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The title bimolecular compound, C4H5N3·C21H18O2, construc­ted from 2-amino­pyrimidine and 3,3,3-triphenyl­propanoic acid, forms a tetra­molecular hydrogen-bonded motif via O—H...N, N—H...O and N—H...N contacts. This aggregate organizes to give crystal-packing motifs with hydro­philic and hydro­phobic regions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270107045799/gd3144sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270107045799/gd3144Isup2.hkl
Contains datablock I

CCDC reference: 669175

Comment top

Over the past decade, the field of supramolecular chemistry has emerged as a significant contributor to the broad area of materials science owing in part to advances in decoding the structural features responsible for molecular cohesion. While much of this progress has been documented in the literature, many areas still require attention before prediction of complex high-order motifs can be successfully achieved with regularity. To this end, two areas that continue to prove useful for understanding the fundamental principles of supramolecular chemistry include new synthon identification and thorough assessment of the recognition profiles of known molecular contacts.

The packing tendencies of Ph3X groups (X = C or P; Scudder & Dance, 1998, 2000; Steiner, 2000) and their use in practical applications (Garcia-Garibay, 2005; Jarowski et al., 2007) have been reported in the literature. Crystallographic studies of molecules containing Ph3X groups show several salient packing motifs, such as the sixfold (6PE) and fourfold (4PE) phenyl embraces (Scudder & Dance, 2000). Although these phenyl embrace motifs have been exploited as a tool for constructing supramolecular assemblies, extending their use to include additional molecular contacts (e.g. hydrogen bonds) has seen less attention. It has been reported by Steiner (1999) that 3,3,3-triphenylpropanoic acid crystallizes with molecules organized into linear motifs via a combination of carboxyl–carboxyl and 6PE interactions. We wondered if the observed linear assemblage could be transferred and extended by cocrystallizing the triphenylpropanoic acid with a complementary hydrogen-bond spacer such as 2-aminopyrimidine.

Cocrystallization of 3,3,3-triphenylpropanoic acid and 2-aminopyrimidine produced the expected bimolecular compound (I); the C—O distances in the acid component (Table 1) are consistent with the location of the hydroxyl H atom, as deduced from the refinement. The asymmetric unit of (I) shows the formation of a hydrogen-bonded R22(8) motif involving both 2-aminopyrimidine and 3,3,3-triphenylpropanoic acid components (Fig. 1). As anticipated, this molecular assemblage is further linked to give a tetrameric motif by use of two additional inversion-related N—H···N hydrogen bonds (Table 2; Lynch et al., 1998). Unlike the structure of 3,3,3-triphenylpropanoic acid, the terminal triphenylmethyl (TPM) groups of our tetrameric unit lack participation in 6PE interactions. Rather, the TPM groups of (I) assemble by use of van der Waals contacts to give hydrophobic and hydrophilic regions (Fig. 2)

The most effective packing of 6PE motifs involves a concerted cycle of six local edge-to-face Ph···Ph interactions. Compounds that align in this manner possess TPM conformations that approach a rotor with pseudo-threefold symmetry. This structural feature is easily quantified by assessing the twist of the three phenyl groups around their C—Cipso bond. Cases that exhibit rotor conformations show similar twist angles of the phenyl groups. For (I), these torsion angles (Table 1) differ markedly and they are consistent with the previously described `flipper' conformation (Scudder & Dance, 2000). Although this arrangement of phenyl groups is capable of forming several phenyl embrace motifs (e.g. 6PE and 4PE), (I) crystallizes with phenyl groups aligned in a skewed 4PE arrangement. In conclusion, this study highlights the successful use of building blocks (i.e. 3,3,3-triphenylpropanoic acid and 2-aminopyrimidine) that form the expected hydrogen-bonded tetramolecular unit with additional, less well defined, phenyl embrace contacts for organizing the supramolecular assembly.

Related literature top

For related literature, see: Garcia-Garibay (2005); Jarowski et al. (2007); Lynch et al. (1998); Scudder & Dance (1998, 2000); Steiner (1999, 2000).

