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The structures of the cocrystalline adducts of 3-nitro­phenol (3-NP) with 1,3,5,7-tetra­aza­tri­cyclo­[3.3.1.13,7]decane [HMTA, (1)] as the 2:1:1 hydrate, 2C6H5NO3·C6H12N4·H2O, (1a), with 1,3,6,8-tetra­aza­tri­cyclo­[4.3.1.13,8]undecane [TATU (2)] as the 2:1 cocrystal, 2C6H5NO3·C7H14N4, (2a), and with 1,3,6,8-tetra­aza­tri­cyclo­[4.4.1.13,8]dodecane [TATD, (3)] as the 2:1 cocrystal, 2C6H5NO3·C8H16N4, (3a), are reported. In the binary crystals (2a) and (3a), the 3-nitro­phenol mol­ecules are linked via O—H...N hydrogen bonds into aminal cage aza­adamantanes. In (1a), the structure is stabilized by O—H...N and O—H...O hydrogen bonds, and generates ternary cocrystals. There are C—H...O hydrogen bonds present in all three cocrystals, and in (1a), there are also C—H...O and C—H...π inter­actions present. The presence of an ethyl­ene bridge in the structures of (2) and (3) defines the formation of a hydrogen-bonded motif in the supra­molecular architectures of (2a) and (3a). The differences in the C—N bond lengths of the aminal cage structures, as a result of hyperconjugative inter­actions and electron delocalization, were analysed. These three cocrystals were obtained by the solvent-free assisted grinding method. Crystals suitable for single-crystal X-ray diffraction were grown by slow evaporation from a mixture of hexa­nes.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S205322961901516X/sk3740sup1.cif
Contains datablocks 1a, 2a, 3a, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205322961901516X/sk37401asup2.hkl
Contains datablock 1a

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205322961901516X/sk37402asup3.hkl
Contains datablock 2a

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205322961901516X/sk37403asup4.hkl
Contains datablock 3a

CCDC references: 1868031; 1964999; 1964998

Computing details top

For all structures, data collection: X-AREA (Stoe & Cie, 2001); cell refinement: X-AREA (Stoe & Cie, 2001); data reduction: X-AREA (Stoe & Cie, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008). Program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015) for (1a), (2a); SHELXL2014 (Sheldrick, 2015) for (3a). For all structures, molecular graphics: XP in SHELXTL-Plus (Sheldrick, 2008). Software used to prepare material for publication: SHELXL for (1a), (3a); SHELXL2018 (Sheldrick, 2015) for (2a).

3-Nitrophenol–1,3,5,7-tetraazatricyclo[3.3.1.13,7]decane–water (2:1:1) (1a) top
Crystal data top
2C6H5NO3·C6H12N4·H2OF(000) = 920
Mr = 436.43Dx = 1.427 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 10.6765 (6) ÅCell parameters from 8615 reflections
b = 28.819 (3) Åθ = 2.4–25.5°
c = 6.8163 (4) ŵ = 0.11 mm1
β = 104.395 (5)°T = 173 K
V = 2031.5 (2) Å3Block, colourless
Z = 40.26 × 0.25 × 0.23 mm
Data collection top
Stoe IPDS II two-circle
diffractometer
3024 reflections with I > 2σ(I)
Radiation source: Genix 3D IµS microfocus X-ray sourceRint = 0.030
ω scansθmax = 25.0°, θmin = 2.4°
Absorption correction: multi-scan
(X-AREA; Stoe & Cie, 2001)
h = 1212
Tmin = 0.678, Tmax = 1.000k = 3234
8615 measured reflectionsl = 88
3559 independent reflections
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.057 w = 1/[σ2(Fo2) + (0.0402P)2 + 1.5429P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.136(Δ/σ)max < 0.001
S = 1.24Δρmax = 0.19 e Å3
3559 reflectionsΔρmin = 0.19 e Å3
297 parametersExtinction correction: SHELXL2018 (Sheldrick, 2015), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0076 (14)
Primary atom site location: structure-invariant direct methods
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
N10.5573 (2)0.67919 (7)0.7511 (4)0.0366 (5)
N20.4781 (2)0.60884 (7)0.5599 (3)0.0327 (5)
N30.33305 (19)0.65519 (7)0.7072 (3)0.0332 (5)
N40.5062 (2)0.61043 (7)0.9282 (3)0.0331 (5)
C10.5915 (3)0.65086 (10)0.9378 (4)0.0401 (7)
H1A0.6819830.6400540.9599150.048*
H1B0.5861000.6704111.0548230.048*
C20.5156 (3)0.58242 (9)0.7514 (4)0.0322 (6)
H2A0.4589360.5549020.7418310.039*
