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

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890

Synthesis and structure of 1,1-bis­­(furan-2-ylmethyl)-3-phenyl­urea

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aRUDN University, 6 Miklukho-Maklaya St., Moscow 117198, Russian Federation, bZelinsky Institute of Organic Chemistry of RAS, Leninsky Prospect 47, Moscow 119991, Russian Federation, cHacettepe University, Department of Physics, 06800 Beytepe-Ankara, Türkiye, dDepartment of Chemistry, Bahir Dar University, PO Box 79, Bahir Dar, Ethiopia, eAzerbaijan Medical University, Scientific Research Centre (SRC), A. Kasumzade Str. 14, AZ 1022, Baku, Azerbaijan, and fDepartment of Chemical Engineering, Baku Engineering University, Hasan Aliyev Str. 120, AZ0101, Khirdalan, Absheron, Azerbaijan
*Correspondence e-mail: [email protected]

Edited by W. T. A. Harrison, University of Aberdeen, United Kingdom (Received 10 September 2026; accepted 25 September 2026; online 2 October 2026)

The asymmetric unit of the title compound, C17H16N2O3, contains two mol­ecules, A and B, with one furan ring in each mol­ecule showing ‘flip' rotational disorder. In the crystal, N—H⋯O hydrogen bonds link the mol­ecules into separate infinite ⋯A⋯A⋯A⋯ and ⋯B⋯B⋯B⋯ chains propagating along the c-axis direction. Weak C—H⋯π inter­actions may help to consolidate the packing. Hirshfeld surface analysis revealed that the most important contributions to the packing are from H⋯H, H⋯C/C⋯H and H⋯O/O⋯H inter­actions with very similar surface percentages for both mol­ecules.

1. Chemical context

Difurfuryl­amine, C10H11NO2 (DiFAM), is a common precursor chemical with potential applications in pharmaceuticals (Zhuang et al., 2022View full citation). Particular inter­est is invested into the use of DiFAM in the synthesis of di­thio­carbamates: such compounds exhibit anti­tumor activity, are used as catalysts and biocides (Tamilvanan et al., 2017View full citation), and thallium(III) N,N-difurfuryldi­thio­carbamate has an oxidative property towards organic mol­ecules, is used within anti-alcohol medicine and possesses significant fungicidial activity (Gomathi et al., 2023View full citation). Ureas themselves have shown a wide variety of applications and their anti­microbial (Resende et al., 2023View full citation) and anti­bacterial (Yang et al., 2025View full citation) activities have led to applications such as soporifics and local and general anaesthetics or herbicides (fenuron, isoproturon, sulfentrazone) and pesticides (diuron, monolinuron, chloro­toluron). The combination of the urea skeleton with a pharmaceutically promising difurfuryl­amine structure may lead to a new library of biologically active compounds. Inter­est in difurfuryl­amine chemistry was sparked in us in 2019, when difurfurylethers, alkenes and amides showed good selectivity in reactions with electron-deficient dimethyl acetyl­enedi­carboxyl­ate, producing kinetically and thermodynamically controlled di­epoxy­naphthalenes (Borisova et al., 2018View full citation). We decided to introduce different substituents to the nitro­gen atom of difurfuryl­amine, in this case transforming it into the title compound, C17H16N2O3 (3) and we now describe its structure.

[Scheme 1]

2. Structural commentary

The asymmetric unit of (3) contains two mol­ecules, A and B (Fig. 1[link]). In each mol­ecule, one furan ring is well ordered, while the other [the furan B ring (O3/C8–C11) in A and the D ring (O5/C20–C23) in B] is disordered over two sets of sites related by a ‘flip' (∼180°) rotation about the C—C bond connecting it to the adjacent methyl­ene group. In mol­ecule A, the ordered furan, A (O2/C3–C6) and phenyl, C (C12–C17) rings are oriented at a dihedral angle of A/C = 87.60 (19)°. In mol­ecule B, the furan, E (O6/C25–C28) and phenyl, F (C29–C34) rings are oriented at a dihedral angle of E/F = 74.12 (17)°. There are no significant differences between the bond distances in A and B but the C7—N1—C1 [121.20 (19)°], C1—N1—C2 [115.52 (19)°], O1—C1—N2 [123.1 (2)°] and C1—N1—C12 [125.8 (2)°] bond angles in A are slightly different from the corresponding C18—N3—C24 [123.74 (19)°], C19—N3—C18 [118.2 (2)°], O4—C18—N4 [122.2 (2)°] and C18—N4—C29 [124.1 (2)°] bond angles in B.

[Figure 1]
Figure 1
The asymmetric unit of (3) with 50% probability ellipsoids. Only the major disorder components of the disordered furan rings are shown.

3. Supra­molecular features

In the crystal, N—H⋯O hydrogen bonds (Table 1[link]) link the mol­ecules into separate infinite ⋯A⋯A⋯A⋯ and ⋯B⋯B⋯B⋯ C(4) chains propagating along the c-axis direction (Fig. 2[link]). Adjacent mol­ecules are generated by c-glide symmetry in each case. Weak C—H⋯π inter­actions may help to consolidate the packing.

