research communications\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890

Crystal structure and Hirshfeld surface analysis of (E)-2-[(anthracen-9-yl­methyl­­idene)amino]-4-nitro­aniline

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aLaboratory of Applied Organic Chemistry, Sidi Mohamed Ben Abdellah University, Faculty Of Science And Technology, Road Immouzer, BP 2202 Fez, Morocco, bDepartment of Chemistry, Tulane University, New Orleans, LA 70118, USA, cDepartment of Physics, Hacettepe University, 06800 Beytepe, Ankara, Türkiye, dUniversity of Lille, CNRS, UAR 3290, MSAP, Miniaturization for Synthesis, Analysis and Proteomics, 59000 Lille, France, and eLaboratory of Heterocyclic Organic Chemistry, Pharmacochemistry Competence Center, Av. Ibn Battouta, BP 1014, Faculty of Sciences, Mohammed V University, in Rabat, Morocco
*Correspondence e-mail: [email protected]

Edited by D. R. Manke, University of Massachusetts Dartmouth, USA (Received 16 October 2025; accepted 30 January 2026; online 5 February 2026)

The title compound, C21H15N3O2, contains a nitro­aniline ring and an anthracene ring system bridged over the methyl­ene amino group. The anthracene ring system is essentially planar with an r.m.s. deviation of 0.03 (2) Å and it is oriented at a dihedral angle of 79.70 (5)° with respect to nitro­aniline ring. There is an intra­molecular N—H⋯N hydrogen bond between N atoms of nitro­aniline ring and amino group. In the crystal, N—H—O hydrogen bonds link the mol­ecules into infinite chains along the b-axis direction. ππ stacking inter­actions between the nitro­aniline rings of adjacent mol­ecules with centroid-to-centroid distance of 3.7682 (2) Å and C—H⋯π(ring) inter­actions may help to consolidate the three-dimensional architecture. A Hirshfeld surface analysis indicates that the most important contributions for the crystal packing are from H⋯H (35.5%), H⋯C/C⋯H (33.7%) and H⋯O/O⋯H (18.3%) inter­actions.

1. Chemical context

The Schiff base family is a class of organic compounds characterized by the presence of an imine group (Moss et al., 1995View full citation; Schiff, 1864View full citation). Their structural features confer notable reactivity and versatility, making them valuable scaffolds with numerous applications, such as fluorescent chemosensors (Udhayakumari et al., 2020View full citation), as catalysts (Boghaei et al., 2002View full citation), in water treatment (Khan et al., 2019View full citation) and as corrosion inhibitors (Ashassi-Sorkhabi et al., 2005View full citation; Verma & Quraishi, 2021View full citation). In medicinal chemistry, numerous investigations have also highlighted their broad spectrum of activities (Hameed et al., 2017View full citation; Mushtaq et al., 2024View full citation; Nidhi et al., 2025View full citation; Younus et al., 2023View full citation), notably as anti-microbial (Barakat et al., 2025View full citation), anti­cancer (Uddin et al., 2020View full citation), anti-inflammatory (Murtaza et al., 2017View full citation), anti­viral (Azzouzi et al., 2024View full citation), anti-diabetic (Adalat et al., 2022View full citation), and anti­oxidant (Madi et al., 2021View full citation) agents. Particular focus on derivatives incorporating nitro­benzene or anthracene moieties has demonstrated significant activities (Aravindan et al., 2021View full citation; Bai et al., 2017View full citation; Gümüş et al., 2020View full citation; Kraicheva et al., 2012View full citation; Mahmoud et al., 2018View full citation). Prompted by these findings, the title compound was synthesized by the condensation of anthracene-9-carbaldehyde and 4-nitro­benzene-1,2-di­amine, giving a new Schiff compound containing both anthracene and nitro­benzene moieties. Its synthesis and mol­ecular and crystal structures are described here, along with the results of a Hirshfeld surface analysis.

