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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 May 31;68(Pt 6):o1974. doi: 10.1107/S1600536812024129

1-[Bis(4-fluoro­phen­yl)meth­yl]-4-[2-(naphthalen-2-yl­oxy)eth­yl]piperazine

Yan Zhong a, Bin Wu b,*
PMCID: PMC3379521  PMID: 22719719

Abstract

In the title mol­ecule, C29H28F2N2O, the piperazine ring adopts a chair conformation with the pendant N—C bonds in equatorial orientations. The conformation of the N—C—C—O linkage is gauche [torsion angle = −64.6 (4)°] and the dihedral angle between the fluoro­benzene rings is 64.02 (15)°.

Related literature  

For related structures and background to 1-[bis­(4-fluoro­phen­yl)meth­yl]piperazine derivatives, see: Wu et al. (2008); Dayananda et al. (2012); Dai et al. (2012).graphic file with name e-68-o1974-scheme1.jpg

Experimental  

Crystal data  

  • C29H28F2N2O

  • M r = 458.53

  • Monoclinic, Inline graphic

  • a = 10.416 (2) Å

  • b = 16.870 (3) Å

  • c = 14.311 (3) Å

  • β = 100.57 (3)°

  • V = 2472.0 (9) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 293 K

  • 0.30 × 0.20 × 0.10 mm

Data collection  

  • Enraf–Nonius CAD-4 diffractometer

  • 4802 measured reflections

  • 4541 independent reflections

  • 2743 reflections with I > 2σ(I)

  • R int = 0.087

  • 3 standard reflections every 200 reflections intensity decay: 1%

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.058

  • wR(F 2) = 0.182

  • S = 1.01

  • 4541 reflections

  • 307 parameters

  • 4 restraints

  • H-atom parameters constrained

  • Δρmax = 0.26 e Å−3

  • Δρmin = −0.22 e Å−3

Data collection: CAD-4 EXPRESS (Enraf–Nonius, 1989); cell refinement: CAD-4 EXPRESS; data reduction: XCAD4 (Harms & Wocadlo, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXL97; software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812024129/hb6811sup1.cif

e-68-o1974-sup1.cif (23.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812024129/hb6811Isup2.hkl

e-68-o1974-Isup2.hkl (222.5KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812024129/hb6811Isup3.cml

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

Acknowledgments

The authors thank Professor Hua-Qin Wang of the Analysis Centre, Nanjing University, for the diffraction measurements. This work was supported by the Natural Science Foundation of Jiangsu Province (grant No. BK2010538).

supplementary crystallographic information

Comment

As a continuation of our study of 1-(bis(4-fluorophenyl)methyl)piperazine derivatives (Wu et al., 2008; Dai et al., 2012), we present here the title compound (I). In (I) (Fig. 1), all bond lengths and angles are normal and correspond to those observed in related compounds (Dai et al., 2012). The piperazine ring adopts a chair conformation with puchering parameters Q = 0.590 (3), Theta = 176.9 (3), Phi = 10 (5). The dihedral angle between the fluorobenzene rings is 64.02 (15).

Experimental

A mixture of 2-(2-bromoethoxy)naphthalene (10 mmol), 1-(bis(4-fluorophenyl)methyl)piperazine (15 mmol) and triethylamine (5 ml) were mixed along with 40 ml acetonitrile and then refluxed for about 24 h. The progress of the reaction was monitored by TLC. After confirming that the reaction was completed, the solvent was removed under reduced pressure. The resultant mixture was cooled. The solid, 1-(bis(4-fluorophenyl)methyl)-4-(2-(naphthalen-2-yloxy)ethyl)piperazine obtained was filtered and was recrystallized from ethanol. Colorless blocks were grown from ethyl acetate:hexane (2:1) solution by a slow evaporation at room temperature.

Refinement

The C-bound H-atoms were included in calculated positions and treated as riding atoms: C—H = 0.93, 0.97 and 0.98 Å for CH(aromatic), CH2 and CH(methine) H-atoms, respectively, with Uĩso~(H) = 1.2 U~eq~ of the carrier atom.

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) with displacement ellipsoids for non-H drawn at 70% probability level.

