organic compounds
5,5′-(1-Phenylethane-1,1-diyl)bis(1H-pyrrole-2-carboxaldehyde)
aVignan's Foundation for Science Technology and Research, Division of Chemistry, Department of Sciences and Humanities, Vadlamudi, Andhra, Pradesh-522213, India
*Correspondence e-mail: ravikottalanka@gmail.com
In the title compound, C18H16N2O2, the dihedral angle between the pyrrole rings is 79.47 (9)°, with the N—H groups approximately orthogonal (H—N⋯N—H pseudo torsion angle = −106°). In the crystal, N—H⋯O hydrogen bonds link the molecules into [11] chains. A C—H⋯O interaction is also observed.
Keywords: crystal structure; pyrrole; hydrogen bonding; Hirshfeld surface analysis.
CCDC reference: 1912418
Structure description
Dipyrromethane-dialdehydes are intermediates for the preparation of various macrocyclic (Love et al., 2003) and acyclic diiminodipyrromethane (e.g.: Deliomeroglu et al., 2016). As a part of our studies in this area, we now report the of the title compound.
The dihedral angles between the N1-pyrrole ring (A), N2-pyrrole ring (B) and the C13–C18 phenyl ring (C) are A/B = 79.47 (9), A/C = 87.21 (8) and B/C = 70.40 (8)°. The N1—C6—C7—O1 [−2.7 (2)°] and N2—C11—C12—O2 [2.8 (2)°] torsion angles indicate that the aldehyde groups are almost coplanar with their adjacent pyrrole ring systems (Fig. 1).
In the crystal, N—H⋯O hydrogen bonds (Table 1) link the molecules into [11] chains (Fig. 2). A weak C—H⋯O hydrogen bond consolidates the chains. The Hirshfeld surface and two-dimensional fingerprint plots were generated with CrystalExplorer17.5 (Turner et al., 2017) (see supplementary materials). The percentage contributions from the different interatomic contacts to the Hirshfeld surfaces are as follows: H⋯H (47.9%), C⋯H/H⋯C (27.5%), O⋯H/H⋯O (21.5%), N⋯H/H⋯N (1.5%) and C⋯O/O⋯C (1.5%).
Synthesis and crystallization
The title compound, C18H16N2O2 was prepared by the reported method (Fig. 3); Muwal et al. 2018) and colourless cubes were recrystallized from a toluene–hexane solvent mixture at −4°C.
Refinement
Crystal data, data collection and structure .
details are summarized in Table 2Structural data
CCDC reference: 1912418
https://doi.org/10.1107/S2414314619016602/hb4326sup1.cif
contains datablock I. DOI:Supporting information file. DOI: https://doi.org/10.1107/S2414314619016602/hb4326Isup3.cdx
Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314619016602/hb4326Isup4.hkl
Hirshfeld surface and fingerprint plots. DOI: https://doi.org/10.1107/S2414314619016602/hb4326sup5.docx
Data collection: CrysAlis PRO (Rigaku OD, 2015); cell
CrysAlis PRO (Rigaku OD, 2015); data reduction: CrysAlis PRO (Rigaku OD, 2015); program(s) used to solve structure: SHELXT2014/5 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2018/3 (Sheldrick, 2015b); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012) and Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL2018/3 (Sheldrick, 2015b).C18H16N2O2 | Z = 2 |
