Crystal structure of 4-(2-azido­phen­yl)-5-benzoyl-2-(1H-indol-3-yl)-1H-pyrrole-3-carbo­nitrile

Vimala, G.; Raja, J.K.; Naaz, Y.A.; Preumal, P.T.; SubbiahPandi, A.

doi:10.1107/S2056989015006921

organic compounds

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ISSN: 2056-9890

Volume 71| Part 5| May 2015| Pages o335-o336

https://doi.org/10.1107/S2056989015006921

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Crystal structure of 4-(2-azidophenyl)-5-benzoyl-2-(1H-indol-3-yl)-1H-pyrrole-3-carbonitrile

G. Vimala,^a J. Kamal Raja,^b Y. Amina Naaz,^a P. T. Preumal ^b and A. SubbiahPandi ^a ^*

^aDepartment of Physics, Presidency College (Autonomous), Chennai 600 005, India, and ^bOrganic Chemistry Division, Central Leather Research Institute (CSIR), Adyar, Chennai 600 020, India
^*Correspondence e-mail: aspandian59@gmail.com

Edited by W. T. A. Harrison, University of Aberdeen, Scotland (Received 28 March 2015; accepted 7 April 2015; online 22 April 2015)

In the title compound, C₂₆H₁₆N₆O, the dihedral angles between the central pyrrole ring and the pendant indole ring system (r.m.s. deviation = 0.027 Å) and the azide-bearing benzene ring are 37.56 (8) and 51.62 (11)°, respectively. The azide group is almost coplanar with its attached benzene ring [C—C—N—N = 3.8 (3)°]. The benzoyl benzene ring is disordered over two orientations twisted with respect to each other by 9.29 (8)° in a 0.514 (2):0.486 (2) ratio. In the crystal, inversion dimers linked by pairs of N_p—H⋯O (p = pyrrole) hydrogen bonds generate R₂²(10) loops. A second inversion dimer arises from a pair of N_i—H⋯N_c (i = indole and c = cyanide) hydrogen bonds, which generates an R₂²(16) loop. Together, the hydrogen bonds lead to [011] chains in the crystal.

Keywords: crystal structure; indole derivatives; pyrrole-3-carbonitrile; hydrogen bonding.

CCDC reference: 933255

1. Related literature

For background to indole derivatives, see: Srivastava, Anupam & Pandeya (2011 ). For related structures, see: Srinivasan et al. (2012 ); Inglebert et al. (2013 ).

2. Experimental

2.1. Crystal data

C₂₆H₁₆N₆O
M_r = 428.45
Triclinic, $[P \overline 1]$
a = 8.1834 (6) Å
b = 11.3713 (8) Å
c = 12.6853 (8) Å
α = 108.070 (3)°
β = 105.164 (4)°
γ = 90.256 (3)°
V = 1078.42 (13) Å³
Z = 2
Mo Kα radiation
μ = 0.09 mm⁻¹
T = 293 K
0.35 × 0.20 × 0.15 mm

2.2. Data collection

Bruker Kappa APEXII CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2004 ) T_min = 0.901, T_max = 0.987
20625 measured reflections
4315 independent reflections
3062 reflections with I > 2σ(I)
R_int = 0.033

2.3. Refinement

R[F² > 2σ(F²)] = 0.046
wR(F²) = 0.143
S = 1.04
4315 reflections
325 parameters
2 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρ_max = 0.21 e Å⁻³
Δρ_min = −0.25 e Å⁻³

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
N2—H2A⋯O1ⁱ	0.92 (1)	1.95 (1)	2.8526 (17)	166 (2)
N1—H1A⋯N3ⁱⁱ	0.92 (1)	2.10 (1)	2.988 (2)	163 (2)
Symmetry codes: (i) -x, -y, -z+1; (ii) -x, -y-1, -z.

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012 ); software used to prepare material for publication: PLATON (Spek, 2009 ).

Supporting information

CCDC reference: 933255

Crystal structure: contains datablocks global, I. DOI: https://doi.org/10.1107/S2056989015006921/hb7394sup1.cif

Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989015006921/hb7394Isup2.hkl

Supporting information file. DOI: https://doi.org/10.1107/S2056989015006921/hb7394Isup3.cml

checkCIF report

Related literature top

For background to indole derivatives, see: Srivastava, Anupam & Pandeya (2011). For related structures, see: Srinivasan et al. (2012); Inglebert et al. (2013).

