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 (Z)-8-methyl-2-(8-methyl-2,3,4,9-tetra­hydro­carbazol-1-yl­­idene)-2,3,4,9-tetra­hydro­carbazol-1-one

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aDepartment of Chemistry, RV College of Engineering, Bangalore 560 059, Karnataka, India, and bPrincipal (Retired), 63 Shanthi Nagar, 5th Street, Nanjikottai Road, Thanjavur 613 006, Tamilnadu, India
*Correspondence e-mail: [email protected], [email protected]

Edited by W. T. A. Harrison, University of Aberdeen, United Kingdom (Received 2 March 2026; accepted 1 April 2026; online 10 April 2026)

In the title compound, C26H24N2O, the dihedral angle between the indole fused ring units is 36.37 (5)° and an intra­molecular N—H⋯O hydrogen bond closes an S(7) ring. In the extended structure, inversion dimers linked by pairwise N—H⋯O hydrogen bonds generate an R22(10) loop. Secondary C—H⋯π contacts consolidate the packing and a ππ stacking inter­action is also observed. The contributions of the different inter­actions towards the crystal packing were analysed using Hirshfeld surface and fingerprint plots, showing that the largest contributions come from H⋯H (59.5%) and C⋯H/H⋯C contacts (28.5%).

1. Chemical context

Dicarbazole derivatives have attracted considerable inter­est in organic optoelectronics due to their high hole mobility, excellent thermal stability, and robust electrochemical durability (Matsuda et al., 2025View full citation). Synthetic strategies for these compounds often involve cascade annulations, palladium-catalysed tandem reactions, or oxidative cyclizations, enabling access to highly functionalized frameworks. With this view, an attempt has been invested to prepare these classes of compounds using 2,3,4,9-tetra­hydro­carbazol-1-ones (Sridharan et al., 2026View full citation) as precursors via an easily accessible inter­mediate. As part of these studies, we now describe the synthesis, crystal structure and Hirshfeld surface analysis of the title compound, C26H24N2O (I).

[Scheme 1]

2. Structural commentary

As shown in Fig. 1[link], compound (I) consists of two indole and two cyclo­hexene units fused via the C13—C14 bond. The dihedral angle between the pyrrole rings (C6–C9/N1 and C18/C17/C20/C25/N2) is 37.29 (8)°. The first pair of fused pyrrole and benzene (C2–C7) rings are nearly co-planar, subtending a dihedral angle of 3.13 (8)°. Similarly, the dihedral angle between the second pair of pyrrole and benzene (C20–C25) rings is 3.02 (7)°. The dihedral angle between the benzene rings is 35.99 (7)°.

[Figure 1]
Figure 1
The mol­ecular structure of (I), showing displacement ellipsoids drawn at the 50% probability level.

A puckering analysis (Cremer & Pople, 1975View full citation) of the six-membered A (C8–C13) cyclo­hexene ring gave the parameters: q2 = 0.3516 (16) Å, q3 = −0.2825 (16) Å, QT = 0.4510 (16) Å, θ = 128.8 (2)° and φ = 12.2 (3)°, corresponding to an envelope conformation where atom C11 is at the flap position and displaced by 0.615 (2) Å from best plane of the remaining atoms. A similar analysis for ring B (C14–C19) gave q2 = 0.3925 (15) Å, q3 = −0.2247 (15) Å, QT = 0.4523 (15) Å, θ = 119.79 (19)° and φ = 240.7 (2)°, indicating an envelope conformation, where atom C15 is at the flap position and 0.621 (2) Å away from best plane of the remaining atoms. An intra­molecular N1—H1⋯O1 hydrogen bond forms an S(7) ring motif (Fig. 1[link] and Table 1[link]).

Table 1
Hydrogen-bond geometry (Å, °)

Cg1 and Cg3 are the centroids of the pyrrole (N1/C7/C6/C9/C8) and benzene (C2–C7) rings, respectively.