[Scheme 1]

2. Structural commentary

The title compound, (I)[link], contains an nitro­aniline ring (A, C1–C6) and an anthracene ring system (B, C8–C21) bridged over the methyl­ene amino group (Fig. 1[link]). The anthracene ring system, consisting of three fused benzene rings, is essentially planar with r.m.s. deviation of 0.03 (2) Å and it is oriented at a dihedral angle of 79.70 (5)° with respect to nitro­aniline ring A. Atoms N1, N2, N3, O1A and O1B are 0.0345 (18), 0.0135 (20), 0.0168 (16), 0.1040 (17) and −0.0276 (18) Å, respectively, away from the best least-squares plane through ring A. Thus, they are nearly coplanar. There is an intra­molecular N–H⋯N hydrogen bond (Table 1[link]) between the N atoms of ring A and the amino group. No unusual bond lengths or inter­bond angles are observed.

Table 1
Hydrogen-bond geometry (Å, °)

Cg1 is the centroid of the C1–C6 ring.

D—H⋯A D—H H⋯A DA D—H⋯A
N2—H2A⋯O1Bi 0.88 2.07 2.939 (2) 168
N2—H2B⋯N3 0.88 2.31 2.672 (2) 104
C19—H19⋯Cg1ii 0.95 2.65 3.492 (2) 149
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation.
[Figure 1]
Figure 1
The mol­ecular structure of the title compound (I)[link] showing 50% probability ellipsoids.

3. Supra­molecular features

In the crystal, N—H—O hydrogen bonds (Table 1[link]) link the mol­ecules into infinite chains along the b-axis direction (Fig. 2[link]). ππ stacking inter­actions between the A rings [centroid-to-centroid distance = 3.7682 (2) Å, α = 0.02 (10)° and slippage = 1.375 Å] of adjacent mol­ecules and C—H⋯π(ring) inter­actions (Table 1[link]) may help to consolidate the three-dimensional architecture.

[Figure 2]
Figure 2
A partial packing diagram of the title compound (I)[link]. The intra­molecular N—H⋯N and inter­molecular N—H⋯O hydrogen bonds are shown as dashed lines. Hydrogen atoms not involved in these inter­actions have been omitted for clarity.

4. Hirshfeld surface analysis

A Hirshfeld surface (HS) analysis was carried out using Crystal Explorer 17.5 (Spackman et al., 2021View full citation) to visualize the inter­molecular inter­actions in the crystal. Fig. 3[link] shows the contact distances where the bright-red spots correspond to the respective donors and/or acceptors. The white surfaces and the red and blue areas indicate contacts with distances equal, shorter and longer, respectively, than the van der Waals radii (Table 2[link]). The ππ stacking and C—H⋯π(ring) inter­actions are shown in Fig. 4[link]a and 4b by the presence of the adjacent red and blue triangles and the red π-holes, respectively. According to the two-dimensional fingerprint plots (McKinnon et al., 2007View full citation), the H⋯H, H⋯C/C⋯H and H⋯O/O⋯H contacts make the most significant contributions to the HS, at 35.5%, 33.7% and 18.3%, respectively (Table 2[link] and Fig. 5[link]).

Table 2
Selected interatomic distances (Å)

N2⋯O1Bi 2.939 (2) C6⋯H7 2.71
O1A⋯H6 2.44 C7⋯H20 2.66
O1B⋯H2 2.41 C7⋯H6 2.81
H2A⋯O1Bi 2.07 C7⋯H10 2.58
N2⋯N3 2.672 (2) C10⋯H7 2.75
N3⋯C20 2.913 (3) H6⋯H7 2.39
N3⋯H2B 2.31 H7⋯H10 2.19
N3⋯H20 2.35    
Symmetry code: (i) Mathematical equation.
[Figure 3]
Figure 3
View of the three-dimensional Hirshfeld surface of the title compound (I)[link] plotted over dnorm.
[Figure 4]
Figure 4
The shape-index surface showing two orientations for (a) ππ stacking and (b) C—H⋯π(ring) inter­actions.
[Figure 5]
Figure 5
The two-dimensional fingerprint plots of the title compound (I)[link], showing (a) all inter­actions, and delineated into (b) H⋯H, (c) H⋯C/C⋯H, (d) H⋯O/O⋯H, (e) C⋯C, (f) H⋯N/N⋯H, (g) C⋯N/N⋯C, (h) C⋯O/O⋯C and (i) N⋯O/O⋯N inter­actions. The di and de values are the closest inter­nal and external distances (in Å) from given points on the Hirshfeld surface.