H2B0.6056530.5712910.7710960.039*
C30.3720 (2)0.62791 (9)0.8928 (4)0.0359 (6)
H3A0.3123990.6012650.8845070.043*
H3B0.3647060.6473361.0092250.043*
C40.5646 (3)0.64920 (10)0.5797 (4)0.0382 (7)
H4A0.5412980.6675540.4530180.046*
H4B0.6546350.6382510.5981630.046*
C50.4215 (2)0.69446 (9)0.7219 (5)0.0373 (6)
H5A0.4145520.7143990.8369980.045*
H5B0.3958930.7132330.5966190.045*
C60.3447 (3)0.62584 (10)0.5374 (4)0.0384 (7)
H6A0.3175360.6437700.4100310.046*
H6B0.2856980.5989560.5276550.046*
O10.67092 (17)0.76454 (7)0.7865 (3)0.0385 (5)
H10.651 (3)0.7352 (13)0.787 (5)0.055 (10)*
N111.1070 (2)0.70433 (8)1.0448 (3)0.0353 (5)
O111.0675 (2)0.66478 (7)1.0085 (4)0.0513 (6)
O121.22130 (18)0.71336 (7)1.1252 (4)0.0513 (6)
C110.8000 (2)0.76995 (9)0.8651 (4)0.0285 (5)
C120.8856 (2)0.73314 (8)0.9132 (4)0.0286 (5)
H120.8561140.7019950.8922130.034*
C131.0151 (2)0.74298 (9)0.9928 (4)0.0290 (6)
C141.0635 (2)0.78777 (9)1.0261 (4)0.0338 (6)
H141.1528910.7933881.0821080.041*
C150.9763 (3)0.82382 (9)0.9747 (4)0.0346 (6)
H151.0063190.8549080.9948830.042*
C160.8464 (2)0.81552 (9)0.8945 (4)0.0322 (6)
H160.7881220.8408300.8591550.039*
O20.7877 (2)0.50228 (8)0.3853 (3)0.0440 (5)
H20.716 (4)0.5208 (14)0.345 (6)0.072 (12)*
C210.8154 (2)0.48511 (9)0.2156 (4)0.0318 (6)
N211.0827 (2)0.41888 (8)0.0861 (4)0.0424 (6)
O211.1452 (2)0.40915 (8)0.2579 (4)0.0583 (6)
O221.1177 (2)0.40958 (8)0.0674 (4)0.0554 (6)
C220.9311 (2)0.46097 (9)0.2370 (4)0.0336 (6)
H220.9887550.4566050.3663830.040*
C230.9595 (2)0.44357 (8)0.0639 (4)0.0329 (6)
C240.8798 (3)0.44897 (9)0.1276 (4)0.0354 (6)
H240.9029660.4368650.2433250.043*
C250.7648 (3)0.47265 (9)0.1451 (4)0.0356 (6)
H250.7075990.4768860.2749720.043*
C260.7322 (2)0.49024 (8)0.0246 (4)0.0314 (6)
H260.6522460.5059710.0103500.038*
O1W0.5718 (2)0.55333 (8)0.2806 (3)0.0446 (5)
H1WA0.536 (5)0.5697 (17)0.356 (8)0.104 (17)*
H1WB0.558 (4)0.5722 (16)0.165 (8)0.098 (15)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0253 (11)0.0278 (11)0.0552 (15)0.0004 (9)0.0070 (10)0.0017 (10)
N20.0364 (12)0.0321 (12)0.0299 (12)0.0056 (9)0.0087 (9)0.0007 (9)
N30.0241 (11)0.0283 (11)0.0467 (13)0.0025 (9)0.0075 (9)0.0030 (10)
N40.0338 (12)0.0310 (11)0.0350 (12)0.0066 (9)0.0094 (9)0.0021 (9)
C10.0293 (13)0.0375 (15)0.0474 (17)0.0020 (11)0.0017 (12)0.0074 (13)
C20.0349 (14)0.0260 (13)0.0361 (14)0.0038 (11)0.0095 (11)0.0015 (11)
C30.0336 (14)0.0325 (14)0.0448 (16)0.0028 (11)0.0157 (12)0.0005 (12)
C40.0348 (14)0.0378 (15)0.0471 (17)0.0044 (12)0.0196 (12)0.0100 (13)
C50.0292 (14)0.0248 (13)0.0578 (18)0.0036 (11)0.0107 (12)0.0028 (12)
C60.0310 (14)0.0368 (14)0.0419 (16)0.0005 (11)0.0014 (11)0.0006 (12)
O10.0287 (10)0.0300 (10)0.0527 (12)0.0047 (8)0.0023 (8)0.0034 (9)
N110.0332 (12)0.0336 (12)0.0403 (13)0.0012 (10)0.0117 (10)0.0003 (10)
O110.0469 (12)0.0291 (11)0.0753 (16)0.0001 (9)0.0103 (11)0.0006 (10)
O120.0274 (10)0.0466 (12)0.0761 (16)0.0010 (9)0.0058 (10)0.0008 (11)
C110.0275 (13)0.0297 (13)0.0297 (13)0.0043 (10)0.0097 (10)0.0011 (10)
C120.0333 (13)0.0258 (12)0.0282 (13)0.0069 (10)0.0104 (10)0.0009 (10)
C130.0276 (13)0.0287 (13)0.0322 (14)0.0009 (10)0.0106 (10)0.0005 (10)
C140.0281 (13)0.0341 (14)0.0393 (15)0.0064 (11)0.0088 (11)0.0038 (11)
C150.0381 (15)0.0276 (13)0.0404 (15)0.0078 (11)0.0140 (12)0.0045 (11)
C160.0354 (14)0.0268 (13)0.0366 (15)0.0021 (11)0.0132 (11)0.0007 (11)
O20.0449 (12)0.0533 (13)0.0325 (11)0.0168 (10)0.0074 (9)0.0002 (9)
C210.0325 (13)0.0279 (13)0.0352 (14)0.0011 (11)0.0089 (11)0.0008 (11)
N210.0312 (12)0.0274 (12)0.0700 (18)0.0008 (10)0.0149 (13)0.0004 (12)
O210.0364 (11)0.0552 (14)0.0786 (17)0.0150 (10)0.0055 (11)0.0075 (12)
O220.0455 (12)0.0463 (13)0.0844 (17)0.0045 (10)0.0347 (12)0.0059 (12)
C220.0289 (13)0.0288 (13)0.0407 (15)0.0018 (11)0.0042 (11)0.0039 (11)
C230.0277 (13)0.0214 (12)0.0510 (17)0.0010 (10)0.0124 (11)0.0000 (11)
C240.0377 (14)0.0300 (14)0.0405 (15)0.0017 (11)0.0134 (12)0.0047 (11)
C250.0359 (14)0.0329 (14)0.0364 (15)0.0009 (11)0.0057 (11)0.0006 (11)
C260.0294 (13)0.0261 (13)0.0383 (15)0.0038 (10)0.0074 (11)0.0036 (11)
O1W0.0502 (12)0.0507 (13)0.0350 (11)0.0204 (10)0.0147 (10)0.0040 (10)