Experimental top

To a stirred mixture of 2-azido aldehydes 1 (1.0 mmol), 2- (1H-3-indolylcarbonyl)-3-aryl-2-propenenitriles 2 (1.0 mmol) and phenacylazides 3 (1.0 mmol) in water (3 ml) piperidine (0.25 mmol) was added at 80 ⁰ C. The turbid solution slowly turned into a clear solution followed by the formation of solid with 0.75 min. After completion of the reaction as indicated by thin layer chromatography (TLC), the solid was filtered and washed with pet-ether: EtOAc mixture (1: 1 ratio v/v, 5 ml) to give pure compounds. The compound was recrystallized from methanol to yield yellow crystals. The yield of the isolated product was 91%. Yellow blocks were obtained by slow evaporation of a solution of the title compound in methanol at room temperature.

Structure description top

For background to indole derivatives, see: Srivastava, Anupam & Pandeya (2011). For related structures, see: Srinivasan et al. (2012); Inglebert et al. (2013).

Computing details top

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT (Bruker, 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012); software used to prepare material for publication: PLATON (Spek, 2009).

Figures top

	Fig. 1. The molecular structure of the title compound, with displacement ellipsoids drawn at 30% probability level.
	Fig. 2. The crystal packing of the title compound viewed along c axis. Hydrogen atoms are omitted for clarity.

4-(2-Azidophenyl)-5-benzoyl-2-(1H-indol-3-yl)-1H-pyrrole-3-carbonitrile top

Crystal data top

C₂₆H₁₆N₆O	Z = 2
M_r = 428.45	F(000) = 444
Triclinic, P1	D_x = 1.319 Mg m⁻³
Hall symbol: -P 1	Mo Kα radiation, λ = 0.71073 Å
a = 8.1834 (6) Å	Cell parameters from 5359 reflections
b = 11.3713 (8) Å	θ = 2.6–24.5°
c = 12.6853 (8) Å	µ = 0.09 mm⁻¹
α = 108.070 (3)°	T = 293 K
β = 105.164 (4)°	Block, yellow
γ = 90.256 (3)°	0.35 × 0.20 × 0.15 mm
V = 1078.42 (13) Å³

Data collection top

Bruker Kappa APEXII CCD diffractometer	4315 independent reflections
Radiation source: fine-focus sealed tube	3062 reflections with I > 2σ(I)
Graphite monochromator	R_int = 0.033
ω and φ scan	θ_max = 26.2°, θ_min = 2.1°
Absorption correction: multi-scan (SADABS; Bruker, 2004)	h = −10→10
T_min = 0.901, T_max = 0.987	k = −14→14
20625 measured reflections	l = −15→11

Refinement top

Refinement on F²	Primary atom site location: structure-invariant direct methods
Least-squares matrix: full	Secondary atom site location: difference Fourier map
R[F² > 2σ(F²)] = 0.046	Hydrogen site location: inferred from neighbouring sites
wR(F²) = 0.143	H atoms treated by a mixture of independent and constrained refinement
S = 1.04	w = 1/[σ²(F_o²) + (0.0727P)² + 0.1697P] where P = (F_o² + 2F_c²)/3
4315 reflections	(Δ/σ)_max < 0.001
325 parameters	Δρ_max = 0.21 e Å⁻³
2 restraints	Δρ_min = −0.25 e Å⁻³

Crystal data top

C₂₆H₁₆N₆O	γ = 90.256 (3)°
M_r = 428.45	V = 1078.42 (13) Å³
Triclinic, P1	Z = 2
a = 8.1834 (6) Å	Mo Kα radiation
b = 11.3713 (8) Å	µ = 0.09 mm⁻¹
c = 12.6853 (8) Å	T = 293 K
α = 108.070 (3)°	0.35 × 0.20 × 0.15 mm
β = 105.164 (4)°

Data collection top

Bruker Kappa APEXII CCD diffractometer	4315 independent reflections
Absorption correction: multi-scan (SADABS; Bruker, 2004)	3062 reflections with I > 2σ(I)
T_min = 0.901, T_max = 0.987	R_int = 0.033
20625 measured reflections