Crystal data

C29H28F2N2O F(000) = 968
Mr = 458.53 Dx = 1.232 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
a = 10.416 (2) Å Cell parameters from 25 reflections
b = 16.870 (3) Å θ = 10–13°
c = 14.311 (3) Å µ = 0.09 mm1
β = 100.57 (3)° T = 293 K
V = 2472.0 (9) Å3 Block, colorless
Z = 4 0.30 × 0.20 × 0.10 mm

Data collection

Enraf–Nonius CAD-4 diffractometer Rint = 0.087
Radiation source: fine-focus sealed tube θmax = 25.4°, θmin = 1.9°
Graphite monochromator h = 0→12
ω/2θ scans k = 0→20
4802 measured reflections l = −17→16
4541 independent reflections 3 standard reflections every 200 reflections
2743 reflections with I > 2σ(I) intensity decay: 1%

Refinement

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)] = 0.058 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.182 H-atom parameters constrained
S = 1.01 w = 1/[σ2(Fo2) + (0.1P)2 + 0.2P] where P = (Fo2 + 2Fc2)/3
4541 reflections (Δ/σ)max < 0.001
307 parameters Δρmax = 0.26 e Å3
4 restraints Δρmin = −0.22 e Å3

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
O 0.27757 (19) 0.41478 (11) 0.47099 (15) 0.0661 (6)
N1 0.2649 (2) 0.58274 (13) 0.52960 (17) 0.0575 (6)
F1 0.90854 (19) 0.59295 (13) 0.96914 (15) 0.0967 (7)
C1 0.1204 (3) 0.22487 (16) 0.3853 (2) 0.0542 (7)
F2 0.4277 (2) 1.05347 (11) 0.74130 (15) 0.0922 (7)
N2 0.4063 (2) 0.68238 (13) 0.67855 (16) 0.0528 (6)
C2 0.0148 (3) 0.19302 (19) 0.3205 (2) 0.0721 (9)
H2A −0.0448 0.2268 0.2840 0.087*
C3 −0.0006 (4) 0.1129 (2) 0.3110 (3) 0.0988 (13)
H3A −0.0707 0.0927 0.2679 0.119*
C4 0.0860 (4) 0.0619 (2) 0.3644 (4) 0.1085 (15)
H4A 0.0740 0.0075 0.3572 0.130*
C5 0.1889 (4) 0.0902 (2) 0.4273 (3) 0.0888 (11)
H5A 0.2464 0.0549 0.4633 0.107*
C6 0.2100 (3) 0.17243 (17) 0.4390 (2) 0.0613 (8)
C7 0.3172 (3) 0.20455 (18) 0.5024 (2) 0.0654 (8)
H7A 0.3758 0.1705 0.5394 0.078*
C8 0.3365 (3) 0.28384 (18) 0.5104 (2) 0.0625 (8)
H8A 0.4091 0.3037 0.5512 0.075*
C9 0.2463 (3) 0.33609 (16) 0.45675 (19) 0.0534 (7)
C10 0.1397 (3) 0.30770 (16) 0.3968 (2) 0.0523 (7)
H10A 0.0792 0.3428 0.3634 0.063*
C11 0.1892 (3) 0.47098 (17) 0.4185 (2) 0.0688 (9)
H11A 0.1065 0.4697 0.4405 0.083*
H11B 0.1731 0.4573 0.3516 0.083*
C12 0.2474 (3) 0.55314 (17) 0.4322 (2) 0.0694 (9)
H12A 0.3315 0.5528 0.4123 0.083*
H12B 0.1912 0.5896 0.3909 0.083*
C13 0.3933 (3) 0.56131 (17) 0.5841 (2) 0.0598 (8)
H13A 0.4607 0.5803 0.5511 0.072*
H13B 0.4003 0.5040 0.5885 0.072*
C14 0.4152 (3) 0.59602 (16) 0.6829 (2) 0.0569 (7)
H14A 0.3503 0.5754 0.7171 0.068*
H14B 0.5008 0.5806 0.7170 0.068*
C15 0.2747 (3) 0.70173 (17) 0.6280 (2) 0.0624 (8)
H15A 0.2635 0.7588 0.6257 0.075*
H15B 0.2106 0.6795 0.6619 0.075*
C16 0.2528 (3) 0.66947 (17) 0.5293 (2) 0.0648 (8)
H16A 0.1663 0.6844 0.4964 0.078*
H16B 0.3161 0.6923 0.4951 0.078*
C17 0.4344 (3) 0.72010 (16) 0.77297 (19) 0.0544 (7)
H17A 0.3647 0.7055 0.8073 0.065*
C18 0.5624 (3) 0.69034 (16) 0.82958 (19) 0.0534 (7)
C19 0.6790 (3) 0.6934 (2) 0.7902 (2) 0.0677 (9)
H19A 0.6775 0.7173 0.7314 0.081*
C20 0.7921 (3) 0.6614 (2) 0.8381 (2) 0.0739 (9)
H20A 0.8672 0.6628 0.8117 0.089*
C21 0.7952 (3) 0.62780 (19) 0.9240 (2) 0.0659 (8)
C22 0.6914 (3) 0.62547 (17) 0.9676 (2) 0.0685 (9)