Geometric parameters (Å, º) top
N1—C41.471 (4)N11—C131.469 (3)
N1—C11.479 (4)C11—C121.385 (4)
N1—C51.481 (3)C11—C161.400 (4)
N2—C41.470 (3)C12—C131.383 (3)
N2—C21.478 (3)C12—H120.9500
N2—C61.478 (3)C13—C141.388 (4)
N3—C31.459 (3)C14—C151.381 (4)
N3—C51.461 (3)C14—H140.9500
N3—C61.464 (4)C15—C161.379 (4)
N4—C11.470 (4)C15—H150.9500
N4—C21.474 (3)C16—H160.9500
N4—C31.481 (3)O2—C211.357 (3)
C1—H1A0.9900O2—H20.92 (4)
C1—H1B0.9900C21—C261.389 (4)
C2—H2A0.9900C21—C221.394 (4)
C2—H2B0.9900N21—O221.225 (3)
C3—H3A0.9900N21—O211.227 (3)
C3—H3B0.9900N21—C231.470 (3)
C4—H4A0.9900C22—C231.383 (4)
C4—H4B0.9900C22—H220.9500
C5—H5A0.9900C23—C241.378 (4)
C5—H5B0.9900C24—C251.384 (4)
C6—H6A0.9900C24—H240.9500
C6—H6B0.9900C25—C261.384 (4)
O1—C111.358 (3)C25—H250.9500
O1—H10.87 (4)C26—H260.9500
N11—O111.219 (3)O1W—H1WA0.85 (5)
N11—O121.234 (3)O1W—H1WB0.94 (5)
C4—N1—C1108.0 (2)H6A—C6—H6B107.9
C4—N1—C5108.1 (2)C11—O1—H1109 (2)
C1—N1—C5107.7 (2)O11—N11—O12122.8 (2)
C4—N2—C2107.5 (2)O11—N11—C13118.9 (2)
C4—N2—C6108.3 (2)O12—N11—C13118.3 (2)
C2—N2—C6107.8 (2)O1—C11—C12123.4 (2)
C3—N3—C5108.5 (2)O1—C11—C16116.9 (2)
C3—N3—C6108.2 (2)C12—C11—C16119.7 (2)
C5—N3—C6108.7 (2)C13—C12—C11118.1 (2)
C1—N4—C2107.7 (2)C13—C12—H12120.9
C1—N4—C3107.5 (2)C11—C12—H12120.9
C2—N4—C3108.2 (2)C12—C13—C14123.4 (2)
N4—C1—N1112.4 (2)C12—C13—N11118.8 (2)
N4—C1—H1A109.1C14—C13—N11117.8 (2)
N1—C1—H1A109.1C15—C14—C13117.3 (2)
N4—C1—H1B109.1C15—C14—H14121.4
N1—C1—H1B109.1C13—C14—H14121.4
H1A—C1—H1B107.9C16—C15—C14121.2 (2)
N4—C2—N2112.4 (2)C16—C15—H15119.4
N4—C2—H2A109.1C14—C15—H15119.4
N2—C2—H2A109.1C15—C16—C11120.3 (2)
N4—C2—H2B109.1C15—C16—H16119.9
N2—C2—H2B109.1C11—C16—H16119.9
H2A—C2—H2B107.9C21—O2—H2107 (2)
N3—C3—N4112.3 (2)O2—C21—C26122.4 (2)
N3—C3—H3A109.1O2—C21—C22117.9 (2)
N4—C3—H3A109.1C26—C21—C22119.7 (2)
N3—C3—H3B109.1O22—N21—O21123.8 (3)
N4—C3—H3B109.1O22—N21—C23118.2 (3)
H3A—C3—H3B107.9O21—N21—C23118.0 (3)
N2—C4—N1112.5 (2)C23—C22—C21117.9 (2)
N2—C4—H4A109.1C23—C22—H22121.0
N1—C4—H4A109.1C21—C22—H22121.0
N2—C4—H4B109.1C24—C23—C22123.5 (2)
N1—C4—H4B109.1C24—C23—N21118.6 (3)
H4A—C4—H4B107.8C22—C23—N21117.9 (2)
N3—C5—N1111.9 (2)C23—C24—C25117.6 (3)
N3—C5—H5A109.2C23—C24—H24121.2
N1—C5—H5A109.2C25—C24—H24121.2
N3—C5—H5B109.2C24—C25—C26120.7 (2)
N1—C5—H5B109.2C24—C25—H25119.7
H5A—C5—H5B107.9C26—C25—H25119.7
N3—C6—N2112.2 (2)C25—C26—C21120.6 (2)
N3—C6—H6A109.2C25—C26—H26119.7
N2—C6—H6A109.2C21—C26—H26119.7
N3—C6—H6B109.2H1WA—O1W—H1WB101 (4)
N2—C6—H6B109.2
C2—N4—C1—N158.2 (3)C11—C12—C13—C140.2 (4)
C3—N4—C1—N158.2 (3)C11—C12—C13—N11179.9 (2)
C4—N1—C1—N458.1 (3)O11—N11—C13—C123.1 (4)
C5—N1—C1—N458.4 (3)O12—N11—C13—C12176.4 (2)
C1—N4—C2—N258.9 (3)O11—N11—C13—C14176.8 (2)
C3—N4—C2—N257.1 (3)O12—N11—C13—C143.7 (4)
C4—N2—C2—N459.0 (3)C12—C13—C14—C150.5 (4)
C6—N2—C2—N457.5 (3)N11—C13—C14—C15179.4 (2)
C5—N3—C3—N459.0 (3)C13—C14—C15—C160.4 (4)
C6—N3—C3—N458.8 (3)C14—C15—C16—C110.5 (4)
C1—N4—C3—N358.3 (3)O1—C11—C16—C15179.7 (2)
C2—N4—C3—N357.7 (3)C12—C11—C16—C151.2 (4)
C2—N2—C4—N158.7 (3)O2—C21—C22—C23179.8 (2)
C6—N2—C4—N157.4 (3)C26—C21—C22—C231.0 (4)
C1—N1—C4—N258.4 (3)C21—C22—C23—C240.2 (4)
C5—N1—C4—N257.9 (3)C21—C22—C23—N21178.9 (2)
C3—N3—C5—N158.9 (3)O22—N21—C23—C249.7 (3)
C6—N3—C5—N158.6 (3)O21—N21—C23—C24171.0 (2)
C4—N1—C5—N358.2 (3)O22—N21—C23—C22169.1 (2)
C1—N1—C5—N358.2 (3)O21—N21—C23—C2210.2 (3)
C3—N3—C6—N259.5 (3)C22—C23—C24—C250.8 (4)
C5—N3—C6—N258.2 (3)N21—C23—C24—C25179.5 (2)
C4—N2—C6—N357.3 (3)C23—C24—C25—C260.2 (4)
C2—N2—C6—N358.7 (3)C24—C25—C26—C211.1 (4)
O1—C11—C12—C13179.9 (2)O2—C21—C26—C25179.2 (2)
C16—C11—C12—C131.0 (4)C22—C21—C26—C251.7 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···N10.87 (4)1.89 (4)2.727 (3)162 (3)
O2—H2···O1W0.92 (4)1.76 (4)2.677 (3)175 (4)
O1W—H1WA···N20.85 (5)2.00 (5)2.852 (3)172 (5)
O1W—H1WB···N4i0.94 (5)1.92 (5)2.852 (3)173 (4)
C1—H1A···O22ii0.992.533.476 (3)161
C1—H1B···O1iii0.992.473.363 (3)149
C4—H4B···O21ii0.992.523.457 (3)158
C14—H14···N3iv0.952.413.278 (3)152
Symmetry codes: (i) x, y, z1; (ii) x+2, y+1, z+1; (iii) x, y+3/2, z+1/2; (iv) x+1, y+3/2, z+1/2.