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1⋯O1 0.887 (18) 1.887 (18) 2.6470 (16) 142.6 (15)
N2—H2⋯O1i 0.887 (19) 2.103 (19) 2.9574 (17) 161.4 (16)
C12—H12BCg1ii 0.99 2.90 3.876 (2) 170
C21—H21⋯Cg3iii 0.95 2.86 3.736 (2) 154
C26—H26CCg1i 0.98 2.70 3.549 (2) 145
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation.

3. Supra­molecular features

In the crystal, the mol­ecules of (I) associate via pairwise N2—H2⋯O1i [symmetry code: (i) 2 − x, −y, −z] hydrogen bonds (Table 1[link]) into inversion dimers with an R22(10) loop graph-set motif (Fig. 2[link]). The packing also exhibits three C—H⋯π inter­actions (Fig. 3[link] and Table 1[link]) involving the pyrrole (N1/C7/C6/C9/C8) and the benzene (C2–C7) rings. The mol­ecules further exhibit slipped ππ stacking inter­actions: Cg2⋯Cg6(1 − x, −y, −z) = 3.5739 (15) Å, slippage = 0.891 Å and Cg6⋯Cg6(1 − x, −y, −z) = 3.6763 (16) Å, slippage = 1.246 Å; where Cg2 and Cg6 are the centroids of the pyrrole ring (N2/C18/C17/C20/C25) and the benzene ring (C20–C25) respectively (Fig. 4[link]).

[Figure 2]
Figure 2
Partial packing view of (I), viewed down the a-axis direction with black dashed lines representing N—H⋯O hydrogen bonds.
[Figure 3]
Figure 3
Straw-style packing view of (I), viewed down the a-axis direction, showing the C—H⋯π contacts. Centroids are given as green spheres and black dashed lines are H⋯π contacts.
[Figure 4]
Figure 4
The stick-style crystal structure of (I), showing the formation of ππ stacking inter­actions [Symmetry code: (a) 1 − x, −y, −z]. Green dashed lines indicate the ππ contacts.

4. Database survey

A search of the Cambridge Structural Database (CSD, Version 6.01, updated to November 2025; Groom et al., 2016View full citation) using the core structure of (I) gave zero hits.

5. Hirshfeld surface (HS) and 2D fingerprint plots

CrystalExplorer (Version 21.5; Spackman et al., 2021View full citation) was used to investigate and visualize further the inter­molecular inter­actions of (I). The HS plotted over dnorm in the range from −0.48 to 1.34 a.u. is shown in Fig. 5[link](a). The electrostatic potential surface using the STO-3G basis set at the Hartree Fock level of theory and mapped on the Hirshfeld surface over the range from −0.05 to 0.05 a.u. clearly shows the positions of the close inter­molecular contacts in the compound [Fig. 5[link](b)]. The positive electrostatic potential (blue area) over the surface indicates hydrogen-donor potential, whereas the negative (red area) represents the hydrogen-bond acceptors.

[Figure 5]
Figure 5
(a) View of the three-dimensional Hirshfeld surface of (I), plotted over dnorm in the range from −0.48 to 1.34 a.u. with a neighbouring mol­ecule. The inter­molecular hydrogen bonds are depicted by green dashed lines. (b) View of the three-dimensional electrostatic potential surface of (I) plotted over the range from −0.05 to 0.05 a.u., using the STO-3 G basis set at the Hartree–Fock method of theory.

