino-4-methyl-3-nitropyridinium) sulfate top
Crystal data top
2C6H8N3O2+·SO42F(000) = 840
Mr = 404.37Dx = 1.540 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 10.557 (4) ÅCell parameters from 1601 reflections
b = 13.632 (4) Åθ = 2.5–28.6°
c = 12.211 (4) ŵ = 0.24 mm1
β = 97.12 (3)°T = 295 K
V = 1743.8 (10) Å3Block, colourless
Z = 40.60 × 0.41 × 0.26 mm
Data collection top
Rigaku Oxford Diffraction Xcalibur Atlas
diffractometer
2042 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source1686 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.024
Detector resolution: 10.6249 pixels mm-1θmax = 29.1°, θmin = 2.8°
ω scansh = 1414
Absorption correction: analytical
[CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived Clark & Reid (1995)]
k = 1418
Tmin = 0.917, Tmax = 0.955l = 1616
4844 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.041 w = 1/[σ2(Fo2) + (0.061P)2 + 0.714P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.120(Δ/σ)max < 0.001
S = 1.07Δρmax = 0.22 e Å3
2042 reflectionsΔρmin = 0.32 e Å3
125 parametersExtinction correction: SHELXL2014 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0042 (10)
Primary atom site location: structure-invariant direct methods
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.00000.50272 (4)0.75000.0363 (2)
O110.11223 (11)0.56597 (9)0.78384 (9)0.0432 (3)
O120.02621 (14)0.44247 (10)0.65665 (11)0.0561 (4)
N10.26670 (13)0.60819 (11)0.63249 (11)0.0394 (4)
H10.21690.58430.67640.047*
O3A0.40140 (15)0.47087 (12)0.36468 (12)0.0635 (4)
N30.36940 (14)0.55646 (13)0.36171 (12)0.0447 (4)
O3B0.34498 (18)0.60392 (13)0.27720 (11)0.0731 (5)
N20.20494 (15)0.48257 (12)0.51249 (13)0.0498 (4)
H2A0.15630.46120.55880.060*
H2B0.20830.45210.45120.060*
C30.35736 (15)0.60566 (12)0.46684 (13)0.0360 (4)
C20.27430 (15)0.56212 (13)0.53545 (12)0.0362 (4)
C60.33368 (18)0.68972 (14)0.66330 (15)0.0457 (4)
H60.32460.71850.73090.055*
C40.42775 (16)0.68808 (13)0.49592 (15)0.0425 (4)
C50.41376 (18)0.73077 (14)0.59838 (16)0.0486 (5)
H50.45940.78700.62140.058*
C410.5217 (2)0.73115 (17)0.42627 (19)0.0648 (6)
H41A0.57730.68040.40580.097*
H41B0.57140.78080.46760.097*
H41C0.47650.75980.36100.097*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0422 (3)0.0330 (3)0.0352 (3)0.0000.0112 (2)0.000
O110.0446 (7)0.0493 (7)0.0359 (6)0.0059 (6)0.0060 (5)0.0039 (5)
O120.0642 (9)0.0474 (8)0.0615 (8)0.0105 (7)0.0270 (7)0.0217 (7)
