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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 May 20;67(Pt 6):m779. doi: 10.1107/S1600536811018162

Bis(2-methyl­benzoato-κ2 O,O′)(1,10′-phenanthroline-κ2 N,N′)copper(II)

Sheng-Liang Ni a,*, Feng Zhou a, Jin-Li Qi a
PMCID: PMC3120328  PMID: 21754662

Abstract

In the title compound, [Cu(C8H7O2)2(C12H8N2)], the CuII atom assumes a distorted octa­hedral coordination geometry, chelated by two N atoms from the 1,10′-phenanthroline ligand and four O atoms from two 2-methyl­benzoate anions. A significant Jahn–Teller distortion is observed with two axial Cu—O distances significantly longer than those in the equatorial CuO2N2 plane. In the crystal, π–π stacking inter­actions, with centroid–centroid distances of 3.547 (3) or 3.728 (3) Å between the phenanthroline rings, form layers parallel to (011).

Related literature

For Jahn–Teller distortions in copper complexes, see: Yang & Vittal (2003); Su et al. (2005); Liu et al. (2010). For phenanthroline complexes, see: Wang et al. (1996); Wall et al. (1999); Naing et al. (1995). For related structures, see: Cano et al. (1997); Rodrigues et al. (1999) Xu & Xu (2004).graphic file with name e-67-0m779-scheme1.jpg

Experimental

Crystal data

  • [Cu(C8H7O2)2(C12H8N2)]

  • M r = 514.02

  • Monoclinic, Inline graphic

  • a = 16.245 (3) Å

  • b = 10.136 (2) Å

  • c = 14.048 (3) Å

  • β = 99.15 (3)°

  • V = 2283.7 (8) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 1.00 mm−1

  • T = 293 K

  • 0.15 × 0.10 × 0.10 mm

Data collection

  • Rigaku R-AXIS RAPID diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995) T min = 0.866, T max = 0.900

  • 17441 measured reflections

  • 4021 independent reflections

  • 2509 reflections with I > 2σ(I)

  • R int = 0.063

Refinement

  • R[F 2 > 2σ(F 2)] = 0.045

  • wR(F 2) = 0.150

  • S = 1.13

  • 4021 reflections

  • 319 parameters

  • H-atom parameters constrained

  • Δρmax = 0.74 e Å−3

  • Δρmin = −1.04 e Å−3

Data collection: RAPID-AUTO (Rigaku, 1998); cell refinement: RAPID-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2004); 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: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811018162/sj5144sup1.cif

e-67-0m779-sup1.cif (20.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811018162/sj5144Isup2.hkl

e-67-0m779-Isup2.hkl (197.1KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected bond lengths (Å).

Cu—O3 1.919 (4)
Cu—O1 1.927 (4)
Cu—N2 2.010 (4)
Cu—N1 2.025 (4)

Acknowledgments

This project was supported by the Foundation of the Education Department of Zhejiang Province (ZC200805662).

supplementary crystallographic information

Comment

The Jahn-Teller distortion of copper(II) complexes is well known. Most copper(II) complexes display an elongated distortion, and the coordinate bonds in the axial direction are usually longer than those in the equatorial coordination plane by 0.2–0.6 Å (Yang & Vittal, 2003; Su et al., 2005; Liu et al., 2010). Metal-phenanthroline complexes and their derivatives have also attracted much attention (Wang et al., 1996; Wall et al., 1999; Naing et al., 1995). In the title copper(II) phenanthroline complex, (I), a pair of long Cu-O bonds is observed.

The molecular structure of the title complex is shown in Fig. 1. The CuII ion binds to a phenanthroline molecule and two 2-methylbenzoate anions in a distorted octahedral geometry. Two N atoms from phen and two O atoms from carboxyl groups form a tetrahedrally distorted equatorial coordination plane, with a dihedral angle of 7.3 (2) ° between the Cu/O1/O3 and Cu/N1/N2 planes. The bond lengths in the equatorial plane are normal (Table 1). In the axial direction, the Cu-O distances (Cu-O2 2.609 (4) Å, Cu-O4 2.666 (4) Å) are longer than the Cu-O distances(Cu-O1 1.927 (4) Å, Cu-O3 1.919 (4) Å) equatorial plane.

