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Two mol­ecular precursors to dendrimeric materials that could serve as slow and sustained NO-releasing therapeutic agents have been synthesized and characterized. N1,N4-Bis(2-nitro­phen­yl)butane-1,4-di­amine, C16H18N4O4, (I), crystallizes in a lattice with equal populations of two mol­ecules of different conformations, both of which possess inversion symmetry through the central C—C bond. One mol­ecule has exclusively anti conformations along the butyl chain, while the other has a gauche conformation of the substituents on the first C—C bond. N2,N2-Bis­[2-(2-nitroanilino)­eth­yl]-N1-(2-nitro­phen­yl)ethane-1,2-di­amine, C24H27N7O6, (II), crystallizes with one unique mol­ecule in the asymmetric unit. Neighboring pairs of mol­ecules are linked into dimers via N—H...O amine–nitro hydrogen bonds. The dimers are assembled into layers that stack in an ABAB sequence such that the repeat distance in the stacking direction is over 46 Å. Mol­ecular NO-release agents N1,N4-bis­(2-nitro­phen­yl)-N1,N4-di­nitroso­butane-1,4-di­amine, C16H16N6O6, (III), and N1-(2-nitro­phen­yl)-N2,N2-bis­{2-[(2-nitro­phen­yl)(nitroso)amino]­eth­yl}-N1-nitroso­ethane-1,2-di­amine, C24H24N10O9, (IV), were prepared via treatment of (I) and (II), respectively, with NaNO2 and acetic acid. The release of NO from solid-phase samples of (III) and (IV) suspended in phosphate buffer was monitored spectroscopically over a period of 21 days. Although (IV) released a greater amount of NO, as expected due to it having three NO moieties for every two in (III), the (IV):(III) ratio of the rate and extent of NO release was significantly less than 1.5:1, suggesting that some combination of electronic, chemical, and/or steric factors may be affecting the release process.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229618011737/ly3073sup1.cif
Contains datablocks C16H18N4O4, C24H27N7O6, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229618011737/ly3073C16H18N4O4sup2.hkl
Contains datablock C16H18N4O4

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229618011737/ly3073C24H27N7O6sup3.hkl
Contains datablock C24H27N7O6

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2053229618011737/ly3073C16H18N4O4sup4.cml
Supplementary material

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2053229618011737/ly3073C24H27N7O6sup5.cml
Supplementary material

CCDC references: 1862846; 1862845

Computing details top