N10.0423 (8)0.0440 (8)0.0322 (7)0.0024 (6)0.0055 (6)0.0021 (6)
O3A0.0673 (9)0.0622 (10)0.0602 (9)0.0180 (8)0.0047 (7)0.0150 (8)
N30.0404 (8)0.0574 (10)0.0374 (8)0.0031 (7)0.0089 (6)0.0015 (7)
O3B0.1030 (13)0.0801 (11)0.0375 (7)0.0059 (10)0.0143 (8)0.0092 (7)
N20.0563 (10)0.0585 (10)0.0358 (8)0.0212 (8)0.0106 (7)0.0055 (7)
C30.0354 (8)0.0393 (9)0.0333 (7)0.0016 (7)0.0040 (6)0.0029 (7)
C20.0370 (8)0.0412 (9)0.0297 (7)0.0008 (7)0.0010 (6)0.0037 (7)
C60.0545 (11)0.0412 (10)0.0407 (9)0.0020 (8)0.0028 (8)0.0071 (8)
C40.0419 (9)0.0367 (9)0.0489 (10)0.0005 (7)0.0057 (7)0.0077 (8)
C50.0541 (11)0.0362 (9)0.0542 (10)0.0045 (8)0.0016 (9)0.0022 (8)
C410.0644 (13)0.0617 (14)0.0720 (14)0.0183 (11)0.0236 (11)0.0048 (12)
Geometric parameters (Å, º) top
S1—O11i1.4820 (13)N2—C21.319 (2)
S1—O111.4820 (13)C3—C21.416 (2)
S1—O12i1.4591 (13)C3—C41.369 (2)
S1—O121.4590 (13)C6—H60.9300
N1—H10.8600C6—C51.350 (3)
N1—C21.352 (2)C4—C51.404 (3)
N1—C61.346 (2)C4—C411.504 (3)
O3A—N31.214 (2)C5—H50.9300
N3—O3B1.218 (2)C41—H41A0.9600
N3—C31.468 (2)C41—H41B0.9600
N2—H2A0.8600C41—H41C0.9600
N2—H2B0.8600
O11—S1—O11i108.85 (11)N1—C2—C3115.60 (15)
O12i—S1—O11i108.84 (7)N2—C2—N1118.45 (15)
O12—S1—O11108.83 (7)N2—C2—C3125.94 (15)
O12i—S1—O11109.40 (8)N1—C6—H6119.2
O12—S1—O11i109.40 (8)N1—C6—C5121.58 (17)
O12—S1—O12i111.48 (12)C5—C6—H6119.2
C2—N1—H1118.6C3—C4—C5117.22 (16)
C6—N1—H1118.6C3—C4—C41123.26 (17)
C6—N1—C2122.85 (15)C5—C4—C41119.46 (17)
O3A—N3—O3B124.38 (16)C6—C5—C4119.62 (17)
O3A—N3—C3117.84 (15)C6—C5—H5120.2
O3B—N3—C3117.77 (16)C4—C5—H5120.2
H2A—N2—H2B120.0C4—C41—H41A109.5
C2—N2—H2A120.0C4—C41—H41B109.5
C2—N2—H2B120.0C4—C41—H41C109.5
C2—C3—N3116.93 (15)H41A—C41—H41B109.5
C4—C3—N3119.91 (15)H41A—C41—H41C109.5
C4—C3—C2123.12 (15)H41B—C41—H41C109.5
N1—C6—C5—C40.2 (3)C3—C4—C5—C60.3 (3)
O3A—N3—C3—C255.9 (2)C2—N1—C6—C50.2 (3)
O3A—N3—C3—C4122.15 (19)C2—C3—C4—C50.9 (3)
N3—C3—C2—N1178.99 (14)C2—C3—C4—C41176.33 (18)
N3—C3—C2—N21.4 (3)C6—N1—C2—N2179.99 (16)
N3—C3—C4—C5178.87 (16)C6—N1—C2—C30.4 (2)
N3—C3—C4—C411.6 (3)C4—C3—C2—N11.0 (2)
O3B—N3—C3—C2123.13 (19)C4—C3—C2—N2179.46 (16)
O3B—N3—C3—C458.8 (2)C41—C4—C5—C6177.07 (18)
Symmetry code: (i) x, y, z+3/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O110.861.832.675 (2)165
N2—H2A···O120.861.952.790 (2)166
N2—H2B···O11ii0.862.182.918 (2)144
N2—H2B···O3A0.862.422.918 (3)117
C5—H5···O12iii0.932.263.168 (2)166
Symmetry codes: (ii) x, y+1, z1/2; (iii) x+1/2, y+1/2, z.
