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

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890

Crystal structure and Hirshfeld surface analysis of 2,6-bis­­[1-(prop-2-yn-1-yl)-1H-benzo[d]imidazol-2-yl]pyridine 0.144-hydrate

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aLaboratory of Heterocyclic Organic Chemistry, Medicines Science Research, Center, Pharmacochemistry Competence Center, Mohammed V University in Rabat, Faculté des Sciences, Av. Ibn Battouta, BP 1014, Rabat, Morocco, bRegional Center for Education and Training Professions in the Rabat Region, Morocco, cDepartment of Physics, Hacettepe University, 06800 Beytepe, Ankara, Türkiye, dUniversity of Zurich, Department of Chemistry B, Winterthurerstrasse 190, 8057 Zurich, Switzerland, and eNational Center for Nuclear Energy, Science and Technology, Rabat, Morocco
*Correspondence e-mail: [email protected]

Edited by M. Weil, Vienna University of Technology, Austria (Received 18 September 2025; accepted 3 November 2025; online 11 November 2025)

The title compound, C25H17N5·0.144H2O, contains two substituted benzimidazole ring systems bridged over a pyridine ring and a disordered non-coord­inating water mol­ecule. In the crystal, O—H⋯N and C—H⋯O hydrogen-bonding inter­actions link the mol­ecules into infinite chains parallel to [101]. Furthermore, ππ stacking inter­actions between the imidazole rings and between the pyridine and imidazole rings of adjacent mol­ecules with inter-centroid distances of 3.6371 (4), 3.9872 (5), 3.4916 (4) and 3.6648 (4) Å are present, but C—H⋯π(ring) inter­actions are not observed. Hirshfeld surface analysis of the crystal structure indicates that the most important contributions for the crystal packing are from H⋯H (39.3%), H⋯C/C⋯H (35.9%) and H⋯N/N⋯H (9.1%).

1. Chemical context

Heterocyclic compounds occupy a central position in medicinal chemistry as they are key elements in the search for the and development of new bioactive mol­ecules for the pharmaceutical industry (Vitaku et al., 2014View full citation). Among them, nitro­gen-containing heterocycles exhibit a wide range of biological activities due to their structural similarities with numerous natural and synthetic mol­ecules already known for their pharmacological properties (Tahlan et al., 2019View full citation). In this context, benzimidazole is a noteworthy representative and an important pharmacophore and scaffold in medicinal chemistry (Al-Ghulikah et al., 2023View full citation). This core structure is frequently employed as a basis for designing therapeutic mol­ecules of pharmaceutical and biological inter­ests. Benzimidazole derivatives have demonstrated a broad spectrum of biological activities, including anti­histaminic, anti­ulcer, anti­bacterial, anti­parasitic, anti­cancer, anti­viral, anti-inflammatory, anti­oxidant and anti­diabetic properties (Saber et al., 2021View full citation; Leonard et al., 2006View full citation; Reddy et al., 2005View full citation).

Building on our previous work on benzimidazole-based systems (Missioui et al., 2022View full citation; Moussaif et al., 2025View full citation), we now report the synthesis, structure and Hirshfeld surface of the title compound, C25H17N5·0.144H2O. The mol­ecular and crystal structure of this compound was established unambiguously by single-crystal X-ray diffraction. To gain deeper insight into its supra­molecular features, a Hirshfeld surface analysis was undertaken, which enabled the identification and qu­anti­fication of the key inter­molecular inter­actions governing the organization of the crystal structure.

[Scheme 1]

2. Structural commentary

The title compound contains two benzimidazole entities bridged over a pyridine ring, two propyl moieties and a disordered non-coordinating water mol­ecule (Fig. 1[link]). The dihedral angles between the imidazole rings (B, N2/N3/C6–C8; D, N4/N5/C16–C18) and the benzene rings (C, C7–C12; E, C17–C22) of the heterocyclic moieties, are B/C = 1.93 (4)° and D/E = 0.97 (5)°. Thus, the two benzimidazole rings are almost planar. The central pyridine ring (A, N1/C1–C5) is oriented at dihedral angles of 11.77 (4) and 6.64 (3)°, respectively, to the mean plane of the benzimidazole rings B and D. The dihedral angle between the two benzimidazole ring systems BD and DE is 18.26 (3)°. There are no unusual bond lengths or inter­bond angles in the mol­ecule.

