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In the title compound, [Ni(C12H11N2)2], the NiII cation lies on an inversion centre and has a square-planar coordination geometry. This transition metal complex is composed of two deprotonated N,N′-bidentate 2-[(phenyl­imino)­ethyl]-1H-pyr­rol-1-ide ligands around a central NiII cation, with the pyrrolide rings and imine groups lying trans to each other. The Ni—N bond lengths range from 1.894 (3) to 1.939 (2) Å and the bite angle is 83.13 (11)°. The Ni—N(pyrrolide) bond is substantially shorter than the Ni—N(imino) bond. The planes of the phenyl rings make a dihedral angle of 78.79 (9)° with respect to the central NiN4 plane. The mol­ecules are linked into simple chains by an intermolecular C—H...π interaction involving a phenyl β-C atom as donor. Intramolecular C—H...π interactions are also present.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270113018118/lg3114sup1.cif
Contains datablocks II, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113018118/lg3114IIsup2.hkl
Contains datablock II

CCDC reference: 963265

Introduction top

Since α-di­imine ligands with bulky aryl substituents form a series of metal complexes (Johnson et al., 1995; Ittel et al., 2000) which present outstanding activities for α-olefin polymerization, investigations have focused on the exploration of nitro­gen-based polydentate ligands (Small et al., 1998; Gibson et al., 1998; Britovsek et al., 2003; Tenza et al., 2009). One of the explorations aims to promote the synthetic application of imino­pyrrolyl ligands for preparing many kinds of transition metal complexes (Mashima & Tsurugi, 2005). However, contrasting with the considerable research reported on symmetric bis­(imino)­pyrrole complexes, metal complexes of ligands containing both an imine and a pyrrolyl group are uncommon. To the best of our knowledge, only a limited number of mono(imino)­pyrrole compounds have been reported in the literature (Dawson et al., 2000; Anderson et al., 2006; Carabineiro et al., 2007; Pérez-Puente et al., 2008; Imhof, 2012, 2013), in most of which the pyrrole ring is unsubstituted. To prepare original structures incorporating bis­(imino)­pyridine ligands (Small et al., 1998; Gibson et al., 1998; Britovsek et al., 2003), we introduced a methyl side arm on the pyrrole ring (Su, Li et al., 2012; Su, Qin et al., 2012) to give the title complex, (II). It is notable that all previous reports of the synthesis of these ligands invariably relate to deprotonation (Tenza et al., 2009), whereas we provide here a simple synthetic route avoiding that process for this kind of complex.

Experimental top

Synthesis and crystallization top

N-[1-(1H-Pyrrol-2-yl)ethyl­idene]aniline (0.100 g, 0.543 mmol) was dissolved in methanol (10 ml) in a 50 ml flask, and a methanol solution of NiCl2.6H2O (0.129 g, 0.543 mmol) was added slowly dropwise. The mixture was stirred at room temperature for 3 h. After filtering and washing with hexane, the solvent was removed and a red powder was obtained. Selecting chloro­form and acetone (1:1 v/v) to dissolve the red powder (methanol and a small amount of water were poor solvents), red–brown [Brown given in CIF tables - please clarify] crystals of (I) suitable for X-ray diffraction analysis were obtained using the liquid-phase diffusion method (yield 69.2%). Analysis, calculated for C24H22N4Ni: C 67.80, H 5.22, N 13.18%; found: C 68.05, H 5.43, N 12.99%. MS (EI): m/z 424 (M+). IR (KBr): ν(CN) 1659 cm-1.

Refinement top

Crystal data, data collection and structure refinement details are summarized in Table 1. All H atoms were positioned geometrically and treated using a riding model, with C—H = 0.93 and 0.96 Å for aromatic and methyl H atoms, respectively, and with Uiso(H) = 1.5Ueq(C) for methyl H atoms and 1.2Ueq(C) otherwise.