(III) 2-Amino-3-methylpyridinium hydrogen sulfate top
Crystal data top
C6H9N2+·HSO4Z = 4
Mr = 206.22F(000) = 432
Triclinic, P1Dx = 1.510 Mg m3
a = 8.029 (3) ÅMo Kα radiation, λ = 0.71073 Å
b = 10.645 (4) ÅCell parameters from 5715 reflections
c = 11.541 (4) Åθ = 2.8–28.0°
α = 82.95 (3)°µ = 0.34 mm1
β = 87.95 (3)°T = 295 K
γ = 67.93 (3)°Plank, colourless
V = 907.1 (6) Å30.41 × 0.15 × 0.07 mm
Data collection top
Rigaku Oxford Diffraction Xcalibur Atlas
diffractometer
4467 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source2889 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.042
Detector resolution: 10.6249 pixels mm-1θmax = 29.5°, θmin = 2.6°
ω scansh = 1110
Absorption correction: analytical
[CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived Clark & Reid (1995)]
k = 1413
Tmin = 0.907, Tmax = 0.976l = 1515
19746 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.048H-atom parameters constrained
wR(F2) = 0.139 w = 1/[σ2(Fo2) + (0.063P)2 + 0.193P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max < 0.001
4467 reflectionsΔρmax = 0.24 e Å3
239 parametersΔρmin = 0.37 e Å3
0 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S20.01914 (8)0.69762 (6)0.29888 (5)0.04795 (19)
S10.54773 (8)0.68435 (6)0.16433 (5)0.04654 (18)
O120.6566 (2)0.65348 (17)0.06171 (14)0.0553 (4)
O210.0772 (2)0.82022 (17)0.26289 (19)0.0667 (5)
H21A0.17430.79390.22980.100*
O110.5640 (2)0.81267 (16)0.20654 (17)0.0587 (5)
H11A0.65850.79010.24310.088*
O240.1603 (2)0.76257 (19)0.34223 (16)0.0639 (5)
O140.3587 (2)0.7288 (2)0.13688 (17)0.0672 (5)
O130.6099 (2)0.57557 (17)0.25920 (14)0.0587 (5)
O220.0269 (2)0.63064 (17)0.19637 (14)0.0561 (4)
O230.1421 (2)0.60922 (18)0.38971 (15)0.0686 (5)
N110.4358 (3)0.3689 (2)0.37549 (17)0.0517 (5)
H110.34650.44520.37740.062*
N210.9474 (3)0.35786 (19)0.25743 (17)0.0511 (5)
H210.86190.43670.25540.061*
C130.6205 (3)0.1894 (2)0.2702 (2)0.0472 (5)
N220.9100 (3)0.3721 (2)0.05915 (18)0.0663 (6)
H22A0.82890.45240.06070.080*
H22B0.93710.33780.00590.080*
N120.3748 (3)0.3853 (2)0.18024 (18)0.0592 (6)
H12A0.28740.46150.18670.071*
H12B0.39690.35400.11380.071*
C231.1284 (3)0.1684 (2)0.1620 (2)0.0479 (5)
C241.2083 (3)0.1088 (2)0.2673 (2)0.0567 (6)
H241.29700.02160.27210.068*
C220.9932 (3)0.3011 (2)0.1571 (2)0.0468 (5)
C251.1625 (4)0.1732 (3)0.3683 (2)0.0617 (7)
H251.22220.13190.43870.074*
C170.6648 (4)0.1269 (3)0.1581 (2)0.0607 (7)
H17A0.56700.10380.13540.091*
H17B0.77190.04600.16860.091*
H17C0.68400.19110.09820.091*
C120.4754 (3)0.3160 (2)0.2728 (2)0.0453 (5)
C271.1760 (4)0.1001 (3)0.0522 (2)0.0636 (7)
H27A1.22630.15090.00300.095*