Mr = 292.33 | F(000) = 308 |
Triclinic, P1 | Dx = 1.292 Mg m−3 |
a = 7.0679 (2) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 9.6856 (4) Å | Cell parameters from 5094 reflections |
c = 12.1510 (5) Å | θ = 3.7–29.9° |
α = 101.560 (3)° | µ = 0.09 mm−1 |
β = 93.302 (3)° | T = 293 K |
γ = 111.270 (4)° | Cube, colourless |
V = 751.66 (5) Å3 | 0.18 × 0.15 × 0.13 mm |
XtaLAB Pro: Kappa dual offset/far diffractometer | Rint = 0.022 |
Radiation source: fine-focus sealed X-ray tube | θmax = 31.1°, θmin = 3.1° |
ω scans | h = −9→10 |
Absorption correction: multi-scan (CrysAlisPro; Rigaku OD, 2015) | k = −13→13 |
Tmin = 0.901, Tmax = 1.000 | l = −17→17 |
13274 measured reflections | Standard reflections: see text; every none reflections |
4208 independent reflections | intensity decay: none |
3307 reflections with I > 2σ(I) |
Refinement on F2 | Primary atom site location: dual |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.050 | H-atom parameters constrained |
wR(F2) = 0.142 | w = 1/[σ2(Fo2) + (0.0767P)2 + 0.1364P] where P = (Fo2 + 2Fc2)/3 |
S = 1.03 | (Δ/σ)max < 0.001 |
4208 reflections | Δρmax = 0.32 e Å−3 |
200 parameters | Δρmin = −0.19 e Å−3 |
0 restraints |
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. |
x | y | z | Uiso*/Ueq | ||
N1 | 0.69498 (16) | 0.13760 (11) | 0.87005 (8) | 0.0348 (2) | |
H1 | 0.592279 | 0.131280 | 0.906260 | 0.042* | |
N2 | 0.94852 (16) | 0.52913 (11) | 0.69220 (8) | 0.0350 (2) | |
H2 | 0.897693 | 0.470214 | 0.625766 | 0.042* | |
O2 | 1.18939 (19) | 0.67425 (13) | 0.53044 (9) | 0.0593 (3) | |
O1 | 0.63340 (19) | −0.10500 (15) | 0.98826 (12) | 0.0649 (3) | |
C8 | 0.87280 (19) | 0.50458 (13) | 0.78942 (10) | 0.0349 (3) | |
C13 | 0.53349 (18) | 0.30398 (14) | 0.68621 (10) | 0.0346 (3) | |
C6 | 0.8011 (2) | 0.04229 (15) | 0.86453 (11) | 0.0399 (3) | |
C3 | 0.77809 (19) | 0.24329 (14) | 0.80925 (10) | 0.0347 (3) | |
C2 | 0.69195 (19) | 0.36169 (13) | 0.79432 (10) | 0.0338 (2) | |
C11 | 1.1197 (2) | 0.66317 (14) | 0.71604 (11) | 0.0398 (3) | |
C14 | 0.4611 (2) | 0.40434 (16) | 0.64815 (12) | 0.0445 (3) | |
H14 | 0.512212 | 0.506479 | 0.686836 | 0.053* | |
C18 | 0.4538 (2) | 0.15255 (16) | 0.62642 (12) | 0.0452 (3) | |
H18 | 0.500715 | 0.083660 | 0.650140 | 0.054* | |
C7 | 0.7592 (2) | −0.07648 (17) | 0.92390 (13) | 0.0471 (3) | |
H7 | 0.835458 | −0.137403 | 0.912050 | 0.057* | |
C12 | 1.2317 (2) | 0.72554 (15) | 0.63178 (13) | 0.0464 (3) | |
H12 | 1.348509 | 0.814225 | 0.657358 | 0.056* | |
C9 | 0.9961 (2) | 0.62497 (16) | 0.87798 (11) | 0.0470 (3) | |
H9 | 0.978635 | 0.637712 | 0.954118 | 0.056* | |
C5 | 0.9541 (2) | 0.09002 (19) | 0.79891 (13) | 0.0505 (3) | |
H5 | 1.049116 | 0.046264 | 0.780729 | 0.061* | |
C1 | 0.5846 (3) | 0.40046 (18) | 0.89673 (12) | 0.0478 (3) | |
