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Dibenzo-24-crown-8 crystallizes with ammonium hexa­fluoro­phosphate to produce a complex in which the ammonium ion is encapsulated by the crown ether, NH4+·C24H32O8·PF6-.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802003100/ww6007sup1.cif
Contains datablocks k55_01, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802003100/ww6007Isup2.hkl
Contains datablock I

CCDC reference: 182635

Key indicators

  • Single-crystal X-ray study
  • T = 123 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.051
  • wR factor = 0.132
  • Data-to-parameter ratio = 17.8

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry








Comment top

The host–guest relationship between crown ethers and ammonium-based cationic components is an important concept in the generation of a number of supramolecular assemblies. From our perspective, this relationship may be useful in providing electronic and structural roles towards the self-assembly of supramolecular photosynthetic mimics (Duggan, 2001). Here, we report on the solid-state structure obtained between ammonium hexafluorophosphate and dibenzo-24-crown-8, (I).

The molecular structure of [(I)·NH4]PF6 is shown in Fig. 1 and 2. The ammonium cation lies within the cavity of the crown ether (Fig. 1) and is stabilized by a series of single (N1—H1d···O6 = 1.90 Å and N1—H1a···O2 = 1.91 Å) and bifocated (N1—H1b···O8 and N1—H1b···O1 2.11 and 2.48 Å, respectively; N1—H1c···O4 and N1—H1c···O5 = 2.08 and 2.48 Å, respectively) hydrogen-bonding interactions. The difference in size complementarity between the radius of the ammonium cation and the 24 C8 cavity causes the macrocycle to adopt a folded and twisted conformation, effectively encapsulating the ammonium cation (Fig. 2). This encapsulation is similar to that observed for Na+ with DB24C8 (Dapporto, 1998), but differs from the large volume of work now published on the interactions of DB24C8 with dialkylammonium salts (Ashton, 1997, 1998), or other alkali metal ions (Gallagher, 1991) in which relatively flat conformations are observed.

Experimental top

Colourless crystals of [(I)·NH4]PF6 suitable for X-ray analysis were grown by slow evaporation from a CD3COCD3 solution of ammonium hexafluorophosphate (1.6 mg, 9.82 mmol) and dibenzo-24-crown-8 (4.2 mg, 9.36 mmol).

Refinement top

The H atoms were included in the riding-model approximation, except those of the ammonium ion which were located by difference fourier and refined.