For both structures, data collection: APEX3 (Bruker, 2015); cell refinement: SAINT (Bruker, 2015); data reduction: SAINT (Bruker, 2015); program(s) used to solve structure: SHELXS97 (Sheldrick 2008); program(s) used to refine structure: SHELXL2016 (Sheldrick, 2015); molecular graphics: CrystalMaker (Palmer, 2014); software used to prepare material for publication: SHELXL2016 (Sheldrick, 2015).

N1,N4-Bis(2-nitrophenyl)butane-1,4-diamine (C16H18N4O4) top
Crystal data top
C16H18N4O4F(000) = 348
Mr = 330.34Dx = 1.466 Mg m3
Triclinic, P1Melting point: 426 K
a = 6.7032 (4) ÅCu Kα radiation, λ = 1.54178 Å
b = 8.1646 (5) ÅCell parameters from 8641 reflections
c = 15.1177 (9) Åθ = 3.0–69.8°
α = 81.099 (2)°µ = 0.90 mm1
β = 79.555 (2)°T = 120 K
γ = 67.488 (2)°Plate, orange
V = 748.34 (8) Å30.08 × 0.07 × 0.03 mm
Z = 2
Data collection top
Bruker APEXII CCD
diffractometer
2595 independent reflections
Radiation source: ImuS2314 reflections with I > 2σ(I)
Multi-layer optics monochromatorRint = 0.027
φ and ω scansθmax = 69.9°, θmin = 3.0°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 78
Tmin = 0.689, Tmax = 0.753k = 99
2595 measured reflectionsl = 018
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)] = 0.043Hydrogen site location: mixed
wR(F2) = 0.138H atoms treated by a mixture of independent and constrained refinement
S = 1.10 w = 1/[σ2(Fo2) + (0.0905P)2 + 0.1858P]
where P = (Fo2 + 2Fc2)/3
2595 reflections(Δ/σ)max < 0.001
226 parametersΔρmax = 0.25 e Å3
0 restraintsΔρmin = 0.34 e Å3
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. Refined as a 2-component twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.3995 (2)0.39294 (16)0.06812 (8)0.0234 (3)
O20.4336 (2)0.18683 (17)0.17903 (9)0.0328 (4)
N10.2731 (2)0.72853 (19)0.09832 (10)0.0184 (3)
N20.3819 (2)0.34646 (18)0.15066 (10)0.0193 (3)
C10.2477 (3)0.9133 (2)0.06805 (11)0.0197 (4)
H1A0.3580570.9155740.0150710.024*
H1B0.2757800.9665500.1168220.024*
C20.0214 (3)1.0264 (2)0.04247 (11)0.0189 (4)
H2A0.0898101.0142680.0932210.023*
H2B0.0063001.1531390.0328340.023*
C30.2460 (3)0.6631 (2)0.18512 (11)0.0170 (4)
C40.3000 (3)0.4780 (2)0.21374 (11)0.0175 (4)
C50.2769 (3)0.4156 (2)0.30547 (12)0.0200 (4)
H50.3154190.2913920.3221890.024*
C60.1996 (3)0.5310 (2)0.37113 (11)0.0212 (4)
H60.1853220.4879010.4331170.025*
C70.1418 (3)0.7143 (2)0.34535 (11)0.0204 (4)
H70.0880220.7954810.3904720.025*
C80.1618 (3)0.7780 (2)0.25606 (11)0.0192 (4)
H80.1179800.9029400.2409220.023*
H1N0.335 (4)0.649 (3)0.0588 (15)0.031 (6)*
O110.7626 (2)0.35662 (16)0.43988 (8)0.0264 (3)
O120.9038 (3)0.15051 (17)0.34842 (9)0.0364 (4)
N110.6419 (2)0.69358 (19)0.37783 (10)0.0191 (3)