Table 1
Hydrogen-bond geometry (Å, °)

Cg1, Cg5 and Cg6 are the centroids of the O2/C3–C6, C12–C17 and C29–C34 rings, respectively.

D—H⋯A D—H H⋯A D⋯A D—H⋯A
N2—H2N⋯O1i 0.90 2.03 2.917 (2) 168
N4—H4N⋯O4ii 0.90 2.07 2.955 (2) 167
C6—H6⋯Cg6iii 0.95 2.62 3.482 150
C24—H24B⋯Cg5iv 0.99 2.90 3.789 149
C28—H28⋯Cg1iv 0.95 2.82 3.658 148
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation.
[Figure 2]
Figure 2
A partial packing diagram of (3) with N—H⋯O hydrogen bonds shown as dashed lines. Non-bonding H atoms have been omitted for clarity.

4. Hirshfeld surface analysis

For visualizing the inter­molecular inter­actions in the crystal of (3), Hirshfeld surface (HS) analyses were carried out using Crystal Explorer 17.5 (Spackman et al., 2021View full citation). Only the major disorder components of furan rings were taken into account for the analysis. In the HSs plotted over dnorm (Fig. 3[link]a,b), the red spots indicate their roles as the respective donors and/or acceptors in hydrogen bonding, as discussed above. The overall two-dimensional fingerprint plots are shown in Fig. 4[link]a and 5a and those delineated into the different contact types are illustrated in Fig. 4[link](b)–(j) and Fig. 5[link](b)–(j) for mol­ecules A and B, respectively. Their contributions to the HSs are presented in Table 2[link]. Comparison of their percentages shows that there are no significant differences, implying that their environments in the crystal are very similar.

Table 2
Comparison of the Hirshfeld fingerprint percentages for mol­ecules A and B

Contact A B
H⋯H 48.4 50.4
H⋯C/C⋯H 30.3 28.3
H⋯O/O⋯H 17.0 16.6
C⋯O/O⋯C 1.7 1.7
H⋯N/N⋯H 1.0 1.5
C⋯C 0.5 0.5
O⋯O 0.5 0.5
O⋯N/N⋯O 0.3 0.3
C⋯N/N⋯C 0.3 0.3
[Figure 3]
Figure 3
Views of the three-dimensional Hirshfeld surfaces for mol­ecules (a) A and (b) B plotted over dnorm in the ranges from −0.49 to 1.58 a.u. and −0.53 to 1.56 a.u., respectively.
[Figure 4]
Figure 4
The full two-dimensional fingerprint plots for mol­ecule A, showing all inter­actions, and delineated into different contact types.
[Figure 5]
Figure 5
The full two-dimensional fingerprint plots for mol­ecule B, showing all inter­actions, and delineated into different contact types.

5. Synthesis and crystallization

Bis(furan-2-yl)amine (1) (100 mg, 0.56 mmol) was dissolved in benzene (5 ml) at room temperature (Fig. 6[link]). Iso­cyanato­benzene (2) (74 mg, 0.62 mmol) was added to the solution and the reaction was refluxed for 6 h (progress monitored by TLC). The resulting mixture was cooled, and the formation of a solid was observed. The crystals were filtered off, washed with diethyl ether (3 × 5 ml), dried under vacuum, and then air. The target compound (3) did not require further purification; yield 70%, 117.1 mg, colourless crystals, m.p. 381–383 K. Single crystals of (3) were grown from a solvent mixture of ethanol and N,N-di­methyl­formamide. IR (KBr), ν (cm−1): 1725, 1H NMR (700 MHz, DMSO-d6, 273 K) (J Hz): δ 8.57 (s, 1H), 7.60 (dd, J = 0.9, 1.9 Hz, 2H), 7.47 (d, J = 7.6 Hz, 2H), 7.24 (t, J = 7.6 Hz, 2H), 6.96 (t, J = 7.6 Hz, 1H), 6.40 (dd, J = 1.9, 3.10 Hz, 2H), 6.31 (d, J = 3.10 Hz, 2H), 4.54 (s, 4H) ppm. 13C {1H} NMR (150.9 MHz, DMSO-d6, 273 K): δ 155.17, 151.67 (2C), 143.12 (2C), 140.66, 128.79 (2C), 122.53, 120.35 (2C), 110.95 (2C), 108.55 (2C), 42.72 (2C) ppm. MS (ESI) m/z: 296 [M + H]+.

[Figure 6]
Figure 6
Reaction scheme for obtaining (3).

6. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 3[link]. The hydrogen atom positions were calculated geometrically at distances of N—H = 0.90 and C—H = 0.95–0.99 Å and refined using a riding model while applying the constraint Uiso(H) = 1.2 × Ueq C, N). One furan ring in each mol­ecule was found to be disordered over two sets of sites and they were refined with site occupancy ratios of 0.6:0.4 in each case.