H27B1.06980.09690.01920.095*
H27C1.26240.00890.07030.095*
C140.7143 (4)0.1294 (3)0.3713 (2)0.0608 (7)
H140.81070.04650.37110.073*
C261.0286 (4)0.2973 (3)0.3608 (2)0.0586 (7)
H260.99230.34140.42740.070*
C160.5294 (4)0.3079 (3)0.4754 (2)0.0621 (7)
H160.49650.34850.54390.075*
C150.6697 (4)0.1890 (3)0.4759 (2)0.0678 (8)
H150.73600.14700.54390.081*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S20.0514 (4)0.0537 (4)0.0352 (3)0.0129 (3)0.0023 (3)0.0132 (3)
S10.0491 (3)0.0506 (3)0.0355 (3)0.0130 (3)0.0013 (2)0.0068 (2)
O120.0594 (10)0.0645 (10)0.0337 (9)0.0127 (8)0.0044 (8)0.0111 (8)
O210.0654 (11)0.0576 (10)0.0785 (15)0.0219 (9)0.0072 (10)0.0191 (10)
O110.0598 (10)0.0485 (9)0.0596 (12)0.0081 (7)0.0115 (9)0.0128 (8)
O240.0531 (10)0.0852 (13)0.0511 (11)0.0180 (9)0.0055 (8)0.0266 (9)
O140.0484 (10)0.0898 (13)0.0592 (12)0.0201 (9)0.0038 (9)0.0108 (10)
O130.0760 (11)0.0542 (10)0.0393 (10)0.0188 (8)0.0006 (8)0.0013 (8)
O220.0670 (10)0.0652 (10)0.0373 (9)0.0221 (8)0.0003 (8)0.0192 (8)
O230.0768 (12)0.0708 (12)0.0374 (10)0.0019 (9)0.0075 (9)0.0108 (9)
N110.0660 (13)0.0482 (11)0.0377 (11)0.0159 (9)0.0007 (10)0.0112 (9)
N210.0656 (12)0.0432 (10)0.0377 (11)0.0116 (9)0.0055 (9)0.0092 (8)
C130.0557 (14)0.0451 (12)0.0399 (13)0.0169 (10)0.0032 (11)0.0070 (10)
N220.0873 (16)0.0519 (12)0.0376 (12)0.0002 (11)0.0033 (11)0.0066 (9)
N120.0695 (13)0.0526 (11)0.0398 (12)0.0019 (10)0.0120 (10)0.0127 (9)
C230.0611 (14)0.0417 (12)0.0401 (13)0.0181 (10)0.0062 (11)0.0076 (10)
C240.0667 (16)0.0472 (13)0.0468 (15)0.0122 (11)0.0000 (12)0.0007 (11)
C220.0580 (14)0.0464 (12)0.0342 (12)0.0172 (11)0.0036 (10)0.0061 (10)
C250.0794 (18)0.0621 (16)0.0379 (14)0.0213 (14)0.0061 (13)0.0008 (12)
C170.0657 (16)0.0612 (15)0.0459 (15)0.0100 (12)0.0012 (12)0.0174 (12)
C120.0550 (13)0.0466 (12)0.0356 (12)0.0192 (10)0.0021 (10)0.0082 (10)
C270.0858 (19)0.0533 (14)0.0456 (15)0.0171 (13)0.0122 (13)0.0156 (12)
C140.0706 (16)0.0525 (14)0.0486 (15)0.0096 (12)0.0123 (13)0.0062 (12)
C260.0829 (18)0.0623 (16)0.0319 (13)0.0280 (14)0.0033 (12)0.0084 (11)
C160.091 (2)0.0644 (16)0.0316 (13)0.0288 (15)0.0051 (13)0.0087 (11)
C150.091 (2)0.0639 (17)0.0414 (15)0.0211 (15)0.0182 (14)0.0011 (12)
Geometric parameters (Å, º) top
S2—O211.550 (2)N12—H12A0.8600
S2—O241.4450 (18)N12—H12B0.8600
S2—O221.4423 (17)N12—C121.326 (3)
S2—O231.4468 (19)C23—C241.361 (3)
S1—O121.4425 (18)C23—C221.417 (3)
S1—O111.5564 (18)C23—C271.504 (3)
S1—O141.4442 (18)C24—H240.9300
S1—O131.4430 (18)C24—C251.392 (4)
O21—H21A0.8200C25—H250.9300
O11—H11A0.8200C25—C261.349 (4)
N11—H110.8600C17—H17A0.9600
N11—C121.351 (3)C17—H17B0.9600