Experimental top

Single crystals of (I) were prepared by slow evaporation at room temperature of an acetone solution containing equimolar quantities of 2-aminopyrimidine and 3,3,3-triphenylpropionic acid (m.p. 383–384 K).

Refinement top

H atoms bonded to N or O atoms were refined without constraint. All other H atoms were included as riding atoms in geometrically idealized positions [C—H = 0.93–0.97 Å and Uiso(H) = 1.2Ueq(C)].

Computing details top

Data collection: XSCANS (Bruker, 1999); cell refinement: XSCANS (Bruker, 1999); data reduction: XPREP (Bruker, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: X-SEED (Barbour, 2001).

Figures top
[Figure 1] Fig. 1. A molecular diagram of (I), showing the labeling scheme, asymmetric unit (50% probability displacement ellipsoids) and hydrogen bonded tetramer. [Symmetry code: (i) −x + 1, −y + 2, −z + 1.]
[Figure 2] Fig. 2. A projection of the unit-cell contents of (I), showing hydrophobic and hydrophilic crystal regions. For the sake of clarity, H atoms have been omitted.
2-Aminopyrimidine–3,3,3-triphenylpropanoic acid (1/1) top
Crystal data top
C4H5N3·C21H18O2F(000) = 840
Mr = 397.46Dx = 1.278 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54178 Å
Hall symbol: -P 2ybcCell parameters from 23 reflections
a = 20.590 (2) Åθ = 53.3–54.4°
b = 9.5109 (8) ŵ = 0.66 mm1
c = 10.640 (2) ÅT = 298 K
β = 97.518 (15)°Transparent plate, colourless
V = 2065.6 (5) Å30.45 × 0.42 × 0.20 mm
Z = 4
Data collection top
Bruker P4
diffractometer
2048 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.043
Graphite monochromatorθmax = 61.8°, θmin = 4.3°
θ//2θ scansh = 2323
Absorption correction: analytical
(XPREP; Bruker, 2001)
k = 101
Tmin = 0.757, Tmax = 0.880l = 112
4193 measured reflections3 standard reflections every 97 reflections
3144 independent reflections intensity decay: none
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)] = 0.057Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.149H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0693P)2 + 0.2673P]
where P = (Fo2 + 2Fc2)/3
3144 reflections(Δ/σ)max < 0.001
278 parametersΔρmax = 0.17 e Å3
0 restraintsΔρmin = 0.23 e Å3
Crystal data top
C4H5N3·C21H18O2V = 2065.6 (5) Å3
Mr = 397.46Z = 4
Monoclinic, P21/cCu Kα radiation
a = 20.590 (2) ŵ = 0.66 mm1
b = 9.5109 (8) ÅT = 298 K
c = 10.640 (2) Å0.45 × 0.42 × 0.20 mm
β = 97.518 (15)°
Data collection top
Bruker P4
diffractometer
2048 reflections with I > 2σ(I)
Absorption correction: analytical
(XPREP; Bruker, 2001)
Rint = 0.043
Tmin = 0.757, Tmax = 0.880θmax = 61.8°
4193 measured reflections3 standard reflections every 97 reflections
3144 independent reflections intensity decay: none
Refinement top
R[F2 > 2σ(F2)] = 0.0570 restraints