5. Database survey

A search of the Cambridge Structural Database (CSD, updated September 2025; Groom et al., 2016View full citation) identified seven compounds with structural similarity to the target compound (E)-2-[(anthracen-9-yl­methyl­ene)amino]-4-nitro­aniline. Structures I to VI (CSD codes: RIRMAH01, LIJQII, WEFBAM, WAZWAX, WAZVUQ and WAZVOK; Geiger & Parsons, 2014View full citation; Goettler & Hamaker, 2022View full citation; Dalapati et al., 2012aView full citation,bView full citation) all possess a nitro­benzene ring but do not correspond to Schiff bases. They are distinguished by the nature of their substituents (methyl, phenyl or imidazo[1,2-a]pyridin-2-ylmethyl groups) and the possible presence of solvation mol­ecules or anions (H2O, H2PO4, HSO4, tetra-n-butyl­ammonium). These differences reflect the structural flexibility and the various supra­molecular organizations that the nitro­benzene skeleton can adopt. On the other hand, compound VII [CSD refcode: SUYSAH, N2-(4-chloro­benzyl­idene)-4-nitro­benzene-1,2-di­amine; Farag et al., 2010View full citation] turns out to be the closest structural analogue of the studied compound and shares the same basic Schiff mol­ecular framework formed by the condensation of a 1,2-di­amine derivative and an aromatic aldehyde, as well as a similar electronic arrangement around the azomethine group (–CH=N–). This analysis highlights the structural consistency of the target compound with the analogues listed in the CSD, while highlighting its originality linked to the presence of the anthracene fragment, likely to influence its electronic and ππ stacking properties in the solid state.

[Scheme 2]

6. Synthesis and crystallization

In a flask, 0.4 g (2.61 mmol) of 4-nitro­benzene-1,2-di­amine was stirred into 20 mL of methanol at 323 K until it was completely dissolved. Then, 0.53 g (2.61 mmol) of anthracene-9-carbaldehyde was added in small portions, with the mixture being warmed to reflux. An orange precipitate formed after 1 h, and the reaction was monitored by TLC until the starting materials were consumed entirely (3 h). The mixture was then cooled to ambient temperature, and the precipitate was collected by filtration. It was washed three times (10 mL) with methanol and dried at 323 K to yield a pure powder. The product was characterized by 1H and 13C NMR, IR and UV-Vis spectroscopy. The slow evaporation of a 2:1 (v/v) mixture of ethyl acetate and methanol was used to obtain single crystals. C21H15N3O2 ; Colour: Orange; Yield: 98.5%, Rf = 0.72 (ethyl acetate/hexa­ne: 1/1), Melting Point: 512.9 K; 1H NMR (DMSO-d6, 300 MHz): δ (ppm) 6.62 (s, 2H, NH2), 9.95 (s, 1H, –CH=N–), 8.81 (m, 3H, HAr), 8.19 (m, 3H, HAr), 8.02 (d, 1H, 3JH–H = 9 Hz, HAr), 7.62 (m, 4H, HAr), 6.89 (d, 1H, 3JH–H = 9 Hz, HAr); 13C NMR (DMSO-d6, 75 MHz): δ (ppm) 127.62, 130.77, 131.30, 136.72, 151.16 (Cq), 160.35 (–CH=N–), 113.29, 114.20, 124.93, 125.53, 126.1, 127.97, 129.40, 131.33 (CAr); FT-IR (cm−1): 3450, 3400 (N—H stretching, –NH2), 3100, 3000 (aromatic C—H stretching), 1650 (C=N stretching, imine), 1500 (C=C stretching, aromatic ring); UV-Vis (DMSO), λmax (nm): 310, 430, 480.

7. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 3[link]. The hydrogen-atom positions were calculated geometrically at N—H = 0.88 Å and C—H = 0.95 Å and refined using a riding model with Uiso(H) = 1.2 × Ueq(N, C).