N120.8198 (2)0.30994 (19)0.36156 (10)0.0213 (3)
C110.5565 (3)0.8826 (2)0.39118 (11)0.0202 (4)
H11A0.4070600.9395070.3746950.024*
H11B0.6493390.9418330.3520110.024*
C120.5537 (3)0.9028 (2)0.48948 (11)0.0208 (4)
H12A0.7051340.8545870.5038700.025*
H12B0.4736490.8324880.5283060.025*
C130.7037 (3)0.6276 (2)0.29682 (11)0.0172 (4)
C140.7889 (3)0.4419 (2)0.28573 (11)0.0178 (4)
C150.8498 (3)0.3795 (2)0.19956 (12)0.0204 (4)
H150.9050610.2550250.1941990.024*
C160.8301 (3)0.4963 (2)0.12335 (12)0.0214 (4)
H160.8707550.4538650.0651800.026*
C170.7489 (3)0.6794 (2)0.13241 (12)0.0202 (4)
H170.7362160.7610440.0797330.024*
C180.6876 (3)0.7431 (2)0.21577 (11)0.0188 (4)
H180.6328150.8681010.2194050.023*
H11N0.641 (4)0.619 (3)0.4231 (17)0.039 (7)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0346 (7)0.0198 (6)0.0138 (6)0.0083 (5)0.0017 (5)0.0023 (5)
O20.0529 (9)0.0136 (6)0.0270 (7)0.0071 (6)0.0057 (6)0.0007 (5)
N10.0244 (7)0.0135 (7)0.0155 (7)0.0047 (6)0.0036 (6)0.0012 (6)
N20.0248 (7)0.0134 (7)0.0187 (8)0.0056 (6)0.0039 (6)0.0005 (6)
C10.0263 (9)0.0148 (8)0.0184 (8)0.0079 (7)0.0041 (7)0.0000 (6)
C20.0251 (9)0.0133 (8)0.0161 (8)0.0052 (7)0.0024 (6)0.0001 (6)
C30.0175 (8)0.0164 (8)0.0168 (8)0.0048 (7)0.0051 (6)0.0009 (6)
C40.0193 (8)0.0167 (8)0.0161 (9)0.0051 (7)0.0030 (6)0.0035 (7)
C50.0238 (8)0.0169 (8)0.0190 (9)0.0069 (7)0.0055 (7)0.0011 (7)
C60.0251 (9)0.0243 (9)0.0146 (8)0.0093 (7)0.0047 (7)0.0003 (7)
C70.0210 (8)0.0214 (9)0.0190 (9)0.0064 (7)0.0025 (6)0.0059 (7)
C80.0210 (8)0.0162 (8)0.0198 (9)0.0050 (7)0.0027 (7)0.0045 (7)
O110.0447 (8)0.0199 (6)0.0150 (6)0.0119 (6)0.0040 (5)0.0026 (5)
O120.0613 (10)0.0126 (6)0.0270 (8)0.0057 (6)0.0022 (7)0.0024 (5)
N110.0270 (8)0.0153 (7)0.0148 (7)0.0074 (6)0.0017 (6)0.0030 (6)
N120.0299 (8)0.0147 (7)0.0189 (8)0.0075 (6)0.0027 (6)0.0029 (6)
C110.0264 (9)0.0152 (8)0.0190 (9)0.0066 (7)0.0024 (7)0.0042 (7)
C120.0278 (9)0.0161 (9)0.0182 (9)0.0077 (7)0.0005 (7)0.0043 (7)
C130.0170 (8)0.0173 (8)0.0177 (8)0.0060 (7)0.0018 (6)0.0037 (7)
C140.0212 (8)0.0160 (8)0.0165 (9)0.0067 (7)0.0030 (6)0.0019 (7)
C150.0227 (8)0.0178 (8)0.0206 (9)0.0065 (7)0.0008 (7)0.0067 (7)
C160.0227 (8)0.0253 (9)0.0173 (9)0.0087 (7)0.0022 (7)0.0057 (7)
C170.0204 (8)0.0234 (9)0.0175 (9)0.0090 (7)0.0034 (6)0.0002 (7)
C180.0216 (8)0.0153 (8)0.0197 (9)0.0065 (7)0.0041 (6)0.0015 (7)
Geometric parameters (Å, º) top
O1—N21.2448 (18)O11—N121.2480 (19)
O2—N21.2400 (19)O12—N121.2365 (19)
N1—C31.346 (2)N11—C131.346 (2)
N1—C11.460 (2)N11—C111.459 (2)
N1—H1N0.88 (2)N11—H11N0.84 (2)
N2—C41.428 (2)N12—C141.432 (2)
C1—C21.527 (2)C11—C121.516 (2)