H22A 0.6975 0.6036 1.0279 0.082*
C23 0.5704 (3) 0.65809 (17) 0.9176 (2) 0.0625 (8)
H23A 0.4968 0.6571 0.9458 0.075*
C24 0.4343 (3) 0.80943 (16) 0.76286 (19) 0.0541 (7)
C25 0.3778 (3) 0.85731 (18) 0.8273 (2) 0.0622 (8)
H25A 0.3412 0.8334 0.8747 0.075*
C26 0.3776 (3) 0.93915 (19) 0.8193 (2) 0.0686 (9)
H26A 0.3419 0.9705 0.8615 0.082*
C27 0.4299 (3) 0.97249 (18) 0.7496 (2) 0.0639 (8)
C28 0.4854 (4) 0.93165 (17) 0.6871 (2) 0.0738 (9)
H28A 0.5213 0.9574 0.6405 0.089*
C29 0.4875 (3) 0.84671 (16) 0.6948 (2) 0.0694 (9)
H29A 0.5257 0.8168 0.6527 0.083*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O 0.0676 (13) 0.0462 (12) 0.0759 (14) 0.0018 (10) −0.0091 (11) −0.0051 (10)
N1 0.0629 (15) 0.0381 (12) 0.0640 (15) 0.0030 (11) −0.0082 (12) −0.0007 (10)
F1 0.0811 (14) 0.1069 (17) 0.0887 (14) 0.0046 (12) −0.0196 (11) 0.0062 (12)
C1 0.0533 (16) 0.0475 (17) 0.0649 (18) 0.0035 (13) 0.0188 (14) −0.0039 (13)
F2 0.1064 (16) 0.0490 (11) 0.1124 (16) 0.0025 (10) −0.0030 (12) −0.0074 (10)
N2 0.0521 (14) 0.0410 (13) 0.0625 (14) 0.0018 (10) 0.0027 (11) −0.0030 (11)
C2 0.069 (2) 0.055 (2) 0.090 (2) −0.0001 (16) 0.0066 (18) −0.0102 (17)
C3 0.085 (3) 0.065 (2) 0.137 (4) −0.009 (2) −0.004 (3) −0.022 (2)
C4 0.108 (3) 0.047 (2) 0.159 (4) −0.004 (2) −0.004 (3) −0.011 (2)
C5 0.087 (3) 0.051 (2) 0.124 (3) 0.0107 (19) 0.007 (2) −0.001 (2)
C6 0.0568 (18) 0.0496 (17) 0.079 (2) 0.0041 (14) 0.0173 (16) −0.0012 (15)
C7 0.0619 (19) 0.0530 (19) 0.081 (2) 0.0157 (15) 0.0110 (17) 0.0063 (15)
C8 0.0539 (18) 0.062 (2) 0.0681 (19) 0.0056 (14) 0.0009 (15) −0.0024 (15)
C9 0.0589 (17) 0.0467 (17) 0.0542 (16) 0.0052 (13) 0.0094 (14) −0.0032 (13)
C10 0.0531 (16) 0.0460 (16) 0.0564 (16) 0.0065 (13) 0.0065 (13) −0.0008 (13)
C11 0.078 (2) 0.0483 (18) 0.0691 (19) 0.0024 (16) −0.0140 (16) −0.0005 (14)
C12 0.086 (2) 0.0466 (17) 0.067 (2) −0.0017 (16) −0.0093 (17) 0.0013 (14)
C13 0.0586 (17) 0.0437 (16) 0.0726 (19) 0.0031 (13) 0.0000 (15) −0.0022 (14)
C14 0.0564 (17) 0.0428 (16) 0.0652 (18) 0.0035 (13) −0.0052 (14) 0.0007 (13)
C15 0.0629 (19) 0.0409 (15) 0.080 (2) 0.0054 (13) 0.0041 (16) −0.0024 (14)
C16 0.071 (2) 0.0421 (16) 0.073 (2) 0.0080 (14) −0.0099 (16) 0.0003 (14)
C17 0.0578 (17) 0.0530 (17) 0.0549 (17) −0.0052 (13) 0.0171 (14) −0.0029 (13)
C18 0.0648 (18) 0.0462 (16) 0.0502 (16) −0.0079 (13) 0.0130 (14) −0.0071 (12)
C19 0.064 (2) 0.088 (2) 0.0504 (17) −0.0104 (17) 0.0069 (15) 0.0033 (16)
C20 0.0564 (19) 0.102 (3) 0.060 (2) −0.0097 (18) 0.0020 (15) −0.0002 (18)
C21 0.067 (2) 0.064 (2) 0.0599 (19) −0.0063 (16) −0.0058 (17) −0.0075 (16)
C22 0.098 (3) 0.0520 (18) 0.0523 (17) −0.0059 (17) 0.0052 (18) 0.0012 (14)
C23 0.081 (2) 0.0505 (18) 0.0587 (18) −0.0065 (16) 0.0211 (16) −0.0028 (14)
C24 0.0537 (16) 0.0503 (17) 0.0581 (17) −0.0044 (13) 0.0094 (13) −0.0080 (13)
C25 0.0598 (18) 0.067 (2) 0.0615 (18) 0.0012 (15) 0.0144 (14) −0.0040 (15)
C26 0.066 (2) 0.062 (2) 0.075 (2) 0.0126 (16) 0.0056 (17) −0.0190 (17)
C27 0.067 (2) 0.0490 (18) 0.069 (2) 0.0003 (15) −0.0056 (16) −0.0108 (15)
C28 0.099 (3) 0.0538 (19) 0.068 (2) −0.0155 (18) 0.0136 (19) −0.0032 (16)
C29 0.095 (2) 0.0533 (18) 0.0664 (19) −0.0074 (17) 0.0318 (18) −0.0123 (15)