N11—C161.352 (3)C17—H17C0.9600
N21—H210.8600C27—H27A0.9600
N21—C221.348 (3)C27—H27B0.9600
N21—C261.347 (3)C27—H27C0.9600
C13—C171.498 (3)C14—H140.9300
C13—C121.415 (3)C14—C151.405 (4)
C13—C141.362 (3)C26—H260.9300
N22—H22A0.8600C16—H160.9300
N22—H22B0.8600C16—C151.341 (4)
N22—C221.327 (3)C15—H150.9300
O24—S2—O21102.57 (11)C25—C24—H24118.7
O24—S2—O23112.14 (11)N21—C22—C23118.1 (2)
O22—S2—O21107.66 (12)N22—C22—N21118.4 (2)
O22—S2—O24114.21 (10)N22—C22—C23123.5 (2)
O22—S2—O23112.21 (11)C24—C25—H25121.1
O23—S2—O21107.24 (12)C26—C25—C24117.9 (2)
O12—S1—O11107.83 (11)C26—C25—H25121.1
O12—S1—O14111.58 (11)C13—C17—H17A109.5
O12—S1—O13112.14 (10)C13—C17—H17B109.5
O14—S1—O11103.25 (11)C13—C17—H17C109.5
O13—S1—O11106.97 (11)H17A—C17—H17B109.5
O13—S1—O14114.35 (12)H17A—C17—H17C109.5
S2—O21—H21A109.5H17B—C17—H17C109.5
S1—O11—H11A109.5N11—C12—C13118.3 (2)
C12—N11—H11118.4N12—C12—N11118.0 (2)
C12—N11—C16123.3 (2)N12—C12—C13123.7 (2)
C16—N11—H11118.4C23—C27—H27A109.5
C22—N21—H21118.3C23—C27—H27B109.5
C26—N21—H21118.3C23—C27—H27C109.5
C26—N21—C22123.3 (2)H27A—C27—H27B109.5
C12—C13—C17119.4 (2)H27A—C27—H27C109.5
C14—C13—C17122.8 (2)H27B—C27—H27C109.5
C14—C13—C12117.8 (2)C13—C14—H14119.0
H22A—N22—H22B120.0C13—C14—C15122.0 (2)
C22—N22—H22A120.0C15—C14—H14119.0
C22—N22—H22B120.0N21—C26—C25120.4 (2)
H12A—N12—H12B120.0N21—C26—H26119.8
C12—N12—H12A120.0C25—C26—H26119.8
C12—N12—H12B120.0N11—C16—H16119.9
C24—C23—C22117.6 (2)C15—C16—N11120.1 (2)
C24—C23—C27123.3 (2)C15—C16—H16119.9
C22—C23—C27119.1 (2)C14—C15—H15120.7
C23—C24—H24118.7C16—C15—C14118.5 (2)
C23—C24—C25122.6 (2)C16—C15—H15120.7
N11—C16—C15—C141.0 (4)C12—N11—C16—C150.2 (4)
C13—C14—C15—C160.6 (4)C12—C13—C14—C150.5 (4)
C23—C24—C25—C262.6 (4)C27—C23—C24—C25179.8 (3)
C24—C23—C22—N212.5 (3)C27—C23—C22—N21177.2 (2)
C24—C23—C22—N22177.4 (2)C27—C23—C22—N222.9 (4)
C24—C25—C26—N212.2 (4)C14—C13—C12—N111.2 (3)
C22—N21—C26—C250.5 (4)C14—C13—C12—N12179.3 (2)
C22—C23—C24—C250.2 (4)C26—N21—C22—N22177.0 (2)
C17—C13—C12—N11178.7 (2)C26—N21—C22—C232.9 (4)
C17—C13—C12—N120.8 (4)C16—N11—C12—C131.0 (4)
C17—C13—C14—C15179.4 (3)C16—N11—C12—N12179.6 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O21—H21A···O140.821.772.575 (3)168
O11—H11A···O24i0.821.802.607 (3)169
N11—H11···O230.861.912.770 (3)176
N21—H21···O130.862.012.829 (3)159
N22—H22A···O120.862.072.924 (3)174
N22—H22B···O22ii0.862.212.976 (3)149
N12—H12A···O220.862.203.043 (3)167
N12—H12B···O12ii0.862.102.906 (3)155
C26—H26···O23iii0.932.363.249 (3)159
C16—H16···O13iii0.932.523.437 (3)170
Symmetry codes: (i) x+1, y, z; (ii) x+1, y+1, z; (iii) x+1, y+1, z+1.