C1—H1A0.9900C11—H11A0.9900
C1—H1B0.9900C11—H11B0.9900
C2—C2i1.523 (3)C12—C12ii1.528 (3)
C2—H2A0.9900C12—H12A0.9900
C2—H2B0.9900C12—H12B0.9900
C3—C81.426 (2)C13—C181.420 (2)
C3—C41.428 (2)C13—C141.426 (2)
C4—C51.404 (2)C14—C151.406 (2)
C5—C61.368 (2)C15—C161.369 (2)
C5—H50.9500C15—H150.9500
C6—C71.404 (2)C16—C171.401 (2)
C6—H60.9500C16—H160.9500
C7—C81.371 (2)C17—C181.371 (2)
C7—H70.9500C17—H170.9500
C8—H80.9500C18—H180.9500
C3—N1—C1124.99 (14)C13—N11—C11124.79 (15)
C3—N1—H1N115.9 (14)C13—N11—H11N115.9 (17)
C1—N1—H1N118.0 (14)C11—N11—H11N119.0 (17)
O2—N2—O1120.78 (14)O12—N12—O11120.77 (14)
O2—N2—C4119.36 (14)O12—N12—C14119.34 (14)
O1—N2—C4119.86 (14)O11—N12—C14119.88 (14)
N1—C1—C2113.07 (14)N11—C11—C12109.10 (14)
N1—C1—H1A109.0N11—C11—H11A109.9
C2—C1—H1A109.0C12—C11—H11A109.9
N1—C1—H1B109.0N11—C11—H11B109.9
C2—C1—H1B109.0C12—C11—H11B109.9
H1A—C1—H1B107.8H11A—C11—H11B108.3
C2i—C2—C1112.72 (17)C11—C12—C12ii112.04 (18)
C2i—C2—H2A109.0C11—C12—H12A109.2
C1—C2—H2A109.0C12ii—C12—H12A109.2
C2i—C2—H2B109.0C11—C12—H12B109.2
C1—C2—H2B109.0C12ii—C12—H12B109.2
H2A—C2—H2B107.8H12A—C12—H12B107.9
N1—C3—C8121.09 (15)N11—C13—C18120.68 (15)
N1—C3—C4123.83 (15)N11—C13—C14123.62 (15)
C8—C3—C4115.07 (15)C18—C13—C14115.70 (15)
C5—C4—C3121.72 (15)C15—C14—C13121.51 (16)
C5—C4—N2116.48 (15)C15—C14—N12116.71 (15)
C3—C4—N2121.80 (15)C13—C14—N12121.77 (15)
C6—C5—C4120.95 (16)C16—C15—C14120.61 (16)
C6—C5—H5119.5C16—C15—H15119.7
C4—C5—H5119.5C14—C15—H15119.7
C5—C6—C7118.87 (16)C15—C16—C17118.99 (15)
C5—C6—H6120.6C15—C16—H16120.5
C7—C6—H6120.6C17—C16—H16120.5
C8—C7—C6121.04 (16)C18—C17—C16121.31 (16)
C8—C7—H7119.5C18—C17—H17119.3
C6—C7—H7119.5C16—C17—H17119.3
C7—C8—C3122.31 (16)C17—C18—C13121.87 (16)
C7—C8—H8118.8C17—C18—H18119.1
C3—C8—H8118.8C13—C18—H18119.1
C4—C3—N1—C1171.20 (15)C3—N1—C1—C295.43 (19)
C14—C13—N11—C11179.27 (15)C13—N11—C11—C12167.33 (15)
C8—C3—N1—C18.0 (2)N1—C1—C2—C2i68.4 (2)
C18—C13—N11—C110.4 (2)N11—C11—C12—C12ii174.65 (17)
Symmetry codes: (i) x, y+2, z; (ii) x+1, y+2, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1N···O10.88 (2)1.95 (2)2.6273 (18)132.2 (19)
N1—H1N···O1iii0.88 (2)2.34 (2)3.0388 (19)136.8 (19)
C8—H8···O12iv0.952.603.256 (2)127
N11—H11N···O110.84 (2)1.97 (2)2.6221 (19)133 (2)
C12—H12B···O11v0.992.553.470 (2)155
C18—H18···O2vi0.952.463.366 (2)159
Symmetry codes: (iii) x+1, y+1, z; (iv) x1, y+1, z; (v) x+1, y+1, z+1; (vi) x, y+1, z.
N1-(2-Nitrophenyl)-N2,N2-bis[2-[(2-nitroanilino)ethyl]ethane-1,2-diamine (C24H27N7O6) top
Crystal data top
C24H27N7O6Dx = 1.436 Mg m3
Mr = 509.52Melting point: 376 K