Results and discussion top

The molecular structure of (II) and the atom-labelling scheme are shown in Fig. 1, and selected geometric parameters are listed in Table 2. Complex (II) crystallizes with the imino group of the ligand ortho to the pyrrolide N atom and has two inverted N,N'-bidentate chelating pyrrolide ligands. The NiII cation is located on a crystallographic inversion centre, tetra­coordinated by two imino N atoms and two pyrrolide N atoms, with the pyrrolide rings and the imine groups trans to each other (Fig. 1). The sum of the angles around the NiII centre is 360°, indicating that this atom is in an essentially square-planar conformation. The phenyl substituents on the

imine N atoms show a dihedral angle of 78.79 (9)° with respect to the NiN4 square plane and are parallel to each other due to the imposed inversion centre. The five-membered pyrrolide (py) ring formed by atoms N2/C8–C11 is planar, with a maximum deviation from the plane of 0.004 (3) Å [For which atom?]. In addition, we note that the Ni—Nimine distance [1.939 (2) Å] is substanti­ally longer than the Ni—Npy bond [1.894 (3) Å], due to the anionic nature of the pyrrolide N atom and the steric hindrances of the phenyl-ring substituents. However, all Ni—N bond lengths in (II) are shorter than the normal values for typical NiII—N bonds (2.07 Å; Orpen et al., 1989), particularly the imine Ni—N distances. This may indicate a stronger σ-donor character of atom N1 induced by the methyl (C12) substituent of the iminic carbon (C7), which may also give rise to a higher degree of steric congestion around the NiII cation.

Comparison of the data for the free ligand, (I) (Su, Li et al., 2012), and its NiII complex, (II), also highlights some structural differences. The first feature to note is that the acetyl­imino­pyrrolyl ligand bite angles of (II) (Nimino—Ni—Npy) are very acute [83.13 (11)°], and this decreases the N1—C7—C8 and N2—C8—C7 angles in relation to those observed in the organic ligand precursor (I) [122.82 (16) and 118.71 (16)°, respectively]. Also, the angles at the pyrrole N atom (C—Npy—C) decrease upon coordination, which is compensated by increases in the angles at the C atoms bound to the pyrrole N atom. The bond lengths within the pyrrole ring appear to be significantly affected, and both the C—C and C—N distances, apart from that opposite the C—C bond of the N atom, appear to increase. The angle at imino atom N1 (C6—N1—C7) decreases, but the imine C7N1 double bond and N1—C6 lengthen upon coordination, indicating that π-back-donation from the NiII centre to the imine fragment is relatively strong.

Evidently, an inter­esting phenomenon could be observed in several structures containing various metal complexes of pyrrole ligands (Anderson et al., 2006; Carabineiro et al., 2007; Pérez-Puente et al., 2008; Imhof, 2012, 2013). It is noted that the M—N bond lengths in these examples reveal that the M—Nimino bonds are ca 0.01–0.05 Å longer than the corresponding M—Npy bond within each metal bidentate-chelate unit. In addition, a significant negative correlation is found between the NiminoM—Npy angle for the five-membered chelate rings of pyrrole complexes and the M—Npy bond length. For example, the M—Npy distance increases from 1.9061 (15) Å for [Ni(imino­pyrrole)2] (Ar = 2,4,6-Me3C6H2 [Where is Ar located? Ar-imino?]; Anderson et al., 2006) to 1.915 (2) Å for [Ni(imino­pyrrole)2] (Ar = 2,6-Me2C6H3; Pérez-Puente et al., 2008) to 1.9388 (13) Å for [Co(imino­pyrrole)2] (Ar = 2,6-diiso­propyl­aniline; Carabineiro et al., 2007) to 2.0189 (19) Å for [Pd(imino­pyrrole)2] (Ar = 2,4,6-Me3C6H2; Imhof, 2013) to 2.022 (2) Å for [Pd(imino­pyrrole)2] (Ar = C6H6, Imhof, 2012), while the corresponding inner bite angle decreases from 83.80 (6) to 83.50 (10) to 82.15 (6) to 80.91 (8) to 80.00 (9)°, respectively; the above values are all averages. However, complex (II) does not conform to the above law. The Ni—Npy bond length is 1.894 (3) Å. The Nimino—Ni—Npy angle should be greater than 83.80 (6)° according to the law, but this is not the case, since the angle is 83.13 (11)°. This special case may be due to packing effects.