[Figure 1]
Figure 1
The mol­ecular structure of the title compound with displacement ellipsoids drawn at the 50% probability level. The disordered water mol­ecule is not shown for clarity.

3. Supra­molecular features

In the crystal, O—H⋯N and C—H⋯O hydrogen-bonding inter­actions (Table 1[link]) between the non-coordinating water mol­ecule and the benzimidazole rings link mol­ecules into infinite chains extending parallel to [101] (Fig. 2[link]). Furthermore, ππ stacking inter­actions between the B rings [centroid-to-centroid distance = 3.6371 (4) Å, α = 0.04 (3)°, slippage = 1.150 Å], B and D rings [centroid-to-centroid distance = 3.9872 (5) Å, α = 1.34 (5)°, slippage = 1.957 Å], D rings [centroid-to-centroid distance = 3.4916 (4) Å, α = 0.00 (5)°, slippage = 0.947 Å] and A and E rings [centroid-to-centroid distance = 3.6648 (4) Å, α = 6.81 (5)°, slippage = 1.461 Å] of adjacent mol­ecules may help to consolidate the packing. C—H⋯π(ring) inter­actions are not observed.

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
O1A—H1A⋯N3iv 0.87 2.14 2.923 (16) 149
O1A—H1B⋯N5 0.87 2.37 3.178 (17) 154
O1B—H1C⋯N3iv 0.87 2.21 2.96 (3) 144
O1B—H1D⋯N5 0.87 2.24 3.07 (4) 161
C9—H9⋯O1Ai 0.95 2.16 2.891 (15) 133
C9—H9⋯O1Bi 0.95 2.15 2.93 (3) 139
C19—H19⋯O1A 0.95 2.36 3.086 (18) 133
Symmetry codes: (i) Mathematical equation; (iv) Mathematical equation.
[Figure 2]
Figure 2
A partial packing diagram of the title compound with inter­molecular O—H⋯N and C—H⋯O hydrogen bonds shown as dashed lines. Hydrogen atoms not involved in these inter­actions have been omitted.

4. Hirshfeld surface analysis

In order to visualize and qu­antify the inter­molecular inter­actions in the crystal, a Hirshfeld surface (HS) analysis was carried out using CrystalExplorer (Spackman et al., 2021View full citation) following the protocol of Tan et al. (2019View full citation) after non-consideration of the partially occupied water molecule. Fig. 3[link] shows the contact distances where the bright-red spots correspond to the respective donors and/or acceptors noted above; numerical values of contact distances are collated in Table 2[link]. According to the two-dimensional fingerprint plots (McKinnon et al., 2007View full citation), the H⋯H, H⋯ C/C⋯H and H⋯N/N⋯H contacts make the most significant contributions to the HS, at 39.3%, 35.9%, 14.5% and 9.1%, respectively (Table 2[link], Fig. 4[link]).

Table 2
Selected interatomic distances (Å)

H9⋯O1Ai 2.16 C12⋯C14 3.376 (2)
H4⋯O1Aii 2.62 C16⋯C17vi 3.3783 (19)
O1A⋯H19 2.36 C1⋯H23B 2.89
O1B⋯H1D 0.87 H1A⋯C4iv 2.85
H9⋯O1Bi 2.15 C5⋯H13B 2.87
H13A⋯O1Biii 2.37 C13⋯H23B 2.86
O1B⋯H1C 0.87 C14⋯H23B 2.78
N1⋯N4 2.9842 (16) C18⋯H1B 2.56
N1⋯C13 3.0587 (18) C18⋯H1D 2.60
N1⋯N2 3.0092 (16) C19⋯H1B 2.38
N1⋯C23 3.012 (2) C19⋯H1D 2.64
N1⋯H23B 2.34 C22⋯H23A 2.87
N1⋯H13B 2.36 C23⋯H13B 2.85
H1A⋯N3iv 2.14 C24⋯H13B 2.74
N3⋯H25v 2.46 H1A⋯H19 2.37
H1C⋯N3iv 2.21 H4⋯H1Aii 1.96
N3⋯H4 2.44 H1B⋯H19 1.83
N5⋯H2 2.45 H4⋯H1Cii 2.37
N5⋯H1B 2.37 H1C⋯H1D 1.38
N5⋯H1D 2.24 H1D⋯H19 2.21
C2⋯C22vi 3.381 (2) H13B⋯H23B 2.19
C5⋯C21vi 3.392 (2) H19⋯H1A 2.37
C5⋯C20vi 3.386 (2)    
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation; (v) Mathematical equation; (vi) Mathematical equation.
[Figure 3]
Figure 3
View of the three-dimensional Hirshfeld surface plotted over dnorm.
[Figure 4]
Figure 4
Two-dimensional fingerprint plots, showing (a) all inter­actions, and delineated into (b) H⋯H, (c) H⋯C/C⋯H, (d) H⋯N/N⋯H, (e) C⋯C, (f) H⋯O/O⋯H, (g) C⋯N/N⋯C and (h) N⋯N inter­actions. The di and de values are the closest inter­nal and external distances (in Å) from given points on the Hirshfeld surface contacts.