Orthorhombic, PbcaCu Kα radiation, λ = 1.54178 Å
a = 7.5749 (2) ÅCell parameters from 9785 reflections
b = 13.4138 (4) Åθ = 3.8–70.0°
c = 46.3793 (14) ŵ = 0.89 mm1
V = 4712.5 (2) Å3T = 120 K
Z = 8Triangular prism, yellow
F(000) = 21440.21 × 0.13 × 0.06 mm
Data collection top
Bruker APEXII CCD
diffractometer
4413 independent reflections
Radiation source: ImuS4182 reflections with I > 2σ(I)
Multi-layer optics monochromatorRint = 0.026
φ and ω scansθmax = 70.0°, θmin = 1.9°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 98
Tmin = 0.655, Tmax = 0.753k = 1616
50384 measured reflectionsl = 5556
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)] = 0.031Hydrogen site location: difference Fourier map
wR(F2) = 0.079All H-atom parameters refined
S = 1.06 w = 1/[σ2(Fo2) + (0.0343P)2 + 2.0708P]
where P = (Fo2 + 2Fc2)/3
4413 reflections(Δ/σ)max = 0.001
442 parametersΔρmax = 0.22 e Å3
0 restraintsΔρmin = 0.24 e Å3
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.10378 (12)1.08863 (7)0.01246 (2)0.0308 (2)
O20.30627 (13)1.14180 (7)0.04137 (2)0.0323 (2)
O30.78758 (13)0.54020 (7)0.12028 (2)0.0343 (2)
O40.84429 (12)0.46457 (6)0.16032 (2)0.0306 (2)
O50.29091 (12)1.04871 (6)0.14961 (2)0.0296 (2)
O60.39256 (12)1.11208 (7)0.18916 (2)0.0375 (2)
N10.18245 (12)0.84159 (7)0.09745 (2)0.0173 (2)
N20.17842 (14)1.04263 (7)0.04110 (2)0.0236 (2)
N30.25888 (14)1.11500 (7)0.01723 (2)0.0230 (2)
N40.58206 (13)0.69789 (8)0.11960 (2)0.0216 (2)
N50.77672 (13)0.53401 (7)0.14699 (2)0.0242 (2)
N60.06877 (13)0.89790 (7)0.15092 (2)0.0188 (2)
N70.30044 (13)1.05048 (7)0.17636 (2)0.0253 (2)
C10.20183 (16)0.88416 (8)0.06863 (2)0.0199 (2)
C20.13671 (18)0.99193 (9)0.06804 (3)0.0255 (3)
C30.34148 (16)1.07529 (8)0.03378 (2)0.0203 (2)
C40.38489 (16)1.11365 (8)0.00601 (2)0.0206 (2)
C50.55501 (17)1.14786 (9)0.00052 (3)0.0258 (3)
C60.68709 (18)1.14413 (9)0.01954 (3)0.0308 (3)
C70.64809 (18)1.10657 (9)0.04694 (3)0.0300 (3)
C80.48243 (17)1.07365 (9)0.05396 (3)0.0254 (3)
C90.29142 (15)0.75279 (8)0.10129 (2)0.0194 (2)
C100.48761 (16)0.77778 (9)0.10495 (2)0.0225 (2)
C110.58330 (14)0.68520 (8)0.14861 (2)0.0179 (2)
C120.68072 (14)0.60927 (8)0.16288 (2)0.0194 (2)
C130.68717 (16)0.60277 (9)0.19294 (3)0.0232 (3)
C140.59608 (17)0.66913 (9)0.20977 (3)0.0253 (3)
C150.49346 (16)0.74231 (9)0.19626 (3)0.0238 (2)
C160.48690 (15)0.75010 (8)0.16682 (2)0.0204 (2)
C170.00235 (15)0.82235 (9)0.10512 (2)0.0196 (2)
C180.02435 (16)0.81483 (8)0.13772 (2)0.0198 (2)
C190.08961 (14)0.90749 (8)0.17968 (2)0.0180 (2)
C200.20124 (15)0.97899 (8)0.19303 (3)0.0214 (2)
C210.21675 (17)0.98492 (10)0.22306 (3)0.0291 (3)