Geometric parameters (Å, º)

O—C9 1.373 (3) C13—C14 1.508 (4)
O—C11 1.434 (3) C13—H13A 0.9700
N1—C12 1.461 (4) C13—H13B 0.9700
N1—C13 1.465 (3) C14—H14A 0.9700
N1—C16 1.468 (3) C14—H14B 0.9700
F1—C21 1.370 (4) C15—C16 1.492 (4)
C1—C6 1.408 (4) C15—H15A 0.9700
C1—C2 1.408 (4) C15—H15B 0.9700
C1—C10 1.417 (4) C16—H16A 0.9700
F2—C27 1.371 (3) C16—H16B 0.9700
N2—C14 1.461 (3) C17—C18 1.513 (4)
N2—C15 1.465 (3) C17—C24 1.514 (4)
N2—C17 1.474 (3) C17—H17A 0.9800
C2—C3 1.364 (5) C18—C23 1.360 (4)
C2—H2A 0.9300 C18—C19 1.431 (3)
C3—C4 1.373 (5) C19—C20 1.361 (4)
C3—H3A 0.9300 C19—H19A 0.9300
C4—C5 1.353 (5) C20—C21 1.349 (4)
C4—H4A 0.9300 C20—H20A 0.9300
C5—C6 1.410 (4) C21—C22 1.344 (4)
C5—H5A 0.9300 C22—C23 1.439 (3)
C6—C7 1.411 (4) C22—H22A 0.9300
C7—C8 1.354 (4) C23—H23A 0.9300
C7—H7A 0.9300 C24—C29 1.360 (4)
C8—C9 1.408 (4) C24—C25 1.431 (3)
C8—H8A 0.9300 C25—C26 1.385 (4)
C9—C10 1.360 (4) C25—H25A 0.9300
C10—H10A 0.9300 C26—C27 1.345 (4)
C11—C12 1.511 (4) C26—H26A 0.9300
C11—H11A 0.9700 C27—C28 1.341 (4)
C11—H11B 0.9700 C28—C29 1.437 (3)
C12—H12A 0.9700 C28—H28A 0.9300
C12—H12B 0.9700 C29—H29A 0.9300
C9—O—C11 116.7 (2) N2—C14—H14B 109.5
C12—N1—C13 111.5 (2) C13—C14—H14B 109.5
C12—N1—C16 110.0 (2) H14A—C14—H14B 108.1
C13—N1—C16 108.5 (2) N2—C15—C16 110.7 (2)
C6—C1—C2 118.6 (3) N2—C15—H15A 109.5
C6—C1—C10 119.4 (3) C16—C15—H15A 109.5
C2—C1—C10 122.0 (3) N2—C15—H15B 109.5
C14—N2—C15 106.8 (2) C16—C15—H15B 109.5
C14—N2—C17 113.1 (2) H15A—C15—H15B 108.1
C15—N2—C17 111.6 (2) N1—C16—C15 111.2 (2)
C3—C2—C1 120.5 (3) N1—C16—H16A 109.4
C3—C2—H2A 119.8 C15—C16—H16A 109.4
C1—C2—H2A 119.8 N1—C16—H16B 109.4
C2—C3—C4 120.8 (4) C15—C16—H16B 109.4
C2—C3—H3A 119.6 H16A—C16—H16B 108.0
C4—C3—H3A 119.6 N2—C17—C18 110.8 (2)
C5—C4—C3 120.6 (4) N2—C17—C24 110.2 (2)
C5—C4—H4A 119.7 C18—C17—C24 111.5 (2)