Table 3
Experimental details

Crystal data
Chemical formula C17H16N2O3
Mr 296.32
Crystal system, space group Monoclinic, P21/c
Temperature (K) 100
a, b, c (Å) 20.1286 (2), 14.76143 (13), 9.97556 (8)
β (°) 92.8316 (8)
V (Å3) 2960.39 (5)
Z 8
Radiation type Cu Kα
μ (mm−1) 0.76
Crystal size (mm) 0.39 × 0.15 × 0.09
 
Data collection
Diffractometer Micro-focus sealed X-ray tube
Absorption correction Gaussian (CrysAlis PRO; Rigaku OD, 2024View full citation)
Tmin, Tmax 0.708, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 34327, 6425, 5840
Rint 0.039
(sin θ/λ)max (Å−1) 0.639
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.068, 0.181, 1.09
No. of reflections 6425
No. of parameters 439
No. of restraints 20
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.59, −0.50
Computer programs: CrysAlis PRO (Rigaku OD, 2024View full citation), SHELXT (Sheldrick, 2015aView full citation), SHELXL (Sheldrick, 2015bView full citation) and SHELXTL (Sheldrick, 2008View full citation).

Supporting information


Computing details top

1,1-Bis(furan-2-ylmethyl)-3-phenylurea top
Crystal data top
C17H16N2O3F(000) = 1248
Mr = 296.32Dx = 1.330 Mg m−3
Monoclinic, P21/cCu Kα radiation, λ = 1.54184 Å
a = 20.1286 (2) ÅCell parameters from 21717 reflections
b = 14.76143 (13) Åθ = 2.3–79.8°
c = 9.97556 (8) ŵ = 0.76 mm−1
β = 92.8316 (8)°T = 100 K
V = 2960.39 (5) Å3Plate, colourless
Z = 80.39 × 0.15 × 0.09 mm
Data collection top
Micro-focus sealed X-ray tube
diffractometer
5840 reflections with I > 2σ(I)
Detector resolution: φ and ω pixels mm-1Rint = 0.039
Rigaku XtaLAB Synergy–S, HyPix–6000HE area–detector scansθmax = 79.9°, θmin = 2.2°
Absorption correction: gaussian
(CrysAlisPro; Rigaku OD, 2024)
h = −25→25
Tmin = 0.708, Tmax = 1.000k = −18→18
34327 measured reflectionsl = −11→12
6425 independent reflections
Refinement top
Refinement on F2Primary atom site location: difference Fourier map
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.068Hydrogen site location: mixed
wR(F2) = 0.181H-atom parameters constrained
S = 1.09 w = 1/[σ2(Fo2) + (0.053P)2 + 5.931P]
where P = (Fo2 + 2Fc2)/3
6425 reflections(Δ/σ)max < 0.001
439 parametersΔρmax = 0.59 e Å−3
20 restraintsΔρmin = −0.50 e Å−3
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)
O10.73597 (8)0.26382 (12)0.41633 (16)0.0238 (4)
O20.93019 (9)0.19490 (13)0.33124 (17)0.0292 (4)
O30.72614 (15)−0.0280 (2)0.2890 (4)0.0258 (7)0.6
O3'0.6514 (4)0.0572 (6)0.1365 (9)0.0369 (11)0.4
N10.78252 (10)0.16531 (14)0.2722 (2)0.0228 (4)
N20.70445 (10)0.27093 (14)0.19393 (19)0.0235 (4)
H2N0.7184670.2544030.1132150.028*
C10.73968 (11)0.23500 (15)0.3017 (2)0.0199 (4)
C20.82410 (12)0.13022 (17)0.3869 (2)0.0251 (5)
H2A0.8408900.0693730.3641520.030*
H2B0.7963380.1237430.4655400.030*
C30.88149 (12)0.19036 (16)0.4231 (2)0.0230 (5)
C40.89752 (12)0.24433 (17)0.5291 (2)0.0256 (5)
H40.8723770.2530270.6061580.031*
C50.95961 (13)0.28578 (18)0.5027 (3)0.0291 (5)
H50.9839030.3273120.5588960.035*