Computing details top

Data collection: COLLECT (Nonius, 1997-2000); cell refinement: HKL SCALEPACK (Otwinowski & Minor 1997); data reduction: HKL DENZO and SCALEPACK (Otwinowski & Minor 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. View of (I·NH4)PF6 (50% probability displacement ellipsoids)
[Figure 2] Fig. 2. Side view illustrating the encapsulating nature of the crown ether around the ammonium guest.
(I) top
Crystal data top
NH4+·C24H32O8·PF6Z = 2
Mr = 611.51F(000) = 640
Triclinic, P1Dx = 1.461 Mg m3
a = 10.1950 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 10.6379 (2) ÅCell parameters from 16366 reflections
c = 14.5447 (3) Åθ = 0.4–28.3°
α = 69.371 (1)°µ = 0.19 mm1
β = 71.536 (1)°T = 123 K
γ = 89.670 (1)°Tabular, colourless
V = 1390.30 (5) Å30.2 × 0.12 × 0.08 mm
Data collection top
KappaCCD
diffractometer
Rint = 0.044
CCD rotation images, thick slices [scan type available ?]θmax = 28.3°, θmin = 2.8°
16366 measured reflectionsh = 1213
6721 independent reflectionsk = 1314
3813 reflections with I > 2σ(I)l = 1819
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.051 w = 1/[σ2(Fo2) + (0.0619P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.133(Δ/σ)max = 0.009
S = 0.97Δρmax = 0.64 e Å3
6721 reflectionsΔρmin = 0.55 e Å3
377 parameters
Crystal data top
NH4+·C24H32O8·PF6γ = 89.670 (1)°
Mr = 611.51V = 1390.30 (5) Å3
Triclinic, P1Z = 2
a = 10.1950 (2) ÅMo Kα radiation
b = 10.6379 (2) ŵ = 0.19 mm1
c = 14.5447 (3) ÅT = 123 K
α = 69.371 (1)°0.2 × 0.12 × 0.08 mm
β = 71.536 (1)°
Data collection top
KappaCCD
diffractometer
3813 reflections with I > 2σ(I)
16366 measured reflectionsRint = 0.044
6721 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0510 restraints
wR(F2) = 0.133H atoms treated by a mixture of independent and constrained refinement
S = 0.97Δρmax = 0.64 e Å3
6721 reflectionsΔρmin = 0.55 e Å3
377 parameters
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
C10.3129 (2)0.1603 (2)0.46349 (16)0.0207 (5)
C20.2641 (2)0.2965 (2)0.50646 (17)0.0258 (5)
H20.26590.34470.46220.031*
C30.2125 (2)0.3635 (2)0.61440 (18)0.0285 (5)
H30.17850.4570.64360.034*
C40.2107 (2)0.2941 (2)0.67843 (18)0.0284 (5)
H40.17690.34040.7520.034*
C50.2579 (2)0.1570 (2)0.63661 (17)0.0254 (5)
H50.25550.10970.68160.031*
C60.3086 (2)0.0886 (2)0.52907 (16)0.0220 (5)
C70.3315 (2)0.1256 (2)0.54566 (16)0.0231 (5)
H7A0.37730.09180.5990.028*
H7B0.23010.1180.58190.028*
C80.3872 (2)0.2705 (2)0.47824 (17)0.0264 (5)
H8A0.36570.3250.52290.032*
H8B0.48980.27680.44860.032*
C90.1858 (2)0.3367 (2)0.42397 (18)0.0289 (5)
H9A0.16750.42660.38210.035*
H9B0.14850.32550.49840.035*
C100.1133 (2)0.2282 (2)0.40712 (17)0.0293 (5)
H10A0.13470.13810.4460.035*
H10B0.01120.22960.43240.035*
C110.1237 (2)0.1419 (2)0.27621 (18)0.0278 (5)
H11A0.02390.10870.31520.033*
H11B0.1790.06740.29850.033*
C120.1506 (2)0.1856 (2)0.16160 (17)0.0254 (5)