H1A | 0.677390 | 0.429200 | 0.965753 | 0.072* | |
H1B | 0.465129 | 0.312760 | 0.898067 | 0.072* | |
H1C | 0.544689 | 0.483480 | 0.889915 | 0.072* | |
C10 | 1.1508 (2) | 0.72322 (16) | 0.83195 (12) | 0.0500 (3) | |
H10 | 1.255985 | 0.812989 | 0.871959 | 0.060* | |
C4 | 0.9407 (2) | 0.21604 (18) | 0.76469 (13) | 0.0495 (3) | |
H4 | 1.025661 | 0.271584 | 0.720018 | 0.059* | |
C15 | 0.3139 (2) | 0.3539 (2) | 0.55333 (14) | 0.0543 (4) | |
H15 | 0.267142 | 0.422408 | 0.528760 | 0.065* | |
C17 | 0.3053 (2) | 0.10196 (19) | 0.53181 (15) | 0.0574 (4) | |
H17 | 0.252517 | −0.000256 | 0.493242 | 0.069* | |
C16 | 0.2361 (2) | 0.2028 (2) | 0.49507 (15) | 0.0587 (4) | |
H16 | 0.137392 | 0.169268 | 0.431307 | 0.070* |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1 | 0.0370 (5) | 0.0360 (5) | 0.0340 (5) | 0.0132 (4) | 0.0090 (4) | 0.0142 (4) |
N2 | 0.0403 (5) | 0.0302 (5) | 0.0283 (5) | 0.0065 (4) | 0.0053 (4) | 0.0066 (4) |
O2 | 0.0674 (7) | 0.0533 (6) | 0.0445 (6) | 0.0066 (5) | 0.0180 (5) | 0.0121 (5) |
O1 | 0.0602 (7) | 0.0681 (7) | 0.0862 (9) | 0.0277 (6) | 0.0297 (6) | 0.0500 (7) |
C8 | 0.0428 (6) | 0.0322 (5) | 0.0298 (5) | 0.0134 (5) | 0.0067 (4) | 0.0090 (4) |
C13 | 0.0334 (5) | 0.0372 (6) | 0.0361 (6) | 0.0122 (5) | 0.0132 (4) | 0.0154 (5) |
C6 | 0.0428 (6) | 0.0395 (6) | 0.0410 (6) | 0.0172 (5) | 0.0057 (5) | 0.0147 (5) |
C3 | 0.0404 (6) | 0.0355 (6) | 0.0300 (5) | 0.0135 (5) | 0.0095 (4) | 0.0126 (4) |
C2 | 0.0419 (6) | 0.0336 (5) | 0.0304 (5) | 0.0157 (5) | 0.0130 (4) | 0.0129 (4) |
C11 | 0.0420 (6) | 0.0316 (6) | 0.0398 (6) | 0.0069 (5) | 0.0042 (5) | 0.0090 (5) |
C14 | 0.0451 (7) | 0.0405 (7) | 0.0518 (8) | 0.0176 (6) | 0.0084 (6) | 0.0168 (6) |
C18 | 0.0481 (7) | 0.0379 (6) | 0.0485 (7) | 0.0141 (6) | 0.0066 (6) | 0.0124 (5) |
C7 | 0.0457 (7) | 0.0445 (7) | 0.0589 (8) | 0.0201 (6) | 0.0090 (6) | 0.0237 (6) |
C12 | 0.0457 (7) | 0.0344 (6) | 0.0493 (8) | 0.0031 (5) | 0.0105 (6) | 0.0106 (5) |
C9 | 0.0616 (8) | 0.0420 (7) | 0.0301 (6) | 0.0133 (6) | 0.0037 (6) | 0.0057 (5) |
C5 | 0.0530 (8) | 0.0583 (9) | 0.0560 (8) | 0.0320 (7) | 0.0202 (6) | 0.0246 (7) |
C1 | 0.0636 (9) | 0.0518 (8) | 0.0415 (7) | 0.0306 (7) | 0.0270 (6) | 0.0191 (6) |
C10 | 0.0560 (8) | 0.0386 (7) | 0.0404 (7) | 0.0050 (6) | −0.0015 (6) | 0.0036 (5) |
C4 | 0.0522 (8) | 0.0569 (8) | 0.0554 (8) | 0.0276 (7) | 0.0270 (6) | 0.0303 (7) |
C15 | 0.0474 (8) | 0.0620 (9) | 0.0625 (9) | 0.0251 (7) | 0.0064 (7) | 0.0270 (8) |
C17 | 0.0521 (8) | 0.0481 (8) | 0.0589 (9) | 0.0100 (7) | 0.0009 (7) | 0.0036 (7) |
C16 | 0.0433 (8) | 0.0718 (11) | 0.0548 (9) | 0.0165 (7) | −0.0016 (6) | 0.0143 (8) |
N1—C3 | 1.3622 (14) | C14—C15 | 1.384 (2) |
N1—C6 | 1.3793 (16) | C14—H14 | 0.9300 |
N1—H1 | 0.8600 | C18—C17 | 1.388 (2) |
N2—C8 | 1.3533 (15) | C18—H18 | 0.9300 |
N2—C11 | 1.3795 (16) | C7—H7 | 0.9300 |
N2—H2 | 0.8600 | C12—H12 | 0.9300 |