C60.97693 (13)0.25468 (19)0.3831 (3)0.0308 (6)
H61.0161400.2716630.3401170.037*
C70.76556 (12)0.09991 (16)0.1638 (2)0.0243 (5)
H7A0.8054350.0632710.1464410.029*
H7B0.7529680.1336740.0806020.029*
C80.7098 (3)0.0376 (6)0.1960 (9)0.0177 (9)0.6
C90.6447 (3)0.0330 (4)0.1597 (7)0.0289 (13)0.6
H9A0.6209940.0715400.0978440.035*0.6
C100.61794 (19)−0.0410 (3)0.2322 (5)0.0270 (10)0.6
H10A0.573193−0.0616970.2276950.032*0.6
C110.66879 (19)−0.0753 (3)0.3076 (4)0.0283 (9)0.6
H11A0.665511−0.1257280.3661570.034*0.6
C8'0.7112 (6)0.0382 (13)0.202 (2)0.0369 (11)0.4
C9'0.7046 (4)−0.0346 (8)0.2804 (12)0.0369 (11)0.4
H9B0.738754−0.0621100.3354020.044*0.4
C10'0.6368 (4)−0.0636 (6)0.2663 (10)0.0369 (11)0.4
H10B0.617100−0.1134500.3095780.044*0.4
C11'0.6071 (4)−0.0056 (5)0.1794 (8)0.0369 (11)0.4
H11B0.561389−0.0077640.1511640.044*0.4
C120.65565 (12)0.33951 (16)0.1991 (2)0.0228 (5)
C130.64293 (12)0.39180 (17)0.0844 (2)0.0257 (5)
H130.6678500.3818250.0073540.031*
C140.59412 (13)0.45840 (18)0.0818 (3)0.0293 (5)
H140.5854190.4929900.0025180.035*
C150.55810 (13)0.4746 (2)0.1940 (3)0.0338 (6)
H150.5250880.5206630.1926650.041*
C160.57075 (15)0.4232 (2)0.3076 (3)0.0422 (7)
H160.5463020.4343620.3849760.051*
C170.61871 (14)0.3551 (2)0.3112 (3)0.0367 (6)
H170.6261910.3194750.3897590.044*
O40.77404 (9)0.78394 (12)0.46392 (16)0.0252 (4)
O50.5736 (2)0.6855 (4)0.3492 (5)0.0407 (13)0.6
O5'0.5886 (6)0.7549 (10)0.5176 (14)0.085 (3)0.4
O60.77833 (9)0.48633 (12)0.33707 (18)0.0283 (4)
N30.72207 (10)0.67406 (14)0.3382 (2)0.0224 (4)
N40.80378 (10)0.76368 (13)0.24824 (19)0.0216 (4)
H4N0.7903120.7426690.1666830.026*
C180.76737 (11)0.74267 (16)0.3562 (2)0.0202 (4)
C190.68232 (12)0.64849 (17)0.4523 (3)0.0260 (5)
H18A0.7090670.6608420.5362680.031*
H19B0.6743250.5823520.4480250.031*
C200.6152 (7)0.6961 (14)0.4609 (11)0.0221 (15)0.6
C210.5916 (3)0.7523 (6)0.5522 (7)0.0411 (18)0.6
H21A0.6130370.7715860.6343530.049*0.6
C220.5269 (3)0.7769 (4)0.4983 (7)0.048 (2)0.6
H22A0.4953440.8141120.5398550.058*0.6
C230.5196 (3)0.7374 (5)0.3783 (7)0.055 (2)0.6
H23A0.4813640.7444510.3195570.066*0.6
C20'0.6202 (11)0.693 (2)0.441 (2)0.0221 (15)0.4
C21'0.5714 (8)0.6598 (13)0.359 (2)0.085 (3)0.4
H21B0.5774580.6114880.2976090.102*0.4
C22'0.5093 (8)0.7047 (10)0.374 (2)0.085 (3)0.4
H22B0.4673950.6925050.3294150.102*0.4
C23'0.5250 (7)0.7681 (13)0.466 (2)0.085 (3)0.4
H23B0.4961920.8153400.4914100.102*0.4
C240.72054 (12)0.61143 (16)0.2234 (2)0.0235 (5)
H24A0.7224510.6468870.1394570.028*
H24B0.6779210.5778320.2200270.028*
C250.77646 (12)0.54547 (15)0.2306 (2)0.0222 (5)
C260.82809 (13)0.53027 (17)0.1531 (3)0.0287 (5)
H260.8380360.5618570.0735510.034*
C270.86519 (13)0.45689 (18)0.2143 (3)0.0300 (5)
H270.9046710.4304200.1835130.036*
C280.83324 (13)0.43317 (18)0.3230 (3)0.0294 (5)
H280.8467960.3857370.3826140.035*
C290.85387 (11)0.83123 (16)0.2496 (2)0.0214 (5)
C300.86190 (12)0.88096 (17)0.1319 (3)0.0253 (5)
H300.8335860.8698050.0545970.030*
C310.91132 (13)0.94669 (17)0.1280 (3)0.0297 (5)
H310.9168190.9799500.0477750.036*