Refinement top

R[F² > 2σ(F²)] = 0.046	2 restraints
wR(F²) = 0.143	H atoms treated by a mixture of independent and constrained refinement
S = 1.04	Δρ_max = 0.21 e Å⁻³
4315 reflections	Δρ_min = −0.25 e Å⁻³
325 parameters

Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F² against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F², conventional R-factors R are based on F, with F set to zero for negative F². The threshold expression of F² > σ(F²) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F² are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å²) top

	x	y	z	U_iso*/U_eq	Occ. (<1)
C1	−0.0917 (3)	−0.39241 (16)	0.12464 (15)	0.0547 (5)
H1	0.0075	−0.4097	0.1024	0.066*
C2	−0.3428 (2)	−0.42040 (17)	0.15320 (15)	0.0543 (5)
C3	−0.4944 (3)	−0.4692 (2)	0.15954 (19)	0.0750 (6)
H3	−0.5245	−0.5544	0.1333	0.090*
C4	−0.5968 (3)	−0.3873 (3)	0.2057 (2)	0.0886 (8)
H4	−0.6987	−0.4173	0.2117	0.106*
C5	−0.5540 (3)	−0.2602 (3)	0.2443 (2)	0.0820 (7)
H5	−0.6281	−0.2069	0.2747	0.098*
C6	−0.4056 (3)	−0.2119 (2)	0.23854 (17)	0.0621 (5)
H6	−0.3783	−0.1264	0.2641	0.075*
C7	−0.2954 (2)	−0.29262 (16)	0.19367 (14)	0.0473 (4)
C8	−0.1326 (2)	−0.27646 (15)	0.17555 (13)	0.0454 (4)
C9	−0.0284 (2)	−0.16159 (14)	0.20815 (13)	0.0431 (4)
C10	0.0785 (2)	−0.12214 (15)	0.15429 (13)	0.0451 (4)
C11	0.1096 (2)	−0.19675 (16)	0.05005 (15)	0.0515 (4)
C12	0.1570 (2)	−0.00185 (15)	0.22359 (14)	0.0449 (4)
C13	0.2907 (2)	0.06488 (15)	0.20018 (15)	0.0504 (4)
C14	0.2675 (3)	0.07898 (19)	0.09230 (18)	0.0664 (5)
H14	0.1646	0.0494	0.0362	0.080*
C15	0.3950 (4)	0.1362 (2)	0.0672 (2)	0.0847 (7)
H15	0.3775	0.1455	−0.0052	0.102*
C16	0.5461 (4)	0.1790 (2)	0.1486 (3)	0.0894 (8)
H16	0.6317	0.2173	0.1314	0.107*
C17	0.5740 (3)	0.1663 (2)	0.2556 (2)	0.0759 (6)
H17	0.6777	0.1965	0.3107	0.091*
C18	0.4479 (3)	0.10869 (17)	0.28161 (17)	0.0561 (5)
C19	0.0923 (2)	0.03026 (15)	0.31786 (14)	0.0447 (4)
C20	0.1247 (2)	0.13755 (16)	0.42355 (14)	0.0476 (4)
N1	−0.2164 (2)	−0.47857 (14)	0.11122 (14)	0.0612 (4)
N2	−0.01795 (18)	−0.06776 (12)	0.30625 (11)	0.0453 (3)
N3	0.1341 (2)	−0.25813 (15)	−0.03298 (14)	0.0697 (5)
N4	0.4701 (2)	0.08726 (16)	0.38885 (14)	0.0642 (4)
N5	0.6075 (2)	0.12980 (17)	0.46065 (17)	0.0697 (5)
O1	0.1155 (2)	0.12110 (12)	0.51215 (10)	0.0720 (4)
N6	0.7264 (2)	0.16569 (9)	0.53511 (10)	0.1037 (7)
C21	0.1467 (2)	0.26296 (9)	0.42353 (10)	0.0457 (16)	0.486 (6)
C22	0.0825 (2)	0.29348 (9)	0.32352 (10)	0.0454 (13)	0.486 (6)
H22	0.0316	0.2315	0.2542	0.054*	0.486 (6)
C23	0.0943 (2)	0.41672 (9)	0.32710 (10)	0.0697 (16)	0.486 (6)
H23	0.0513	0.4371	0.2602	0.084*	0.486 (6)
C24	0.1703 (2)	0.50943 (9)	0.43068 (10)	0.094 (2)	0.486 (6)
H24	0.1781	0.5919	0.4331	0.113*	0.486 (6)
C25	0.2345 (2)	0.47891 (9)	0.53069 (10)	0.104 (2)	0.486 (6)
H25	0.2853	0.5409	0.6000	0.125*	0.486 (6)
C26	0.2227 (2)	0.35568 (9)	0.52712 (10)	0.086 (2)	0.486 (6)
H26	0.2657	0.3353	0.5940	0.103*	0.486 (6)
C21'	0.1727 (2)	0.26171 (9)	0.41748 (10)	0.0465 (16)	0.514 (6)
C22'	0.1178 (2)	0.29254 (9)	0.31689 (10)	0.0723 (18)	0.514 (6)
H22'	0.0559	0.2330	0.2489	0.087*	0.514 (6)
C23'	0.1552 (2)	0.41233 (9)	0.31797 (10)	0.095 (2)	0.514 (6)
H23'	0.1185	0.4330	0.2507	0.114*	0.514 (6)
C24'	0.2476 (2)	0.50129 (9)	0.41964 (10)	0.095 (2)	0.514 (6)
H24'	0.2727	0.5814	0.4204	0.114*	0.514 (6)
C25'	0.3026 (2)	0.47046 (9)	0.52023 (10)	0.0780 (17)	0.514 (6)
H25'	0.3644	0.5300	0.5883	0.094*	0.514 (6)
C26'	0.2651 (2)	0.35067 (9)	0.51915 (10)	0.0523 (12)	0.514 (6)
H26'	0.3019	0.3300	0.5865	0.063*	0.514 (6)
H2A	−0.060 (2)	−0.0740 (17)	0.3647 (12)	0.059 (5)*
H1A	−0.214 (3)	−0.5632 (10)	0.0821 (18)	0.082 (7)*