5. Database survey

A search of the Cambridge Structural Database (CSD, July 2025 update; Groom et al., 2016View full citation) revealed several entries closely related to the title compound, a derivative of 2-(6-(1H-benzo[d]imidazol-2-yl)pyridin-2-yl)-1H-benzo[d]imidazole. The most relevant analogs are illustrated in Fig. 5[link] and include compounds I (CSD refcode DIXNUU; Liu et al., 2007View full citation), II (MOTGEI; Chen et al., 2009View full citation), III (WAKJID01; Gong et al., 2012View full citation), IV (VAPTEN; Gong et al., 2012View full citation), V (VAPTEN; Gong et al., 2012View full citation), and VI (VAPVEP; Gong et al., 2012View full citation). A detailed comparative analysis of these structures and the title compound highlights both common structural characteristics and distinctive features.

[Figure 5]
Figure 5
Structures closely related to the title compound according to a CSD search.

Core mol­ecular geometry. All compounds display a benzimidazole–pyridine–benzimidazole framework that remains essentially planar. Compounds IIII, exhibit classical N—H⋯N or N—H⋯O hydrogen bonds between the constituents, which leads to the formation of supra­molecular chains or layers. In the title compound, however, the hydrogen-bonding network is more compact and directional, leading to a more compact packing arrangement than in the other analogues.

Influence of metal coordination. Compounds IVVI feature coordination to metals, which significantly alters both structural details within the organic ligands and in the supra­molecular packing modes.

Crystal packing and ππ stacking. In all of the above related structures, ππ stacking appears to play a significant role in consolidating the crystal structure. Notably, the title compound exhibits slightly shorter centroid-to-centroid distances compared to its metal-coordinating analogues, indicating stronger inter­molecular ππ inter­actions. This comparative structural analysis demonstrates that the title compound, although it shares a common mol­ecular framework with its analogues, has a unique supra­molecular organization that is governed by the absence of metal coordination and the predominance of hydrogen-bonding and ππ stacking inter­actions. These observations provide insight into the impact of structural modifications on mol­ecular packing and overall crystal architectures.

6. Synthesis and crystallization

The synthesis of the title compound is shown schematically in Fig. 6[link]. In a 100 ml round-bottom flask, 2,6-bis­(1H-benzo[d]imidazol-2-yl)pyridine (1) (0.30 g, 0.96 mmol) was combined with potassium carbonate (K2CO3) (0.34 g, 2.49 mmol) in 10 ml of dimethylformamide (DMF). The mixture was stirred at room temperature for 15 min to ensure homogenization. Subsequently, propargyl bromide (2) (0.20 ml, 2.30 mmol) was added dropwise under continuous stirring. The progress of the reaction was monitored by thin-layer chromatography (TLC), and stirring was continued for 8 h at room temperature. After completion, the solvent was removed under reduced pressure using a rotary evaporator. The resulting crude residue was extracted with ethyl acetate and water. The organic layer was collected, dried over anhydrous sodium sulfate, and filtered. Purification by recrystallization from ethanol solution afforded the title compound (3) in 75% yield (Fig. 6[link]). 1H NMR (500 MHz, DMSO-d6) δ (ppm): 9.30 (d; J = 7.9 Hz; 2H; CHpyr); 9.11 (dd; J = 8.2, 7.6 Hz; 1H; CHpyr); 8.69–8.20 (m; 8H; CHAr); 6.68 (d; 4H; J = 2.5 Hz; –NCH2); 4.23 (t; 2H; –CCH).