3-Nitrophenol–1,3,6,8-tetraazatricyclo[4.3.1.13,8]undecane (2:1) (2a) top
Crystal data top
C7H14N4·2C6H5NO3F(000) = 456
Mr = 432.44Dx = 1.413 Mg m3
Monoclinic, CmMo Kα radiation, λ = 0.71073 Å
a = 7.2053 (7) ÅCell parameters from 8351 reflections
b = 25.253 (2) Åθ = 3.4–27.8°
c = 6.5134 (6) ŵ = 0.11 mm1
β = 120.939 (6)°T = 173 K
V = 1016.52 (17) Å3Plate, yellow
Z = 20.23 × 0.17 × 0.08 mm
Data collection top
Stoe IPDS II two-circle
diffractometer
2119 reflections with I > 2σ(I)
Radiation source: Genix 3D IµS microfocus X-ray sourceRint = 0.036
ω scansθmax = 27.6°, θmin = 3.4°
Absorption correction: multi-scan
(X-AREA; Stoe & Cie, 2001)
h = 99
Tmin = 0.529, Tmax = 1.000k = 3232
8351 measured reflectionsl = 88
2401 independent reflections
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.039 w = 1/[σ2(Fo2) + (0.0567P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.094(Δ/σ)max < 0.001
S = 1.05Δρmax = 0.17 e Å3
2401 reflectionsΔρmin = 0.19 e Å3
149 parametersAbsolute structure: Flack x determined using 883 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
2 restraintsAbsolute structure parameter: 1.8 (10)
Primary atom site location: structure-invariant direct methods
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*/UeqOcc. (<1)
O10.5286 (3)0.16364 (8)0.7582 (3)0.0347 (5)
H10.530 (6)0.1304 (15)0.718 (6)0.042 (9)*
O20.5119 (4)0.37561 (9)0.3797 (4)0.0585 (7)
O30.5330 (4)0.35709 (9)0.7134 (4)0.0495 (6)
N10.5539 (4)0.05764 (9)0.7291 (4)0.0322 (5)
N20.8694 (6)0.0000001.0000 (6)0.0405 (8)
N30.5526 (6)0.0000001.0384 (6)0.0380 (8)
N110.5176 (4)0.34371 (9)0.5246 (4)0.0361 (6)
C10.7924 (5)0.04855 (11)0.8566 (6)0.0392 (7)
H1A0.8374070.0476950.7363940.047*
H1B0.8654360.0791350.9632430.047*
C20.4302 (6)0.03087 (11)0.4979 (5)0.0403 (7)
H2A0.4864130.0429280.3955080.048*
H2B0.2781140.0429290.4212940.048*
C30.4749 (5)0.04851 (11)0.8952 (5)0.0376 (7)
H3A0.5179240.0790871.0056330.045*
H3B0.3147790.0475120.8010870.045*
C40.7891 (8)0.0000001.1659 (7)0.0430 (10)
H4A0.8444580.0317081.2697490.052*0.5
H4B0.8444590.0317081.2697500.052*0.5
C110.5156 (4)0.19734 (10)0.5904 (4)0.0246 (5)
C120.5266 (4)0.25136 (11)0.6409 (4)0.0258 (5)
H120.5463830.2634500.7889970.031*
C130.5077 (4)0.28686 (10)0.4689 (4)0.0267 (5)
C140.4793 (4)0.27170 (11)0.2496 (4)0.0301 (6)
H140.4660710.2971220.1353150.036*
C150.4711 (4)0.21778 (11)0.2049 (4)0.0298 (5)
H150.4538450.2059830.0575490.036*
C160.4876 (4)0.18075 (10)0.3706 (4)0.0276 (5)
H160.4797870.1440380.3352160.033*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0577 (13)0.0219 (9)0.0310 (9)0.0006 (9)0.0274 (9)0.0025 (7)
O20.0795 (19)0.0290 (12)0.0552 (14)0.0007 (11)0.0261 (13)0.0148 (10)
O30.0660 (15)0.0305 (11)0.0626 (14)0.0020 (10)0.0405 (12)0.0109 (11)
N10.0488 (14)0.0221 (10)0.0312 (11)0.0011 (10)0.0245 (10)0.0017 (9)
N20.043 (2)0.0312 (17)0.0422 (19)0.0000.0187 (16)0.000
N30.067 (2)0.0230 (15)0.0340 (16)0.0000.0327 (17)0.000
N110.0346 (13)0.0232 (11)0.0461 (15)0.0018 (9)0.0175 (11)0.0030 (10)