H12A0.12220.10930.14540.03*
H12B0.09590.26060.13920.03*
C130.3387 (2)0.2886 (2)0.00041 (16)0.0203 (5)
C140.2543 (2)0.2851 (2)0.05749 (17)0.0251 (5)
H140.16280.23830.02310.03*
C150.3036 (2)0.3505 (2)0.16579 (18)0.0279 (5)
H150.24540.3480.2050.033*
C160.4359 (2)0.4185 (2)0.21610 (17)0.0256 (5)
H160.46860.46360.28980.031*
C170.5221 (2)0.4209 (2)0.15839 (17)0.0241 (5)
H170.61350.4680.19310.029*
C180.4754 (2)0.3556 (2)0.05178 (16)0.0206 (5)
C190.6980 (2)0.4006 (2)0.04130 (16)0.0227 (5)
H19A0.71070.49660.08840.027*
H19B0.74090.34650.08370.027*
C200.7664 (2)0.3860 (2)0.03955 (17)0.0251 (5)
H20A0.86750.41480.00320.03*
H20B0.72920.44870.07560.03*
C210.8072 (2)0.1501 (2)0.07834 (18)0.0269 (5)
H21A0.85610.09410.12440.032*
H21B0.87630.19360.00750.032*
C220.6964 (2)0.0610 (2)0.07462 (17)0.0283 (5)
H22A0.64510.11620.03020.034*
H22B0.73920.00610.0450.034*
C230.4812 (2)0.0731 (2)0.18246 (17)0.0266 (5)
H23A0.50590.12570.13640.032*
H23B0.42040.00590.15780.032*
C240.4062 (2)0.1658 (2)0.29223 (16)0.0253 (5)
H24A0.32130.21470.29570.03*
H24B0.46680.23330.31680.03*
N10.4623 (2)0.2082 (2)0.24701 (16)0.0218 (4)
O10.35901 (15)0.04659 (14)0.48033 (11)0.0225 (3)
O20.33418 (14)0.32964 (15)0.39406 (11)0.0254 (4)
O30.16171 (15)0.25410 (15)0.29787 (11)0.0271 (4)
O40.29767 (14)0.22981 (15)0.10713 (11)0.0232 (3)
O50.55144 (14)0.35355 (15)0.01218 (11)0.0215 (3)
O60.74804 (15)0.25306 (15)0.11655 (11)0.0237 (3)
O70.60376 (15)0.00615 (15)0.17881 (11)0.0264 (4)
O80.36844 (15)0.08689 (14)0.35784 (11)0.0234 (3)
F10.01733 (15)0.67182 (18)0.18470 (12)0.0529 (5)
F20.17876 (14)0.82921 (16)0.17226 (11)0.0459 (4)
F30.02872 (17)0.86009 (18)0.30988 (14)0.0668 (5)
F40.13337 (13)0.70644 (15)0.32083 (10)0.0400 (4)
F50.03158 (18)0.88075 (17)0.16863 (15)0.0735 (6)
F60.07863 (18)0.65261 (17)0.32354 (14)0.0674 (6)
P10.02327 (6)0.76736 (6)0.24695 (5)0.02525 (17)
H1C0.418 (3)0.227 (3)0.199 (2)0.058 (9)*
H1D0.562 (3)0.224 (3)0.211 (2)0.042 (7)*
H1A0.429 (3)0.266 (3)0.287 (2)0.053 (8)*
H1B0.436 (3)0.122 (3)0.288 (2)0.043 (8)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0187 (11)0.0226 (13)0.0177 (11)0.0043 (9)0.0052 (9)0.0047 (10)
C20.0259 (12)0.0245 (13)0.0263 (13)0.0026 (10)0.0088 (10)0.0086 (10)
C30.0271 (12)0.0211 (13)0.0295 (13)0.0002 (10)0.0082 (11)0.0013 (11)
C40.0257 (12)0.0279 (14)0.0218 (12)0.0005 (10)0.0054 (10)0.0001 (11)
C50.0238 (11)0.0303 (14)0.0229 (12)0.0069 (10)0.0091 (10)0.0096 (10)
C60.0187 (11)0.0194 (12)0.0256 (12)0.0043 (9)0.0080 (10)0.0053 (10)
C70.0268 (12)0.0244 (13)0.0207 (11)0.0060 (10)0.0082 (10)0.0114 (10)
C80.0277 (12)0.0283 (14)0.0254 (12)0.0051 (10)0.0103 (10)0.0112 (10)
C90.0267 (12)0.0344 (14)0.0243 (12)0.0149 (11)0.0064 (11)0.0116 (11)
C100.0217 (11)0.0398 (15)0.0194 (12)0.0055 (11)0.0016 (10)0.0074 (11)
C110.0216 (11)0.0257 (13)0.0305 (13)0.0003 (10)0.0056 (10)0.0066 (11)
C120.0182 (11)0.0265 (13)0.0272 (13)0.0001 (10)0.0062 (10)0.0063 (10)