The Cu-O-C angles of (Cu-O1-C13 105.9 (3) °, Cu-O3-C21 108.2 (3) °) are similar to values found in copper(II) complexes with a chelating benzoate ligand, for example, 106.1 (4) ° (Cano et al., 1997) and 104.5 (1) ° (Xu & Xu, 2004), but are much smaller than those in copper(II) complexes with a monodentate benzoate ligand, for example, 131.8 (1) ° (Rodrigues et al., 1999). This suggests the existence of a bonding interaction between atoms Cu and O2, Cu and O4. Besides the elongated Jahn-Teller distortion, the smaller O2-Cu-O4 angle of 132.1 (1) Å is also a possible reason for the larger differences within the same carboxylate group.

In the crystal structure two-dimensional layers form parallel to (011) through π–π packing interactions with centroid to centroid distances 3.547 (3) Å and 3.728 (3) Å between the phenanthroline rings, as shown in Fig. 2.

Experimental

Freshly prepared CuCO3 was essential for an optimal synthesis. 1.0 cm3 (1 M) aqueous Na2CO3 was added dropwise to a stirred aqueous solution of (0.2490 g, 1.0 mmol)CuSO4.5H2O in 4 cm3 of doubly distilled water. This produced a blue precipitate, of Cu(OH)2-2x(CO3)x.yH2O, which was centrifuged and washed with doubly distilled water until no SO4-2 anions were detected in the supernatant liquid. The fresh blue precipitate was subsequently added to a stirred solution of 2-methylbenzoic acid (0.2725 g, 2.0 mmol) and 1,10'-phenanthroline (0.1982 g, 1.0 mmol) in 20 cm3 C2H5OH-H2O (1:1, v/v). The mixture was stirred for 30 min and filtered. The insoluble solid was then filtered off, and the resulting blue filtrate (pH = 5.20) was allowed to stand at room temperature. Blue block-like crystals were grown by slow evaporation over a week. Yield: 45% based on the initial CuSO4.5 H2O.

Refinement

All H-atoms bonded to C were positioned geometrically and refined using a riding model with d(C-H) = 0.093 Å, Uiso(H) = 1.2 Ueq(C) for aromatic, and 0.96 Å, Uiso(H) = 1.5 Ueq(C) for CH3 atoms. H atoms attached to O atoms were found in a difference Fourier synthesis and were refined using a riding model, with the O-H distances fixed as initially found and with Uiso(H) values set at 1.5 Ueq(O).

Figures

Fig. 1.

Fig. 1.

The structure of the title compound with dispalcement ellipsoids drawn at the 45% probability level.

Fig. 2.

Fig. 2.

Crystal packing showing the two-dimensional layer structure linked through π–π stacking interactions.

Crystal data

[Cu(C8H7O2)2(C12H8N2)] F(000) = 1060
Mr = 514.02 Dx = 1.495 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 25 reflections
a = 16.245 (3) Å θ = 3.0–25.0°
b = 10.136 (2) Å µ = 1.00 mm1
c = 14.048 (3) Å T = 293 K
β = 99.15 (3)° Plate, blue
V = 2283.7 (8) Å3 0.15 × 0.10 × 0.10 mm
Z = 4

Data collection

Rigaku R-AXIS RAPID diffractometer 4021 independent reflections
Radiation source: fine-focus sealed tube 2509 reflections with I > 2σ(I)
graphite Rint = 0.063
ω scans θmax = 25.0°, θmin = 3.0°
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) h = −19→19
Tmin = 0.866, Tmax = 0.900 k = −12→12
17441 measured reflections l = −16→16