[Figure 6]
Figure 6
Reaction scheme for obtaining the title compound.

7. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 3[link]. After refinement of the organic mol­ecule (R1/wR2 = 0.0528/0.1440), relatively high residual electron density was located between mol­ecules, pointing to an underoccupied oxygen atom of a water mol­ecule. Additional positional disorder using SIMU restraints was introduced, and the occupancies independently refined. The ‘add-H′ tool in OLEX2 (Dolomanov et al., 2009View full citation) was used for the H atoms of the water mol­ecules, with a fixed O—H distance of 0.87 Å and Uiso(H) = 1.5Ueq(O). Other hydrogen atom positions were calculated geometrically at CH = 0.95 Å and CH2 = 0.99 Å and refined using a riding model with Uiso(H) = 1.2Ueq(C).

Table 3
Experimental details

Crystal data
Chemical formula C25H17N5·0.144H2O
Mr 390.04
Crystal system, space group Monoclinic, P21/n
Temperature (K) 160
a, b, c (Å) 9.6858 (2), 13.7005 (2), 15.0908 (3)
β (°) 102.943 (2)
V3) 1951.68 (6)
Z 4
Radiation type Cu Kα
μ (mm−1) 0.65
Crystal size (mm) 0.22 × 0.15 × 0.07
 
Data collection
Diffractometer XtaLAB Synergy, Dualflex, HyPix
Absorption correction Analytical [CrysAlis PRO (Rigaku OD, 2024View full citation) using a multifaceted crystal model (Clark & Reid, 1995View full citation)]
Tmin, Tmax 0.900, 0.965
No. of measured, independent and observed [I > 2σ(I)] reflections 21779, 4122, 3852
Rint 0.022
(sin θ/λ)max−1) 0.633
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.102, 1.07
No. of reflections 4122
No. of parameters 298
No. of restraints 6
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.26, −0.17
Computer programs: CrysAlis PRO (Rigaku OD, 2024View full citation), SHELXT (Sheldrick, 2015aView full citation), SHELXL (Sheldrick, 2015bView full citation), OLEX2 (Dolomanov et al., 2009View full citation) and publCIF (Westrip, 2010View full citation).