C320.95276 (13)0.96400 (18)0.2409 (3)0.0320 (6)
H320.9857421.0099550.2389640.038*
C330.94535 (13)0.91352 (19)0.3560 (3)0.0312 (6)
H330.9739210.9246380.4329160.037*
C340.89680 (12)0.84679 (17)0.3611 (3)0.0260 (5)
H340.8929000.8118960.4403470.031*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0288 (9)0.0276 (9)0.0151 (7)0.0001 (7)0.0024 (6)0.0014 (6)
O20.0275 (9)0.0370 (10)0.0234 (8)−0.0056 (8)0.0036 (7)0.0004 (7)
O30.0258 (17)0.0215 (16)0.0304 (16)0.0044 (14)0.0038 (16)0.0046 (13)
O3'0.032 (2)0.042 (3)0.038 (2)−0.009 (2)0.0042 (17)−0.0037 (19)
N10.0245 (10)0.0221 (10)0.0218 (10)0.0007 (8)−0.0001 (8)0.0000 (8)
N20.0293 (10)0.0281 (10)0.0133 (8)0.0035 (8)0.0018 (7)−0.0012 (7)
C10.0206 (10)0.0212 (11)0.0179 (10)−0.0029 (8)0.0015 (8)0.0009 (8)
C20.0255 (12)0.0230 (11)0.0264 (12)0.0005 (9)−0.0017 (9)0.0052 (9)
C30.0230 (11)0.0249 (11)0.0210 (11)0.0022 (9)0.0014 (9)0.0069 (9)
C40.0266 (12)0.0259 (12)0.0242 (11)0.0019 (9)−0.0003 (9)0.0026 (9)
C50.0292 (12)0.0277 (12)0.0298 (12)−0.0029 (10)−0.0051 (10)0.0038 (10)
C60.0254 (12)0.0360 (14)0.0307 (13)−0.0075 (10)−0.0004 (10)0.0049 (11)
C70.0293 (12)0.0236 (11)0.0203 (11)0.0005 (9)0.0045 (9)−0.0015 (9)
C80.029 (2)0.0126 (18)0.012 (2)0.0080 (16)0.0002 (16)−0.0028 (15)
C90.025 (3)0.023 (3)0.037 (3)−0.001 (2)−0.006 (2)−0.004 (2)
C100.022 (2)0.026 (3)0.033 (3)0.0009 (19)0.004 (2)−0.005 (2)
C110.030 (2)0.021 (2)0.035 (2)−0.0007 (18)0.012 (2)0.0022 (17)
C8'0.032 (2)0.042 (3)0.038 (2)−0.009 (2)0.0042 (17)−0.0037 (19)
C9'0.032 (2)0.042 (3)0.038 (2)−0.009 (2)0.0042 (17)−0.0037 (19)
C10'0.032 (2)0.042 (3)0.038 (2)−0.009 (2)0.0042 (17)−0.0037 (19)
C11'0.032 (2)0.042 (3)0.038 (2)−0.009 (2)0.0042 (17)−0.0037 (19)
C120.0212 (11)0.0260 (11)0.0210 (11)−0.0011 (9)−0.0016 (8)−0.0026 (9)
C130.0256 (12)0.0278 (12)0.0239 (11)−0.0008 (9)0.0016 (9)0.0013 (9)
C140.0264 (12)0.0280 (12)0.0330 (13)−0.0015 (10)−0.0028 (10)0.0052 (10)
C150.0243 (12)0.0366 (14)0.0401 (15)0.0064 (11)−0.0027 (11)−0.0027 (12)
C160.0338 (14)0.064 (2)0.0292 (14)0.0192 (14)0.0037 (11)−0.0027 (13)
C170.0317 (14)0.0534 (18)0.0251 (13)0.0133 (13)0.0033 (10)0.0053 (12)
O40.0304 (9)0.0293 (9)0.0161 (7)0.0015 (7)0.0027 (6)−0.0009 (6)
O50.0256 (17)0.074 (4)0.0217 (16)0.023 (2)−0.0078 (13)−0.003 (2)
O5'0.053 (4)0.076 (5)0.123 (7)0.017 (3)−0.020 (4)−0.046 (5)
O60.0329 (9)0.0257 (9)0.0268 (9)0.0035 (7)0.0059 (7)0.0060 (7)
N30.0246 (10)0.0230 (10)0.0198 (9)0.0002 (8)0.0045 (7)0.0016 (7)
N40.0258 (10)0.0229 (10)0.0161 (9)−0.0023 (8)0.0019 (7)−0.0018 (7)
C180.0221 (11)0.0223 (11)0.0162 (10)0.0042 (8)0.0012 (8)0.0028 (8)
C190.0238 (11)0.0273 (12)0.0271 (12)0.0016 (9)0.0051 (9)0.0069 (10)
C200.024 (2)0.0258 (17)0.017 (4)0.0033 (15)0.011 (3)0.003 (3)
C210.045 (4)0.032 (3)0.049 (4)−0.009 (3)0.030 (3)−0.005 (3)
C220.038 (3)0.030 (3)0.081 (5)0.023 (2)0.038 (3)0.025 (3)
C230.020 (3)0.079 (6)0.065 (4)0.021 (3)−0.010 (3)0.017 (5)
C20'0.024 (2)0.0258 (17)0.017 (4)0.0033 (15)0.011 (3)0.003 (3)