C10.0489 (17)0.0279 (14)0.0464 (16)0.0057 (12)0.0284 (14)0.0011 (11)
C20.0609 (19)0.0271 (15)0.0302 (13)0.0047 (12)0.0215 (13)0.0031 (10)
C30.059 (2)0.0246 (13)0.0409 (15)0.0027 (12)0.0343 (15)0.0000 (11)
C40.066 (3)0.028 (2)0.0284 (18)0.0000.0198 (19)0.000
C110.0256 (12)0.0249 (12)0.0232 (11)0.0006 (10)0.0123 (9)0.0015 (9)
C120.0263 (12)0.0261 (12)0.0237 (11)0.0009 (10)0.0120 (9)0.0003 (9)
C130.0249 (12)0.0230 (12)0.0289 (11)0.0010 (9)0.0114 (10)0.0015 (9)
C140.0286 (13)0.0333 (13)0.0266 (12)0.0024 (11)0.0129 (10)0.0076 (10)
C150.0275 (13)0.0381 (14)0.0234 (11)0.0004 (11)0.0127 (10)0.0002 (10)
C160.0308 (13)0.0245 (12)0.0279 (12)0.0002 (10)0.0154 (11)0.0039 (10)
Geometric parameters (Å, º) top
O1—C111.350 (3)C2—H2A0.9900
O1—H10.88 (4)C2—H2B0.9900
O2—N111.225 (3)C3—H3A0.9900
O3—N111.224 (3)C3—H3B0.9900
N1—C21.463 (4)C4—H4A0.9900
N1—C31.477 (3)C4—H4B0.9900
N1—C11.493 (4)C11—C121.396 (3)
N2—C41.465 (5)C11—C161.403 (3)
N2—C1i1.466 (3)C12—C131.386 (3)
N2—C11.466 (3)C12—H120.9500
N3—C41.462 (6)C13—C141.388 (4)
N3—C3i1.465 (3)C14—C151.387 (4)
N3—C31.465 (3)C14—H140.9500
N11—C131.474 (3)C15—C161.386 (4)
C1—H1A0.9900C15—H150.9500
C1—H1B0.9900C16—H160.9500
C2—C2i1.559 (6)
C11—O1—H1111 (2)N3—C3—H3B108.4
C2—N1—C3114.9 (2)N1—C3—H3B108.4
C2—N1—C1114.8 (2)H3A—C3—H3B107.5
C3—N1—C1109.6 (2)N3—C4—N2111.6 (3)
C4—N2—C1i107.8 (2)N3—C4—H4A109.3
C4—N2—C1107.8 (2)N2—C4—H4A109.3
C1i—N2—C1113.4 (3)N3—C4—H4B109.3
C4—N3—C3i108.3 (2)N2—C4—H4B109.3
C4—N3—C3108.3 (2)H4A—C4—H4B108.0
C3i—N3—C3113.5 (3)O1—C11—C12117.0 (2)
O3—N11—O2122.8 (3)O1—C11—C16123.5 (2)
O3—N11—C13119.0 (2)C12—C11—C16119.5 (2)
O2—N11—C13118.2 (2)C13—C12—C11118.1 (2)
N2—C1—N1115.7 (2)C13—C12—H12120.9
N2—C1—H1A108.4C11—C12—H12120.9
N1—C1—H1A108.4C12—C13—C14123.7 (2)
N2—C1—H1B108.4C12—C13—N11117.3 (2)
N1—C1—H1B108.4C14—C13—N11119.0 (2)
H1A—C1—H1B107.4C15—C14—C13117.0 (2)
N1—C2—C2i117.53 (13)C15—C14—H14121.5
N1—C2—H2A107.9C13—C14—H14121.5
C2i—C2—H2A107.9C16—C15—C14121.4 (2)
N1—C2—H2B107.9C16—C15—H15119.3
C2i—C2—H2B107.9C14—C15—H15119.3
H2A—C2—H2B107.2C15—C16—C11120.2 (2)
N3—C3—N1115.6 (2)C15—C16—H16119.9
N3—C3—H3A108.4C11—C16—H16119.9
N1—C3—H3A108.4
C4—N2—C1—N154.3 (3)O1—C11—C12—C13178.3 (2)
C1i—N2—C1—N165.0 (4)C16—C11—C12—C130.4 (3)
C2—N1—C1—N284.3 (3)C11—C12—C13—C140.2 (4)
C3—N1—C1—N246.9 (3)C11—C12—C13—N11179.4 (2)
C3—N1—C2—C2i64.1 (2)O3—N11—C13—C122.9 (3)
C1—N1—C2—C2i64.4 (2)O2—N11—C13—C12176.5 (3)
C4—N3—C3—N154.7 (3)O3—N11—C13—C14176.8 (3)
C3i—N3—C3—N165.6 (4)O2—N11—C13—C143.9 (4)
C2—N1—C3—N384.2 (3)C12—C13—C14—C150.4 (4)
C1—N1—C3—N346.8 (3)N11—C13—C14—C15180.0 (2)
C3i—N3—C4—N261.73 (19)C13—C14—C15—C160.9 (4)
C3—N3—C4—N261.73 (19)C14—C15—C16—C110.7 (4)
C1i—N2—C4—N361.4 (2)O1—C11—C16—C15178.6 (3)
C1—N2—C4—N361.4 (2)C12—C11—C16—C150.1 (3)
Symmetry code: (i) x, y, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···N10.88 (4)1.84 (4)2.696 (3)162 (3)
C4—H4A···O2ii0.992.563.476 (3)154
C4—H4B···O2iii0.992.563.476 (3)154
C15—H15···O1iv0.952.513.427 (3)161
Symmetry codes: (ii) x+1/2, y1/2, z+1; (iii) x+1/2, y+1/2, z+1; (iv) x, y, z1.
