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 ethyl 2-amino-4-(4-chloro­phen­yl)-5,6,7,8,9,10-hexa­hydro­cyclo­octa­[b]pyridine-3-carboxyl­ate

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aDepartment of Chemistry, Annamalai University, Annamalainagar, Chidambaram 608 002, India, and bPG & Research Department of Physics, Government Arts College, Melur 625 106, India
*Correspondence e-mail: [email protected]

Edited by M. Weil, Vienna University of Technology, Austria (Received 2 March 2026; accepted 23 March 2026; online 27 March 2026)

In the title compound, C20H23ClN2O2, the cyclo­octene ring has a boat–chair conformation. The ethyl formate moiety is equally disordered over two positions. The dihedral angle between the pyridine and chloro­phenyl rings is 81.33 (13)°. An intra­molecular N—H⋯O hydrogen bond helps to stabilize the mol­ecular conformation. In the crystal, N—H⋯N hydrogen-bonding leads to the formation of dimers with an R22(8) graph-set motif. Additional consolidation of the packing in the crystal is achieved through C—H⋯π and ππ stacking inter­actions. The inter­molecular inter­actions were qu­anti­fied and analysed using Hirshfeld surface analysis, revealing that H⋯H inter­actions contribute by far the most to the crystal packing (63.6%).

1. Chemical context

The synthesis of functionalized N-heterocycles is an imprtant objective in organic and medicinal chemistry, as these moieties constitute the core of over 60% of US Food and Drug Administration (FDA) approved small-mol­ecule drugs. Among these, the pyridine entity is arguably the most ubiquitous, appearing in essential vitamins such as nicotinic acid and various synthetic pharmaceuticals like Delafloxacin (Van Bambeke, 2015View full citation). Within this family, 2-amino­nicotinate esters have garnered significant attention as privileged scaffolds. These multifunctional mol­ecules possess a unique 1,2,3-arrangement of substituents – an amino group and a carboxyl­ate ester – which provides a rich landscape for both mol­ecular recognition and chemical transformation (Bagley et al., 2015View full citation). The chemical appeal of 2-amino­nicotinate esters lies in their synthetic versatility. They serve as precursors for the construction of fused heterocyclic systems, such as pyrido[2,3-d]pyrimidines and 1,8-naphthyridines, which are themselves pharmacologically active. Modern synthetic routes have shifted toward multicomponent reactions (MCRs), which allow for the one-pot assembly of these esters from readily available aldehydes, malono­nitriles, and alcohols. These methods are beneficial for their economy and compliance with green chemistry principles, often utilizing heterogeneous catalysts or aqueous media (Shaaban et al., 2020View full citation). Biologically, these esters are highly multifunctional. The amino and ester groups provide critical hydrogen-bonding sites that facilitate high-affinity binding to various enzyme pockets. It has been demonstrated that deriv­atives of 2-amino­nicotinates exhibit a broad spectrum of bio-activities, including anti-inflammatory and analgesic when acting as non-selective or COX-2 selective inhibitors (Bekhit et al., 2017View full citation), and anti­microbial by demonstrating potency against Gram-positive and Gram-negative pathogens through disrupting metabolic pathways (El-Gazzar & Hafez, 2021View full citation). Given the rising challenge of drug resistance in both oncology and infectious diseases, the development of diverse 2-amino­nicotinate derivatives offers a promising avenue for the discovery of next-generation therapeutic agents.

[Scheme 1]

In this work, we describe the synthesis, structure and Hirshfeld surface analysis of the title compound, C20H23ClN2O2, (I)[link].

2. Structural commentary

The mol­ecular structure of (I)[link] is displayed in Fig. 1[link]. The pyridine ring (C1/C2/C9/N1/C10/C11) is essentially planar, with a maximum deviation of −0.016 (3) Å for atom C11, while its attached amino nitro­gen atom N2 deviates by 0.005 (3) Å from this plane. The chloro­phenyl ring is also almost planar, and its attached chlorine atom deviates by −0.031 (1) Å from this plane. The dihedral angle between the pyridine and chloro­phenyl rings is 81.33 (13)°. The cyclo­octene ring (C2–C9) has a boat–chair conformation based on a puckering analysis and endocyclic torsion angles (Evans & Boeyens, 1988View full citation). An intra­molecular N—H⋯O hydrogen bond (Table 1[link]) between atoms N2 and O1A contributes to the stability of the mol­ecular conformation. This N2—H2B⋯O1A inter­action generates an S(6) ring motif (Bernstein et al., 1995View full citation), as shown in Fig. 1[link].