(IV) Bis(2-amino-3-methylpyridinium) sulfate monohydrate top
Crystal data top
2C6H9N2+·SO42·H2OF(000) = 704
Mr = 332.38Dx = 1.414 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 10.909 (4) ÅCell parameters from 3026 reflections
b = 10.700 (4) Åθ = 3.5–27.1°
c = 14.267 (4) ŵ = 0.24 mm1
β = 110.34 (3)°T = 295 K
V = 1561.5 (10) Å3Block, colourless
Z = 40.47 × 0.38 × 0.24 mm
Data collection top
Rigaku Oxford Diffraction Xcalibur Atlas
diffractometer
3627 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source2471 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.023
Detector resolution: 10.6249 pixels mm-1θmax = 29.3°, θmin = 3.0°
ω scansh = 1313
Absorption correction: analytical
[CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived Clark & Reid (1995)]
k = 1013
Tmin = 0.920, Tmax = 0.956l = 1317
8806 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.045H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.116 w = 1/[σ2(Fo2) + (0.046P)2 + 0.366P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
3627 reflectionsΔρmax = 0.17 e Å3
209 parametersΔρmin = 0.35 e Å3
0 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.72531 (5)0.29571 (5)0.46286 (4)0.04223 (16)
O10.62744 (12)0.39662 (12)0.45202 (10)0.0483 (4)
O40.67656 (15)0.21620 (15)0.37315 (11)0.0662 (5)
O30.73891 (16)0.22195 (14)0.55118 (11)0.0594 (4)
N210.67255 (15)0.64287 (15)0.47175 (11)0.0410 (4)
H210.66430.56330.46320.049*
O20.84963 (13)0.35313 (14)0.46971 (13)0.0661 (5)
O1W0.7618 (2)0.12591 (18)0.22015 (17)0.0717 (5)
N110.41313 (18)0.17852 (17)0.29541 (12)0.0521 (5)
H110.49490.19680.32040.063*
N220.89453 (15)0.61269 (16)0.52966 (13)0.0516 (4)
H22A0.88080.53370.52080.062*
H22B0.97320.64090.55270.062*
N120.36908 (17)0.38697 (17)0.30324 (13)0.0553 (5)
H12A0.45170.40050.33020.066*
H12B0.31480.44820.29270.066*
C230.8078 (2)0.82167 (19)0.52160 (14)0.0443 (5)
C260.56326 (19)0.7130 (2)0.44841 (15)0.0468 (5)
H260.48160.67490.42420.056*
C220.79406 (18)0.69127 (18)0.50771 (13)0.0388 (4)
C130.1901 (2)0.2416 (2)0.23286 (14)0.0493 (5)
C120.3255 (2)0.2719 (2)0.27786 (13)0.0445 (5)
C250.5721 (2)0.8377 (2)0.46011 (16)0.0544 (6)
H250.49720.88670.44440.065*
C240.6960 (2)0.8922 (2)0.49637 (16)0.0546 (6)
H240.70300.97850.50360.066*
C270.9415 (2)0.8768 (2)0.56570 (19)0.0685 (7)
H27A0.98390.84360.63160.103*
H27B0.93480.96600.56940.103*
H27C0.99180.85620.52440.103*
C160.3790 (3)0.0576 (2)0.27570 (17)0.0658 (7)