Supporting information


Computing details top

2,6-Bis[1-(prop-2-yn-1-yl)-1H-benzo[d]imidazol-2-yl]pyridine 0.144-hydrate top
Crystal data top
C25H17N5·0.144H2OF(000) = 814
Mr = 390.04Dx = 1.327 Mg m3
Monoclinic, P21/nCu Kα radiation, λ = 1.54184 Å
a = 9.6858 (2) ÅCell parameters from 13938 reflections
b = 13.7005 (2) Åθ = 3.0–78.9°
c = 15.0908 (3) ŵ = 0.65 mm1
β = 102.943 (2)°T = 160 K
V = 1951.68 (6) Å3Plate, colourless
Z = 40.22 × 0.15 × 0.07 mm
Data collection top
XtaLAB Synergy, Dualflex, HyPix
diffractometer
4122 independent reflections
Radiation source: micro-focus sealed X-ray tube, PhotonJet (Cu) X-ray Source3852 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.022
Detector resolution: 10.0000 pixels mm-1θmax = 77.4°, θmin = 4.4°
ω scansh = 1212
Absorption correction: analytical
[CrysAlisPro (Rigaku OD, 2024) using a multifaceted crystal model (Clark & Reid, 1995)]
k = 1617
Tmin = 0.900, Tmax = 0.965l = 1917
21779 measured reflections
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.043 w = 1/[σ2(Fo2) + (0.0359P)2 + 0.7695P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.102(Δ/σ)max = 0.001
S = 1.07Δρmax = 0.26 e Å3
4122 reflectionsΔρmin = 0.16 e Å3
298 parametersExtinction correction: SHELXL-2019/2 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
6 restraintsExtinction coefficient: 0.00117 (14)
Primary atom site location: dual
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)
O1A0.5569 (16)0.8667 (13)0.4309 (17)0.053 (5)0.094 (6)
H1A0.6315310.8888040.4144290.079*0.094 (6)
H1B0.5806000.8082010.4511400.079*0.094 (6)
O1B0.586 (3)0.877 (3)0.479 (3)0.055 (6)0.050 (5)
H1C0.6491540.8902040.4484560.083*0.050 (5)
H1D0.5869360.8132220.4832980.083*0.050 (5)
N10.46815 (11)0.54778 (8)0.72961 (8)0.0360 (3)
N20.47168 (11)0.42143 (8)0.89321 (8)0.0353 (2)
N30.26310 (12)0.49018 (9)0.89744 (8)0.0422 (3)
N40.64889 (11)0.52420 (8)0.59477 (8)0.0356 (2)
N50.55002 (13)0.66248 (9)0.52978 (8)0.0437 (3)
C10.46243 (14)0.61188 (10)0.66146 (10)0.0386 (3)
C20.36641 (17)0.68994 (11)0.64552 (11)0.0476 (4)
H20.3676140.7352840.5980730.057*
C30.27084 (18)0.69972 (12)0.69953 (11)0.0518 (4)
H30.2041340.7516430.6895510.062*
C40.27245 (17)0.63337 (11)0.76859 (10)0.0477 (4)
H40.2060540.6381480.8061570.057*
C50.37380 (14)0.55902 (10)0.78210 (9)0.0382 (3)
C60.37072 (14)0.49008 (10)0.85648 (9)0.0372 (3)
C70.42394 (14)0.37547 (10)0.96244 (9)0.0372 (3)
C80.29418 (15)0.41936 (10)0.96437 (10)0.0404 (3)
C90.21911 (17)0.39074 (12)1.02873 (11)0.0485 (4)
H90.1308870.4198851.0308060.058*
C100.27767 (18)0.31844 (12)1.08943 (11)0.0509 (4)
H100.2293060.2981931.1345360.061*
C110.40679 (17)0.27434 (11)1.08590 (11)0.0480 (4)
H110.4433270.2244441.1284180.058*
C120.48269 (15)0.30134 (11)1.02228 (10)0.0427 (3)
H120.5698820.2710541.0195710.051*