3-Nitrophenol–1,3,6,8-tetraazatricyclo[4.4.1.13,8]dodecane (2:1) (3a) top
Crystal data top
C8H16N4·2C6H5NO3F(000) = 944
Mr = 446.47Dx = 1.421 Mg m3
Monoclinic, CcMo Kα radiation, λ = 0.71073 Å
a = 26.159 (3) ÅCell parameters from 11125 reflections
b = 6.4931 (4) Åθ = 3.5–25.8°
c = 12.8070 (14) ŵ = 0.11 mm1
β = 106.338 (8)°T = 173 K
V = 2087.5 (4) Å3Plate, yellow
Z = 40.26 × 0.24 × 0.09 mm
Data collection top
Stoe IPDS II two-circle
diffractometer
3297 reflections with I > 2σ(I)
Radiation source: Genix 3D IµS microfocus X-ray sourceRint = 0.027
ω scansθmax = 25.6°, θmin = 3.5°
Absorption correction: multi-scan
(X-AREA; Stoe & Cie, 2001)
h = 3131
Tmin = 0.582, Tmax = 1.000k = 77
11125 measured reflectionsl = 1515
3505 independent reflections
Refinement top
Refinement on F2H atoms treated by a mixture of independent and constrained refinement
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0416P)2 + 1.2092P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.036(Δ/σ)max < 0.001
wR(F2) = 0.087Δρmax = 0.14 e Å3
S = 1.08Δρmin = 0.15 e Å3
3505 reflectionsExtinction correction: SHELXL2014 (Sheldrick, 2015), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
298 parametersExtinction coefficient: 0.0087 (10)
2 restraintsAbsolute structure: Flack x determined using 1329 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.2 (9)
Hydrogen site location: mixed
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
N10.44528 (9)0.2931 (4)0.4785 (2)0.0231 (5)
N20.55900 (10)0.3302 (3)0.5346 (2)0.0244 (5)
N30.50770 (10)0.0032 (4)0.4661 (2)0.0252 (5)
N40.49760 (9)0.3696 (4)0.3449 (2)0.0247 (5)
C10.47168 (12)0.4020 (5)0.5808 (3)0.0337 (7)
H1A0.46510.32340.64190.040*
H1B0.45450.53830.57910.040*
C20.53212 (12)0.4353 (5)0.6047 (3)0.0370 (8)
H2A0.53860.58500.60080.044*
H2B0.54910.39150.68060.044*
C30.45716 (12)0.0699 (4)0.4817 (3)0.0272 (6)
H3A0.45530.01660.55300.033*
H3B0.42830.00220.42520.033*
C40.45002 (11)0.4014 (4)0.3795 (2)0.0264 (6)
H4A0.41900.36130.31850.032*
H4B0.44680.55100.39140.032*
C50.55491 (12)0.1024 (4)0.5363 (3)0.0305 (7)
H5A0.58630.04520.51770.037*
H5B0.55780.06050.61210.037*
C60.54774 (12)0.4195 (5)0.4247 (3)0.0300 (7)
H6A0.54960.57120.43270.036*
H6B0.57690.37760.39400.036*
C70.50771 (14)0.0199 (5)0.3531 (3)0.0351 (7)
H7A0.48010.12180.31800.042*
H7B0.54260.07710.35160.042*
C80.49764 (13)0.1784 (5)0.2851 (2)0.0306 (7)
H8A0.52520.18920.24610.037*
H8B0.46280.16550.22960.037*
N110.15684 (11)0.4297 (6)0.3322 (2)0.0422 (8)
O110.33946 (9)0.2081 (4)0.4343 (2)0.0402 (6)
H110.3734 (18)0.252 (7)0.449 (3)0.048 (11)*
O120.14277 (10)0.2493 (5)0.3334 (2)0.0594 (8)
O130.12521 (9)0.5734 (5)0.2996 (2)0.0596 (8)
C110.30418 (11)0.3667 (5)0.4201 (2)0.0267 (6)
C120.25005 (12)0.3201 (5)0.3832 (2)0.0308 (7)
H120.23830.18230.36680.037*
C130.21382 (11)0.4798 (6)0.3711 (2)0.0310 (7)
C140.22866 (13)0.6835 (6)0.3947 (3)0.0355 (8)
H140.20280.78960.38590.043*
C150.28227 (14)0.7260 (5)0.4311 (3)0.0358 (7)
H150.29360.86420.44770.043*
C160.32020 (12)0.5711 (5)0.4442 (3)0.0316 (7)
H160.35700.60390.46960.038*
N210.84474 (10)0.5845 (5)0.6896 (2)0.0377 (7)
O210.66682 (9)0.3172 (3)0.6068 (2)0.0402 (7)
H210.635 (2)0.344 (7)0.582 (4)0.061 (14)*
O220.86017 (10)0.4093 (4)0.6811 (3)0.0532 (8)
O230.87489 (10)0.7320 (5)0.7172 (3)0.0589 (8)
C210.69850 (11)0.4855 (4)0.6209 (2)0.0258 (6)
C220.75329 (11)0.4526 (5)0.6475 (3)0.0281 (7)
H220.76740.31680.65480.034*
C230.78669 (12)0.6217 (5)0.6629 (2)0.0274 (6)
C240.76851 (13)0.8228 (5)0.6538 (3)0.0322 (7)
H240.79250.93600.66560.039*
C250.71378 (13)0.8522 (5)0.6266 (3)0.0319 (7)
H250.69990.98830.61860.038*
C260.67895 (12)0.6860 (5)0.6109 (2)0.0274 (7)