Table 3
Experimental details

Crystal data
Chemical formula C21H15N3O2
Mr 341.36
Crystal system, space group Monoclinic, P21/c
Temperature (K) 120
a, b, c (Å) 12.8213 (9), 15.7634 (9), 8.3763 (5)
β (°) 107.140 (7)
V3) 1617.72 (18)
Z 4
Radiation type Cu Kα
μ (mm−1) 0.75
Crystal size (mm) 0.1 × 0.05 × 0.03
 
Data collection
Diffractometer XtaLAB Synergy R, DW system, HyPix
Absorption correction Multi-scan (CrysAlis PRO; Rigaku OD, 2022View full citation)
Tmin, Tmax 0.419, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 38890, 2880, 2609
Rint 0.094
(sin θ/λ)max−1) 0.598
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.053, 0.140, 1.07
No. of reflections 2880
No. of parameters 235
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.25, −0.28
Computer programs: CrysAlis PRO (Rigaku OD, 2022View full citation), SHELXT2018/2 (Sheldrick, 2015aView full citation), SHELXL2018/3 (Sheldrick, 2015bView full citation) and OLEX2 (Dolomanov et al., 2009View full citation).

Supporting information


Computing details top

(E)-2-[(Anthracen-9-ylmethylidene)amino]-4-nitroaniline top
Crystal data top
C21H15N3O2F(000) = 712
Mr = 341.36Dx = 1.402 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54184 Å
a = 12.8213 (9) ÅCell parameters from 19910 reflections
b = 15.7634 (9) Åθ = 3.6–66.6°
c = 8.3763 (5) ŵ = 0.75 mm1
β = 107.140 (7)°T = 120 K
V = 1617.72 (18) Å3Prism, orange
Z = 40.1 × 0.05 × 0.03 mm
Data collection top
XtaLAB Synergy R, DW system, HyPix
diffractometer
2880 independent reflections
Radiation source: Rotating-anode X-ray tube, Rigaku (Cu) X-ray Source2609 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.094
Detector resolution: 10.0000 pixels mm-1θmax = 67.1°, θmin = 3.6°
ω scansh = 1515
Absorption correction: multi-scan
(CrysAlisPro; Rigaku OD, 2022)
k = 1818
Tmin = 0.419, Tmax = 1.000l = 99
38890 measured reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.053H-atom parameters constrained
wR(F2) = 0.140 w = 1/[σ2(Fo2) + (0.0631P)2 + 1.1761P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
2880 reflectionsΔρmax = 0.25 e Å3
235 parametersΔρmin = 0.28 e Å3
0 restraints
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
O1A0.11419 (12)0.33297 (9)0.7317 (2)0.0445 (4)
O1B0.01412 (13)0.37615 (10)0.8334 (2)0.0488 (4)
N30.25699 (13)0.60375 (9)0.5409 (2)0.0288 (4)
N10.05785 (14)0.39013 (11)0.7645 (2)0.0360 (4)
N20.12391 (14)0.72245 (11)0.5991 (3)0.0419 (5)
H2A0.0824330.7636310.6171690.050*