The overall two-dimensional fingerprint plot is shown in Fig. 6[link](a), while those delineated into C⋯H/H⋯C, C⋯N/N⋯C, H⋯N/N⋯H, H⋯O/O⋯H, C⋯C and H⋯H contacts are illustrated in Fig. 6[link](b)–6(g), respectively, together with their relative contributions to the Hirshfeld surface. The most significant inter­action type is H⋯H, contributing 59.5% to the Hirshfeld surface, which is reflected in Fig. 6[link](g) as widely scattered points of high density due to the large hydrogen content of the mol­ecule. In the presence of C⋯H inter­actions, the pair of characteristic wings in the fingerprint plot is delineated into C⋯H/H⋯C contacts [28.5% contribution to the HS; Fig. 6[link](b)]. The C⋯N/N⋯C contacts contribute only 0.8% [Fig. 6[link](c)]. The H⋯N/N⋯H contacts contribute 2.9% [Fig. 6[link](d)]. The H⋯O/O⋯H contribute 5.7% [Fig. 6[link](e)] and finally, the C⋯C contacts [Fig. 6[link](f)] contribute only 2.7%. The packing of (I) is thus dominated by van der Waals inter­actions despite the presence of N—H⋯O hydrogen bonds.

[Figure 6]
Figure 6
Two-dimensional fingerprint plots for (I), showing (a) all inter­actions, and delineated into (b) C⋯H/H.·C, (c) C⋯N/N⋯C, (d) H⋯N/N⋯H, (e) H⋯O/O⋯H, (f) C⋯C and (g) H⋯H inter­actions. The di and de values are the closest inter­nal and external distances (in Å) from given points on the Hirshfeld surface.

6. Synthesis and crystallization

8-Methyl-2,3,4,9-tetrahydrocarbazol-1-one (1.0 g, 0.005 mol) in di­chloro­methane (15 ml) was added to an ice-cooled solution of di­eth­oxy­carbenium fluoro­borate (prepared in situ from BF3·Et2O (1.65 ml, 0.01 mol) and HC(OEt3) (1.25 ml, 0.01 mol). The reaction mixture was kept at 258–263 K. To this mixture, tri­ethyl­amine (0.01 mol) was added dropwise and the stirring was continued over a period of five h. The reaction was monitored by TLC. After the completion of the reaction, the excess solvent was then removed and extracted using ethyl acetate dried over anhydrous sodium sulfate. The brown solid separated out was then separated by column chromatography over silica gel using petroleum ether: ethyl acetate as eluants (99:1) and (95:5) to yield (Z)-8-methyl-2,3,4,9-tetra­hydro-2-(8′-methyl-2′,3′,4′,9′-tetra­hydro­carbazol-1-yl­idene)-carbazol-1-one (2) and (Z)-2-(eth­oxy­methyl­ene)-8-methyl-2,3,4,9-tetra­hydro-1H-carbazol-1-one (3), respectively. The chemical structure of the final products was confirmed by NMR Spectroscopy and elemental analysis data. Compound 2 was recrystallized using ethanol as solvent as yellow prisms of (I) (0.355 g, 18%), m.p.415–417 K. The rection scheme is shown in Fig. 7[link].

[Figure 7]
Figure 7
The synthesis scheme for (I).

7. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link]. The N-bonded H atoms were located in a difference Fourier map and refined isotropically with Uiso(H) = 1.2Ueq(N). All the other H atoms were placed in calculated positions and were refined as riding atoms with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C). The methyl hydrogen atoms were allowed to rotate, but not to tip, to best fit the experimental electron density.

Table 2
Experimental details

Crystal data
Chemical formula C26H24N2O
Mr 380.47
Crystal system, space group Monoclinic, P21/n
Temperature (K) 100
a, b, c (Å) 9.424 (3), 15.566 (5), 13.530 (5)
β (°) 101.748 (6)
V3) 1943.3 (11)
Z 4
Radiation type Mo Kα
μ (mm−1) 0.08
Crystal size (mm) 0.55 × 0.45 × 0.35
 
Data collection
Diffractometer Bruker SMART APEX CCD
Absorption correction Multi-scan (SADABS; Krause et al., 2015View full citation)
Tmin, Tmax 0.907, 0.973
No. of measured, independent and observed [I > 2σ(I)] reflections 15853, 4766, 3926
Rint 0.030
(sin θ/λ)max−1) 0.667
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.050, 0.130, 1.07
No. of reflections 4766
No. of parameters 270
H-atom treatment H atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å−3) 0.32, −0.22
Computer programs: SMART (Bruker, 2002View full citation), SAINT-Plus (Bruker, 2003View full citation), SHELXS (Sheldrick, 2008View full citation), SHELXL2025/1 (Sheldrick, 2015View full citation), ORTEP-3 for Windows (Farrugia, 2012View full citation), PLATON (Spek, 2020View full citation) and publCIF (Westrip, 2010View full citation).