Examination of the structure with PLATON (Spek, 2009) shows that there is no classical donor (N) present, whereas there are two C—H···π inter­actions (Table 3), thus saturating the hydrogen-bonding capability of the π-electron clouds. One is an inter­molecular inter­action, with phenyl atom C5 acting as the donor, while the other is intra­molecular (see Figs. 1 and 2), with pyrrolide atom C11 acting as the donor. The molecules are linked into simple chains by means of two C—H···π hydrogen bonds in which the molecules act as hydrogen-bond donors and acceptors, resulting in infinite chains.

The supra­molecular assembly of (II) takes the form of a one-dimensional hydrogen-bonded structure. The angles of approach of the H···Cg vector to the planes of the aromatic rings are about 77 and 71° [For which order of the rings?], respectively, and the perpendicular projections of the H atoms onto the pyrrolide ring planes are 0.604 (2) and 0.867 (7) Å, respectively, from the centroids of the rings. In both inter­actions, the H atom lies above the centre of the ring, with the C—H bond pointing towards a pyrrolide and phenyl ring C atom. This corresponds to a type III inter­action, according to the classification of Malone et al. (1997). Furthermore, it has been recognized that these weak C—H···π inter­actions can play an important role in the conformations of organic molecules (Umezawa et al., 1999).

Related literature top

For related literature, see: Anderson et al. (2006); Britovsek et al. (2003); Carabineiro et al. (2007); Dawson et al. (2000); Gibson et al. (1998); Imhof (2012, 2013); Ittel et al. (2000); Johnson et al. (1995); Malone et al. (1997); Mashima & Tsurugi (2005); Orpen et al. (1989); Pérez-Puente, de Jesús, Flores & Gómez-Sal (2008); Small et al. (1998); Spek (2009); Su, Li, Wang & Li (2012); Su, Qin, Jiao & Wang (2012); Tenza et al. (2009); Umezawa et al. (1999).

Computing details top

Data collection: APEX2 (Bruker,2008); cell refinement: SAINT (Bruker,2008); data reduction: SAINT (Bruker,2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: publCIF (Westrip, 2010).