Table 1
Hydrogen-bond geometry (Å, °)

Cg is the centroid of pyridine ring (C1/C2/C9/N1/C10/C11).

D—H⋯A D—H H⋯A DA D—H⋯A
N2—H2B⋯O1A 0.86 1.96 2.605 (10) 131
N2—H2A⋯N1i 0.86 2.29 3.129 (3) 165
C17—H17⋯Cgii 0.93 2.84 3.657 (3) 147
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation.
[Figure 1]
Figure 1
A view of the mol­ecular structure of compound (I)[link], showing the atom labelling. Displacement ellipsoids are drawn at the 30% probability level. Only one of the disordered parts of the ethyl formate chain is displayed for clarity; the intra­molecular hydrogen bond is shown as a dashed line.

3. Supra­molecular features

In the crystal, mol­ecules associate pairwise through N2—H2A⋯N1i hydrogen bonds (Table 1[link]) into inversion dimers with an R22(8) graph-set motif (Etter et al., 1990View full citation; Bernstein et al., 1995View full citation), as shown in Fig. 2[link]. Mol­ecules are linked into chains parallel to [010] by C—H⋯π inter­actions, C17—H17⋯Cg, where Cg is the centroid of the pyridine ring (Table 1[link], Fig. 3[link]). Moreover, ππ inter­actions are observed between the centroids of inversion-related pyridine rings with a centroid-to-centroid distance of 3.764 (2) Å and a slippage of 0.711 Å.

[Figure 2]
Figure 2
The formation of a centrosymmetric dimer in the crystal structure of (I)[link] through N—H⋯N hydrogen bonds. For clarity, H atoms not involved in these inter­actions have been omitted, and only one of the disordered parts of the ethyl formate chain is displayed. [Symmetry code: (a) −x, −y − 1, −z + 1].
[Figure 3]
Figure 3
The crystal packing of (I)[link]. C—H⋯π inter­actions are shown as dashed lines. For clarity, H atoms not involved in these inter­actions have been omitted, and only one of the disordered parts of the ethyl formate chain is displayed.

4. Hirshfeld surface analysis

A Hirshfeld surface (HS) analysis (Spackman & Jayatilaka, 2009View full citation) was carried out using CrystalExplorer (Spackman et al., 2021View full citation) to characterize and qu­antify the inter­molecular inter­actions in the title compound. For this purpose, a model without the disorder of the ethyl formate moiety was used (the ethyl formate moiety was set to full occupancy for the Hirshfeld surface analysis). The HS mapped over dnorm is illustrated in Fig. 4[link], where deep-red spots indicative of strong inter­actions occur at N1 and H2A, and these atoms are responsible for the inter­molecular hydrogen bonds discussed above. The associated two-dimensional fingerprint plots (McKinnon et al., 2007View full citation) provide qu­anti­tative information about the non-covalent inter­actions in the crystal packing in terms of the percentage contribution of the inter­atomic contacts (Spackman & McKinnon, 2002View full citation). As shown in Fig. 5[link], the overall two-dimensional fingerprint plot for compound (I)[link] is delineated into H⋯H, H⋯Cl/Cl⋯H, H⋯O/O⋯H, H⋯C/ C⋯H, H⋯N/N⋯H, Cl⋯C/C⋯Cl, C⋯C and N⋯C/C⋯N contacts, revealing that H⋯H inter­actions are by far the main contributor to the crystal packing.