C220.12409 (18)0.92142 (11)0.24059 (3)0.0322 (3)
C230.01299 (17)0.85070 (10)0.22796 (3)0.0274 (3)
C240.00427 (15)0.84361 (9)0.19865 (2)0.0214 (2)
H2N0.103 (2)1.0378 (12)0.0267 (3)0.036 (4)*
H4N0.648 (2)0.6565 (12)0.1101 (3)0.031 (4)*
H6N0.139 (2)0.9301 (11)0.1401 (3)0.025 (4)*
H1A0.1409 (18)0.8448 (10)0.0537 (3)0.025 (3)*
H1B0.3274 (18)0.8833 (9)0.0637 (3)0.017 (3)*
H2A0.005 (2)0.9948 (11)0.0697 (3)0.032 (4)*
H2B0.1903 (19)1.0281 (11)0.0848 (3)0.028 (4)*
H50.572 (2)1.1733 (11)0.0196 (3)0.030 (4)*
H60.804 (2)1.1655 (12)0.0147 (3)0.037 (4)*
H70.740 (2)1.1021 (11)0.0615 (3)0.034 (4)*
H80.461 (2)1.0464 (11)0.0726 (3)0.031 (4)*
H9A0.2767 (18)0.7064 (10)0.0854 (3)0.025 (3)*
H9B0.2520 (17)0.7198 (9)0.1188 (3)0.017 (3)*
H10A0.5474 (18)0.7857 (10)0.0861 (3)0.024 (3)*
H10B0.5010 (18)0.8401 (11)0.1163 (3)0.026 (4)*
H130.758 (2)0.5507 (11)0.2014 (3)0.032 (4)*
H140.600 (2)0.6643 (11)0.2305 (3)0.033 (4)*
H150.4245 (19)0.7886 (11)0.2077 (3)0.027 (4)*
H160.4179 (19)0.7999 (11)0.1586 (3)0.025 (3)*
H17A0.0486 (18)0.7592 (10)0.0961 (3)0.022 (3)*
H17B0.0755 (18)0.8780 (10)0.0982 (3)0.020 (3)*
H18A0.0214 (18)0.7488 (10)0.1453 (3)0.022 (3)*
H18B0.1512 (18)0.8185 (10)0.1423 (3)0.021 (3)*
H210.293 (2)1.0352 (12)0.2308 (3)0.040 (4)*
H220.134 (2)0.9250 (13)0.2619 (4)0.046 (5)*
H230.054 (2)0.8052 (11)0.2402 (3)0.031 (4)*
H240.0815 (19)0.7948 (11)0.1908 (3)0.023 (3)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0283 (5)0.0345 (5)0.0297 (5)0.0039 (4)0.0047 (4)0.0102 (4)
O20.0478 (6)0.0311 (5)0.0180 (4)0.0027 (4)0.0064 (4)0.0050 (3)
O30.0355 (5)0.0365 (5)0.0308 (5)0.0114 (4)0.0050 (4)0.0041 (4)
O40.0252 (5)0.0192 (4)0.0475 (5)0.0049 (4)0.0046 (4)0.0028 (4)
O50.0262 (5)0.0261 (4)0.0365 (5)0.0055 (4)0.0007 (4)0.0064 (4)
O60.0272 (5)0.0276 (5)0.0577 (6)0.0077 (4)0.0061 (4)0.0115 (4)
N10.0196 (5)0.0178 (4)0.0147 (4)0.0002 (4)0.0014 (3)0.0024 (3)
N20.0258 (5)0.0236 (5)0.0214 (5)0.0018 (4)0.0019 (4)0.0073 (4)
N30.0326 (6)0.0171 (5)0.0194 (5)0.0022 (4)0.0022 (4)0.0020 (4)
N40.0201 (5)0.0245 (5)0.0201 (5)0.0025 (4)0.0011 (4)0.0015 (4)
N50.0184 (5)0.0209 (5)0.0332 (6)0.0010 (4)0.0006 (4)0.0006 (4)
N60.0197 (5)0.0191 (5)0.0178 (5)0.0046 (4)0.0030 (4)0.0001 (4)
N70.0173 (5)0.0191 (5)0.0395 (6)0.0006 (4)0.0029 (4)0.0036 (4)
C10.0249 (6)0.0199 (6)0.0149 (5)0.0019 (5)0.0022 (4)0.0012 (4)
C20.0326 (7)0.0214 (6)0.0225 (6)0.0047 (5)0.0080 (5)0.0054 (5)
C30.0260 (6)0.0135 (5)0.0214 (5)0.0041 (4)0.0020 (5)0.0008 (4)
C40.0263 (6)0.0153 (5)0.0201 (5)0.0014 (4)0.0025 (5)0.0016 (4)
C50.0312 (7)0.0179 (6)0.0283 (6)0.0006 (5)0.0099 (5)0.0039 (5)