Atomic displacement parameters (Å²) top

	U¹¹	U²²	U³³	U¹²	U¹³	U²³
C1	0.0648 (12)	0.0460 (10)	0.0521 (10)	0.0055 (9)	0.0199 (9)	0.0112 (8)
C2	0.0572 (11)	0.0520 (10)	0.0468 (10)	−0.0059 (9)	0.0027 (8)	0.0162 (8)
C3	0.0660 (14)	0.0772 (15)	0.0734 (14)	−0.0191 (12)	−0.0016 (11)	0.0303 (12)
C4	0.0491 (13)	0.128 (2)	0.0960 (18)	−0.0048 (15)	0.0107 (12)	0.0547 (17)
C5	0.0555 (13)	0.110 (2)	0.0913 (17)	0.0225 (13)	0.0218 (12)	0.0458 (15)
C6	0.0607 (12)	0.0651 (12)	0.0627 (12)	0.0152 (10)	0.0148 (10)	0.0251 (10)
C7	0.0530 (10)	0.0472 (10)	0.0397 (9)	0.0038 (8)	0.0070 (7)	0.0160 (7)
C8	0.0558 (10)	0.0413 (9)	0.0378 (8)	0.0030 (8)	0.0124 (7)	0.0115 (7)
C9	0.0537 (10)	0.0392 (9)	0.0381 (8)	0.0053 (7)	0.0144 (7)	0.0132 (7)
C10	0.0586 (10)	0.0421 (9)	0.0391 (8)	0.0082 (8)	0.0204 (8)	0.0136 (7)
C11	0.0669 (12)	0.0448 (9)	0.0489 (10)	0.0070 (8)	0.0234 (9)	0.0175 (8)
C12	0.0570 (10)	0.0413 (9)	0.0423 (9)	0.0072 (8)	0.0197 (8)	0.0165 (7)
C13	0.0664 (12)	0.0412 (9)	0.0556 (10)	0.0095 (8)	0.0334 (9)	0.0185 (8)
C14	0.0871 (15)	0.0662 (12)	0.0653 (12)	0.0134 (11)	0.0384 (11)	0.0336 (10)
C15	0.116 (2)	0.0852 (16)	0.0867 (17)	0.0164 (15)	0.0601 (17)	0.0484 (14)
C16	0.099 (2)	0.0833 (17)	0.119 (2)	0.0062 (15)	0.0690 (18)	0.0466 (16)
C17	0.0720 (14)	0.0661 (13)	0.1031 (18)	0.0009 (11)	0.0456 (13)	0.0283 (13)
C18	0.0648 (12)	0.0458 (10)	0.0679 (12)	0.0084 (9)	0.0336 (10)	0.0199 (9)
C19	0.0577 (10)	0.0397 (9)	0.0411 (9)	0.0007 (8)	0.0196 (8)	0.0143 (7)
C20	0.0571 (10)	0.0467 (10)	0.0415 (9)	−0.0014 (8)	0.0220 (8)	0.0109 (7)
N1	0.0754 (11)	0.0384 (9)	0.0607 (10)	−0.0011 (8)	0.0138 (8)	0.0075 (7)
N2	0.0604 (9)	0.0415 (8)	0.0373 (7)	−0.0008 (6)	0.0205 (7)	0.0115 (6)
N3	0.1019 (14)	0.0555 (10)	0.0578 (10)	0.0102 (9)	0.0425 (10)	0.0099 (8)
N4	0.0575 (10)	0.0688 (11)	0.0639 (10)	−0.0039 (8)	0.0140 (8)	0.0207 (9)
N5	0.0620 (11)	0.0653 (11)	0.0799 (13)	0.0065 (9)	0.0191 (10)	0.0210 (10)
O1	0.1137 (12)	0.0603 (8)	0.0442 (7)	−0.0204 (8)	0.0357 (7)	0.0086 (6)
N6	0.0723 (14)	0.1120 (18)	0.1114 (18)	−0.0078 (13)	0.0005 (13)	0.0353 (15)
C21	0.049 (3)	0.048 (4)	0.039 (3)	0.005 (2)	0.020 (3)	0.006 (3)
C22	0.058 (2)	0.038 (3)	0.042 (3)	0.012 (2)	0.019 (2)	0.012 (2)
C23	0.098 (4)	0.053 (3)	0.062 (3)	0.010 (2)	0.020 (3)	0.025 (3)
C24	0.137 (6)	0.051 (3)	0.109 (5)	0.004 (3)	0.044 (4)	0.036 (3)
C25	0.129 (6)	0.061 (4)	0.105 (5)	−0.017 (3)	0.019 (4)	0.017 (4)
C26	0.107 (4)	0.066 (5)	0.076 (5)	0.003 (3)	0.021 (4)	0.016 (4)
C21'	0.055 (3)	0.040 (3)	0.053 (4)	0.002 (2)	0.028 (3)	0.016 (3)
C22'	0.077 (3)	0.069 (4)	0.070 (4)	−0.005 (3)	0.014 (3)	0.027 (3)
C23'	0.115 (4)	0.072 (4)	0.108 (5)	0.005 (3)	0.020 (4)	0.052 (4)
C24'	0.149 (6)	0.046 (3)	0.090 (4)	−0.008 (3)	0.034 (4)	0.022 (3)
C25'	0.113 (4)	0.044 (3)	0.065 (3)	−0.018 (2)	0.016 (3)	0.008 (2)
C26'	0.075 (3)	0.037 (3)	0.039 (3)	−0.012 (2)	0.012 (2)	0.008 (2)