C130.60936 (13)0.39938 (10)0.87291 (10)0.0368 (3)
H13A0.6837420.4022830.9297740.044*
H13B0.6315480.4493530.8307960.044*
C140.61060 (14)0.30259 (10)0.83176 (10)0.0391 (3)
C150.61316 (17)0.22284 (12)0.80235 (12)0.0507 (4)
H150.6152120.1587240.7787000.061*
C160.55498 (14)0.59963 (10)0.59699 (9)0.0378 (3)
C170.70860 (14)0.54168 (10)0.52136 (9)0.0387 (3)
C180.64509 (15)0.62793 (11)0.48159 (10)0.0429 (3)
C190.68005 (17)0.66414 (12)0.40296 (11)0.0511 (4)
H190.6368230.7216200.3741860.061*
C200.77899 (17)0.61388 (13)0.36863 (11)0.0547 (4)
H200.8048020.6376320.3154450.066*
C210.84308 (16)0.52855 (13)0.40971 (11)0.0503 (4)
H210.9118300.4963110.3841390.060*
C220.80837 (15)0.49030 (12)0.48667 (10)0.0445 (3)
H220.8504880.4319970.5143470.053*
C230.68304 (13)0.43763 (9)0.65209 (9)0.0353 (3)
H23A0.6887190.3801650.6132930.042*
H23B0.6063400.4257330.6844800.042*
C240.81836 (14)0.44900 (10)0.71894 (9)0.0377 (3)
C250.92809 (15)0.45846 (12)0.77189 (11)0.0470 (4)
H251.0160510.4660480.8143360.056*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O1A0.027 (7)0.053 (7)0.080 (13)0.000 (5)0.016 (8)0.010 (9)
O1B0.032 (10)0.053 (10)0.081 (15)0.001 (8)0.014 (11)0.002 (13)
N10.0326 (5)0.0309 (5)0.0393 (6)0.0027 (4)0.0030 (4)0.0031 (5)
N20.0305 (5)0.0328 (5)0.0391 (6)0.0029 (4)0.0006 (4)0.0035 (5)
N30.0374 (6)0.0421 (6)0.0450 (6)0.0055 (5)0.0046 (5)0.0088 (5)
N40.0299 (5)0.0328 (5)0.0404 (6)0.0006 (4)0.0000 (4)0.0046 (5)
N50.0413 (6)0.0350 (6)0.0482 (7)0.0020 (5)0.0036 (5)0.0063 (5)
C10.0368 (7)0.0310 (6)0.0416 (7)0.0028 (5)0.0047 (5)0.0025 (5)
C20.0534 (9)0.0372 (7)0.0456 (8)0.0131 (6)0.0030 (7)0.0011 (6)
C30.0571 (9)0.0442 (8)0.0480 (8)0.0242 (7)0.0012 (7)0.0042 (7)
C40.0480 (8)0.0453 (8)0.0452 (8)0.0172 (7)0.0005 (6)0.0066 (6)
C50.0357 (7)0.0348 (7)0.0395 (7)0.0062 (5)0.0014 (5)0.0075 (5)
C60.0331 (6)0.0345 (6)0.0395 (7)0.0050 (5)0.0014 (5)0.0091 (5)
C70.0360 (7)0.0343 (7)0.0382 (7)0.0034 (5)0.0015 (5)0.0075 (5)
C80.0385 (7)0.0374 (7)0.0423 (7)0.0009 (6)0.0032 (6)0.0108 (6)
C90.0456 (8)0.0477 (8)0.0539 (9)0.0032 (6)0.0145 (7)0.0141 (7)
C100.0580 (9)0.0463 (8)0.0501 (9)0.0118 (7)0.0159 (7)0.0094 (7)
C110.0546 (9)0.0417 (8)0.0453 (8)0.0078 (7)0.0058 (7)0.0020 (6)
C120.0410 (7)0.0382 (7)0.0449 (8)0.0012 (6)0.0014 (6)0.0020 (6)
C130.0286 (6)0.0339 (6)0.0443 (7)0.0026 (5)0.0010 (5)0.0000 (6)
C140.0332 (6)0.0384 (7)0.0448 (7)0.0050 (5)0.0069 (6)0.0031 (6)
C150.0524 (9)0.0385 (8)0.0637 (10)0.0051 (7)0.0185 (8)0.0041 (7)
C160.0332 (6)0.0307 (6)0.0430 (7)0.0011 (5)0.0051 (5)0.0017 (5)
C170.0305 (6)0.0407 (7)0.0399 (7)0.0081 (5)0.0024 (5)0.0038 (6)
C180.0372 (7)0.0387 (7)0.0455 (8)0.0104 (6)0.0060 (6)0.0067 (6)
C190.0462 (8)0.0495 (9)0.0505 (9)0.0148 (7)0.0041 (7)0.0135 (7)
C200.0472 (9)0.0660 (10)0.0455 (8)0.0238 (8)0.0008 (7)0.0105 (8)
C210.0363 (7)0.0656 (10)0.0463 (8)0.0139 (7)0.0036 (6)0.0009 (7)