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.045 H-atom parameters constrained
wR(F2) = 0.150 w = 1/[σ2(Fo2) + (0.0447P)2 + 4.7675P] where P = (Fo2 + 2Fc2)/3
S = 1.13 (Δ/σ)max < 0.001
4021 reflections Δρmax = 0.74 e Å3
319 parameters Δρmin = −1.04 e Å3
0 restraints Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0013 (5)

Special details

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)

x y z Uiso*/Ueq
Cu −0.33221 (4) 0.96309 (7) −0.17022 (4) 0.0480 (2)
O1 −0.2996 (2) 1.1433 (4) −0.1871 (3) 0.0703 (12)
O2 −0.2404 (2) 1.1033 (4) −0.0382 (3) 0.0606 (10)
O3 −0.2325 (2) 0.8925 (4) −0.2077 (3) 0.0635 (11)
O4 −0.3140 (2) 0.8977 (4) −0.3495 (3) 0.0609 (10)
N1 −0.3735 (2) 0.7809 (4) −0.1419 (3) 0.0450 (10)
N2 −0.4462 (2) 1.0137 (4) −0.1442 (3) 0.0423 (9)
C1 −0.3348 (4) 0.6641 (6) −0.1404 (4) 0.0584 (15)
H1 −0.2794 0.6613 −0.1496 0.070*
C2 −0.3756 (5) 0.5461 (6) −0.1255 (4) 0.0698 (17)
H2 −0.3471 0.4665 −0.1251 0.084*
C3 −0.4558 (4) 0.5468 (6) −0.1115 (4) 0.0607 (15)
H3 −0.4825 0.4678 −0.1024 0.073*
C4 −0.4990 (3) 0.6670 (5) −0.1108 (3) 0.0478 (13)
C5 −0.5834 (3) 0.6805 (6) −0.0943 (4) 0.0587 (15)
H5 −0.6141 0.6053 −0.0854 0.070*
C6 −0.6191 (3) 0.7998 (7) −0.0914 (4) 0.0588 (15)
H6 −0.6734 0.8055 −0.0785 0.071*
C7 −0.5753 (3) 0.9185 (6) −0.1076 (3) 0.0482 (13)
C8 −0.6084 (4) 1.0457 (6) −0.1077 (4) 0.0606 (16)
H8 −0.6627 1.0579 −0.0962 0.073*
C9 −0.5615 (4) 1.1519 (6) −0.1244 (4) 0.0623 (16)
H9 −0.5833 1.2366 −0.1235 0.075*
C10 −0.4806 (4) 1.1328 (5) −0.1431 (4) 0.0565 (14)
H10 −0.4494 1.2061 −0.1552 0.068*
C11 −0.4933 (3) 0.9076 (5) −0.1268 (3) 0.0395 (11)
C12 −0.4540 (3) 0.7812 (5) −0.1262 (3) 0.0406 (11)
C13 −0.2490 (3) 1.1732 (5) −0.1108 (4) 0.0476 (12)
C14 −0.2009 (3) 1.3008 (5) −0.1152 (3) 0.0416 (11)
C15 −0.2043 (3) 1.3578 (5) −0.2067 (4) 0.0509 (13)
H15 −0.2348 1.3161 −0.2599 0.061*
C16 −0.1637 (3) 1.4737 (6) −0.2196 (4) 0.0619 (15)
H16 −0.1660 1.5092 −0.2811 0.074*
C17 −0.1197 (4) 1.5370 (6) −0.1411 (5) 0.0667 (16)
H17 −0.0928 1.6163 −0.1490 0.080*
C18 −0.1157 (3) 1.4830 (6) −0.0517 (5) 0.0604 (15)
H18 −0.0859 1.5272 0.0008 0.072*
C19 −0.1545 (3) 1.3636 (5) −0.0356 (4) 0.0496 (13)
C20 −0.1458 (4) 1.3130 (7) 0.0666 (4) 0.080 (2)
H20A −0.1327 1.2206 0.0676 0.120*
H20B −0.1973 1.3262 0.0907 0.120*
H20C −0.1019 1.3600 0.1063 0.120*
C21 −0.2458 (3) 0.8741 (5) −0.2988 (4) 0.0494 (13)
C22 −0.1747 (3) 0.8162 (5) −0.3429 (3) 0.0425 (11)
C23 −0.1959 (3) 0.7396 (5) −0.4251 (3) 0.0531 (14)
H23 −0.2517 0.7325 −0.4527 0.064*
C24 −0.1363 (4) 0.6736 (6) −0.4669 (4) 0.0615 (15)
H24 −0.1517 0.6217 −0.5214 0.074*
C25 −0.0538 (4) 0.6861 (6) −0.4265 (4) 0.0612 (15)
H25 −0.0130 0.6410 −0.4528 0.073*