wR(F2) = 0.149H atoms treated by a mixture of independent and constrained refinement
S = 1.04Δρmax = 0.17 e Å3
3144 reflectionsΔρmin = 0.23 e Å3
278 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.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.33412 (10)0.5739 (2)0.5844 (2)0.0648 (7)
O20.28867 (11)0.7839 (2)0.5572 (3)0.0736 (8)
N10.42512 (12)0.6656 (3)0.4299 (3)0.0633 (8)
N20.41846 (16)0.8917 (4)0.5024 (4)0.0878 (11)
N30.51321 (15)0.8273 (4)0.4269 (3)0.0835 (10)
C20.45260 (16)0.7924 (4)0.4509 (3)0.0620 (9)
C40.5445 (2)0.7287 (5)0.3695 (4)0.0872 (13)
H40.58650.74920.35150.105*
C50.51947 (18)0.6004 (5)0.3354 (4)0.0799 (12)
H50.54160.53570.29110.094 (14)*
C60.45898 (17)0.5731 (4)0.3710 (4)0.0765 (11)
H60.44070.48490.35280.092*
C110.29037 (14)0.6687 (3)0.6065 (3)0.0495 (8)
C120.24507 (14)0.6278 (3)0.6995 (3)0.0462 (8)
H12A0.21530.70560.70650.055*
H12B0.27100.61630.78170.055*
C130.20315 (12)0.4920 (3)0.6707 (2)0.0365 (6)
C210.24573 (12)0.3580 (3)0.6781 (3)0.0354 (6)
C220.29166 (13)0.3375 (3)0.7856 (3)0.0459 (7)
H220.30130.41110.84250.055*
C230.32285 (14)0.2099 (4)0.8088 (3)0.0515 (8)
H230.35280.19830.88140.062*
C240.31003 (14)0.0997 (3)0.7257 (3)0.0490 (8)
H240.33060.01350.74240.059*
C250.26660 (14)0.1182 (3)0.6180 (3)0.0469 (8)
H250.25850.04480.56040.056*
C260.23440 (13)0.2468 (3)0.5940 (3)0.0409 (7)
H260.20500.25780.52060.049*
C310.15745 (12)0.4691 (3)0.7737 (3)0.0387 (7)
C320.15060 (14)0.5643 (3)0.8695 (3)0.0489 (8)
H320.17440.64760.87420.059*
C330.10850 (16)0.5371 (4)0.9589 (3)0.0609 (9)
H330.10430.60251.02230.073*
C340.07316 (15)0.4148 (4)0.9542 (3)0.0594 (10)
H340.04560.39641.01480.071*
C350.07881 (14)0.3191 (4)0.8589 (3)0.0545 (9)
H350.05470.23620.85460.065*
C360.12032 (13)0.3465 (3)0.7700 (3)0.0449 (7)
H360.12360.28130.70590.054*
C410.16147 (12)0.5175 (3)0.5409 (3)0.0370 (6)
C420.18735 (13)0.5039 (3)0.4278 (3)0.0418 (7)
H420.23040.47340.42940.050*
C430.15100 (14)0.5343 (3)0.3129 (3)0.0493 (8)
H430.16970.52400.23850.059*
C440.08718 (15)0.5797 (3)0.3073 (3)0.0528 (8)
H440.06230.59870.22980.063*
C450.06106 (14)0.5964 (3)0.4189 (3)0.0514 (8)
H450.01830.62860.41670.062*
C460.09744 (13)0.5661 (3)0.5344 (3)0.0432 (7)
H460.07880.57830.60870.052*
H1C0.360 (2)0.610 (5)0.522 (4)0.134 (18)*
H2A0.3782 (19)0.874 (4)0.521 (3)0.087 (13)*
H2B0.439 (2)0.979 (6)0.517 (5)0.15 (2)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0507 (12)0.0464 (13)0.1030 (19)0.0066 (11)0.0322 (13)0.0108 (13)
O20.0684 (15)0.0384 (13)0.121 (2)0.0018 (11)0.0374 (15)0.0146 (14)
N10.0466 (15)0.0569 (18)0.088 (2)0.0135 (14)0.0129 (15)0.0018 (17)
N20.069 (2)0.069 (2)0.134 (3)0.0219 (19)0.045 (2)0.013 (2)
N30.0678 (19)0.079 (2)0.111 (3)0.0307 (18)0.0421 (19)0.006 (2)
C20.0490 (18)0.068 (2)0.071 (2)0.0192 (19)0.0119 (17)0.004 (2)