C60.0251 (6)0.0221 (6)0.0451 (8)0.0017 (5)0.0056 (6)0.0095 (5)
C70.0296 (7)0.0231 (6)0.0372 (7)0.0047 (5)0.0082 (6)0.0098 (5)
C80.0329 (7)0.0204 (6)0.0229 (6)0.0051 (5)0.0027 (5)0.0029 (5)
C90.0222 (6)0.0170 (5)0.0189 (5)0.0012 (4)0.0015 (4)0.0013 (4)
C100.0221 (6)0.0247 (6)0.0208 (6)0.0024 (5)0.0001 (5)0.0061 (5)
C110.0136 (5)0.0176 (5)0.0226 (5)0.0041 (4)0.0006 (4)0.0013 (4)
C120.0151 (5)0.0172 (5)0.0260 (6)0.0015 (4)0.0000 (4)0.0005 (4)
C130.0208 (6)0.0205 (6)0.0281 (6)0.0033 (5)0.0037 (5)0.0062 (5)
C140.0277 (6)0.0279 (6)0.0201 (6)0.0047 (5)0.0020 (5)0.0023 (5)
C150.0226 (6)0.0240 (6)0.0248 (6)0.0012 (5)0.0010 (5)0.0043 (5)
C160.0185 (5)0.0175 (5)0.0252 (6)0.0004 (4)0.0022 (4)0.0007 (4)
C170.0192 (6)0.0211 (6)0.0184 (5)0.0022 (5)0.0008 (4)0.0008 (4)
C180.0208 (6)0.0199 (6)0.0188 (5)0.0040 (5)0.0018 (4)0.0006 (4)
C190.0156 (5)0.0183 (5)0.0200 (5)0.0046 (4)0.0008 (4)0.0009 (4)
C200.0166 (5)0.0195 (5)0.0281 (6)0.0042 (4)0.0012 (4)0.0031 (4)
C210.0240 (6)0.0323 (7)0.0310 (7)0.0065 (5)0.0076 (5)0.0109 (5)
C220.0327 (7)0.0442 (8)0.0198 (6)0.0097 (6)0.0039 (5)0.0051 (5)
C230.0285 (7)0.0331 (7)0.0206 (6)0.0071 (5)0.0034 (5)0.0029 (5)
C240.0212 (6)0.0225 (6)0.0205 (5)0.0017 (5)0.0021 (4)0.0000 (4)
Geometric parameters (Å, º) top
O1—N31.2467 (14)C7—C81.3695 (19)
O2—N31.2294 (13)C7—H70.970 (16)
O3—N51.2444 (13)C8—H80.953 (15)
O4—N51.2296 (13)C9—C101.5328 (16)
O5—N71.2432 (14)C9—H9A0.972 (14)
O6—N71.2337 (14)C9—H9B0.973 (13)
N1—C91.4602 (14)C10—H10A0.993 (14)
N1—C11.4608 (13)C10—H10B0.993 (14)
N1—C171.4672 (14)C11—C161.4157 (16)
N2—C31.3539 (16)C11—C121.4212 (16)
N2—C21.4571 (14)C12—C131.3978 (16)
N2—H2N0.884 (17)C13—C141.3702 (18)
N3—C41.4400 (15)C13—H130.963 (16)
N4—C111.3563 (14)C14—C151.4000 (17)
N4—C101.4566 (15)C14—H140.962 (15)
N4—H4N0.868 (16)C15—C161.3703 (16)
N5—C121.4460 (15)C15—H150.970 (15)
N6—C191.3493 (14)C16—H160.930 (15)
N6—C181.4539 (14)C17—C181.5245 (15)
N6—H6N0.849 (15)C17—H17A1.008 (14)
N7—C201.4427 (16)C17—H17B0.982 (14)
C1—C21.5276 (16)C18—H18A1.014 (14)
C1—H1A0.987 (14)C18—H18B0.985 (14)
C1—H1B0.978 (13)C19—C241.4192 (16)
C2—H2A0.999 (16)C19—C201.4206 (16)
C2—H2B1.004 (15)C20—C211.4002 (17)
C3—C81.4200 (17)C21—C221.371 (2)
C3—C41.4253 (16)C21—H210.956 (17)
C4—C51.4011 (17)C22—C231.397 (2)
C5—C61.367 (2)C22—H220.994 (17)
C5—H50.958 (15)C23—C241.3690 (16)
C6—C71.399 (2)C23—H230.977 (15)
C6—H60.955 (17)C24—H240.950 (15)
C9—N1—C1111.96 (9)H9A—C9—H9B107.9 (11)
C9—N1—C17111.48 (9)N4—C10—C9111.53 (9)
C1—N1—C17112.73 (9)N4—C10—H10A105.4 (8)
C3—N2—C2124.33 (11)C9—C10—H10A111.6 (8)
C3—N2—H2N115.2 (10)N4—C10—H10B108.8 (8)