C26 −0.0319 (3) 0.7651 (6) −0.3470 (4) 0.0555 (14)
H26 0.0243 0.7750 −0.3220 0.067*
C27 −0.0903 (3) 0.8306 (5) −0.3028 (3) 0.0430 (12)
C28 −0.0598 (3) 0.9171 (6) −0.2164 (4) 0.0629 (16)
H18A −0.0909 0.9981 −0.2215 0.094*
H28B −0.0017 0.9361 −0.2144 0.094*
H28C −0.0676 0.8720 −0.1584 0.094*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu 0.0409 (4) 0.0540 (4) 0.0480 (4) −0.0059 (3) 0.0037 (3) 0.0006 (3)
O1 0.067 (2) 0.074 (3) 0.063 (2) −0.024 (2) −0.011 (2) 0.009 (2)
O2 0.075 (3) 0.049 (2) 0.057 (2) −0.006 (2) 0.0108 (19) 0.0059 (19)
O3 0.049 (2) 0.094 (3) 0.048 (2) −0.005 (2) 0.0121 (17) 0.000 (2)
O4 0.045 (2) 0.060 (2) 0.074 (3) −0.0035 (18) −0.0034 (18) 0.005 (2)
N1 0.040 (2) 0.053 (3) 0.041 (2) 0.010 (2) 0.0046 (17) −0.003 (2)
N2 0.051 (2) 0.035 (2) 0.039 (2) 0.0028 (19) 0.0003 (18) 0.0003 (18)
C1 0.059 (3) 0.059 (4) 0.056 (3) 0.022 (3) 0.005 (3) −0.002 (3)
C2 0.105 (5) 0.041 (3) 0.065 (4) 0.018 (4) 0.019 (4) 0.004 (3)
C3 0.091 (5) 0.044 (3) 0.050 (3) −0.007 (3) 0.019 (3) −0.001 (3)
C4 0.056 (3) 0.047 (3) 0.039 (3) −0.009 (3) 0.001 (2) −0.003 (2)
C5 0.054 (3) 0.075 (4) 0.047 (3) −0.027 (3) 0.005 (3) −0.001 (3)
C6 0.041 (3) 0.084 (5) 0.050 (3) −0.007 (3) 0.004 (2) −0.007 (3)
C7 0.040 (3) 0.062 (4) 0.039 (3) 0.006 (3) −0.002 (2) −0.005 (2)
C8 0.050 (3) 0.078 (4) 0.050 (3) 0.025 (3) −0.002 (2) −0.009 (3)
C9 0.070 (4) 0.059 (4) 0.053 (3) 0.031 (3) −0.004 (3) −0.009 (3)
C10 0.081 (4) 0.040 (3) 0.044 (3) 0.006 (3) −0.004 (3) 0.003 (2)
C11 0.039 (3) 0.044 (3) 0.033 (2) 0.002 (2) −0.003 (2) −0.002 (2)
C12 0.041 (3) 0.042 (3) 0.035 (2) 0.005 (2) −0.003 (2) −0.005 (2)
C13 0.041 (3) 0.042 (3) 0.061 (3) 0.001 (2) 0.013 (3) 0.000 (3)
C14 0.036 (2) 0.039 (3) 0.050 (3) 0.000 (2) 0.007 (2) −0.001 (2)
C15 0.043 (3) 0.054 (3) 0.056 (3) −0.003 (2) 0.006 (2) 0.005 (3)
C16 0.057 (3) 0.061 (4) 0.071 (4) 0.003 (3) 0.021 (3) 0.021 (3)
C17 0.060 (4) 0.047 (3) 0.096 (5) −0.006 (3) 0.023 (3) 0.000 (4)
C18 0.049 (3) 0.053 (4) 0.079 (4) −0.007 (3) 0.008 (3) −0.018 (3)
C19 0.046 (3) 0.053 (3) 0.051 (3) −0.005 (3) 0.011 (2) −0.006 (3)
C20 0.086 (5) 0.098 (5) 0.053 (4) −0.023 (4) 0.002 (3) −0.003 (3)
C21 0.039 (3) 0.053 (3) 0.057 (3) −0.013 (2) 0.007 (2) 0.006 (3)
C22 0.044 (3) 0.042 (3) 0.043 (3) −0.005 (2) 0.009 (2) 0.007 (2)
C23 0.058 (3) 0.056 (3) 0.043 (3) −0.015 (3) 0.002 (2) 0.003 (3)
C24 0.088 (4) 0.050 (3) 0.049 (3) −0.014 (3) 0.017 (3) −0.007 (3)
C25 0.070 (4) 0.054 (4) 0.063 (4) 0.006 (3) 0.022 (3) 0.000 (3)
C26 0.051 (3) 0.062 (4) 0.053 (3) −0.001 (3) 0.007 (3) 0.002 (3)
C27 0.042 (3) 0.041 (3) 0.045 (3) −0.002 (2) 0.007 (2) 0.005 (2)
C28 0.048 (3) 0.079 (4) 0.061 (3) −0.014 (3) 0.003 (3) −0.013 (3)