C40.068 (3)0.102 (3)0.098 (3)0.025 (3)0.035 (2)0.002 (3)
C50.059 (2)0.088 (3)0.096 (3)0.009 (2)0.023 (2)0.010 (3)
C60.055 (2)0.070 (3)0.104 (3)0.009 (2)0.009 (2)0.011 (2)
C110.0392 (16)0.0361 (18)0.074 (2)0.0056 (14)0.0105 (15)0.0032 (17)
C120.0436 (16)0.0379 (16)0.0581 (19)0.0024 (13)0.0105 (15)0.0032 (15)
C130.0368 (14)0.0353 (16)0.0383 (15)0.0005 (12)0.0082 (12)0.0008 (13)
C210.0338 (14)0.0359 (16)0.0377 (15)0.0008 (12)0.0085 (12)0.0019 (13)
C220.0415 (16)0.0510 (19)0.0451 (18)0.0034 (15)0.0046 (14)0.0044 (15)
C230.0416 (16)0.064 (2)0.0477 (19)0.0091 (16)0.0022 (14)0.0063 (17)
C240.0436 (16)0.0437 (19)0.061 (2)0.0066 (14)0.0109 (16)0.0075 (16)
C250.0511 (17)0.0361 (16)0.0555 (19)0.0013 (14)0.0152 (16)0.0027 (15)
C260.0412 (16)0.0397 (17)0.0421 (16)0.0003 (13)0.0066 (13)0.0022 (14)
C310.0348 (14)0.0425 (17)0.0391 (16)0.0054 (13)0.0063 (12)0.0008 (14)
C320.0554 (18)0.0477 (18)0.0447 (17)0.0084 (15)0.0112 (15)0.0001 (15)
C330.074 (2)0.068 (2)0.0446 (19)0.020 (2)0.0215 (17)0.0003 (18)
C340.055 (2)0.073 (3)0.054 (2)0.0180 (19)0.0250 (17)0.0178 (19)
C350.0457 (17)0.055 (2)0.066 (2)0.0046 (16)0.0187 (16)0.0141 (18)
C360.0418 (15)0.0458 (18)0.0489 (18)0.0000 (14)0.0126 (14)0.0030 (15)
C410.0390 (14)0.0324 (15)0.0410 (16)0.0022 (12)0.0098 (12)0.0017 (13)
C420.0375 (14)0.0419 (17)0.0474 (18)0.0033 (13)0.0109 (14)0.0006 (15)
C430.0586 (19)0.0492 (19)0.0423 (18)0.0050 (16)0.0146 (15)0.0028 (15)
C440.0539 (18)0.058 (2)0.0449 (18)0.0061 (16)0.0015 (15)0.0074 (16)
C450.0399 (15)0.057 (2)0.057 (2)0.0073 (15)0.0052 (15)0.0078 (17)
C460.0388 (15)0.0482 (18)0.0440 (17)0.0046 (14)0.0111 (13)0.0008 (15)
Geometric parameters (Å, º) top
O1—C111.318 (3)C24—C251.369 (4)
O1—H1C0.96 (5)C24—H240.9300
O2—C111.213 (4)C25—C261.398 (4)
N1—C21.338 (4)C25—H250.9300
N1—C61.329 (4)C26—H260.9300
N2—C21.336 (5)C31—C321.384 (4)
N2—H2A0.89 (4)C31—C361.393 (4)
N2—H2B0.94 (5)C32—C331.392 (4)
N3—C21.348 (4)C32—H320.9300
N3—C41.331 (5)C33—C341.370 (5)
C4—C51.355 (6)C33—H330.9300
C4—H40.9300C34—C351.378 (4)
C5—C61.373 (5)C34—H340.9300
C5—H50.9300C35—C361.381 (4)
C6—H60.9300C35—H350.9300
C11—C121.496 (4)C36—H360.9300
C12—C131.562 (4)C41—C421.385 (4)
C12—H12A0.9700C41—C461.390 (3)
C12—H12B0.9700C42—C431.378 (4)
C13—C211.542 (4)C42—H420.9300
C13—C311.550 (4)C43—C441.377 (4)
C13—C411.547 (4)C43—H430.9300
C21—C261.385 (4)C44—C451.375 (4)
C21—C221.400 (4)C44—H440.9300
C22—C231.380 (4)C45—C461.383 (4)
C22—H220.9300C45—H450.9300
C23—C241.374 (4)C46—H460.9300
C23—H230.9300
C11—O1—H1C109 (3)C25—C24—H24120.3
C2—N1—C6116.0 (3)C24—C25—C26120.5 (3)
N1—C2—N2118.1 (3)C24—C25—H25119.8
C2—N2—H2A121 (3)C26—C25—H25119.8
C2—N2—H2B116 (3)C21—C26—C25121.0 (3)
H2A—N2—H2B123 (4)C21—C26—H26119.5
C2—N3—C4115.4 (3)C25—C26—H26119.5
N2—C2—N3117.0 (3)C13—C31—C32124.0 (3)