C2—N2—H2N118.3 (10)C9—C10—H10B110.0 (8)
O2—N3—O1121.32 (10)H10A—C10—H10B109.3 (11)
O2—N3—C4119.46 (10)N4—C11—C16120.73 (10)
O1—N3—C4119.22 (9)N4—C11—C12123.74 (10)
C11—N4—C10123.95 (10)C16—C11—C12115.52 (10)
C11—N4—H4N114.8 (10)C13—C12—C11121.82 (11)
C10—N4—H4N121.1 (10)C13—C12—N5116.56 (10)
O4—N5—O3121.58 (10)C11—C12—N5121.62 (10)
O4—N5—C12118.82 (10)C14—C13—C12120.66 (11)
O3—N5—C12119.60 (10)C14—C13—H13121.2 (9)
C19—N6—C18123.09 (9)C12—C13—H13118.1 (9)
C19—N6—H6N117.6 (10)C13—C14—C15118.71 (11)
C18—N6—H6N116.4 (10)C13—C14—H14120.5 (9)
O6—N7—O5121.72 (11)C15—C14—H14120.7 (9)
O6—N7—C20118.82 (11)C16—C15—C14121.29 (11)
O5—N7—C20119.46 (9)C16—C15—H15118.6 (8)
N1—C1—C2110.72 (9)C14—C15—H15120.1 (8)
N1—C1—H1A112.8 (8)C15—C16—C11121.92 (11)
C2—C1—H1A110.0 (8)C15—C16—H16118.9 (9)
N1—C1—H1B107.9 (7)C11—C16—H16119.1 (9)
C2—C1—H1B108.7 (8)N1—C17—C18110.88 (9)
H1A—C1—H1B106.5 (11)N1—C17—H17A112.3 (8)
N2—C2—C1112.77 (10)C18—C17—H17A108.6 (7)
N2—C2—H2A105.3 (8)N1—C17—H17B109.0 (8)
C1—C2—H2A110.9 (9)C18—C17—H17B108.1 (7)
N2—C2—H2B110.6 (8)H17A—C17—H17B107.9 (10)
C1—C2—H2B108.2 (8)N6—C18—C17108.29 (9)
H2A—C2—H2B108.9 (12)N6—C18—H18A110.9 (8)
N2—C3—C8121.04 (11)C17—C18—H18A111.4 (7)
N2—C3—C4123.65 (11)N6—C18—H18B110.1 (8)
C8—C3—C4115.31 (11)C17—C18—H18B108.5 (8)
C5—C4—C3121.73 (11)H18A—C18—H18B107.6 (11)
C5—C4—N3116.34 (10)N6—C19—C24119.78 (10)
C3—C4—N3121.87 (10)N6—C19—C20124.39 (10)
C6—C5—C4120.92 (12)C24—C19—C20115.83 (10)
C6—C5—H5122.9 (9)C21—C20—C19121.46 (11)
C4—C5—H5116.2 (9)C21—C20—N7116.84 (11)
C5—C6—C7118.49 (12)C19—C20—N7121.69 (10)
C5—C6—H6120.5 (9)C22—C21—C20120.79 (12)
C7—C6—H6121.0 (9)C22—C21—H21121.6 (9)
C8—C7—C6121.70 (12)C20—C21—H21117.6 (9)
C8—C7—H7118.1 (9)C21—C22—C23118.79 (12)
C6—C7—H7120.2 (9)C21—C22—H22121.4 (10)
C7—C8—C3121.84 (12)C23—C22—H22119.8 (10)
C7—C8—H8119.7 (9)C24—C23—C22121.41 (12)
C3—C8—H8118.5 (9)C24—C23—H23118.8 (9)
N1—C9—C10112.53 (9)C22—C23—H23119.8 (9)
N1—C9—H9A111.4 (8)C23—C24—C19121.72 (11)
C10—C9—H9A109.6 (8)C23—C24—H24119.1 (8)
N1—C9—H9B107.5 (8)C19—C24—H24119.2 (8)
C10—C9—H9B107.7 (8)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2N···O10.884 (17)1.939 (16)2.6214 (13)132.9 (14)
N2—H2N···O1i0.884 (17)2.399 (16)3.0715 (14)133.1 (13)
N4—H4N···O30.868 (16)1.942 (16)2.6265 (13)134.7 (13)
N6—H6N···O50.849 (15)2.013 (15)2.6320 (13)129.1 (12)
C10—H10A···O2ii0.993 (14)2.543 (14)3.5068 (14)163.6 (11)
C18—H18B···O4iii0.985 (14)2.584 (14)3.3177 (15)131.3 (10)
Symmetry codes: (i) x, y+2, z; (ii) x+1, y+2, z; (iii) x+1/2, y+1/2, z.
 

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