Geometric parameters (Å, °)

Cu—O3 1.919 (4) C11—C12 1.431 (6)
Cu—O1 1.927 (4) C13—C14 1.518 (7)
Cu—N2 2.010 (4) C14—C19 1.399 (7)
Cu—N1 2.025 (4) C14—C15 1.402 (7)
O1—C13 1.279 (6) C15—C16 1.374 (7)
O2—C13 1.230 (6) C15—H15 0.9300
O3—C21 1.277 (6) C16—C17 1.374 (8)
O4—C21 1.240 (6) C16—H16 0.9300
N1—C1 1.339 (6) C17—C18 1.362 (8)
N1—C12 1.361 (6) C17—H17 0.9300
N2—C10 1.332 (6) C18—C19 1.399 (7)
N2—C11 1.364 (6) C18—H18 0.9300
C1—C2 1.399 (8) C19—C20 1.510 (7)
C1—H1 0.9300 C20—H20A 0.9600
C2—C3 1.348 (8) C20—H20B 0.9600
C2—H2 0.9300 C20—H20C 0.9600
C3—C4 1.406 (7) C21—C22 1.515 (7)
C3—H3 0.9300 C22—C23 1.388 (7)
C4—C12 1.404 (7) C22—C27 1.404 (6)
C4—C5 1.434 (7) C23—C24 1.382 (8)
C5—C6 1.345 (8) C23—H23 0.9300
C5—H5 0.9300 C24—C25 1.375 (8)
C6—C7 1.435 (8) C24—H24 0.9300
C6—H6 0.9300 C25—C26 1.374 (7)
C7—C8 1.398 (7) C25—H25 0.9300
C7—C11 1.404 (7) C26—C27 1.383 (7)
C8—C9 1.360 (8) C26—H26 0.9300
C8—H8 0.9300 C27—C28 1.516 (7)
C9—C10 1.393 (8) C28—H18A 0.9600
C9—H9 0.9300 C28—H28B 0.9600
C10—H10 0.9300 C28—H28C 0.9600
O3—Cu—O1 93.39 (18) O1—C13—C14 115.7 (5)
O3—Cu—N2 170.71 (16) C19—C14—C15 118.9 (5)
O1—Cu—N2 93.45 (17) C19—C14—C13 124.8 (4)
O3—Cu—N1 91.94 (17) C15—C14—C13 116.3 (4)
O1—Cu—N1 173.96 (17) C16—C15—C14 121.6 (5)
N2—Cu—N1 81.58 (15) C16—C15—H15 119.2
C13—O1—Cu 105.9 (3) C14—C15—H15 119.2
C21—O3—Cu 108.2 (3) C15—C16—C17 119.5 (5)
C1—N1—C12 117.4 (5) C15—C16—H16 120.3
C1—N1—Cu 129.8 (4) C17—C16—H16 120.3
C12—N1—Cu 112.7 (3) C18—C17—C16 119.7 (6)
C10—N2—C11 117.7 (4) C18—C17—H17 120.2
C10—N2—Cu 129.3 (4) C16—C17—H17 120.2
C11—N2—Cu 113.0 (3) C17—C18—C19 122.7 (5)
N1—C1—C2 121.7 (5) C17—C18—H18 118.7
N1—C1—H1 119.1 C19—C18—H18 118.7
C2—C1—H1 119.1 C14—C19—C18 117.6 (5)