C21'0.053 (4)0.076 (5)0.123 (7)0.017 (3)−0.020 (4)−0.046 (5)
C22'0.053 (4)0.076 (5)0.123 (7)0.017 (3)−0.020 (4)−0.046 (5)
C23'0.053 (4)0.076 (5)0.123 (7)0.017 (3)−0.020 (4)−0.046 (5)
C240.0237 (11)0.0239 (11)0.0227 (11)−0.0027 (9)−0.0006 (9)0.0010 (9)
C250.0267 (11)0.0191 (11)0.0205 (11)−0.0047 (9)0.0001 (9)0.0015 (8)
C260.0348 (13)0.0250 (12)0.0269 (12)−0.0032 (10)0.0083 (10)−0.0023 (10)
C270.0286 (12)0.0256 (12)0.0358 (14)0.0001 (10)0.0034 (10)−0.0074 (10)
C280.0340 (13)0.0234 (12)0.0304 (13)0.0044 (10)−0.0019 (10)−0.0013 (10)
C290.0204 (10)0.0203 (11)0.0237 (11)0.0025 (8)0.0038 (8)−0.0017 (9)
C300.0223 (11)0.0242 (11)0.0295 (12)0.0025 (9)0.0022 (9)0.0029 (9)
C310.0263 (12)0.0244 (12)0.0390 (14)0.0024 (10)0.0071 (10)0.0060 (10)
C320.0234 (12)0.0237 (12)0.0492 (16)−0.0013 (10)0.0036 (11)−0.0022 (11)
C330.0244 (12)0.0319 (13)0.0371 (14)−0.0006 (10)0.0000 (10)−0.0096 (11)
C340.0234 (11)0.0285 (12)0.0262 (12)0.0032 (9)0.0013 (9)−0.0033 (10)
Geometric parameters (Å, º) top
O1—C11.226 (3)O4—C181.236 (3)
O2—C61.372 (3)O5—C201.369 (3)
O2—C31.376 (3)O5—C231.373 (3)
O3—C111.370 (3)O5'—C20'1.368 (3)
O3—C81.371 (3)O5'—C23'1.372 (3)
O3'—C11'1.369 (3)O6—C281.368 (3)
O3'—C8'1.371 (3)O6—C251.374 (3)
N1—C11.383 (3)N3—C181.369 (3)
N1—C71.477 (3)N3—C241.471 (3)
N1—C21.478 (3)N3—C191.472 (3)
N2—C11.366 (3)N4—C181.368 (3)
N2—C121.413 (3)N4—C291.418 (3)
N2—H2N0.8999N4—H4N0.8999
C2—C31.487 (3)C19—C20'1.414 (14)
C2—H2A0.9900C19—C201.530 (9)
C2—H2B0.9900C19—H18A0.9900
C3—C41.350 (4)C19—H19B0.9900
C4—C51.428 (4)C20—C211.336 (3)
C4—H40.9500C21—C221.432 (3)
C5—C61.341 (4)C21—H21A0.9500
C5—H50.9500C22—C231.333 (3)
C6—H60.9500C22—H22A0.9500
C7—C8'1.487 (12)C23—H23A0.9500
C7—C81.499 (7)C20'—C21'1.340 (3)
C7—H7A0.9900C21'—C22'1.429 (3)
C7—H7B0.9900C21'—H21B0.9500
C8—C91.343 (3)C22'—C23'1.338 (3)
C9—C101.430 (3)C22'—H22B0.9500
C9—H9A0.9500C23'—H23B0.9500
C10—C111.339 (3)C24—C251.487 (3)
C10—H10A0.9500C24—H24A0.9900
C11—H11A0.9500C24—H24B0.9900
C8'—C9'1.341 (3)C25—C261.345 (3)
C9'—C10'1.429 (3)C26—C271.435 (4)
C9'—H9B0.9500C26—H260.9500
C10'—C11'1.339 (3)C27—C281.335 (4)
C10'—H10B0.9500C27—H270.9500
C11'—H11B0.9500C28—H280.9500
C12—C171.392 (4)C29—C341.394 (3)
C12—C131.393 (3)C29—C301.401 (3)
C13—C141.389 (4)C30—C311.391 (4)
C13—H130.9500C30—H300.9500
C14—C151.384 (4)C31—C321.392 (4)
C14—H140.9500C31—H310.9500
C15—C161.377 (4)C32—C331.383 (4)
C15—H150.9500C32—H320.9500
C16—C171.393 (4)C33—C341.390 (4)
C16—H160.9500C33—H330.9500
C17—H170.9500C34—H340.9500
C6—O2—C3106.2 (2)C20—O5—C23102.9 (6)
C11—O3—C8106.0 (4)C20'—O5'—C23'109.5 (14)
C11'—O3'—C8'106.4 (8)C28—O6—C25106.06 (19)
C1—N1—C7121.20 (19)C18—N3—C24123.74 (19)
C1—N1—C2115.52 (19)C18—N3—C19118.2 (2)
C7—N1—C2116.07 (19)C24—N3—C19116.70 (19)
C1—N2—C12125.8 (2)C18—N4—C29124.1 (2)
C1—N2—H2N115.2C18—N4—H4N119.0
C12—N2—H2N118.4C29—N4—H4N115.7
O1—C1—N2123.1 (2)O4—C18—N4122.2 (2)
O1—C1—N1121.6 (2)O4—C18—N3121.4 (2)
N2—C1—N1115.2 (2)N4—C18—N3116.3 (2)
N1—C2—C3112.47 (19)C20'—C19—N3109.2 (14)
N1—C2—H2A109.1N3—C19—C20116.2 (8)