Supporting information


Computing details top

(Z)-8-Methyl-2-(8-methyl-2,3,4,9-tetrahydrocarbazol-1-ylidene)-2,3,4,9-tetrahydrocarbazol-1-one top
Crystal data top
C26H24N2OF(000) = 808
Mr = 380.47Dx = 1.300 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 9.424 (3) ÅCell parameters from 7497 reflections
b = 15.566 (5) Åθ = 2.4–30.5°
c = 13.530 (5) ŵ = 0.08 mm1
β = 101.748 (6)°T = 100 K
V = 1943.3 (11) Å3Block, red
Z = 40.55 × 0.45 × 0.35 mm
Data collection top
Bruker SMART APEX CCD
diffractometer
4766 independent reflections
Radiation source: fine-focus sealed tube3926 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.030
ω scansθmax = 28.3°, θmin = 2.0°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 1012
Tmin = 0.907, Tmax = 0.973k = 2020
15853 measured reflectionsl = 1818
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)] = 0.050Hydrogen site location: mixed
wR(F2) = 0.130H atoms treated by a mixture of independent and constrained refinement
S = 1.07 w = 1/[σ2(Fo2) + (0.0626P)2 + 0.5658P]
where P = (Fo2 + 2Fc2)/3
4766 reflections(Δ/σ)max < 0.001
270 parametersΔρmax = 0.32 e Å3
0 restraintsΔρmin = 0.21 e Å3
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
C11.15744 (18)0.23918 (10)0.20283 (11)0.0336 (3)
H1A1.1928860.2030610.1536810.050*
H1B1.0522430.2323950.1941700.050*
H1C1.1803390.2994490.1921420.050*
C21.22915 (16)0.21259 (9)0.30769 (10)0.0275 (3)
C31.32978 (16)0.26340 (10)0.37065 (11)0.0312 (3)
H31.3529570.3181720.3473150.037*
C41.39898 (17)0.23656 (11)0.46818 (11)0.0341 (3)
H41.4669060.2736310.5088880.041*
C51.36983 (16)0.15755 (10)0.50546 (11)0.0314 (3)
H51.4169630.1398130.5711410.038*
C61.26840 (15)0.10365 (9)0.44384 (10)0.0270 (3)
C71.19930 (15)0.13284 (9)0.34684 (10)0.0251 (3)
C81.12132 (15)0.00201 (9)0.36441 (10)0.0250 (3)
C91.21708 (15)0.01840 (9)0.45374 (10)0.0268 (3)
C101.25226 (17)0.04076 (10)0.54245 (10)0.0319 (3)
H10A1.3564650.0363160.5739070.038*
H10B1.1952500.0246030.5935060.038*
C111.21602 (17)0.13246 (10)0.50681 (10)0.0313 (3)
H11A1.2895360.1528650.4693880.038*
H11B1.2206670.1701220.5663500.038*
C121.06567 (16)0.13981 (9)0.43879 (10)0.0294 (3)
H12A1.0492380.2003540.4170570.035*
H12B0.9921110.1248100.4787610.035*
C131.04263 (15)0.08257 (9)0.34476 (10)0.0245 (3)