C130.0241 (11)0.0163 (12)0.0190 (11)0.0049 (9)0.0050 (10)0.0067 (9)
C140.0240 (11)0.0226 (13)0.0304 (13)0.0050 (10)0.0102 (11)0.0107 (11)
C150.0338 (13)0.0273 (13)0.0298 (13)0.0077 (11)0.0185 (11)0.0121 (11)
C160.0359 (13)0.0239 (13)0.0197 (12)0.0075 (10)0.0126 (11)0.0084 (10)
C170.0267 (12)0.0215 (12)0.0232 (12)0.0049 (10)0.0078 (10)0.0079 (10)
C180.0230 (11)0.0197 (12)0.0220 (12)0.0047 (9)0.0095 (10)0.0095 (10)
C190.0199 (11)0.0238 (13)0.0210 (11)0.0022 (9)0.0040 (10)0.0068 (10)
C200.0238 (12)0.0225 (13)0.0290 (13)0.0035 (10)0.0094 (10)0.0091 (10)
C210.0280 (12)0.0248 (13)0.0252 (12)0.0087 (10)0.0056 (11)0.0092 (10)
C220.0345 (13)0.0234 (13)0.0205 (12)0.0053 (10)0.0002 (11)0.0087 (10)
C230.0316 (13)0.0269 (14)0.0245 (12)0.0050 (10)0.0102 (11)0.0124 (11)
C240.0313 (12)0.0234 (13)0.0234 (12)0.0042 (10)0.0089 (11)0.0115 (10)
N10.0226 (11)0.0204 (12)0.0184 (10)0.0037 (9)0.0038 (9)0.0051 (9)
O10.0263 (8)0.0192 (8)0.0200 (8)0.0043 (7)0.0059 (7)0.0066 (7)
O20.0249 (8)0.0265 (9)0.0221 (8)0.0060 (7)0.0053 (7)0.0081 (7)
O30.0286 (8)0.0279 (9)0.0211 (8)0.0029 (7)0.0057 (7)0.0069 (7)
O40.0202 (8)0.0248 (9)0.0210 (8)0.0008 (6)0.0051 (7)0.0056 (7)
O50.0192 (7)0.0250 (9)0.0195 (8)0.0017 (6)0.0064 (6)0.0073 (7)
O60.0266 (8)0.0221 (9)0.0223 (8)0.0058 (7)0.0079 (7)0.0083 (7)
O70.0268 (8)0.0268 (9)0.0215 (8)0.0000 (7)0.0041 (7)0.0074 (7)
O80.0286 (8)0.0205 (8)0.0195 (8)0.0042 (7)0.0061 (7)0.0073 (7)
F10.0375 (8)0.0759 (12)0.0536 (10)0.0070 (8)0.0012 (8)0.0481 (9)
F20.0294 (8)0.0660 (11)0.0357 (8)0.0117 (7)0.0008 (7)0.0197 (8)
F30.0626 (11)0.0683 (12)0.0683 (12)0.0244 (9)0.0108 (9)0.0524 (10)
F40.0315 (7)0.0495 (10)0.0339 (8)0.0119 (7)0.0070 (6)0.0253 (7)
F50.0589 (11)0.0520 (12)0.0856 (14)0.0115 (9)0.0358 (11)0.0125 (10)
F60.0682 (12)0.0492 (11)0.0782 (13)0.0054 (9)0.0482 (11)0.0049 (9)
P10.0258 (3)0.0247 (4)0.0232 (3)0.0022 (3)0.0058 (3)0.0086 (3)
Geometric parameters (Å, º) top
C1—O81.378 (2)C15—C161.375 (3)
C1—C21.382 (3)C15—H150.95
C1—C61.407 (3)C16—C171.401 (3)
C2—C31.394 (3)C16—H160.95
C2—H20.95C17—C181.375 (3)
C3—C41.373 (3)C17—H170.95
C3—H30.95C18—O51.382 (2)
C4—C51.388 (3)C19—O51.445 (2)
C4—H40.95C19—C201.511 (3)
C5—C61.390 (3)C19—H19A0.99
C5—H50.95C19—H19B0.99
C6—O11.376 (3)C20—O61.429 (3)
C7—O11.442 (2)C20—H20A0.99
C7—C81.501 (3)C20—H20B0.99
C7—H7A0.99C21—O61.443 (3)
C7—H7B0.99C21—C221.504 (3)
C8—O21.435 (2)C21—H21A0.99
C8—H8A0.99C21—H21B0.99
C8—H8B0.99C22—O71.427 (3)
C9—O21.445 (2)C22—H22A0.99
C9—C101.504 (3)C22—H22B0.99
C9—H9A0.99C23—O71.419 (3)
C9—H9B0.99C23—C241.494 (3)
C10—O31.429 (3)C23—H23A0.99
C10—H10A0.99C23—H23B0.99
C10—H10B0.99C24—O81.446 (2)
C11—O31.421 (3)C24—H24A0.99
C11—C121.495 (3)C24—H24B0.99
C11—H11A0.99N1—H1C0.90 (3)
C11—H11B0.99N1—H1D0.97 (3)
C12—O41.445 (2)N1—H1A0.97 (3)
C12—H12A0.99N1—H1B0.88 (3)
C12—H12B0.99F1—P11.5938 (15)
C13—C141.381 (3)F2—P11.5949 (14)