H2B0.1762550.7337820.5540240.050*
C50.17698 (14)0.57686 (12)0.6150 (2)0.0264 (4)
C210.40967 (15)0.61781 (11)0.3369 (3)0.0285 (4)
C80.43686 (15)0.59916 (11)0.5097 (2)0.0277 (4)
C160.49189 (16)0.65214 (11)0.2696 (3)0.0308 (4)
C70.35290 (15)0.57129 (11)0.5861 (2)0.0280 (4)
H70.3700330.5286820.6700480.034*
C40.10739 (15)0.64265 (12)0.6402 (2)0.0300 (4)
C60.16031 (15)0.49425 (12)0.6552 (2)0.0286 (4)
H60.2055060.4499910.6361130.034*
C140.62579 (15)0.64459 (12)0.5440 (3)0.0316 (4)
C150.59693 (16)0.66442 (12)0.3750 (3)0.0333 (5)
H150.6508640.6871700.3300520.040*
C30.02430 (16)0.62217 (12)0.7127 (3)0.0318 (4)
H30.0214160.6657530.7328590.038*
C200.30485 (16)0.60228 (12)0.2218 (3)0.0319 (4)
H200.2493630.5777620.2611190.038*
C100.57722 (16)0.59476 (12)0.7901 (3)0.0327 (4)
H100.5255400.5720880.8397470.039*
C10.07603 (15)0.47650 (12)0.7242 (2)0.0294 (4)
C90.54482 (15)0.61075 (11)0.6148 (3)0.0295 (4)
C170.46355 (18)0.67369 (12)0.0969 (3)0.0361 (5)
H170.5172810.6981100.0534620.043*
C20.00881 (16)0.53992 (13)0.7543 (3)0.0316 (4)
H20.0472280.5264430.8032460.038*
C190.28237 (17)0.62179 (12)0.0565 (3)0.0345 (5)
H190.2122220.6094530.0175150.041*
C130.73284 (16)0.66070 (13)0.6513 (3)0.0378 (5)
H130.7866330.6827130.6051520.045*
C180.36215 (18)0.66023 (13)0.0065 (3)0.0372 (5)
H180.3443590.6763950.1206700.045*
C110.68046 (17)0.61122 (13)0.8878 (3)0.0377 (5)
H110.6997480.5997791.0042180.045*
C120.75971 (17)0.64530 (14)0.8178 (3)0.0402 (5)
H120.8312980.6572800.8874020.048*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O1A0.0455 (9)0.0245 (7)0.0688 (11)0.0010 (6)0.0252 (8)0.0059 (7)
O1B0.0479 (9)0.0385 (9)0.0720 (11)0.0101 (7)0.0364 (9)0.0093 (8)
N30.0309 (8)0.0226 (8)0.0399 (9)0.0006 (6)0.0214 (7)0.0013 (6)
N10.0343 (9)0.0299 (9)0.0462 (10)0.0051 (7)0.0158 (8)0.0043 (7)
N20.0407 (10)0.0231 (9)0.0747 (13)0.0032 (7)0.0369 (10)0.0030 (8)
C50.0263 (9)0.0250 (9)0.0321 (10)0.0018 (7)0.0150 (8)0.0003 (7)
C210.0336 (10)0.0163 (8)0.0427 (11)0.0027 (7)0.0223 (9)0.0031 (7)
C80.0306 (10)0.0161 (8)0.0426 (11)0.0027 (7)0.0206 (8)0.0024 (7)
C160.0375 (10)0.0189 (9)0.0441 (11)0.0016 (7)0.0244 (9)0.0042 (8)
C70.0325 (10)0.0183 (8)0.0381 (11)0.0009 (7)0.0182 (8)0.0008 (7)
C40.0291 (10)0.0245 (9)0.0403 (11)0.0003 (7)0.0165 (8)0.0010 (8)
C60.0284 (9)0.0256 (10)0.0348 (10)0.0002 (7)0.0139 (8)0.0013 (8)
C140.0302 (10)0.0225 (9)0.0493 (12)0.0022 (7)0.0228 (9)0.0069 (8)
C150.0347 (11)0.0256 (10)0.0499 (12)0.0015 (8)0.0285 (9)0.0063 (8)