C140.94946 (15)0.10826 (9)0.25786 (10)0.0243 (3)
C150.85684 (16)0.18871 (9)0.25623 (11)0.0291 (3)
H15A0.8979730.2349040.2203260.035*
H15B0.8615040.2081140.3265040.035*
C160.69784 (16)0.17513 (10)0.20514 (10)0.0287 (3)
H16A0.6495450.1387710.2484870.034*
H16B0.6472850.2311960.1958210.034*
C170.68889 (15)0.13276 (8)0.10503 (10)0.0241 (3)
C180.80528 (15)0.08720 (8)0.08480 (9)0.0229 (3)
C190.93568 (15)0.06650 (8)0.15694 (9)0.0235 (3)
C200.57464 (15)0.12418 (8)0.01881 (10)0.0249 (3)
C210.42983 (15)0.15252 (9)0.00365 (11)0.0286 (3)
H210.3920480.1876450.0423050.034*
C220.34448 (16)0.12776 (10)0.09437 (11)0.0314 (3)
H220.2461210.1456680.1107780.038*
C230.40032 (16)0.07647 (9)0.16307 (11)0.0306 (3)
H230.3378370.0609970.2248270.037*
C240.54187 (16)0.04754 (9)0.14491 (10)0.0267 (3)
C250.62890 (15)0.07274 (8)0.05203 (10)0.0239 (3)
C260.59845 (17)0.01107 (10)0.21590 (11)0.0325 (3)
H26A0.5248160.0180010.2779290.049*
H26B0.6211160.0672380.1838430.049*
H26C0.6864160.0137080.2323240.049*
N11.10610 (13)0.06987 (7)0.30159 (9)0.0257 (3)
N20.77040 (13)0.05201 (7)0.01111 (8)0.0237 (2)
O11.02768 (11)0.01812 (7)0.13183 (7)0.0289 (2)
H11.0722 (19)0.0643 (11)0.2358 (14)0.035*
H20.8269 (19)0.0197 (12)0.0410 (13)0.035*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0405 (9)0.0315 (7)0.0287 (7)0.0002 (6)0.0068 (6)0.0039 (6)
C20.0275 (7)0.0305 (7)0.0264 (6)0.0019 (6)0.0097 (6)0.0003 (5)
C30.0286 (7)0.0320 (7)0.0349 (7)0.0026 (6)0.0108 (6)0.0014 (6)
C40.0268 (7)0.0404 (8)0.0343 (7)0.0043 (6)0.0042 (6)0.0068 (6)
C50.0277 (7)0.0406 (8)0.0249 (6)0.0002 (6)0.0034 (6)0.0032 (6)
C60.0239 (7)0.0337 (7)0.0242 (6)0.0014 (6)0.0069 (5)0.0008 (5)
C70.0242 (7)0.0284 (7)0.0234 (6)0.0014 (5)0.0065 (5)0.0016 (5)
C80.0248 (7)0.0296 (7)0.0212 (6)0.0030 (5)0.0059 (5)0.0027 (5)
C90.0260 (7)0.0334 (7)0.0212 (6)0.0025 (6)0.0054 (5)0.0014 (5)
C100.0344 (8)0.0377 (8)0.0224 (6)0.0026 (6)0.0027 (6)0.0036 (6)
C110.0332 (8)0.0352 (8)0.0240 (6)0.0055 (6)0.0025 (6)0.0066 (6)
C120.0311 (8)0.0318 (7)0.0248 (6)0.0011 (6)0.0046 (6)0.0080 (5)
C130.0240 (7)0.0273 (6)0.0231 (6)0.0048 (5)0.0069 (5)0.0046 (5)
C140.0233 (7)0.0258 (6)0.0247 (6)0.0016 (5)0.0069 (5)0.0044 (5)
C150.0289 (7)0.0292 (7)0.0285 (7)0.0022 (6)0.0043 (6)0.0066 (5)