H160.44360.00340.28920.079*
C170.0920 (2)0.3434 (2)0.20901 (18)0.0659 (7)
H17A0.09000.37990.26990.099*
H17B0.00730.31010.17170.099*
H17C0.11500.40620.17000.099*
C150.2520 (3)0.0243 (3)0.23659 (18)0.0732 (7)
H150.22750.05910.22470.088*
C140.1587 (3)0.1193 (2)0.21458 (16)0.0627 (6)
H140.07090.09770.18610.075*
H1WA0.746 (3)0.166 (3)0.261 (2)0.099 (12)*
H1WB0.759 (3)0.177 (3)0.177 (2)0.095 (12)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0335 (3)0.0393 (3)0.0549 (3)0.0003 (2)0.0168 (2)0.0003 (2)
O10.0340 (7)0.0388 (8)0.0710 (9)0.0019 (6)0.0169 (6)0.0020 (7)
O40.0582 (10)0.0753 (11)0.0661 (10)0.0010 (8)0.0230 (8)0.0241 (8)
O30.0675 (10)0.0502 (9)0.0609 (9)0.0090 (8)0.0228 (8)0.0120 (7)
N210.0355 (8)0.0400 (9)0.0489 (9)0.0032 (7)0.0165 (7)0.0028 (7)
O20.0366 (8)0.0582 (10)0.1082 (13)0.0027 (7)0.0309 (8)0.0041 (9)
O1W0.0992 (15)0.0568 (12)0.0617 (12)0.0058 (10)0.0313 (11)0.0016 (10)
N110.0539 (11)0.0579 (12)0.0420 (10)0.0042 (9)0.0135 (8)0.0007 (8)
N220.0348 (9)0.0484 (10)0.0696 (12)0.0014 (8)0.0158 (8)0.0002 (9)
N120.0434 (10)0.0512 (11)0.0641 (11)0.0017 (9)0.0094 (8)0.0014 (9)
C230.0469 (11)0.0444 (12)0.0442 (11)0.0103 (10)0.0192 (9)0.0023 (9)
C260.0327 (10)0.0588 (14)0.0499 (12)0.0005 (10)0.0154 (8)0.0024 (10)
C220.0346 (10)0.0446 (11)0.0387 (10)0.0032 (9)0.0149 (8)0.0009 (8)
C130.0510 (12)0.0586 (14)0.0357 (11)0.0063 (11)0.0117 (9)0.0012 (9)
C120.0469 (11)0.0508 (13)0.0344 (10)0.0032 (10)0.0123 (8)0.0033 (9)
C250.0516 (13)0.0539 (14)0.0619 (14)0.0133 (11)0.0250 (10)0.0087 (11)
C240.0705 (15)0.0411 (12)0.0591 (13)0.0013 (11)0.0312 (11)0.0028 (10)
C270.0628 (15)0.0621 (15)0.0815 (17)0.0272 (13)0.0261 (13)0.0129 (13)
C160.0914 (19)0.0531 (15)0.0548 (14)0.0156 (14)0.0281 (13)0.0017 (11)
C170.0463 (13)0.0798 (17)0.0616 (14)0.0017 (12)0.0062 (11)0.0001 (12)
C150.107 (2)0.0537 (15)0.0604 (15)0.0119 (16)0.0312 (15)0.0092 (12)
C140.0704 (16)0.0673 (16)0.0490 (13)0.0161 (14)0.0189 (11)0.0081 (11)
Geometric parameters (Å, º) top
S1—O11.4882 (14)C23—C271.494 (3)
S1—O41.4737 (16)C26—H260.9300
S1—O31.4500 (16)C26—C251.344 (3)
S1—O21.4609 (15)C13—C121.428 (3)
N21—H210.8600C13—C171.482 (3)
N21—C261.349 (2)C13—C141.354 (3)
N21—C221.347 (2)C25—H250.9300
O1W—H1WA0.78 (3)C25—C241.396 (3)
O1W—H1WB0.82 (3)C24—H240.9300
N11—H110.8600C27—H27A0.9600
N11—C121.345 (3)C27—H27B0.9600
N11—C161.349 (3)C27—H27C0.9600
N22—H22A0.8600C16—H160.9300
N22—H22B0.8600C16—C151.349 (4)