C30.0278 (10)0.0289 (10)0.0443 (11)0.0002 (7)0.0194 (9)0.0037 (8)
C200.0345 (10)0.0245 (9)0.0433 (12)0.0023 (8)0.0218 (9)0.0025 (8)
C100.0336 (10)0.0251 (10)0.0446 (12)0.0034 (8)0.0197 (9)0.0022 (8)
C10.0298 (10)0.0252 (9)0.0359 (10)0.0039 (7)0.0141 (8)0.0025 (8)
C90.0306 (10)0.0193 (9)0.0448 (11)0.0034 (7)0.0207 (9)0.0045 (8)
C170.0460 (12)0.0259 (10)0.0467 (12)0.0027 (8)0.0296 (10)0.0039 (8)
C20.0270 (9)0.0345 (10)0.0381 (11)0.0045 (8)0.0167 (8)0.0012 (8)
C190.0376 (11)0.0281 (10)0.0417 (12)0.0030 (8)0.0177 (9)0.0050 (8)
C130.0296 (10)0.0347 (11)0.0555 (14)0.0008 (8)0.0227 (10)0.0094 (9)
C180.0521 (13)0.0282 (10)0.0377 (11)0.0017 (9)0.0230 (10)0.0022 (8)
C110.0370 (11)0.0350 (11)0.0435 (12)0.0060 (9)0.0157 (9)0.0034 (9)
C120.0286 (10)0.0395 (12)0.0537 (14)0.0009 (9)0.0141 (9)0.0103 (10)
Geometric parameters (Å, º) top
O1A—N11.235 (2)C14—C91.441 (3)
O1B—N11.244 (2)C14—C131.424 (3)
N3—C51.412 (2)C15—H150.9500
N3—C71.282 (2)C3—H30.9500
N1—C11.438 (2)C3—C21.372 (3)
N2—H2A0.8800C20—H200.9500
N2—H2B0.8800C20—C191.363 (3)
N2—C41.337 (3)C10—H100.9500
C5—C41.424 (3)C10—C91.425 (3)
C5—C61.377 (3)C10—C111.361 (3)
C21—C81.417 (3)C1—C21.391 (3)
C21—C161.439 (3)C17—H170.9500
C21—C201.425 (3)C17—C181.350 (3)
C8—C71.472 (2)C2—H20.9500
C8—C91.416 (3)C19—H190.9500
C16—C151.389 (3)C19—C181.418 (3)
C16—C171.425 (3)C13—H130.9500
C7—H70.9500C13—C121.357 (3)
C4—C31.410 (3)C18—H180.9500
C6—H60.9500C11—H110.9500
C6—C11.396 (3)C11—C121.420 (3)
C14—C151.389 (3)C12—H120.9500
N2···O1Bi2.939 (2)C6···H72.71
O1A···H62.44C7···H202.66
O1B···H22.41C7···H62.81
H2A···O1Bi2.07C7···H102.58
N2···N32.672 (2)C10···H72.75
N3···C202.913 (3)H6···H72.39
N3···H2B2.31H7···H102.19
N3···H202.35
C7—N3—C5120.54 (16)C2—C3—C4120.67 (18)
O1A—N1—O1B122.45 (17)C2—C3—H3119.7
O1A—N1—C1119.49 (16)C21—C20—H20119.2
O1B—N1—C1118.06 (17)C19—C20—C21121.54 (19)
H2A—N2—H2B120.0C19—C20—H20119.2
C4—N2—H2A120.0C9—C10—H10119.2
C4—N2—H2B120.0C11—C10—H10119.2
N3—C5—C4114.51 (16)C11—C10—C9121.50 (19)
C6—C5—N3125.19 (16)C6—C1—N1119.07 (17)
C6—C5—C4120.23 (16)C2—C1—N1119.07 (17)
C8—C21—C16119.36 (18)C2—C1—C6121.86 (17)
C8—C21—C20123.68 (17)C8—C9—C14118.87 (18)
C20—C21—C16116.93 (18)C8—C9—C10123.50 (18)
C21—C8—C7121.00 (17)C10—C9—C14117.55 (18)
C9—C8—C21120.62 (17)C16—C17—H17119.2
C9—C8—C7118.32 (18)C18—C17—C16121.55 (19)
C15—C16—C21119.19 (19)C18—C17—H17119.2
C15—C16—C17121.46 (18)C3—C2—C1119.28 (17)
C17—C16—C21119.35 (19)C3—C2—H2120.4
N3—C7—C8120.87 (17)C1—C2—H2120.4
N3—C7—H7119.6C20—C19—H19119.5