N1—C2—N3124.9 (4)C13—C31—C36118.6 (2)
N3—C4—C5124.6 (4)C32—C31—C36117.4 (3)
N3—C4—H4117.7C33—C32—C31120.9 (3)
C5—C4—H4117.7C31—C32—H32119.5
C4—C5—C6115.0 (4)C33—C32—H32119.5
C4—C5—H5122.5C32—C33—C34120.6 (3)
C6—C5—H5122.5C32—C33—H33119.7
N1—C6—C5123.7 (4)C34—C33—H33119.7
N1—C6—H6118.1C33—C34—C35119.5 (3)
C5—C6—H6118.1C33—C34—H34120.3
O1—C11—C12116.1 (3)C35—C34—H34120.3
O1—C11—O2121.5 (3)C34—C35—C36119.9 (3)
O2—C11—C12122.4 (3)C34—C35—H35120.0
C11—C12—C13117.5 (2)C36—C35—H35120.0
C11—C12—H12A107.9C31—C36—C35121.7 (3)
C11—C12—H12B107.9C31—C36—H36119.2
C13—C12—H12A107.9C35—C36—H36119.2
C13—C12—H12B107.9C42—C41—C46117.3 (3)
H12A—C12—H12B107.2C13—C41—C42122.0 (2)
C12—C13—C21112.2 (2)C13—C41—C46120.6 (2)
C12—C13—C31110.4 (2)C41—C42—C43121.7 (3)
C12—C13—C41105.8 (2)C41—C42—H42119.2
C21—C13—C31104.0 (2)C43—C42—H42119.2
C21—C13—C41114.9 (2)C42—C43—C44120.6 (3)
C31—C13—C41109.6 (2)C42—C43—H43119.7
C13—C21—C22118.4 (2)C44—C43—H43119.7
C13—C21—C26123.5 (2)C43—C44—C45118.5 (3)
C22—C21—C26117.4 (3)C43—C44—H44120.7
C21—C22—C23121.2 (3)C45—C44—H44120.7
C21—C22—H22119.4C44—C45—C46121.0 (3)
C23—C22—H22119.4C44—C45—H45119.5
C22—C23—C24120.6 (3)C46—C45—H45119.5
C24—C23—H23119.7C41—C46—C45120.9 (3)
C22—C23—H23119.7C41—C46—H46119.6
C23—C24—C25119.3 (3)C45—C46—H46119.6
C23—C24—H24120.3
C6—N1—C2—N2175.7 (4)C41—C13—C31—C32110.1 (3)
C6—N1—C2—N36.0 (6)C12—C13—C31—C326.1 (4)
C4—N3—C2—N2176.5 (4)C21—C13—C31—C3654.1 (3)
C4—N3—C2—N15.1 (6)C41—C13—C31—C3669.2 (3)
C2—N1—C6—C51.7 (6)C12—C13—C31—C36174.6 (2)
N1—C6—C5—C42.7 (6)C36—C31—C32—C330.5 (4)
C2—N3—C4—C50.1 (7)C13—C31—C32—C33179.9 (3)
C6—C5—C4—N33.7 (7)C31—C32—C33—C340.3 (5)
O2—C11—C12—C13125.1 (3)C32—C33—C34—C350.9 (5)
O1—C11—C12—C1357.2 (4)C33—C34—C35—C360.6 (5)
C11—C12—C13—C2166.7 (3)C34—C35—C36—C310.3 (4)
C11—C12—C13—C4159.3 (3)C32—C31—C36—C350.8 (4)
C11—C12—C13—C31177.9 (2)C13—C31—C36—C35179.7 (3)
C41—C13—C21—C2619.2 (4)C21—C13—C41—C4245.8 (3)
C31—C13—C21—C26100.6 (3)C31—C13—C41—C42162.4 (2)
C12—C13—C21—C26140.0 (3)C12—C13—C41—C4278.5 (3)
C41—C13—C21—C22171.1 (2)C21—C13—C41—C46139.3 (3)
C31—C13—C21—C2269.1 (3)C31—C13—C41—C4622.6 (3)
C12—C13—C21—C2250.3 (3)C12—C13—C41—C4696.4 (3)
C26—C21—C22—C232.0 (4)C46—C41—C42—C431.3 (4)
C13—C21—C22—C23168.4 (3)C13—C41—C42—C43176.4 (3)
C21—C22—C23—C240.7 (4)C41—C42—C43—C440.1 (5)
C22—C23—C24—C251.0 (4)C42—C43—C44—C451.1 (5)
C23—C24—C25—C261.5 (4)C43—C44—C45—C461.1 (5)
C22—C21—C26—C251.5 (4)C44—C45—C46—C410.1 (5)
C13—C21—C26—C25168.3 (2)C42—C41—C46—C451.3 (4)
C24—C25—C26—C210.2 (4)C13—C41—C46—C45176.5 (3)
C21—C13—C31—C32126.6 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1C···N10.96 (5)1.85 (5)2.790 (3)166 (4)
N2—H2A···O20.89 (4)2.11 (4)2.990 (4)167 (4)
N2—H2B···N3i0.94 (5)2.13 (5)3.068 (5)173 (4)
Symmetry code: (i) x+1, y+2, z+1.