H260.64160.70930.59320.033*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0177 (11)0.0254 (12)0.0264 (12)0.0001 (9)0.0063 (10)0.0009 (10)
N20.0196 (11)0.0234 (12)0.0282 (13)0.0034 (10)0.0035 (9)0.0021 (10)
N30.0234 (11)0.0203 (11)0.0318 (13)0.0001 (9)0.0074 (10)0.0028 (10)
N40.0224 (11)0.0237 (12)0.0267 (12)0.0002 (9)0.0051 (9)0.0059 (10)
C10.0282 (15)0.0410 (18)0.0323 (17)0.0010 (14)0.0091 (13)0.0085 (14)
C20.0280 (15)0.049 (2)0.0329 (17)0.0013 (14)0.0065 (13)0.0157 (15)
C30.0233 (14)0.0270 (14)0.0329 (15)0.0012 (12)0.0106 (12)0.0100 (13)
C40.0228 (13)0.0239 (14)0.0301 (15)0.0042 (11)0.0034 (12)0.0055 (12)
C50.0225 (13)0.0243 (15)0.0391 (17)0.0031 (12)0.0005 (12)0.0061 (13)
C60.0231 (14)0.0289 (15)0.0358 (17)0.0049 (11)0.0048 (12)0.0068 (13)
C70.0417 (18)0.0287 (16)0.0390 (18)0.0035 (13)0.0178 (15)0.0049 (13)
C80.0297 (15)0.0364 (18)0.0252 (15)0.0032 (12)0.0069 (12)0.0012 (12)
N110.0211 (13)0.076 (2)0.0289 (14)0.0010 (14)0.0055 (11)0.0050 (14)
O110.0204 (11)0.0334 (12)0.0642 (17)0.0017 (10)0.0076 (11)0.0007 (11)
O120.0291 (13)0.084 (2)0.0609 (18)0.0197 (14)0.0050 (12)0.0018 (15)
O130.0238 (13)0.095 (2)0.0580 (18)0.0156 (14)0.0078 (12)0.0007 (16)
C110.0220 (14)0.0308 (15)0.0266 (15)0.0019 (11)0.0054 (12)0.0014 (12)
C120.0258 (15)0.0383 (18)0.0288 (16)0.0042 (13)0.0084 (12)0.0022 (13)
C130.0203 (14)0.052 (2)0.0208 (15)0.0022 (14)0.0062 (12)0.0016 (13)
C140.0275 (15)0.049 (2)0.0308 (17)0.0090 (14)0.0097 (13)0.0038 (15)
C150.0384 (17)0.0337 (18)0.0357 (18)0.0006 (14)0.0113 (14)0.0048 (14)
C160.0227 (14)0.0407 (19)0.0301 (16)0.0035 (13)0.0052 (12)0.0029 (14)
N210.0237 (13)0.0477 (18)0.0387 (15)0.0027 (13)0.0039 (11)0.0018 (14)
O210.0184 (11)0.0252 (12)0.0715 (18)0.0016 (9)0.0036 (12)0.0019 (11)
O220.0256 (12)0.0537 (17)0.073 (2)0.0081 (12)0.0027 (12)0.0022 (14)
O230.0296 (13)0.0651 (18)0.077 (2)0.0200 (13)0.0070 (13)0.0159 (16)
C210.0238 (14)0.0236 (15)0.0273 (16)0.0030 (12)0.0030 (11)0.0006 (12)
C220.0249 (15)0.0262 (16)0.0310 (15)0.0056 (12)0.0043 (12)0.0002 (12)
C230.0221 (14)0.0343 (16)0.0227 (14)0.0029 (12)0.0014 (11)0.0012 (12)
C240.0380 (18)0.0298 (17)0.0303 (15)0.0084 (13)0.0120 (14)0.0043 (13)
C250.0427 (18)0.0228 (14)0.0301 (16)0.0049 (13)0.0101 (14)0.0001 (12)
C260.0259 (15)0.0279 (16)0.0282 (15)0.0077 (12)0.0074 (12)0.0029 (12)
Geometric parameters (Å, º) top
N1—C11.478 (4)N11—O121.229 (5)
N1—C31.481 (4)N11—O131.239 (4)
N1—C41.484 (4)N11—C131.469 (4)
N2—C21.457 (4)O11—C111.360 (4)
N2—C61.473 (4)O11—H110.90 (5)
N2—C51.484 (4)C11—C121.394 (4)
N3—C71.455 (4)C11—C161.400 (4)
N3—C31.457 (4)C12—C131.384 (5)
N3—C51.457 (4)C12—H120.9500
N4—C41.449 (4)C13—C141.388 (5)
N4—C61.455 (4)C14—C151.376 (5)
N4—C81.459 (4)C14—H140.9500
C1—C21.539 (4)C15—C161.389 (5)
C1—H1A0.9900C15—H150.9500
C1—H1B0.9900C16—H160.9500
C2—H2A0.9900N21—O221.222 (4)
C2—H2B0.9900N21—O231.228 (4)
C3—H3A0.9900N21—C231.480 (4)
C3—H3B0.9900O21—C211.353 (4)
C4—H4A0.9900O21—H210.83 (5)
C4—H4B0.9900C21—C261.391 (4)
C5—H5A0.9900C21—C221.393 (4)
C5—H5B0.9900C22—C231.383 (4)
C6—H6A0.9900C22—H220.9500
C6—H6B0.9900C23—C241.383 (4)
C7—C81.535 (5)C24—C251.388 (5)
C7—H7A0.9900C24—H240.9500
C7—H7B0.9900C25—C261.390 (4)
C8—H8A0.9900C25—H250.9500
C8—H8B0.9900C26—H260.9500
C1—N1—C3113.7 (2)C8—C7—H7B108.4
C1—N1—C4113.6 (2)H7A—C7—H7B107.5
C3—N1—C4114.8 (2)N4—C8—C7116.2 (3)
C2—N2—C6113.8 (2)N4—C8—H8A108.2
C2—N2—C5114.1 (3)C7—C8—H8A108.2
C6—N2—C5114.2 (2)N4—C8—H8B108.2
C7—N3—C3114.9 (2)C7—C8—H8B108.2
C7—N3—C5115.0 (2)H8A—C8—H8B107.4
C3—N3—C5115.3 (3)O12—N11—O13123.2 (3)
C4—N4—C6115.8 (2)O12—N11—C13119.1 (3)
C4—N4—C8114.2 (2)O13—N11—C13117.7 (3)
C6—N4—C8115.1 (2)C11—O11—H11112 (3)
N1—C1—C2116.2 (3)O11—C11—C12117.9 (3)