[Figure 4]
Figure 4
A view of the Hirshfeld surface mapped over dnorm for compound (I)[link].
[Figure 5]
Figure 5
Two-dimensional fingerprint plots for the compound (I)[link], showing (a) all inter­actions, and delineated into (b) H⋯H, (c) H⋯Cl/Cl⋯H, (d) H⋯O/O⋯H, (e) H⋯C/C⋯H, (f) H⋯N/N⋯H, (g) Cl⋯C/C⋯Cl, (h) C⋯C and (i) N⋯C/C⋯N inter­actions. The di and de values are the closest inter­nal and external distances (in Å) from given points on the Hirshfeld surface.

5. Synthesis and crystallization

Compound (I)[link] was prepared using a mixture of cyclo­octa­none (1.0 mmol, 0.126 g), 4-chloro­benzaldehyde (1.0 mmol, 0.140 g), ethyl cyano­acetate (1.0 mmol, 0.113 g) and ammonium acetate (1.5 mmol, 0.116 g) taken in a 100 ml round-bottom flask and dissolved using ethanol. The resulting solution was heated under reflux with stirring for 4–6 h. The progress of the reaction was periodically monitored by thin-layer chromatography using ethyl acetate:hexane (3:7) as the eluent. Upon completion of the reaction, the mixture was allowed to cool to room temperature, leading to the formation of a solid precipitate. The solid was collected by vacuum filtration and washed with cold ethanol to remove residual impurities. For final purification, the product was recrystallized from ethanol solution, yielding clean, well-formed crystals suitable for single crystal X-ray diffraction studies.

6. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link]. Hydrogen atoms were placed in idealized positions and allowed to ride on their parent atoms, N—H = 0.86 Å and C—H = 0.93–0.97 Å, with Uiso(H) = 1.5Ueq for methyl H atoms and Uiso(H) = 1.2Ueq(C,N) for all other H atoms. The ethyl formate group (C12, O1, O2, C13, C14) is equally disordered over two sets of sites. For modelling of this disorder, pairs of C—O and C=O bond lengths were restrained to 1.31 (1) and 1.20 (1) Å, respectively, and the displacement parameters of all atoms involved were restrained to be within 0.01 Å of each other.

Table 2
Experimental details

Crystal data
Chemical formula C20H23ClN2O2
Mr 358.85
Crystal system, space group Monoclinic, P21/n
Temperature (K) 300
a, b, c (Å) 13.2386 (12), 7.2770 (7), 19.7223 (18)
β (°) 101.461 (3)
V3) 1862.1 (3)
Z 4
Radiation type Mo Kα
μ (mm−1) 0.22
Crystal size (mm) 0.26 × 0.12 × 0.08
 
Data collection
Diffractometer Bruker APEXII CCD
Absorption correction Multi-scan (SADABS; Krause et al., 2015View full citation)
Tmin, Tmax 0.945, 0.983
No. of measured, independent and observed [I > 2σ(I)] reflections 34945, 4649, 2682
Rint 0.050
(sin θ/λ)max−1) 0.669
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.064, 0.207, 1.06
No. of reflections 4649
No. of parameters 264
No. of restraints 108
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.55, −0.27
Computer programs: APEX3 and SAINT (Bruker, 2017View full citation), SHELXT (Sheldrick, 2015aView full citation), SHELXL (Sheldrick, 2015bView 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