C160.0281 (7)0.0321 (7)0.0267 (6)0.0030 (6)0.0073 (6)0.0035 (5)
C170.0241 (7)0.0241 (6)0.0247 (6)0.0022 (5)0.0065 (5)0.0009 (5)
C180.0255 (7)0.0222 (6)0.0218 (6)0.0023 (5)0.0066 (5)0.0005 (5)
C190.0246 (7)0.0245 (6)0.0219 (6)0.0023 (5)0.0057 (5)0.0012 (5)
C200.0249 (7)0.0243 (6)0.0259 (6)0.0020 (5)0.0061 (5)0.0038 (5)
C210.0263 (7)0.0290 (7)0.0311 (7)0.0007 (6)0.0075 (6)0.0052 (5)
C220.0250 (7)0.0326 (7)0.0354 (7)0.0009 (6)0.0030 (6)0.0096 (6)
C230.0293 (8)0.0315 (7)0.0282 (7)0.0035 (6)0.0009 (6)0.0068 (6)
C240.0287 (7)0.0259 (6)0.0244 (6)0.0022 (5)0.0027 (5)0.0051 (5)
C250.0245 (7)0.0226 (6)0.0244 (6)0.0029 (5)0.0043 (5)0.0042 (5)
C260.0314 (8)0.0386 (8)0.0259 (7)0.0045 (6)0.0020 (6)0.0014 (6)
N10.0284 (6)0.0268 (6)0.0211 (5)0.0000 (5)0.0033 (5)0.0018 (4)
N20.0236 (6)0.0253 (6)0.0220 (5)0.0005 (5)0.0040 (4)0.0011 (4)
O10.0291 (5)0.0344 (5)0.0231 (5)0.0059 (4)0.0056 (4)0.0021 (4)
Geometric parameters (Å, º) top
C1—C21.500 (2)C14—C191.4938 (18)
C1—H1A0.9800C14—C151.524 (2)
C1—H1B0.9800C15—C161.532 (2)
C1—H1C0.9800C15—H15A0.9900
C2—C31.386 (2)C15—H15B0.9900
C2—C71.401 (2)C16—C171.4934 (19)
C3—C41.411 (2)C16—H16A0.9900
C3—H30.9500C16—H16B0.9900
C4—C51.378 (2)C17—C181.3796 (19)
C4—H40.9500C17—C201.4235 (19)
C5—C61.410 (2)C18—N21.3849 (17)
C5—H50.9500C18—C191.4416 (19)
C6—C71.4158 (19)C19—O11.2466 (17)
C6—C91.428 (2)C20—C211.407 (2)
C7—N11.3741 (18)C20—C251.422 (2)
C8—C91.3900 (19)C21—C221.378 (2)
C8—N11.3946 (18)C21—H210.9500
C8—C131.454 (2)C22—C231.406 (2)
C9—C101.4955 (19)C22—H220.9500
C10—C111.523 (2)C23—C241.382 (2)
C10—H10A0.9900C23—H230.9500
C10—H10B0.9900C24—C251.4093 (19)
C11—C121.529 (2)C24—C261.499 (2)
C11—H11A0.9900C25—N21.3742 (18)
C11—H11B0.9900C26—H26A0.9800
C12—C131.5320 (18)C26—H26B0.9800
C12—H12A0.9900C26—H26C0.9800
C12—H12B0.9900N1—H10.887 (18)
C13—C141.3759 (19)N2—H20.887 (19)
C2—C1—H1A109.5C19—C14—C15113.67 (11)
C2—C1—H1B109.5C14—C15—C16113.45 (12)
H1A—C1—H1B109.5C14—C15—H15A108.9
C2—C1—H1C109.5C16—C15—H15A108.9
H1A—C1—H1C109.5C14—C15—H15B108.9
H1B—C1—H1C109.5C16—C15—H15B108.9
C3—C2—C7116.00 (13)H15A—C15—H15B107.7
C3—C2—C1122.95 (14)C17—C16—C15109.86 (12)
C7—C2—C1121.04 (13)C17—C16—H16A109.7
C2—C3—C4122.27 (14)C15—C16—H16A109.7
C2—C3—H3118.9C17—C16—H16B109.7
C4—C3—H3118.9C15—C16—H16B109.7