Figures top
[Figure 1] Fig. 1. The molecular structure of (II), showing the atom-numbering scheme. Displacement ellipsiods are drawn at 30% probability level. Dashed lines indicate C—H···π interactions. [Symmetry code: (A) -x + 1, -y + 2, -z.]
[Figure 2] Fig. 2. The unit-cell packing in (II), viewed along b, with the C—H···π bonding scheme shown as dashed lines. H atoms not participating in C—H···π interactions have been omitted for clarity. The largest spheres indicate the centroids of the N2/C8–C11 (Cg1) and C1–C6 (Cg2) rings. See Table 2 for symmetry codes.
Bis{2-[(phenylimino)ethyl]-1H-pyrrol-1-ido-κ2N,N'}nickel(II) top
Crystal data top
[Ni(C12H11N2)2]F(000) = 444
Mr = 425.17Dx = 1.427 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 668 reflections
a = 11.379 (2) Åθ = 2.7–18.6°
b = 15.174 (3) ŵ = 1.00 mm1
c = 5.8453 (11) ÅT = 296 K
β = 101.447 (3)°Needle, brown
V = 989.2 (3) Å30.35 × 0.27 × 0.15 mm
Z = 2
Data collection top
Bruker APEXII CCD area-detector
diffractometer
1757 independent reflections
Radiation source: fine-focus sealed tube1272 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.059
ϕ and ω scansθmax = 25.1°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Bruker, 2008)
h = 1311
Tmin = 0.723, Tmax = 0.862k = 1618
4871 measured reflectionsl = 64
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)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.088H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0291P)2]
where P = (Fo2 + 2Fc2)/3
1757 reflections(Δ/σ)max < 0.001
134 parametersΔρmax = 0.30 e Å3
0 restraintsΔρmin = 0.26 e Å3
Crystal data top
[Ni(C12H11N2)2]V = 989.2 (3) Å3
Mr = 425.17Z = 2
Monoclinic, P21/cMo Kα radiation
a = 11.379 (2) ŵ = 1.00 mm1
b = 15.174 (3) ÅT = 296 K
c = 5.8453 (11) Å0.35 × 0.27 × 0.15 mm
β = 101.447 (3)°
Data collection top
Bruker APEXII CCD area-detector
diffractometer
1757 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2008)
1272 reflections with I > 2σ(I)
Tmin = 0.723, Tmax = 0.862Rint = 0.059
4871 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.088H-atom parameters constrained
S = 1.03Δρmax = 0.30 e Å3
1757 reflectionsΔρmin = 0.26 e Å3
134 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
xyzUiso*/Ueq
Ni10.50001.00000.00000.0317 (2)
N10.5746 (2)0.92309 (17)0.2522 (4)0.0338 (6)
N20.3597 (2)0.93713 (17)0.0280 (4)0.0352 (7)
C10.7620 (3)0.8610 (2)0.1920 (6)0.0404 (9)
H10.72160.84120.04710.048*
C20.8826 (3)0.8445 (2)0.2620 (6)0.0500 (10)
H20.92290.81240.16590.060*
C30.9439 (3)0.8753 (3)0.4743 (7)0.0531 (10)
H31.02580.86510.52040.064*
C40.8831 (3)0.9212 (3)0.6175 (6)0.0503 (10)
H40.92410.94180.76120.060*
C50.7619 (3)0.9368 (2)0.5490 (6)0.0424 (9)
H50.72120.96760.64680.051*
C60.7005 (3)0.9067 (2)0.3349 (5)0.0332 (8)
C70.4969 (3)0.8786 (2)0.3466 (5)0.0344 (8)
C80.3769 (3)0.8849 (2)0.2259 (5)0.0348 (8)
C90.2713 (3)0.8418 (2)0.2425 (6)0.0452 (9)
H90.25930.80360.36020.054*
C100.1877 (3)0.8671 (2)0.0495 (6)0.0499 (10)
H100.10830.84860.01150.060*
C110.2437 (3)0.9251 (2)0.0773 (6)0.0428 (9)
H110.20670.95200.21590.051*
C120.5279 (3)0.8213 (2)0.5590 (5)0.0471 (10)
H12A0.60720.79790.57000.071*
H12B0.47150.77360.54720.071*
H12C0.52480.85550.69570.071*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ni10.0316 (3)0.0352 (4)0.0284 (3)0.0003 (3)0.0059 (2)0.0037 (3)