Ethyl 2-amino-4-(4-chlorophenyl)-5,6,7,8,9,10-hexahydrocycloocta[b]pyridine-3-carboxylate top
Crystal data top
C20H23ClN2O2F(000) = 760
Mr = 358.85Dx = 1.280 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 13.2386 (12) ÅCell parameters from 9916 reflections
b = 7.2770 (7) Åθ = 3.0–26.3°
c = 19.7223 (18) ŵ = 0.22 mm1
β = 101.461 (3)°T = 300 K
V = 1862.1 (3) Å3Block, colourless
Z = 40.26 × 0.12 × 0.08 mm
Data collection top
Bruker APEXII CCD
diffractometer
2682 reflections with I > 2σ(I)
Radiation source: i-mu-s microfocus sourceRint = 0.050
φ and ω scansθmax = 28.4°, θmin = 2.1°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 1717
Tmin = 0.945, Tmax = 0.983k = 99
34945 measured reflectionsl = 2626
4649 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.064 w = 1/[σ2(Fo2) + (0.0769P)2 + 1.3578P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.207(Δ/σ)max < 0.001
S = 1.06Δρmax = 0.55 e Å3
4649 reflectionsΔρmin = 0.27 e Å3
264 parametersExtinction correction: SHELXL (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
108 restraintsExtinction coefficient: 0.0053 (14)
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)
N10.07369 (17)0.2785 (3)0.52707 (12)0.0531 (6)
N20.00533 (19)0.3486 (3)0.41712 (13)0.0654 (7)
H2A0.0343660.4390140.4338510.078*
H2B0.0177220.3294640.3732180.078*
Cl10.44196 (7)0.62949 (12)0.41161 (5)0.0778 (3)
C10.17789 (18)0.0195 (3)0.48544 (13)0.0458 (6)
C20.19016 (19)0.0236 (3)0.55599 (13)0.0485 (6)
C30.2612 (2)0.0864 (4)0.61089 (15)0.0604 (7)
H3A0.2297620.0943280.6512350.072*
H3B0.2655230.2103150.5936020.072*
C40.3700 (2)0.0133 (5)0.63391 (17)0.0750 (9)
H4A0.3967610.0146330.5927270.090*
H4B0.4120060.1116000.6579600.090*
C60.3400 (3)0.3296 (6)0.6488 (2)0.0872 (11)
H6A0.3882930.4283820.6641820.105*
H6B0.3320280.3203390.5989700.105*
C80.1485 (3)0.2405 (4)0.64719 (15)0.0675 (8)
H8A0.0840390.2935940.6539970.081*
H8B0.1638880.1360910.6781070.081*
C70.2338 (3)0.3826 (5)0.66593 (18)0.0817 (10)
H7A0.2108480.4960520.6419120.098*
H7B0.2437290.4071320.7151510.098*
C50.3855 (3)0.1551 (5)0.6802 (2)0.0858 (11)
H5A0.4589800.1736470.6958960.103*
H5B0.3565620.1295800.7206550.103*
C90.1357 (2)0.1747 (4)0.57360 (14)0.0499 (6)
C100.05992 (19)0.2364 (4)0.45992 (14)0.0508 (6)
C110.1101 (2)0.0837 (4)0.43593 (13)0.0501 (6)
C150.24158 (19)0.1722 (3)0.46504 (13)0.0471 (6)
C160.2137 (2)0.3543 (4)0.46938 (16)0.0581 (7)
H160.1527750.3828140.4838210.070*
C170.2744 (2)0.4943 (4)0.45269 (15)0.0605 (7)