C3—C2—H2A109.1N3—C19—H18A108.2
N1—C2—H2B109.1C20—C19—H18A108.2
C3—C2—H2B109.1N3—C19—H19B108.2
H2A—C2—H2B107.8C20—C19—H19B108.2
C4—C3—O2110.0 (2)H18A—C19—H19B107.4
C4—C3—C2134.0 (2)C21—C20—O5113.8 (7)
O2—C3—C2116.0 (2)C21—C20—C19131.9 (6)
C3—C4—C5106.6 (2)O5—C20—C19114.1 (5)
C3—C4—H4126.7C20—C21—C22104.4 (6)
C5—C4—H4126.7C20—C21—H21A127.8
C6—C5—C4106.6 (2)C22—C21—H21A127.8
C6—C5—H5126.7C23—C22—C21106.5 (5)
C4—C5—H5126.7C23—C22—H22A126.7
C5—C6—O2110.6 (2)C21—C22—H22A126.7
C5—C6—H6124.7C22—C23—O5112.4 (5)
O2—C6—H6124.7C22—C23—H23A123.8
N1—C7—C8'111.0 (11)O5—C23—H23A123.8
N1—C7—C8113.1 (5)C21'—C20'—O5'103.9 (16)
N1—C7—H7A109.0C21'—C20'—C19119.8 (14)
C8—C7—H7A109.0O5'—C20'—C19134.3 (11)
N1—C7—H7B109.0C20'—C21'—C22'112.6 (16)
C8—C7—H7B109.0C20'—C21'—H21B123.7
H7A—C7—H7B107.8C22'—C21'—H21B123.7
C9—C8—O3110.2 (5)C23'—C22'—C21'102.6 (15)
C9—C8—C7134.8 (4)C23'—C22'—H22B128.7
O3—C8—C7114.9 (4)C21'—C22'—H22B128.7
C8—C9—C10106.8 (5)C22'—C23'—O5'110.1 (15)
C8—C9—H9A126.6C22'—C23'—H23B124.9
C10—C9—H9A126.6O5'—C23'—H23B124.9
C11—C10—C9106.1 (4)N3—C24—C25112.77 (19)
C11—C10—H10A127.0N3—C24—H24A109.0
C9—C10—H10A127.0C25—C24—H24A109.0
C10—C11—O3110.9 (3)N3—C24—H24B109.0
C10—C11—H11A124.5C25—C24—H24B109.0
O3—C11—H11A124.5H24A—C24—H24B107.8
C9'—C8'—O3'109.3 (10)C26—C25—O6110.3 (2)
C9'—C8'—C7137.5 (8)C26—C25—C24133.3 (2)
O3'—C8'—C7113.1 (7)O6—C25—C24116.4 (2)
C8'—C9'—C10'107.8 (9)C25—C26—C27106.4 (2)
C8'—C9'—H9B126.1C25—C26—H26126.8
C10'—C9'—H9B126.1C27—C26—H26126.8
C11'—C10'—C9'105.4 (8)C28—C27—C26106.4 (2)
C11'—C10'—H10B127.3C28—C27—H27126.8
C9'—C10'—H10B127.3C26—C27—H27126.8
C10'—C11'—O3'111.1 (8)C27—C28—O6110.9 (2)
C10'—C11'—H11B124.5C27—C28—H28124.5
O3'—C11'—H11B124.5O6—C28—H28124.5
C17—C12—C13118.9 (2)C34—C29—C30119.3 (2)
C17—C12—N2123.2 (2)C34—C29—N4122.4 (2)
C13—C12—N2117.8 (2)C30—C29—N4118.2 (2)
C14—C13—C12120.6 (2)C31—C30—C29120.1 (2)
C14—C13—H13119.7C31—C30—H30120.0
C12—C13—H13119.7C29—C30—H30120.0
C15—C14—C13120.3 (2)C30—C31—C32120.4 (2)
C15—C14—H14119.8C30—C31—H31119.8
C13—C14—H14119.8C32—C31—H31119.8
C16—C15—C14119.1 (3)C33—C32—C31119.2 (2)
C16—C15—H15120.4C33—C32—H32120.4
C14—C15—H15120.4C31—C32—H32120.4
C15—C16—C17121.2 (3)C32—C33—C34121.1 (3)
C15—C16—H16119.4C32—C33—H33119.4
C17—C16—H16119.4C34—C33—H33119.4
C12—C17—C16119.7 (3)C33—C34—C29119.8 (2)
C12—C17—H17120.1C33—C34—H34120.1
C16—C17—H17120.1C29—C34—H34120.1
C12—N2—C1—O1−5.6 (4)C29—N4—C18—O42.5 (4)
C12—N2—C1—N1177.0 (2)C29—N4—C18—N3−178.5 (2)
C7—N1—C1—O1147.7 (2)C24—N3—C18—O4−167.8 (2)
C2—N1—C1—O1−1.4 (3)C19—N3—C18—O4−1.7 (3)
C7—N1—C1—N2−34.8 (3)C24—N3—C18—N413.2 (3)
C2—N1—C1—N2176.1 (2)C19—N3—C18—N4179.3 (2)
C1—N1—C2—C3−77.9 (3)C18—N3—C19—C20'96.2 (10)
C7—N1—C2—C3131.4 (2)C24—N3—C19—C20'−96.6 (10)
C6—O2—C3—C4−0.7 (3)C18—N3—C19—C2092.1 (7)
C6—O2—C3—C2178.9 (2)C24—N3—C19—C20−100.7 (7)
N1—C2—C3—C4111.0 (3)C23—O5—C20—C21−2.2 (19)
N1—C2—C3—O2−68.4 (3)C23—O5—C20—C19−176.8 (13)
O2—C3—C4—C50.3 (3)N3—C19—C20—C21−116 (2)
C2—C3—C4—C5−179.1 (3)N3—C19—C20—O557.0 (18)