C8—C7—H7119.6C20—C19—C18121.0 (2)
N2—C4—C5119.56 (17)C18—C19—H19119.5
N2—C4—C3121.54 (17)C14—C13—H13119.3
C3—C4—C5118.87 (17)C12—C13—C14121.47 (19)
C5—C6—H6120.5C12—C13—H13119.3
C5—C6—C1119.04 (17)C17—C18—C19119.5 (2)
C1—C6—H6120.5C17—C18—H18120.2
C15—C14—C9119.64 (18)C19—C18—H18120.2
C15—C14—C13121.36 (18)C10—C11—H11119.6
C13—C14—C9118.94 (19)C10—C11—C12120.8 (2)
C16—C15—H15118.9C12—C11—H11119.6
C14—C15—C16122.27 (18)C13—C12—C11119.8 (2)
C14—C15—H15118.9C13—C12—H12120.1
C4—C3—H3119.7C11—C12—H12120.1
O1A—N1—C1—C62.7 (3)C7—C8—C9—C14175.00 (15)
O1A—N1—C1—C2176.97 (19)C7—C8—C9—C101.7 (3)
O1B—N1—C1—C6176.55 (18)C4—C5—C6—C11.5 (3)
O1B—N1—C1—C23.8 (3)C4—C3—C2—C10.1 (3)
N3—C5—C4—N22.2 (3)C6—C5—C4—N2179.33 (19)
N3—C5—C4—C3179.62 (17)C6—C5—C4—C32.5 (3)
N3—C5—C6—C1178.32 (17)C6—C1—C2—C31.1 (3)
N1—C1—C2—C3178.57 (18)C14—C13—C12—C110.9 (3)
N2—C4—C3—C2179.8 (2)C15—C16—C17—C18178.65 (18)
C5—N3—C7—C8179.82 (16)C15—C14—C9—C80.5 (3)
C5—C4—C3—C21.7 (3)C15—C14—C9—C10177.41 (16)
C5—C6—C1—N1179.36 (17)C15—C14—C13—C12176.69 (18)
C5—C6—C1—C20.3 (3)C20—C21—C8—C77.4 (3)
C21—C8—C7—N338.6 (3)C20—C21—C8—C9175.56 (16)
C21—C8—C9—C142.1 (3)C20—C21—C16—C15176.78 (16)
C21—C8—C9—C10178.78 (16)C20—C21—C16—C174.0 (2)
C21—C16—C15—C140.1 (3)C20—C19—C18—C173.5 (3)
C21—C16—C17—C182.1 (3)C10—C11—C12—C130.8 (3)
C21—C20—C19—C181.5 (3)C9—C8—C7—N3138.46 (18)
C8—C21—C16—C151.5 (3)C9—C14—C15—C160.6 (3)
C8—C21—C16—C17177.80 (16)C9—C14—C13—C120.3 (3)
C8—C21—C20—C19179.61 (17)C9—C10—C11—C120.2 (3)
C16—C21—C8—C7174.45 (15)C17—C16—C15—C14179.34 (17)
C16—C21—C8—C92.6 (3)C13—C14—C15—C16177.57 (17)
C16—C21—C20—C192.2 (3)C13—C14—C9—C8176.56 (16)
C16—C17—C18—C191.6 (3)C13—C14—C9—C100.3 (3)
C7—N3—C5—C4142.86 (18)C11—C10—C9—C8176.31 (17)
C7—N3—C5—C640.1 (3)C11—C10—C9—C140.4 (3)
Symmetry code: (i) x, y+1/2, z+3/2.
Hydrogen-bond geometry (Å, º) top
Cg1 is the centroid of the C1–C6 ring.
D—H···AD—HH···AD···AD—H···A
N2—H2A···O1Bi0.882.072.939 (2)168
N2—H2B···N30.882.312.672 (2)104
C19—H19···Cg1ii0.952.653.492 (2)149
Symmetry codes: (i) x, y+1/2, z+3/2; (ii) x, y, z+1.
 

Acknowledgements

TH is grateful to Hacettepe University Scientific Research Project Unit (grant No. 013 D04 602 004). We extend our gratitude to Dr Samia Benmansour, Assistant Professor in the Department of Inorganic Chemistry, University of Valencia (Dr Moliner 50, Burjassot, Valencia, Spain), for her valuable collaboration in the crystallographic analyses.

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