C5—C4—C3121.19 (14)H16A—C16—H16B108.2
C5—C4—H4119.4C18—C17—C20106.77 (12)
C3—C4—H4119.4C18—C17—C16120.44 (12)
C4—C5—C6118.45 (13)C20—C17—C16132.71 (13)
C4—C5—H5120.8C17—C18—N2110.03 (12)
C6—C5—H5120.8C17—C18—C19125.68 (12)
C5—C6—C7119.05 (13)N2—C18—C19123.57 (12)
C5—C6—C9134.37 (13)O1—C19—C18119.66 (12)
C7—C6—C9106.53 (12)O1—C19—C14125.18 (12)
N1—C7—C2128.55 (13)C18—C19—C14115.15 (12)
N1—C7—C6108.41 (12)C21—C20—C25119.81 (12)
C2—C7—C6123.03 (13)C21—C20—C17133.31 (13)
C9—C8—N1108.34 (12)C25—C20—C17106.82 (12)
C9—C8—C13124.95 (12)C22—C21—C20117.97 (14)
N1—C8—C13126.54 (12)C22—C21—H21121.0
C8—C9—C6107.64 (12)C20—C21—H21121.0
C8—C9—C10123.76 (13)C21—C22—C23121.22 (14)
C6—C9—C10128.58 (13)C21—C22—H22119.4
C9—C10—C11108.92 (12)C23—C22—H22119.4
C9—C10—H10A109.9C24—C23—C22123.03 (13)
C11—C10—H10A109.9C24—C23—H23118.5
C9—C10—H10B109.9C22—C23—H23118.5
C11—C10—H10B109.9C23—C24—C25115.68 (13)
H10A—C10—H10B108.3C23—C24—C26122.74 (13)
C10—C11—C12112.42 (12)C25—C24—C26121.49 (13)
C10—C11—H11A109.1N2—C25—C24129.40 (13)
C12—C11—H11A109.1N2—C25—C20108.27 (12)
C10—C11—H11B109.1C24—C25—C20122.28 (13)
C12—C11—H11B109.1C24—C26—H26A109.5
H11A—C11—H11B107.9C24—C26—H26B109.5
C11—C12—C13114.43 (12)H26A—C26—H26B109.5
C11—C12—H12A108.7C24—C26—H26C109.5
C13—C12—H12A108.7H26A—C26—H26C109.5
C11—C12—H12B108.7H26B—C26—H26C109.5
C13—C12—H12B108.7C7—N1—C8108.88 (11)
H12A—C12—H12B107.6C7—N1—H1125.7 (11)
C14—C13—C8128.31 (12)C8—N1—H1120.3 (11)
C14—C13—C12119.90 (13)C25—N2—C18108.08 (12)
C8—C13—C12111.67 (11)C25—N2—H2124.9 (11)
C13—C14—C19125.19 (12)C18—N2—H2127.0 (11)
C13—C14—C15121.00 (12)
C7—C2—C3—C40.3 (2)C15—C16—C17—C20162.64 (14)
C1—C2—C3—C4178.38 (14)C20—C17—C18—N21.35 (15)
C2—C3—C4—C50.3 (2)C16—C17—C18—N2178.38 (12)
C3—C4—C5—C60.1 (2)C20—C17—C18—C19169.14 (13)
C4—C5—C6—C70.7 (2)C16—C17—C18—C197.9 (2)
C4—C5—C6—C9176.26 (16)C17—C18—C19—O1173.36 (13)
C3—C2—C7—N1179.54 (14)N2—C18—C19—O14.1 (2)
C1—C2—C7—N10.8 (2)C17—C18—C19—C147.94 (19)
C3—C2—C7—C61.2 (2)N2—C18—C19—C14177.21 (12)
C1—C2—C7—C6177.52 (13)C13—C14—C19—O118.7 (2)
C5—C6—C7—N1179.95 (13)C15—C14—C19—O1157.01 (13)
C9—C6—C7—N12.32 (16)C13—C14—C19—C18162.71 (13)
C5—C6—C7—C21.4 (2)C15—C14—C19—C1821.60 (17)
C9—C6—C7—C2176.29 (13)C18—C17—C20—C21176.85 (14)
N1—C8—C9—C63.10 (16)C16—C17—C20—C210.3 (3)