C220.0335 (7)0.0503 (8)0.0459 (8)0.0062 (6)0.0009 (6)0.0041 (7)
C230.0325 (6)0.0296 (6)0.0410 (7)0.0018 (5)0.0022 (5)0.0040 (5)
C240.0340 (7)0.0351 (7)0.0430 (7)0.0042 (5)0.0064 (6)0.0048 (6)
C250.0358 (7)0.0521 (9)0.0488 (8)0.0023 (6)0.0006 (6)0.0066 (7)
Geometric parameters (Å, º) top
O1A—H1A0.8700C9—H90.9500
O1A—H1B0.8697C9—C101.382 (2)
O1B—H1C0.8704C10—H100.9500
O1B—H1D0.8701C10—C111.401 (2)
N1—C11.3441 (18)C11—H110.9500
N1—C51.3456 (18)C11—C121.384 (2)
N2—C61.3804 (16)C12—H120.9500
N2—C71.3850 (18)C13—H13A0.9900
N2—C131.4650 (17)C13—H13B0.9900
N3—C61.3257 (18)C13—C141.4654 (19)
N3—C81.3841 (19)C14—C151.182 (2)
N4—C161.3821 (17)C15—H150.9500
N4—C171.3805 (18)C17—C181.403 (2)
N4—C231.4616 (16)C17—C221.389 (2)
N5—C161.3231 (18)C18—C191.396 (2)
N5—C181.379 (2)C19—H190.9500
C1—C21.4022 (19)C19—C201.372 (3)
C1—C161.473 (2)C20—H200.9500
C2—H20.9500C20—C211.401 (2)
C2—C31.370 (2)C21—H210.9500
C3—H30.9500C21—C221.383 (2)
C3—C41.380 (2)C22—H220.9500
C4—H40.9500C23—H23A0.9900
C4—C51.3975 (19)C23—H23B0.9900
C5—C61.472 (2)C23—C241.4722 (18)
C7—C81.3995 (19)C24—C251.185 (2)
C7—C121.393 (2)C25—H250.9500
C8—C91.394 (2)
H9···O1Ai2.16C12···C143.376 (2)
H4···O1Aii2.62C16···C17vi3.3783 (19)
O1A···H192.36C1···H23B2.89
O1B···H1D0.87H1A···C4iv2.85
H9···O1Bi2.15C5···H13B2.87
H13A···O1Biii2.37C13···H23B2.86
O1B···H1C0.87C14···H23B2.78
N1···N42.9842 (16)C18···H1B2.56
N1···C133.0587 (18)C18···H1D2.60
N1···N23.0092 (16)C19···H1B2.38
N1···C233.012 (2)C19···H1D2.64
N1···H23B2.34C22···H23A2.87
N1···H13B2.36C23···H13B2.85
H1A···N3iv2.14C24···H13B2.74
N3···H25v2.46H1A···H192.37
H1C···N3iv2.21H4···H1Aii1.96
N3···H42.44H1B···H191.83
N5···H22.45H4···H1Cii2.37
N5···H1B2.37H1C···H1D1.38
N5···H1D2.24H1D···H192.21
C2···C22vi3.381 (2)H13B···H23B2.19
C5···C21vi3.392 (2)H19···H1A2.37
C5···C20vi3.386 (2)
H1A—O1A—H1B104.5C12—C11—C10121.92 (15)
H1C—O1B—H1D104.5C12—C11—H11119.0
C1—N1—C5117.30 (11)C7—C12—H12121.9
C6—N2—C7106.65 (11)C11—C12—C7116.18 (14)
C6—N2—C13130.75 (12)C11—C12—H12121.9
C7—N2—C13122.50 (11)N2—C13—H13A109.3
C6—N3—C8105.92 (11)N2—C13—H13B109.3
C16—N4—C23130.94 (12)N2—C13—C14111.68 (11)
C17—N4—C16106.62 (11)H13A—C13—H13B107.9
C17—N4—C23122.40 (11)C14—C13—H13A109.3
C16—N5—C18105.49 (12)C14—C13—H13B109.3
N1—C1—C2122.79 (14)C15—C14—C13177.08 (16)
N1—C1—C16120.28 (12)C14—C15—H15180.0
C2—C1—C16116.88 (13)N4—C16—C1127.05 (12)
C1—C2—H2120.6N5—C16—N4112.28 (13)
C3—C2—C1118.89 (15)N5—C16—C1120.61 (12)
C3—C2—H2120.6N4—C17—C18105.48 (13)
C2—C3—H3120.3N4—C17—C22131.78 (13)
C2—C3—C4119.33 (14)C22—C17—C18122.73 (14)
C4—C3—H3120.3N5—C18—C17110.13 (13)
C3—C4—H4120.7N5—C18—C19130.10 (14)
C3—C4—C5118.62 (15)C19—C18—C17119.75 (15)
C5—C4—H4120.7C18—C19—H19121.1
N1—C5—C4123.03 (14)C20—C19—C18117.73 (15)
N1—C5—C6120.51 (11)C20—C19—H19121.1
C4—C5—C6116.44 (13)C19—C20—H20119.0