Experimental details

Crystal data
Chemical formulaC4H5N3·C21H18O2
Mr397.46
Crystal system, space groupMonoclinic, P21/c
Temperature (K)298
a, b, c (Å)20.590 (2), 9.5109 (8), 10.640 (2)
β (°) 97.518 (15)
V3)2065.6 (5)
Z4
Radiation typeCu Kα
µ (mm1)0.66
Crystal size (mm)0.45 × 0.42 × 0.20
Data collection
DiffractometerBruker P4
diffractometer
Absorption correctionAnalytical
(XPREP; Bruker, 2001)
Tmin, Tmax0.757, 0.880
No. of measured, independent and
observed [I > 2σ(I)] reflections
4193, 3144, 2048
Rint0.043
θmax (°)61.8
(sin θ/λ)max1)0.572
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.057, 0.149, 1.04
No. of reflections3144
No. of parameters278
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.17, 0.23

Computer programs: XSCANS (Bruker, 1999), XPREP (Bruker, 2001), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), X-SEED (Barbour, 2001).

Selected geometric parameters (Å, º) top
O1—C111.318 (3)N3—C21.348 (4)
O2—C111.213 (4)N3—C41.331 (5)
N1—C21.338 (4)C4—C51.355 (6)
N1—C61.329 (4)C5—C61.373 (5)
N2—C21.336 (5)
C12—C13—C21—C2250.3 (3)C12—C13—C41—C4278.5 (3)
C12—C13—C31—C326.1 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1C···N10.96 (5)1.85 (5)2.790 (3)166 (4)
N2—H2A···O20.89 (4)2.11 (4)2.990 (4)167 (4)
N2—H2B···N3i0.94 (5)2.13 (5)3.068 (5)173 (4)
Symmetry code: (i) x+1, y+2, z+1.
 

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