H170.2547420.6162170.4559040.073*
C180.3638 (2)0.4525 (4)0.43137 (14)0.0548 (7)
C190.3934 (2)0.2739 (4)0.42640 (17)0.0650 (8)
H190.4540330.2468190.4114190.078*
C200.3327 (2)0.1336 (4)0.44375 (16)0.0594 (7)
H200.3534650.0121670.4410670.071*
C120.0893 (2)0.0450 (4)0.36086 (15)0.0642 (8)
O1A0.0236 (10)0.1269 (16)0.3190 (5)0.085 (3)0.51 (2)
O1B0.0739 (13)0.1670 (13)0.3166 (5)0.088 (3)0.49 (2)
O2A0.1083 (12)0.1269 (14)0.3464 (11)0.063 (2)0.51 (2)
O2B0.1305 (15)0.1061 (19)0.3421 (12)0.081 (4)0.49 (2)
C13A0.0965 (17)0.178 (3)0.2723 (15)0.075 (3)0.51 (2)
H13A0.1041320.0689900.2453340.091*0.51 (2)
H13B0.0281330.2275660.2556730.091*0.51 (2)
C13B0.1142 (19)0.148 (3)0.2708 (16)0.080 (3)0.49 (2)
H13C0.0449420.1147080.2475790.095*0.49 (2)
H13D0.1633900.0839310.2487710.095*0.49 (2)
C14A0.1750 (15)0.316 (3)0.2633 (8)0.112 (4)0.51 (2)
H14A0.1665050.3473520.2152290.134*0.51 (2)
H14B0.1667870.4239280.2895630.134*0.51 (2)
H14C0.2426410.2656540.2792440.134*0.51 (2)
C14B0.1308 (13)0.3638 (19)0.2693 (8)0.085 (3)0.49 (2)
H14D0.1211160.4049840.2222400.103*0.49 (2)
H14E0.0818950.4238360.2918690.103*0.49 (2)
H14F0.1994530.3932900.2930520.103*0.49 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0523 (12)0.0505 (13)0.0574 (14)0.0021 (10)0.0134 (10)0.0020 (11)
N20.0636 (15)0.0623 (15)0.0640 (15)0.0174 (12)0.0026 (12)0.0024 (12)
Cl10.0826 (6)0.0708 (5)0.0807 (6)0.0202 (4)0.0181 (4)0.0063 (4)
C10.0449 (13)0.0400 (13)0.0505 (14)0.0051 (10)0.0044 (10)0.0004 (11)
C20.0524 (14)0.0402 (13)0.0507 (15)0.0039 (11)0.0053 (11)0.0012 (11)
C30.0747 (19)0.0500 (16)0.0521 (15)0.0059 (14)0.0022 (14)0.0014 (12)
C40.0681 (19)0.087 (2)0.0620 (18)0.0129 (18)0.0056 (15)0.0080 (17)
C60.083 (2)0.088 (3)0.082 (2)0.026 (2)0.0030 (19)0.001 (2)
C80.084 (2)0.0660 (19)0.0550 (17)0.0136 (16)0.0210 (15)0.0035 (15)
C70.109 (3)0.064 (2)0.066 (2)0.0059 (19)0.0022 (19)0.0197 (16)
C50.072 (2)0.097 (3)0.081 (2)0.006 (2)0.0015 (18)0.016 (2)
C90.0498 (14)0.0486 (14)0.0520 (15)0.0039 (11)0.0115 (11)0.0022 (12)
C100.0449 (13)0.0492 (15)0.0558 (16)0.0026 (11)0.0038 (11)0.0024 (12)
C110.0517 (14)0.0471 (14)0.0491 (14)0.0035 (12)0.0044 (11)0.0013 (12)
C150.0497 (14)0.0438 (13)0.0446 (13)0.0015 (11)0.0019 (10)0.0013 (11)
C160.0605 (16)0.0469 (15)0.0703 (19)0.0066 (12)0.0210 (14)0.0046 (13)
C170.0732 (19)0.0438 (14)0.0666 (18)0.0060 (13)0.0186 (15)0.0027 (13)
C180.0607 (16)0.0505 (15)0.0507 (15)0.0059 (13)0.0050 (12)0.0021 (12)
C190.0569 (16)0.0631 (19)0.078 (2)0.0010 (14)0.0210 (15)0.0009 (16)