Geometric parameters (Å, º) top

C1—N1	1.351 (2)	C18—N4	1.421 (2)
C1—C8	1.362 (2)	C19—N2	1.378 (2)
C1—H1	0.9300	C19—C20	1.467 (2)
C2—N1	1.367 (3)	C20—O1	1.2158 (19)
C2—C3	1.388 (3)	C20—C21	1.4368 (19)
C2—C7	1.398 (2)	C20—C21'	1.4940 (19)
C3—C4	1.356 (4)	N1—H1A	0.920 (10)
C3—H3	0.9300	N2—H2A	0.916 (9)
C4—C5	1.384 (4)	N4—N5	1.231 (2)
C4—H4	0.9300	N5—N6	1.132 (2)
C5—C6	1.359 (3)	C21—C22	1.3900
C5—H5	0.9300	C21—C26	1.3900
C6—C7	1.390 (3)	C22—C23	1.3900
C6—H6	0.9300	C22—H22	0.9300
C7—C8	1.430 (2)	C23—C24	1.3900
C8—C9	1.441 (2)	C23—H23	0.9300
C9—N2	1.347 (2)	C24—C25	1.3900
C9—C10	1.390 (2)	C24—H24	0.9300
C10—C12	1.417 (2)	C25—C26	1.3900
C10—C11	1.419 (2)	C25—H25	0.9300
C11—N3	1.137 (2)	C26—H26	0.9300
C12—C19	1.381 (2)	C21'—C22'	1.3900
C12—C13	1.471 (2)	C21'—C26'	1.3900
C13—C14	1.391 (3)	C22'—C23'	1.3900
C13—C18	1.396 (3)	C22'—H22'	0.9300
C14—C15	1.382 (3)	C23'—C24'	1.3900
C14—H14	0.9300	C23'—H23'	0.9300
C15—C16	1.359 (4)	C24'—C25'	1.3900
C15—H15	0.9300	C24'—H24'	0.9300
C16—C17	1.369 (4)	C25'—C26'	1.3900
C16—H16	0.9300	C25'—H25'	0.9300
C17—C18	1.382 (3)	C26'—H26'	0.9300
C17—H17	0.9300

N1—C1—C8	110.10 (17)	N2—C19—C20	117.84 (14)
N1—C1—H1	124.9	C12—C19—C20	134.10 (15)
C8—C1—H1	124.9	O1—C20—C21	118.38 (15)
N1—C2—C3	130.43 (19)	O1—C20—C19	118.84 (15)
N1—C2—C7	107.62 (16)	C21—C20—C19	122.36 (14)
C3—C2—C7	121.9 (2)	O1—C20—C21'	123.14 (15)
C4—C3—C2	117.1 (2)	C21—C20—C21'	9.3
C4—C3—H3	121.4	C19—C20—C21'	117.99 (13)
C2—C3—H3	121.4	C1—N1—C2	109.22 (15)
C3—C4—C5	121.9 (2)	C1—N1—H1A	125.6 (14)
C3—C4—H4	119.0	C2—N1—H1A	125.1 (14)
C5—C4—H4	119.0	C9—N2—C19	111.13 (13)
C6—C5—C4	121.2 (2)	C9—N2—H2A	124.4 (12)