C13—O41.383 (2)F3—P11.5758 (15)
C13—C181.409 (3)F4—P11.5998 (14)
C14—C151.396 (3)F5—P11.5789 (15)
C14—H140.95F6—P11.5753 (15)
O8—C1—C2124.16 (19)C17—C18—O5124.86 (19)
O8—C1—C6116.02 (19)C17—C18—C13119.57 (18)
C2—C1—C6119.82 (19)O5—C18—C13115.53 (18)
C1—C2—C3120.3 (2)O5—C19—C20108.30 (17)
C1—C2—H2119.8O5—C19—H19A110
C3—C2—H2119.8C20—C19—H19A110
C4—C3—C2119.9 (2)O5—C19—H19B110
C4—C3—H3120.1C20—C19—H19B110
C2—C3—H3120.1H19A—C19—H19B108.4
C3—C4—C5120.6 (2)O6—C20—C19115.54 (18)
C3—C4—H4119.7O6—C20—H20A108.4
C5—C4—H4119.7C19—C20—H20A108.4
C4—C5—C6120.1 (2)O6—C20—H20B108.4
C4—C5—H5119.9C19—C20—H20B108.4
C6—C5—H5119.9H20A—C20—H20B107.5
O1—C6—C5124.42 (19)O6—C21—C22111.23 (17)
O1—C6—C1116.31 (18)O6—C21—H21A109.4
C5—C6—C1119.3 (2)C22—C21—H21A109.4
O1—C7—C8108.56 (17)O6—C21—H21B109.4
O1—C7—H7A110C22—C21—H21B109.4
C8—C7—H7A110H21A—C21—H21B108
O1—C7—H7B110O7—C22—C21107.73 (18)
C8—C7—H7B110O7—C22—H22A110.2
H7A—C7—H7B108.4C21—C22—H22A110.2
O2—C8—C7115.49 (17)O7—C22—H22B110.2
O2—C8—H8A108.4C21—C22—H22B110.2
C7—C8—H8A108.4H22A—C22—H22B108.5
O2—C8—H8B108.4O7—C23—C24108.98 (17)
C7—C8—H8B108.4O7—C23—H23A109.9
H8A—C8—H8B107.5C24—C23—H23A109.9
O2—C9—C10110.67 (18)O7—C23—H23B109.9
O2—C9—H9A109.5C24—C23—H23B109.9
C10—C9—H9A109.5H23A—C23—H23B108.3
O2—C9—H9B109.5O8—C24—C23109.02 (18)
C10—C9—H9B109.5O8—C24—H24A109.9
H9A—C9—H9B108.1C23—C24—H24A109.9
O3—C10—C9107.83 (19)O8—C24—H24B109.9
O3—C10—H10A110.1C23—C24—H24B109.9
C9—C10—H10A110.1H24A—C24—H24B108.3
O3—C10—H10B110.1H1C—N1—H1D109 (2)
C9—C10—H10B110.1H1C—N1—H1A106 (2)
H10A—C10—H10B108.5H1D—N1—H1A114 (2)
O3—C11—C12108.88 (18)H1C—N1—H1B107 (2)
O3—C11—H11A109.9H1D—N1—H1B111 (2)
C12—C11—H11A109.9H1A—N1—H1B110 (2)
O3—C11—H11B109.9C6—O1—C7116.35 (16)
C12—C11—H11B109.9C8—O2—C9115.79 (16)
H11A—C11—H11B108.3C11—O3—C10111.97 (17)
O4—C12—C11108.60 (16)C13—O4—C12116.32 (15)
O4—C12—H12A110C18—O5—C19115.06 (15)
C11—C12—H12A110C20—O6—C21115.92 (16)
O4—C12—H12B110C23—O7—C22112.34 (16)
C11—C12—H12B110C1—O8—C24115.60 (16)
H12A—C12—H12B108.4F6—P1—F389.39 (11)
C14—C13—O4123.93 (19)F6—P1—F5178.84 (11)
C14—C13—C18119.9 (2)F3—P1—F591.74 (11)
O4—C13—C18116.13 (17)F6—P1—F189.95 (10)
C13—C14—C15119.9 (2)F3—P1—F1179.23 (10)
C13—C14—H14120.1F5—P1—F188.92 (10)
C15—C14—H14120.1F6—P1—F290.85 (9)
C16—C15—C14120.4 (2)F3—P1—F289.38 (9)
C16—C15—H15119.8F5—P1—F288.90 (9)
C14—C15—H15119.8F1—P1—F291.02 (8)
C15—C16—C17119.8 (2)F6—P1—F489.82 (9)
C15—C16—H16120.1F3—P1—F490.76 (8)
C17—C16—H16120.1F5—P1—F490.44 (9)
C18—C17—C16120.4 (2)F1—P1—F488.85 (8)
C18—C17—H17119.8F2—P1—F4179.32 (9)
C16—C17—H17119.8
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O10.88 (3)2.48 (3)3.038 (2)122 (2)
N1—H1A···O20.97 (3)1.91 (3)2.848 (2)163 (2)
N1—H1C···O40.90 (3)2.08 (3)2.973 (2)168 (3)
N1—H1C···O50.90 (3)2.48 (3)3.035 (2)120 (2)
N1—H1D···O60.97 (3)1.90 (3)2.862 (2)168 (2)
N1—H1B···O80.88 (3)2.11 (3)2.977 (3)168 (2)