C200.0596 (16)0.0453 (15)0.0739 (19)0.0067 (12)0.0145 (14)0.0015 (13)
C120.0742 (19)0.0606 (18)0.0526 (16)0.0057 (15)0.0001 (14)0.0008 (14)
O1A0.105 (6)0.081 (5)0.058 (3)0.032 (4)0.015 (4)0.001 (3)
O1B0.127 (6)0.074 (4)0.058 (3)0.012 (4)0.006 (4)0.013 (3)
O2A0.077 (5)0.059 (3)0.048 (3)0.001 (3)0.001 (3)0.005 (2)
O2B0.098 (8)0.091 (5)0.048 (4)0.031 (5)0.001 (5)0.011 (5)
C13A0.094 (6)0.079 (6)0.048 (3)0.003 (4)0.000 (5)0.009 (4)
C13B0.098 (7)0.085 (6)0.049 (4)0.012 (5)0.000 (5)0.011 (5)
C14A0.138 (10)0.121 (9)0.067 (5)0.043 (7)0.002 (7)0.016 (6)
C14B0.104 (8)0.086 (6)0.063 (5)0.008 (5)0.008 (5)0.017 (4)
Geometric parameters (Å, º) top
N1—C101.336 (3)C10—C111.423 (4)
N1—C91.337 (3)C11—C121.478 (4)
N2—C101.355 (3)C15—C161.383 (4)
N2—H2A0.8600C15—C201.383 (4)
N2—H2B0.8600C16—C171.378 (4)
Cl1—C181.744 (3)C16—H160.9300
C1—C21.404 (3)C17—C181.367 (4)
C1—C111.405 (4)C17—H170.9300
C1—C151.498 (4)C18—C191.366 (4)
C2—C91.397 (4)C19—C201.383 (4)
C2—C31.514 (4)C19—H190.9300
C3—C41.518 (4)C20—H200.9300
C3—H3A0.9700C12—O1A1.228 (6)
C3—H3B0.9700C12—O2A1.319 (9)
C4—C51.517 (5)O2A—C13A1.48 (3)
C4—H4A0.9700O2B—C13B1.41 (3)
C4—H4B0.9700C13A—C14A1.48 (3)
C6—C51.486 (5)C13A—H13A0.9700
C6—C71.558 (6)C13A—H13B0.9700
C6—H6A0.9700C13B—C14B1.59 (3)
C6—H6B0.9700C13B—H13C0.9700
C8—C91.505 (4)C13B—H13D0.9700
C8—C71.522 (5)C14A—H14A0.9600
C8—H8A0.9700C14A—H14B0.9600
C8—H8B0.9700C14A—H14C0.9600
C7—H7A0.9700C14B—H14D0.9600
C7—H7B0.9700C14B—H14E0.9600
C5—H5A0.9700C14B—H14F0.9600
C5—H5B0.9700
C10—N1—C9119.7 (2)N2—C10—C11123.0 (2)
C10—N2—H2A120.0C1—C11—C10117.5 (2)
C10—N2—H2B120.0C1—C11—C12124.0 (2)
H2A—N2—H2B120.0C10—C11—C12118.4 (2)
C2—C1—C11120.1 (2)C16—C15—C20118.3 (3)
C2—C1—C15118.1 (2)C16—C15—C1121.5 (2)
C11—C1—C15121.7 (2)C20—C15—C1120.2 (2)
C9—C2—C1117.3 (2)C17—C16—C15121.2 (3)
C9—C2—C3121.1 (2)C17—C16—H16119.4
C1—C2—C3121.6 (2)C15—C16—H16119.4
C2—C3—C4116.5 (3)C18—C17—C16119.4 (3)
C2—C3—H3A108.2C18—C17—H17120.3
C4—C3—H3A108.2C16—C17—H17120.3
C2—C3—H3B108.2C19—C18—C17120.8 (3)
C4—C3—H3B108.2C19—C18—Cl1119.7 (2)
H3A—C3—H3B107.3C17—C18—Cl1119.5 (2)
C5—C4—C3118.0 (3)C18—C19—C20119.7 (3)
C5—C4—H4A107.8C18—C19—H19120.1
C3—C4—H4A107.8C20—C19—H19120.1
C5—C4—H4B107.8C19—C20—C15120.6 (3)
C3—C4—H4B107.8C19—C20—H20119.7
H4A—C4—H4B107.1C15—C20—H20119.7
C5—C6—C7115.5 (3)O1A—C12—O2A117.1 (10)
C5—C6—H6A108.4O1A—C12—C11123.1 (5)
C7—C6—H6A108.4O2A—C12—C11113.1 (10)
C5—C6—H6B108.4C12—O2A—C13A117.5 (15)
C7—C6—H6B108.4C14A—C13A—O2A110.4 (17)
H6A—C6—H6B107.5C14A—C13A—H13A109.6