N22—C221.330 (2)C17—H17A0.9600
N12—H12A0.8600C17—H17B0.9600
N12—H12B0.8600C17—H17C0.9600
N12—C121.324 (3)C15—H150.9300
C23—C221.410 (3)C15—C141.395 (4)
C23—C241.371 (3)C14—H140.9300
O4—S1—O1107.42 (9)N11—C12—C13118.2 (2)
O3—S1—O1109.77 (9)N12—C12—N11118.36 (19)
O3—S1—O4109.73 (10)N12—C12—C13123.5 (2)
O3—S1—O2111.01 (10)C26—C25—H25120.7
O2—S1—O1108.52 (9)C26—C25—C24118.6 (2)
O2—S1—O4110.32 (10)C24—C25—H25120.7
C26—N21—H21118.4C23—C24—C25121.7 (2)
C22—N21—H21118.4C23—C24—H24119.1
C22—N21—C26123.26 (17)C25—C24—H24119.1
H1WA—O1W—H1WB104 (3)C23—C27—H27A109.5
C12—N11—H11118.4C23—C27—H27B109.5
C12—N11—C16123.2 (2)C23—C27—H27C109.5
C16—N11—H11118.4H27A—C27—H27B109.5
H22A—N22—H22B120.0H27A—C27—H27C109.5
C22—N22—H22A120.0H27B—C27—H27C109.5
C22—N22—H22B120.0N11—C16—H16119.7
H12A—N12—H12B120.0N11—C16—C15120.6 (2)
C12—N12—H12A120.0C15—C16—H16119.7
C12—N12—H12B120.0C13—C17—H17A109.5
C22—C23—C27119.36 (19)C13—C17—H17B109.5
C24—C23—C22117.78 (19)C13—C17—H17C109.5
C24—C23—C27122.8 (2)H17A—C17—H17B109.5
N21—C26—H26119.9H17A—C17—H17C109.5
C25—C26—N21120.16 (19)H17B—C17—H17C109.5
C25—C26—H26119.9C16—C15—H15121.1
N21—C22—C23118.45 (17)C16—C15—C14117.7 (2)
N22—C22—N21117.90 (18)C14—C15—H15121.1
N22—C22—C23123.64 (17)C13—C14—C15123.0 (2)
C12—C13—C17119.2 (2)C13—C14—H14118.5
C14—C13—C12117.3 (2)C15—C14—H14118.5
C14—C13—C17123.5 (2)
N21—C26—C25—C240.2 (3)C27—C23—C22—N21177.27 (18)
N11—C16—C15—C142.0 (4)C27—C23—C22—N221.6 (3)
C26—N21—C22—N22178.88 (17)C27—C23—C24—C25176.6 (2)
C26—N21—C22—C230.1 (3)C16—N11—C12—N12177.62 (19)
C26—C25—C24—C231.1 (3)C16—N11—C12—C132.3 (3)
C22—N21—C26—C250.4 (3)C16—C15—C14—C131.6 (4)
C22—C23—C24—C251.4 (3)C17—C13—C12—N11177.54 (18)
C12—N11—C16—C150.1 (3)C17—C13—C12—N122.5 (3)
C12—C13—C14—C150.8 (3)C17—C13—C14—C15179.4 (2)
C24—C23—C22—N210.8 (3)C14—C13—C12—N112.7 (3)
C24—C23—C22—N22179.67 (18)C14—C13—C12—N12177.26 (19)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N21—H21···O10.861.822.677 (2)172
N11—H11···O40.861.872.727 (3)173
N22—H22A···O20.862.052.897 (3)168
N22—H22B···O2i0.862.072.812 (2)145
N12—H12A···O10.862.092.881 (2)152
N12—H12B···O1Wii0.862.062.890 (3)162
C26—H26···O1iii0.932.573.127 (3)119
O1W—H1WA···O40.78 (3)2.07 (3)2.824 (3)161 (3)
O1W—H1WB···O3iv0.82 (3)2.04 (3)2.847 (3)169 (3)
Symmetry codes: (i) x+2, y+1, z+1; (ii) x+1, y+1/2, z+1/2; (iii) x+1, y+1, z+1; (iv) x, y+1/2, z1/2.
 

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