C13—C8—C9—C6178.54 (13)C18—C17—C20—C250.36 (15)
N1—C8—C9—C10175.53 (13)C16—C17—C20—C25176.87 (14)
C13—C8—C9—C100.1 (2)C25—C20—C21—C220.95 (19)
C5—C6—C9—C8176.72 (16)C17—C20—C21—C22175.98 (14)
C7—C6—C9—C80.51 (16)C20—C21—C22—C230.6 (2)
C5—C6—C9—C104.7 (3)C21—C22—C23—C240.2 (2)
C7—C6—C9—C10178.05 (14)C22—C23—C24—C250.0 (2)
C8—C9—C10—C1121.1 (2)C22—C23—C24—C26176.55 (13)
C6—C9—C10—C11160.57 (15)C23—C24—C25—N2177.39 (13)
C9—C10—C11—C1247.78 (17)C26—C24—C25—N20.8 (2)
C10—C11—C12—C1357.26 (17)C23—C24—C25—C200.35 (19)
C9—C8—C13—C14178.14 (14)C26—C24—C25—C20176.26 (12)
N1—C8—C13—C147.3 (2)C21—C20—C25—N2178.42 (12)
C9—C8—C13—C125.8 (2)C17—C20—C25—N20.76 (15)
N1—C8—C13—C12168.78 (13)C21—C20—C25—C240.8 (2)
C11—C12—C13—C14149.79 (14)C17—C20—C25—C24176.83 (12)
C11—C12—C13—C833.79 (17)C2—C7—N1—C8174.22 (14)
C8—C13—C14—C1915.0 (2)C6—C7—N1—C84.29 (16)
C12—C13—C14—C19169.26 (13)C9—C8—N1—C74.62 (16)
C8—C13—C14—C15169.63 (14)C13—C8—N1—C7179.97 (13)
C12—C13—C14—C156.1 (2)C24—C25—N2—C18175.78 (13)
C13—C14—C15—C16132.98 (14)C20—C25—N2—C181.59 (14)
C19—C14—C15—C1651.13 (16)C17—C18—N2—C251.85 (15)
C14—C15—C16—C1749.66 (16)C19—C18—N2—C25168.88 (12)
C15—C16—C17—C1821.23 (18)
Hydrogen-bond geometry (Å, º) top
Cg1 and Cg3 are the centroids of the pyrrole (N1/C7/C6/C9/C8) and benzene (C2–C7) rings, respectively.
D—H···AD—HH···AD···AD—H···A
N1—H1···O10.887 (18)1.887 (18)2.6470 (16)142.6 (15)
N2—H2···O1i0.887 (19)2.103 (19)2.9574 (17)161.4 (16)
C12—H12B···Cg1ii0.992.903.876 (2)170
C21—H21···Cg3iii0.952.863.736 (2)154
C26—H26C···Cg1i0.982.703.549 (2)145
Symmetry codes: (i) x+2, y, z; (ii) x+2, y, z+1; (iii) x+3/2, y+1/2, z+1/2.
 

Acknowledgements

Authors contributions are as follows: conceptualization, synthesis, methodology and writing original draft, MS; crystallographic analysis, Hirshfeld surface analysis, software, validation, review and editing, AAT. MS thanks the academic and administrative authorities of RV College of Engineering for their support and encouragement. The authors thank Dr M. Zeller for the X-ray data collection. The X-ray diffractometer was funded by NSF Grant CHE 0087210, Ohio Board of Regents Grant CAP-491, and by Youngstown State University.

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