C9—C8—C7112.7 (3)O2A—C13A—H13A109.6
C9—C8—H8A109.0C14A—C13A—H13B109.6
C7—C8—H8A109.0O2A—C13A—H13B109.6
C9—C8—H8B109.0H13A—C13A—H13B108.1
C7—C8—H8B109.0O2B—C13B—C14B103.6 (17)
H8A—C8—H8B107.8O2B—C13B—H13C111.0
C8—C7—C6115.9 (3)C14B—C13B—H13C111.0
C8—C7—H7A108.3O2B—C13B—H13D111.0
C6—C7—H7A108.3C14B—C13B—H13D111.0
C8—C7—H7B108.3H13C—C13B—H13D109.0
C6—C7—H7B108.3C13A—C14A—H14A109.5
H7A—C7—H7B107.4C13A—C14A—H14B109.5
C6—C5—C4116.4 (3)H14A—C14A—H14B109.5
C6—C5—H5A108.2C13A—C14A—H14C109.5
C4—C5—H5A108.2H14A—C14A—H14C109.5
C6—C5—H5B108.2H14B—C14A—H14C109.5
C4—C5—H5B108.2C13B—C14B—H14D109.5
H5A—C5—H5B107.3C13B—C14B—H14E109.5
N1—C9—C2123.5 (2)H14D—C14B—H14E109.5
N1—C9—C8114.7 (2)C13B—C14B—H14F109.5
C2—C9—C8121.7 (2)H14D—C14B—H14F109.5
N1—C10—N2115.1 (2)H14E—C14B—H14F109.5
N1—C10—C11121.9 (2)
C11—C1—C2—C92.2 (4)N1—C10—C11—C12.0 (4)
C15—C1—C2—C9175.5 (2)N2—C10—C11—C1178.5 (2)
C11—C1—C2—C3179.0 (2)N1—C10—C11—C12179.0 (3)
C15—C1—C2—C33.2 (4)N2—C10—C11—C120.5 (4)
C9—C2—C3—C484.5 (3)C2—C1—C15—C1681.3 (3)
C1—C2—C3—C494.3 (3)C11—C1—C15—C16101.0 (3)
C2—C3—C4—C574.1 (4)C2—C1—C15—C2096.2 (3)
C9—C8—C7—C651.0 (4)C11—C1—C15—C2081.5 (3)
C5—C6—C7—C856.5 (4)C20—C15—C16—C170.3 (4)
C7—C6—C5—C498.5 (4)C1—C15—C16—C17177.8 (3)
C3—C4—C5—C666.4 (5)C15—C16—C17—C180.1 (5)
C10—N1—C9—C21.5 (4)C16—C17—C18—C190.1 (4)
C10—N1—C9—C8177.5 (2)C16—C17—C18—Cl1178.9 (2)
C1—C2—C9—N10.2 (4)C17—C18—C19—C200.6 (5)
C3—C2—C9—N1178.6 (2)Cl1—C18—C19—C20178.4 (2)
C1—C2—C9—C8175.9 (2)C18—C19—C20—C151.0 (5)
C3—C2—C9—C82.8 (4)C16—C15—C20—C190.9 (4)
C7—C8—C9—N186.3 (3)C1—C15—C20—C19178.4 (3)
C7—C8—C9—C289.8 (3)C1—C11—C12—O1A173.8 (10)
C9—N1—C10—N2179.2 (2)C10—C11—C12—O1A7.3 (10)
C9—N1—C10—C110.4 (4)C1—C11—C12—O2A23.5 (8)
C2—C1—C11—C103.3 (4)C10—C11—C12—O2A157.6 (8)
C15—C1—C11—C10174.4 (2)O1A—C12—O2A—C13A31.6 (17)
C2—C1—C11—C12177.8 (3)C11—C12—O2A—C13A176.1 (10)
C15—C1—C11—C124.5 (4)C12—O2A—C13A—C14A145 (2)
Hydrogen-bond geometry (Å, º) top
Cg is the centroid of pyridine ring (C1/C2/C9/N1/C10/C11).
D—H···AD—HH···AD···AD—H···A
N2—H2B···O1A0.861.962.605 (10)131
N2—H2A···N1i0.862.293.129 (3)165
C17—H17···Cgii0.932.843.657 (3)147
Symmetry codes: (i) x, y1, z+1; (ii) x, y+1, z.
 

Footnotes

Additional correspondence author, e-mail: [email protected].

Acknowledgements

The authors thank the Single Crystal XRD Facility at VIT, Vellore, Tamil Nadu, India, for providing the instrumentation and support necessary for this study.

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