N1—C1—H1A108.2O11—C11—C16122.6 (3)
C2—C1—H1A108.2C12—C11—C16119.5 (3)
N1—C1—H1B108.2C13—C12—C11118.3 (3)
C2—C1—H1B108.2C13—C12—H12120.9
H1A—C1—H1B107.4C11—C12—H12120.9
N2—C2—C1117.3 (3)C12—C13—C14123.3 (3)
N2—C2—H2A108.0C12—C13—N11118.0 (3)
C1—C2—H2A108.0C14—C13—N11118.7 (3)
N2—C2—H2B108.0C15—C14—C13117.5 (3)
C1—C2—H2B108.0C15—C14—H14121.3
H2A—C2—H2B107.2C13—C14—H14121.3
N3—C3—N1118.6 (2)C14—C15—C16121.4 (3)
N3—C3—H3A107.7C14—C15—H15119.3
N1—C3—H3A107.7C16—C15—H15119.3
N3—C3—H3B107.7C15—C16—C11120.0 (3)
N1—C3—H3B107.7C15—C16—H16120.0
H3A—C3—H3B107.1C11—C16—H16120.0
N4—C4—N1118.6 (2)O22—N21—O23123.4 (3)
N4—C4—H4A107.7O22—N21—C23118.4 (3)
N1—C4—H4A107.7O23—N21—C23118.2 (3)
N4—C4—H4B107.7C21—O21—H21113 (3)
N1—C4—H4B107.7O21—C21—C26123.2 (3)
H4A—C4—H4B107.1O21—C21—C22117.3 (3)
N3—C5—N2118.9 (2)C26—C21—C22119.5 (3)
N3—C5—H5A107.6C23—C22—C21118.6 (3)
N2—C5—H5A107.6C23—C22—H22120.7
N3—C5—H5B107.6C21—C22—H22120.7
N2—C5—H5B107.6C22—C23—C24123.3 (3)
H5A—C5—H5B107.0C22—C23—N21118.0 (3)
N4—C6—N2118.8 (2)C24—C23—N21118.7 (3)
N4—C6—H6A107.6C23—C24—C25117.2 (3)
N2—C6—H6A107.6C23—C24—H24121.4
N4—C6—H6B107.6C25—C24—H24121.4
N2—C6—H6B107.6C24—C25—C26121.1 (3)
H6A—C6—H6B107.0C24—C25—H25119.4
N3—C7—C8115.4 (3)C26—C25—H25119.4
N3—C7—H7A108.4C25—C26—C21120.3 (3)
C8—C7—H7A108.4C25—C26—H26119.9
N3—C7—H7B108.4C21—C26—H26119.9
C3—N1—C1—C272.9 (4)C16—C11—C12—C130.4 (5)
C4—N1—C1—C260.8 (4)C11—C12—C13—C140.5 (5)
C6—N2—C2—C173.0 (4)C11—C12—C13—N11180.0 (3)
C5—N2—C2—C160.6 (4)O12—N11—C13—C1215.0 (4)
N1—C1—C2—N29.3 (5)O13—N11—C13—C12165.0 (3)
C7—N3—C3—N185.0 (3)O12—N11—C13—C14164.5 (3)
C5—N3—C3—N152.3 (4)O13—N11—C13—C1415.5 (4)
C1—N1—C3—N379.7 (3)C12—C13—C14—C150.4 (5)
C4—N1—C3—N353.5 (3)N11—C13—C14—C15179.9 (3)
C6—N4—C4—N157.2 (3)C13—C14—C15—C160.2 (5)
C8—N4—C4—N180.0 (3)C14—C15—C16—C110.1 (5)
C1—N1—C4—N484.3 (3)O11—C11—C16—C15178.1 (3)
C3—N1—C4—N448.9 (3)C12—C11—C16—C150.2 (5)
C7—N3—C5—N280.1 (4)O21—C21—C22—C23179.7 (3)
C3—N3—C5—N257.2 (4)C26—C21—C22—C230.1 (4)
C2—N2—C5—N384.1 (4)C21—C22—C23—C240.2 (5)
C6—N2—C5—N349.2 (4)C21—C22—C23—N21179.2 (3)
C4—N4—C6—N251.8 (3)O22—N21—C23—C2210.5 (5)
C8—N4—C6—N285.1 (3)O23—N21—C23—C22170.7 (3)
C2—N2—C6—N479.0 (3)O22—N21—C23—C24168.9 (3)
C5—N2—C6—N454.5 (4)O23—N21—C23—C249.9 (5)
C3—N3—C7—C863.2 (3)C22—C23—C24—C250.6 (5)
C5—N3—C7—C874.3 (3)N21—C23—C24—C25178.8 (3)
C4—N4—C8—C775.2 (3)C23—C24—C25—C260.9 (5)
C6—N4—C8—C762.4 (4)C24—C25—C26—C210.8 (5)
N3—C7—C8—N49.3 (4)O21—C21—C26—C25179.9 (3)
O11—C11—C12—C13178.4 (3)C22—C21—C26—C250.4 (5)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O11—H11···N10.90 (5)1.83 (5)2.722 (3)170 (4)
O21—H21···N20.83 (5)1.90 (5)2.711 (3)164 (5)
C15—H15···O11i0.952.563.465 (4)158
C25—H25···O21i0.952.293.243 (4)178
Symmetry code: (i) x, y+1, z.
Selected bond lengths (Å) for the aminal cages structures (1)–(3) of (1a), (2a) and (3a) top
HMTA is 1,3,5,7-tetraazatricyclo[3.3.1.13,7]decane and TATD is 1,3,6,8-tetraazatricyclo[4.4.1.13,8]dodecane.
Parameter(1a)(2a)(3a)HMTAaTATDb
α11.471 (4)1.493 (4)1.481 (4)1.462 (5)1.456 (2)
α21.481 (3)1.477 (3)1.484 (4)1.462 (5)1.456 (2)
α31.479 (4)1.463 (4)1.478 (4)1.462 (5)1.459 (5)
β11.470 (3)1.466 (3)1.484 (4)1.462 (5)1.456 (2)
β21.478 (3)1.466 (3)1.473 (4)1.462 (5)1.456 (2)
β31.478 (3)1.465 (5)1.457 (4)1.462 (5)1.459 (5)
γ11.461 (3)1.465 (3)1.457 (4)1.462 (5)1.456 (2)
γ21.464 (4)1.465 (3)1.457 (4)1.462 (5)1.456 (2)
γ31.459 (3)1.462 (6)1.455 (4)1.462 (5)1.459 (5)
δ11.470 (4)1.449 (4)1.462 (5)1.456 (2)
δ21.474 (3)1.455 (4)1.462 (5)1.456 (2)
δ31.481 (3)1.459 (4)1.462 (5)1.459 (5)
References: (a) Terpstra et al. (1993); (b) Rivera et al. (2014).
 

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