N10.0333 (15)0.0385 (17)0.0303 (15)0.0023 (13)0.0079 (12)0.0011 (12)
N20.0345 (16)0.0371 (17)0.0338 (16)0.0013 (13)0.0067 (12)0.0059 (13)
C10.042 (2)0.044 (2)0.036 (2)0.0029 (17)0.0095 (17)0.0057 (16)
C20.038 (2)0.058 (3)0.058 (3)0.0017 (19)0.0182 (19)0.006 (2)
C30.029 (2)0.058 (3)0.068 (3)0.0020 (18)0.0008 (19)0.007 (2)
C40.046 (2)0.059 (3)0.041 (2)0.002 (2)0.0033 (18)0.0024 (19)
C50.051 (2)0.044 (2)0.032 (2)0.0046 (18)0.0073 (17)0.0024 (16)
C60.0332 (19)0.035 (2)0.0309 (18)0.0030 (16)0.0058 (15)0.0063 (14)
C70.041 (2)0.0306 (19)0.0336 (18)0.0039 (15)0.0130 (16)0.0017 (15)
C80.033 (2)0.037 (2)0.0356 (19)0.0019 (16)0.0101 (15)0.0030 (15)
C90.045 (2)0.045 (2)0.050 (2)0.0028 (18)0.0201 (19)0.0068 (18)
C100.035 (2)0.051 (2)0.063 (3)0.0077 (18)0.0099 (19)0.009 (2)
C110.035 (2)0.046 (2)0.043 (2)0.0017 (17)0.0015 (16)0.0050 (17)
C120.055 (2)0.048 (2)0.039 (2)0.0053 (18)0.0115 (18)0.0133 (16)
Geometric parameters (Å, º) top
Ni1—N21.894 (3)C4—C51.379 (4)
Ni1—N2i1.894 (3)C4—H40.9300
Ni1—N11.939 (2)C5—C61.384 (4)
Ni1—N1i1.939 (2)C5—H50.9300
N1—C71.317 (4)C7—C81.410 (4)
N1—C61.440 (4)C7—C121.500 (4)
N2—C111.354 (4)C8—C91.389 (4)
N2—C81.383 (4)C9—C101.378 (4)
C1—C21.375 (4)C9—H90.9300
C1—C61.379 (4)C10—C111.385 (4)
C1—H10.9300C10—H100.9300
C2—C31.378 (5)C11—H110.9300
C2—H20.9300C12—H12A0.9600
C3—C41.376 (5)C12—H12B0.9600
C3—H30.9300C12—H12C0.9600
N2—Ni1—N2i180.0C6—C5—H5119.9
N2—Ni1—N183.13 (11)C1—C6—C5119.2 (3)
N2i—Ni1—N196.87 (11)C1—C6—N1118.3 (3)
N2—Ni1—N1i96.87 (11)C5—C6—N1122.5 (3)
N2i—Ni1—N1i83.13 (11)N1—C7—C8114.8 (3)
N1—Ni1—N1i179.998 (1)N1—C7—C12125.2 (3)
C7—N1—C6118.5 (3)C8—C7—C12119.9 (3)
C7—N1—Ni1113.4 (2)N2—C8—C9110.3 (3)
C6—N1—Ni1128.0 (2)N2—C8—C7114.8 (3)
C11—N2—C8105.4 (3)C9—C8—C7134.3 (3)
C11—N2—Ni1142.3 (2)C10—C9—C8106.2 (3)
C8—N2—Ni1112.3 (2)C10—C9—H9126.9
C2—C1—C6120.5 (3)C8—C9—H9126.9
C2—C1—H1119.7C9—C10—C11107.4 (3)
C6—C1—H1119.7C9—C10—H10126.3
C1—C2—C3120.2 (3)C11—C10—H10126.3
C1—C2—H2119.9N2—C11—C10110.7 (3)
C3—C2—H2119.9N2—C11—H11124.7
C4—C3—C2119.6 (3)C10—C11—H11124.7
C4—C3—H3120.2C7—C12—H12A109.5
C2—C3—H3120.2C7—C12—H12B109.5
C3—C4—C5120.3 (3)H12A—C12—H12B109.5
C3—C4—H4119.9C7—C12—H12C109.5
C5—C4—H4119.9H12A—C12—H12C109.5
C4—C5—C6120.2 (3)H12B—C12—H12C109.5
C4—C5—H5119.9
N2—Ni1—N1—C711.1 (2)Ni1—N1—C6—C5109.8 (3)
N2i—Ni1—N1—C7168.9 (2)C6—N1—C7—C8167.8 (3)
N2—Ni1—N1—C6165.4 (3)Ni1—N1—C7—C89.1 (3)
N2i—Ni1—N1—C614.6 (3)C6—N1—C7—C129.5 (5)
N1—Ni1—N2—C11170.7 (4)Ni1—N1—C7—C12173.6 (2)
N1i—Ni1—N2—C119.3 (4)C11—N2—C8—C90.6 (4)
N1—Ni1—N2—C810.6 (2)Ni1—N2—C8—C9178.5 (2)
N1i—Ni1—N2—C8169.4 (2)C11—N2—C8—C7172.0 (3)
C6—C1—C2—C31.4 (5)Ni1—N2—C8—C78.8 (3)
C1—C2—C3—C41.2 (6)N1—C7—C8—N20.3 (4)
C2—C3—C4—C50.3 (6)C12—C7—C8—N2177.7 (3)
C3—C4—C5—C60.3 (5)N1—C7—C8—C9170.1 (3)
C2—C1—C6—C50.8 (5)C12—C7—C8—C97.4 (6)
C2—C1—C6—N1179.3 (3)N2—C8—C9—C100.7 (4)
C4—C5—C6—C10.1 (5)C7—C8—C9—C10169.9 (4)
C4—C5—C6—N1178.4 (3)C8—C9—C10—C110.6 (4)
C7—N1—C6—C1107.6 (3)C8—N2—C11—C100.2 (4)
Ni1—N1—C6—C168.8 (4)Ni1—N2—C11—C10178.5 (3)
C7—N1—C6—C573.9 (4)C9—C10—C11—N20.2 (4)
Symmetry code: (i) x+1, y+2, z.
Hydrogen-bond geometry (Å, º) top
Cg1 is the centroid of the N2/C8–C11 ring and Cg2 is the centroid of the C1–C6 ring.
D—H···AD—HH···AD···AD—H···A
C5—H5···Cg1ii0.932.643.458 (8)147
C11—H11···Cg2i0.932.623.384 (9)140
Symmetry codes: (i) x+1, y+2, z; (ii) x+1, y+2, z+1.