C6—C5—H5	119.4	C19—N2—H2A	123.3 (12)
C4—C5—H5	119.4	N5—N4—C18	115.33 (17)
C5—C6—C7	118.7 (2)	N6—N5—N4	172.4 (2)
C5—C6—H6	120.6	C22—C21—C26	120.0
C7—C6—H6	120.6	C22—C21—C20	120.87 (8)
C6—C7—C2	119.01 (17)	C26—C21—C20	118.97 (8)
C6—C7—C8	134.25 (17)	C21—C22—C23	120.0
C2—C7—C8	106.73 (15)	C21—C22—H22	120.0
C1—C8—C7	106.32 (15)	C23—C22—H22	120.0
C1—C8—C9	126.31 (16)	C24—C23—C22	120.0
C7—C8—C9	127.33 (15)	C24—C23—H23	120.0
N2—C9—C10	106.05 (14)	C22—C23—H23	120.0
N2—C9—C8	122.71 (14)	C25—C24—C23	120.0
C10—C9—C8	131.23 (15)	C25—C24—H24	120.0
C9—C10—C12	109.26 (13)	C23—C24—H24	120.0
C9—C10—C11	123.89 (15)	C24—C25—C26	120.0
C12—C10—C11	126.73 (15)	C24—C25—H25	120.0
N3—C11—C10	178.92 (19)	C26—C25—H25	120.0
C19—C12—C10	105.61 (14)	C25—C26—C21	120.0
C19—C12—C13	129.39 (16)	C25—C26—H26	120.0
C10—C12—C13	124.77 (14)	C21—C26—H26	120.0
C14—C13—C18	117.82 (17)	C22'—C21'—C26'	120.0
C14—C13—C12	120.37 (18)	C22'—C21'—C20	122.25 (8)
C18—C13—C12	121.68 (15)	C26'—C21'—C20	117.58 (8)
C15—C14—C13	121.1 (2)	C23'—C22'—C21'	120.0
C15—C14—H14	119.5	C23'—C22'—H22'	120.0
C13—C14—H14	119.5	C21'—C22'—H22'	120.0
C16—C15—C14	119.8 (2)	C22'—C23'—C24'	120.0
C16—C15—H15	120.1	C22'—C23'—H23'	120.0
C14—C15—H15	120.1	C24'—C23'—H23'	120.0
C15—C16—C17	120.9 (2)	C25'—C24'—C23'	120.0
C15—C16—H16	119.6	C25'—C24'—H24'	120.0
C17—C16—H16	119.6	C23'—C24'—H24'	120.0
C16—C17—C18	119.9 (2)	C24'—C25'—C26'	120.0
C16—C17—H17	120.0	C24'—C25'—H25'	120.0
C18—C17—H17	120.0	C26'—C25'—H25'	120.0
C17—C18—C13	120.53 (19)	C25'—C26'—C21'	120.0
C17—C18—N4	123.1 (2)	C25'—C26'—H26'	120.0
C13—C18—N4	116.33 (15)	C21'—C26'—H26'	120.0
N2—C19—C12	107.93 (14)