C3—C4—C5—C60.2 (3)O5—C20—C21—C223.4 (19)
C4—C5—C6—O2−0.7 (3)C19—C20—C21—C22176.8 (19)
C3—O2—C6—C50.9 (3)C20—C21—C22—C23−3.2 (13)
C1—N1—C7—C8'−71.0 (6)C21—C22—C23—O52.1 (8)
C2—N1—C7—C8'77.9 (5)C20—O5—C23—C22−0.1 (12)
C1—N1—C7—C8−69.6 (3)C23'—O5'—C20'—C21'−10 (3)
C2—N1—C7—C879.4 (3)C23'—O5'—C20'—C19−173 (3)
C11—O3—C8—C91.2 (10)N3—C19—C20'—C21'81 (3)
C11—O3—C8—C7178.1 (7)N3—C19—C20'—O5'−118 (4)
N1—C7—C8—C9102.4 (12)O5'—C20'—C21'—C22'5 (3)
N1—C7—C8—O3−73.4 (9)C19—C20'—C21'—C22'171 (2)
O3—C8—C9—C10−1.0 (11)C20'—C21'—C22'—C23'2 (3)
C7—C8—C9—C10−177.0 (10)C21'—C22'—C23'—O5'−8 (3)
C8—C9—C10—C110.4 (8)C20'—O5'—C23'—C22'12 (3)
C9—C10—C11—O30.3 (6)C18—N3—C24—C2572.2 (3)
C8—O3—C11—C10−1.0 (7)C19—N3—C24—C25−94.2 (2)
C11'—O3'—C8'—C9'1 (2)C28—O6—C25—C26−0.1 (3)
C11'—O3'—C8'—C7178.7 (14)C28—O6—C25—C24−179.9 (2)
N1—C7—C8'—C9'−77 (3)N3—C24—C25—C26−116.6 (3)
N1—C7—C8'—O3'106.3 (17)N3—C24—C25—O663.1 (3)
O3'—C8'—C9'—C10'−1 (2)O6—C25—C26—C27−0.1 (3)
C7—C8'—C9'—C10'−178 (3)C24—C25—C26—C27179.6 (2)
C8'—C9'—C10'—C11'0.1 (18)C25—C26—C27—C280.3 (3)
C9'—C10'—C11'—O3'0.6 (12)C26—C27—C28—O6−0.4 (3)
C8'—O3'—C11'—C10'−1.1 (16)C25—O6—C28—C270.3 (3)
C1—N2—C12—C17−25.9 (4)C18—N4—C29—C3437.3 (3)
C1—N2—C12—C13156.1 (2)C18—N4—C29—C30−145.6 (2)
C17—C12—C13—C14−0.1 (4)C34—C29—C30—C31−1.5 (4)
N2—C12—C13—C14178.0 (2)N4—C29—C30—C31−178.7 (2)
C12—C13—C14—C151.0 (4)C29—C30—C31—C32−0.5 (4)
C13—C14—C15—C16−0.8 (4)C30—C31—C32—C331.6 (4)
C14—C15—C16—C17−0.3 (5)C31—C32—C33—C34−0.8 (4)
C13—C12—C17—C16−1.0 (4)C32—C33—C34—C29−1.2 (4)
N2—C12—C17—C16−179.0 (3)C30—C29—C34—C332.4 (4)
C15—C16—C17—C121.2 (5)N4—C29—C34—C33179.4 (2)
Hydrogen-bond geometry (Å, º) top
Cg1, Cg5 and Cg6 are the centroids of the O2/C3–C6, C12–C17 and C29–C34 rings, respectively.
D—H···AD—HH···AD···AD—H···A
N2—H2N···O1i0.902.032.917 (2)168
N4—H4N···O4ii0.902.072.955 (2)167
C6—H6···Cg6iii0.952.623.482150
C24—H24B···Cg5iv0.992.903.789149
C28—H28···Cg1iv0.952.823.658148
Symmetry codes: (i) x, −y+1/2, z−1/2; (ii) x, −y+3/2, z−1/2; (iii) −x, y+1/2, −z+1/2; (iv) x, y−1, z.
Comparison of the Hirshfeld fingerprint percentages for molecules A and B top
ContactAB
H···H48.450.4
H···C/C···H30.328.3
H···O/O···H17.016.6
C···O/O···C1.71.7
H···N/N···H1.01.5
C···C0.50.5
O···O0.50.5
O···N/N···O0.30.3
C···N/N···C0.30.3
 

Acknowledgements

The authors' contributions are as follows. Conceptualization, TH and ANB; synthesis, DFM and DMS; X-ray analysis, VNK and TH; Hirshfeld surface analysis, TH; founding, KIH; writing (review and editing of the manuscript) TH, KIH and IHM, supervision, TH and ANB.

Funding information

This work was supported by the Russian Science Foundation (Project No. 25–23-00879, https://rscf.ru/project/25–23-00879/). TH is also grateful to Hacettepe University Scientific Research Project Unit (grant No. 013 D04 602 004). This work has also been supported by the Azerbaijan Medical University and Baku Engineering University.

References

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