Experimental details

Crystal data
Chemical formula[Ni(C12H11N2)2]
Mr425.17
Crystal system, space groupMonoclinic, P21/c
Temperature (K)296
a, b, c (Å)11.379 (2), 15.174 (3), 5.8453 (11)
β (°) 101.447 (3)
V3)989.2 (3)
Z2
Radiation typeMo Kα
µ (mm1)1.00
Crystal size (mm)0.35 × 0.27 × 0.15
Data collection
DiffractometerBruker APEXII CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 2008)
Tmin, Tmax0.723, 0.862
No. of measured, independent and
observed [I > 2σ(I)] reflections
4871, 1757, 1272
Rint0.059
(sin θ/λ)max1)0.597
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.088, 1.03
No. of reflections1757
No. of parameters134
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.30, 0.26

Computer programs: APEX2 (Bruker,2008), SAINT (Bruker,2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008), publCIF (Westrip, 2010).

Selected geometric parameters (Å, º) top
Ni1—N21.894 (3)N2—C81.383 (4)
Ni1—N11.939 (2)C7—C81.410 (4)
N1—C71.317 (4)C8—C91.389 (4)
N1—C61.440 (4)C9—C101.378 (4)
N2—C111.354 (4)C10—C111.385 (4)
N2—Ni1—N183.13 (11)N1—C7—C8114.8 (3)
N2—Ni1—N1i96.87 (11)N2—C8—C9110.3 (3)
C7—N1—C6118.5 (3)N2—C8—C7114.8 (3)
C11—N2—C8105.4 (3)N2—C11—C10110.7 (3)
N1—C7—C8—N20.3 (4)
Symmetry code: (i) x+1, y+2, z.
Hydrogen-bond geometry (Å, º) top
Cg1 is the centroid of the N2/C8–C11 ring and Cg2 is the centroid of the C1–C6 ring.
D—H···AD—HH···AD···AD—H···A
C5—H5···Cg1ii0.932.643.458 (8)147
C11—H11···Cg2i0.932.623.384 (9)140
Symmetry codes: (i) x+1, y+2, z; (ii) x+1, y+2, z+1.
 

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