Experimental details

Crystal data
Chemical formulaNH4+·C24H32O8·PF6
Mr611.51
Crystal system, space groupTriclinic, P1
Temperature (K)123
a, b, c (Å)10.1950 (2), 10.6379 (2), 14.5447 (3)
α, β, γ (°)69.371 (1), 71.536 (1), 89.670 (1)
V3)1390.30 (5)
Z2
Radiation typeMo Kα
µ (mm1)0.19
Crystal size (mm)0.2 × 0.12 × 0.08
Data collection
DiffractometerKappaCCD
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
16366, 6721, 3813
Rint0.044
(sin θ/λ)max1)0.667
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.051, 0.133, 0.97
No. of reflections6721
No. of parameters377
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.64, 0.55

Computer programs: COLLECT (Nonius, 1997-2000), HKL SCALEPACK (Otwinowski & Minor 1997), HKL DENZO and SCALEPACK (Otwinowski & Minor 1997), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEP-3 for Windows (Farrugia, 1997), WinGX (Farrugia, 1999).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O10.88 (3)2.48 (3)3.038 (2)122 (2)
N1—H1A···O20.97 (3)1.91 (3)2.848 (2)163 (2)
N1—H1C···O40.90 (3)2.08 (3)2.973 (2)168 (3)
N1—H1C···O50.90 (3)2.48 (3)3.035 (2)120 (2)
N1—H1D···O60.97 (3)1.90 (3)2.862 (2)168 (2)
N1—H1B···O80.88 (3)2.11 (3)2.977 (3)168 (2)
 

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