N1—C2—C3—C4	−179.6 (2)	C13—C12—C19—N2	−173.68 (16)
C7—C2—C3—C4	0.8 (3)	C10—C12—C19—C20	176.61 (18)
C2—C3—C4—C5	0.5 (3)	C13—C12—C19—C20	1.9 (3)
C3—C4—C5—C6	−0.7 (4)	N2—C19—C20—O1	29.5 (3)
C4—C5—C6—C7	−0.5 (3)	C12—C19—C20—O1	−145.7 (2)
C5—C6—C7—C2	1.7 (3)	N2—C19—C20—C21	−142.88 (17)
C5—C6—C7—C8	−179.35 (19)	C12—C19—C20—C21	41.8 (3)
N1—C2—C7—C6	178.41 (16)	N2—C19—C20—C21'	−152.33 (16)
C3—C2—C7—C6	−1.9 (3)	C12—C19—C20—C21'	32.4 (3)
N1—C2—C7—C8	−0.81 (19)	C8—C1—N1—C2	0.1 (2)
C3—C2—C7—C8	178.89 (16)	C3—C2—N1—C1	−179.22 (19)
N1—C1—C8—C7	−0.6 (2)	C7—C2—N1—C1	0.4 (2)
N1—C1—C8—C9	177.26 (15)	C10—C9—N2—C19	−0.33 (19)
C6—C7—C8—C1	−178.18 (19)	C8—C9—N2—C19	178.93 (15)
C2—C7—C8—C1	0.87 (19)	C12—C19—N2—C9	−0.45 (19)
C6—C7—C8—C9	4.0 (3)	C20—C19—N2—C9	−176.88 (15)
C2—C7—C8—C9	−176.98 (15)	C17—C18—N4—N5	3.8 (3)
C1—C8—C9—N2	−141.04 (18)	C13—C18—N4—N5	−177.93 (17)
C7—C8—C9—N2	36.4 (3)	C18—N4—N5—N6	170.4 (15)
C1—C8—C9—C10	38.0 (3)	O1—C20—C21—C22	−149.95 (13)
C7—C8—C9—C10	−144.54 (18)	C19—C20—C21—C22	22.5 (2)
N2—C9—C10—C12	0.97 (19)	C21'—C20—C21—C22	86.80 (6)
C8—C9—C10—C12	−178.21 (16)	O1—C20—C21—C26	25.4 (2)
N2—C9—C10—C11	177.12 (16)	C19—C20—C21—C26	−162.12 (12)
C8—C9—C10—C11	−2.1 (3)	C21'—C20—C21—C26	−97.82 (7)
C9—C10—C11—N3	−30 (11)	C26—C21—C22—C23	0.0
C12—C10—C11—N3	145 (11)	C20—C21—C22—C23	175.34 (13)
C9—C10—C12—C19	−1.23 (19)	C21—C22—C23—C24	0.0
C11—C10—C12—C19	−177.24 (16)	C22—C23—C24—C25	0.0
C9—C10—C12—C13	173.77 (16)	C23—C24—C25—C26	0.0
C11—C10—C12—C13	−2.2 (3)	C24—C25—C26—C21	0.0
C19—C12—C13—C14	−134.4 (2)	C22—C21—C26—C25	0.0
C10—C12—C13—C14	51.9 (2)	C20—C21—C26—C25	−175.43 (13)
C19—C12—C13—C18	49.9 (3)	O1—C20—C21'—C22'	−152.61 (14)
C10—C12—C13—C18	−123.87 (19)	C21—C20—C21'—C22'	−91.12 (7)
C18—C13—C14—C15	−1.0 (3)	C19—C20—C21'—C22'	29.3 (2)
C12—C13—C14—C15	−176.89 (18)	O1—C20—C21'—C26'	22.6 (2)
C13—C14—C15—C16	0.4 (3)	C21—C20—C21'—C26'	84.11 (7)
C14—C15—C16—C17	−0.1 (4)	C19—C20—C21'—C26'	−155.43 (12)
C15—C16—C17—C18	0.4 (4)	C26'—C21'—C22'—C23'	0.0
C16—C17—C18—C13	−1.1 (3)	C20—C21'—C22'—C23'	175.12 (12)
C16—C17—C18—N4	177.1 (2)	C21'—C22'—C23'—C24'	0.0
C14—C13—C18—C17	1.3 (3)	C22'—C23'—C24'—C25'	0.0
C12—C13—C18—C17	177.15 (17)	C23'—C24'—C25'—C26'	0.0
C14—C13—C18—N4	−176.97 (16)	C24'—C25'—C26'—C21'	0.0
C12—C13—C18—N4	−1.1 (2)	C22'—C21'—C26'—C25'	0.0
C10—C12—C19—N2	1.01 (19)	C20—C21'—C26'—C25'	−175.34 (12)