C3—C2—C1 120.6 (6) C14—C19—C20 124.2 (5)
C3—C2—H2 119.7 C18—C19—C20 118.1 (5)
C1—C2—H2 119.7 C19—C20—H20A 109.5
C2—C3—C4 120.0 (5) C19—C20—H20B 109.5
C2—C3—H3 120.0 H20A—C20—H20B 109.5
C4—C3—H3 120.0 C19—C20—H20C 109.5
C12—C4—C3 116.2 (5) H20A—C20—H20C 109.5
C12—C4—C5 118.7 (5) H20B—C20—H20C 109.5
C3—C4—C5 125.1 (5) O4—C21—O3 122.7 (5)
C6—C5—C4 121.3 (5) O4—C21—C22 120.6 (5)
C6—C5—H5 119.4 O3—C21—C22 116.6 (4)
C4—C5—H5 119.4 C23—C22—C27 119.3 (5)
C5—C6—C7 121.4 (5) C23—C22—C21 116.9 (4)
C5—C6—H6 119.3 C27—C22—C21 123.7 (4)
C7—C6—H6 119.3 C24—C23—C22 121.7 (5)
C8—C7—C11 116.7 (5) C24—C23—H23 119.2
C8—C7—C6 124.9 (5) C22—C23—H23 119.2
C11—C7—C6 118.4 (5) C25—C24—C23 118.8 (5)
C9—C8—C7 120.3 (5) C25—C24—H24 120.6
C9—C8—H8 119.9 C23—C24—H24 120.6
C7—C8—H8 119.9 C26—C25—C24 119.9 (5)
C8—C9—C10 119.6 (5) C26—C25—H25 120.0
C8—C9—H9 120.2 C24—C25—H25 120.0
C10—C9—H9 120.2 C25—C26—C27 122.4 (5)
N2—C10—C9 122.5 (5) C25—C26—H26 118.8
N2—C10—H10 118.7 C27—C26—H26 118.8
C9—C10—H10 118.7 C26—C27—C22 117.7 (5)
N2—C11—C7 123.2 (5) C26—C27—C28 118.5 (4)
N2—C11—C12 116.4 (4) C22—C27—C28 123.7 (4)
C7—C11—C12 120.3 (5) C27—C28—H18A 109.5
N1—C12—C4 124.1 (4) C27—C28—H28B 109.5
N1—C12—C11 116.1 (4) H18A—C28—H28B 109.5
C4—C12—C11 119.8 (4) C27—C28—H28C 109.5
O2—C13—O1 122.1 (5) H18A—C28—H28C 109.5
O2—C13—C14 122.2 (5) H28B—C28—H28C 109.5

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SJ5144).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811018162/sj5144sup1.cif

e-67-0m779-sup1.cif (20.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811018162/sj5144Isup2.hkl

e-67-0m779-Isup2.hkl (197.1KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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