O2—C12 | 1.2071 (18) | C9—C10 | 1.394 (2) |
O1—C7 | 1.2113 (18) | C9—H9 | 0.9300 |
C8—C9 | 1.3888 (18) | C5—C4 | 1.398 (2) |
C8—C2 | 1.5202 (16) | C5—H5 | 0.9300 |
C13—C18 | 1.3867 (19) | C1—H1A | 0.9600 |
C13—C14 | 1.3907 (18) | C1—H1B | 0.9600 |
C13—C2 | 1.5410 (17) | C1—H1C | 0.9600 |
C6—C5 | 1.3798 (19) | C10—H10 | 0.9300 |
C6—C7 | 1.4288 (18) | C4—H4 | 0.9300 |
C3—C4 | 1.3850 (18) | C15—C16 | 1.380 (3) |
C3—C2 | 1.5152 (17) | C15—H15 | 0.9300 |
C2—C1 | 1.5470 (16) | C17—C16 | 1.374 (3) |
C11—C10 | 1.3833 (19) | C17—H17 | 0.9300 |
C11—C12 | 1.4261 (18) | C16—H16 | 0.9300 |
C3—N1—C6 | 109.44 (10) | O1—C7—C6 | 125.90 (14) |
C3—N1—H1 | 125.3 | O1—C7—H7 | 117.0 |
C6—N1—H1 | 125.3 | C6—C7—H7 | 117.0 |
C8—N2—C11 | 109.55 (10) | O2—C12—C11 | 126.24 (13) |
C8—N2—H2 | 125.2 | O2—C12—H12 | 116.9 |
C11—N2—H2 | 125.2 | C11—C12—H12 | 116.9 |
N2—C8—C9 | 107.91 (11) | C8—C9—C10 | 107.53 (12) |
N2—C8—C2 | 123.11 (10) | C8—C9—H9 | 126.2 |
C9—C8—C2 | 128.86 (11) | C10—C9—H9 | 126.2 |
C18—C13—C14 | 118.02 (12) | C6—C5—C4 | 107.65 (12) |
C18—C13—C2 | 122.18 (11) | C6—C5—H5 | 126.2 |
C14—C13—C2 | 119.76 (11) | C4—C5—H5 | 126.2 |
N1—C6—C5 | 107.49 (11) | C2—C1—H1A | 109.5 |
N1—C6—C7 | 123.62 (12) | C2—C1—H1B | 109.5 |
C5—C6—C7 | 128.80 (13) | H1A—C1—H1B | 109.5 |
N1—C3—C4 | 107.70 (11) | C2—C1—H1C | 109.5 |
N1—C3—C2 | 122.84 (10) | H1A—C1—H1C | 109.5 |
C4—C3—C2 | 129.42 (11) | H1B—C1—H1C | 109.5 |
C3—C2—C8 | 106.88 (10) | C11—C10—C9 | 107.68 (12) |
C3—C2—C13 | 111.23 (10) | C11—C10—H10 | 126.2 |
C8—C2—C13 | 111.41 (9) | C9—C10—H10 | 126.2 |
C3—C2—C1 | 110.70 (9) | C3—C4—C5 | 107.72 (12) |
C8—C2—C1 | 108.65 (10) | C3—C4—H4 | 126.1 |
C13—C2—C1 | 107.96 (11) | C5—C4—H4 | 126.1 |
N2—C11—C10 | 107.32 (11) | C16—C15—C14 | 120.39 (15) |
N2—C11—C12 | 123.89 (12) | C16—C15—H15 | 119.8 |
C10—C11—C12 | 128.73 (13) | C14—C15—H15 | 119.8 |
C15—C14—C13 | 120.75 (14) | C16—C17—C18 | 120.05 (15) |
C15—C14—H14 | 119.6 | C16—C17—H17 | 120.0 |
C13—C14—H14 | 119.6 | C18—C17—H17 | 120.0 |
C13—C18—C17 | 121.17 (14) | C17—C16—C15 | 119.60 (15) |
C13—C18—H18 | 119.4 | C17—C16—H16 | 120.2 |
C17—C18—H18 | 119.4 | C15—C16—H16 | 120.2 |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1i | 0.86 | 2.08 | 2.9321 (16) | 171 |
N2—H2···O2ii | 0.86 | 2.03 | 2.8838 (15) | 173 |
C1—H1B···O1i | 0.96 | 2.58 | 3.3419 (18) | 137 |
Symmetry codes: (i) −x+1, −y, −z+2; (ii) −x+2, −y+1, −z+1. |
Acknowledgements
This work was supported by the VFSTR Deemed to be University, Vadlamudi, Andhra Pradesh, India, under the scheme of seed grant for research faculties. SKL and EP thanks to VFSTR for providing facilities and fellowships.
Funding information
Funding for this research was provided by: Vignan's Foundation for Science, Technology and Research (grant No. VFSTRU/Reg/A4/14/2017-18/278 to Dr. Ravi K Kottalanka).
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