Hydrogen-bond geometry (Å, º) top

D—H···A	D—H	H···A	D···A	D—H···A
N2—H2A···O1ⁱ	0.92 (1)	1.95 (1)	2.8526 (17)	166 (2)
N1—H1A···N3ⁱⁱ	0.92 (1)	2.10 (1)	2.988 (2)	163 (2)

Symmetry codes: (i) −x, −y, −z+1; (ii) −x, −y−1, −z.

Hydrogen-bond geometry (Å, º) top

D—H···A	D—H	H···A	D···A	D—H···A
N2—H2A···O1ⁱ	0.916 (9)	1.954 (10)	2.8526 (17)	166.1 (17)
N1—H1A···N3ⁱⁱ	0.920 (10)	2.095 (12)	2.988 (2)	163 (2)

Symmetry codes: (i) −x, −y, −z+1; (ii) −x, −y−1, −z.

Acknowledgements

GV and ASP thank Dr Babu Varghese, SAIF, IIT, Chennai, India, for the X-ray data collection.

References

Bruker (2004). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854. Web of Science CrossRef CAS IUCr Journals Google Scholar
Inglebert, S. A., Arun, Y., Sethusankar, K. & Perumal, P. T. (2013). Acta Cryst. E69, o1585. CSD CrossRef IUCr Journals Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Spek, A. L. (2009). Acta Cryst. D65, 148–155. Web of Science CrossRef CAS IUCr Journals Google Scholar
Srinivasan, T., Suhitha, S., Purushothaman, S., Raghunathan, R. & Velmurugan, D. (2012). Acta Cryst. E68, o2469. CSD CrossRef IUCr Journals Google Scholar
Srivastava, Anupam & Pandeya, S. N. (2011). JCPR, 1, 1–17. Google Scholar

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ISSN: 2056-9890

Volume 71| Part 5| May 2015| Pages o335-o336

https://doi.org/10.1107/S2056989015006921

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organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Crystal structure of 4-(2-azido­phen­yl)-5-benzoyl-2-(1H-indol-3-yl)-1H-pyrrole-3-carbo­nitrile

1. Related literature

2. Experimental

2.1. Crystal data

2.2. Data collection

2.3. Refinement

Supporting information

Acknowledgements

References

organic compounds

Crystal structure of 4-(2-azidophenyl)-5-benzoyl-2-(1H-indol-3-yl)-1H-pyrrole-3-carbonitrile