N2—C6—C5127.57 (12)C19—C20—C21121.95 (15)
N3—C6—N2111.95 (13)C21—C20—H20119.0
N3—C6—C5120.47 (12)C20—C21—H21119.3
N2—C7—C8105.87 (12)C22—C21—C20121.39 (16)
N2—C7—C12131.57 (13)C22—C21—H21119.3
C12—C7—C8122.56 (14)C17—C22—H22121.8
N3—C8—C7109.61 (13)C21—C22—C17116.43 (15)
N3—C8—C9130.06 (14)C21—C22—H22121.8
C9—C8—C7120.32 (14)N4—C23—H23A109.3
C8—C9—H9121.2N4—C23—H23B109.3
C10—C9—C8117.58 (15)N4—C23—C24111.62 (11)
C10—C9—H9121.2H23A—C23—H23B108.0
C9—C10—H10119.3C24—C23—H23A109.3
C9—C10—C11121.43 (15)C24—C23—H23B109.3
C11—C10—H10119.3C25—C24—C23179.18 (16)
C10—C11—H11119.0C24—C25—H25180.0
N1—C1—C2—C32.3 (2)C8—N3—C6—N20.42 (15)
N1—C1—C16—N43.0 (2)C8—N3—C6—C5178.67 (11)
N1—C1—C16—N5179.95 (12)C8—C7—C12—C111.4 (2)
N1—C5—C6—N213.2 (2)C8—C9—C10—C110.9 (2)
N1—C5—C6—N3167.82 (12)C9—C10—C11—C120.6 (2)
N2—C7—C8—N30.31 (15)C10—C11—C12—C70.5 (2)
N2—C7—C8—C9178.53 (12)C12—C7—C8—N3179.96 (12)
N2—C7—C12—C11178.18 (13)C12—C7—C8—C91.1 (2)
N3—C8—C9—C10178.54 (14)C13—N2—C6—N3176.46 (12)
N4—C17—C18—N50.41 (15)C13—N2—C6—C52.6 (2)
N4—C17—C18—C19178.00 (12)C13—N2—C7—C8176.56 (11)
N4—C17—C22—C21178.90 (13)C13—N2—C7—C123.1 (2)
N5—C18—C19—C20179.42 (14)C16—N4—C17—C180.70 (14)
C1—N1—C5—C40.05 (19)C16—N4—C17—C22179.75 (14)
C1—N1—C5—C6178.26 (11)C16—N4—C23—C24102.55 (15)
C1—C2—C3—C40.7 (2)C16—N5—C18—C170.06 (15)
C2—C1—C16—N4174.45 (13)C16—N5—C18—C19178.26 (14)
C2—C1—C16—N52.62 (19)C16—C1—C2—C3175.04 (14)
C2—C3—C4—C51.1 (2)C17—N4—C16—N50.79 (15)
C3—C4—C5—N11.5 (2)C17—N4—C16—C1178.07 (12)
C3—C4—C5—C6179.86 (13)C17—N4—C23—C2480.13 (15)
C4—C5—C6—N2168.33 (13)C17—C18—C19—C201.4 (2)
C4—C5—C6—N310.61 (19)C18—N5—C16—N40.53 (15)
C5—N1—C1—C21.97 (19)C18—N5—C16—C1178.00 (11)
C5—N1—C1—C16175.30 (11)C18—C17—C22—C210.0 (2)
C6—N2—C7—C80.05 (14)C18—C19—C20—C210.5 (2)
C6—N2—C7—C12179.67 (14)C19—C20—C21—C220.6 (2)
C6—N2—C13—C14113.23 (15)C20—C21—C22—C170.9 (2)
C6—N3—C8—C70.45 (15)C22—C17—C18—N5179.57 (12)
C6—N3—C8—C9178.24 (14)C22—C17—C18—C191.2 (2)
C7—N2—C6—N30.23 (15)C23—N4—C16—N5176.85 (12)
C7—N2—C6—C5178.78 (12)C23—N4—C16—C10.4 (2)
C7—N2—C13—C1471.06 (15)C23—N4—C17—C18177.19 (11)
C7—C8—C9—C100.0 (2)C23—N4—C17—C221.9 (2)
Symmetry codes: (i) x+1/2, y1/2, z+3/2; (ii) x1/2, y+3/2, z+1/2; (iii) x+3/2, y1/2, z+3/2; (iv) x+1/2, y+3/2, z1/2; (v) x1, y, z; (vi) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1A—H1A···N3iv0.872.142.923 (16)149
O1A—H1B···N50.872.373.178 (17)154
O1B—H1C···N3iv0.872.212.96 (3)144
O1B—H1D···N50.872.243.07 (4)161
C9—H9···O1Ai0.952.162.891 (15)133
C9—H9···O1Bi0.952.152.93 (3)139
C19—H19···O1A0.952.363.086 (18)133
Symmetry codes: (i) x+1/2, y1/2, z+3/2; (iv) x+1/2, y+3/2, z1/2.
 

Funding information

TH is grateful to Hacettepe University Scientific Research Project Unit (grant No. 013 D04 602 004).

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