C3—C4—H4A 119.7 N2—C17—H17A 108.1
C4—C5—C6 120.8 (3) C18—C17—H17A 108.1
C4—C5—H5A 119.6 C24—C17—H17A 108.1
C6—C5—H5A 119.6 C23—C18—C19 117.8 (3)
C1—C6—C5 118.7 (3) C23—C18—C17 121.8 (2)
C1—C6—C7 118.5 (3) C19—C18—C17 120.3 (2)
C5—C6—C7 122.8 (3) C20—C19—C18 120.4 (3)
C8—C7—C6 121.4 (3) C20—C19—H19A 119.8
C8—C7—H7A 119.3 C18—C19—H19A 119.8
C6—C7—H7A 119.3 C21—C20—C19 120.0 (3)
C7—C8—C9 119.9 (3) C21—C20—H20A 120.0
C7—C8—H8A 120.1 C19—C20—H20A 120.0
C9—C8—H8A 120.1 C22—C21—C20 123.3 (3)
C10—C9—O 125.3 (2) C22—C21—F1 117.8 (3)
C10—C9—C8 120.6 (3) C20—C21—F1 119.0 (3)
O—C9—C8 114.1 (2) C21—C22—C23 117.6 (3)
C9—C10—C1 120.2 (3) C21—C22—H22A 121.2
C9—C10—H10A 119.9 C23—C22—H22A 121.2
C1—C10—H10A 119.9 C18—C23—C22 120.8 (3)
O—C11—C12 109.6 (2) C18—C23—H23A 119.6
O—C11—H11A 109.8 C22—C23—H23A 119.6
C12—C11—H11A 109.8 C29—C24—C25 118.0 (3)
O—C11—H11B 109.8 C29—C24—C17 122.4 (2)
C12—C11—H11B 109.8 C25—C24—C17 119.6 (3)
H11A—C11—H11B 108.2 C26—C25—C24 120.3 (3)
N1—C12—C11 114.4 (3) C26—C25—H25A 119.9
N1—C12—H12A 108.7 C24—C25—H25A 119.9
C11—C12—H12A 108.7 C27—C26—C25 118.9 (3)
N1—C12—H12B 108.7 C27—C26—H26A 120.6
C11—C12—H12B 108.7 C25—C26—H26A 120.6
H12A—C12—H12B 107.6 C28—C27—C26 124.3 (3)
N1—C13—C14 111.7 (2) C28—C27—F2 117.1 (3)
N1—C13—H13A 109.3 C26—C27—F2 118.6 (3)
C14—C13—H13A 109.3 C27—C28—C29 117.6 (3)
N1—C13—H13B 109.3 C27—C28—H28A 121.2
C14—C13—H13B 109.3 C29—C28—H28A 121.2
H13A—C13—H13B 107.9 C24—C29—C28 120.9 (3)
N2—C14—C13 110.5 (2) C24—C29—H29A 119.5
N2—C14—H14A 109.5 C28—C29—H29A 119.5
C13—C14—H14A 109.5
C6—C1—C2—C3 0.7 (5) C13—N1—C16—C15 −55.9 (3)
C10—C1—C2—C3 179.8 (3) N2—C15—C16—N1 60.9 (3)
C1—C2—C3—C4 0.1 (6) C14—N2—C17—C18 51.5 (3)
C2—C3—C4—C5 −0.2 (7) C15—N2—C17—C18 171.9 (2)
C3—C4—C5—C6 −0.5 (7) C14—N2—C17—C24 175.4 (2)
C2—C1—C6—C5 −1.4 (4) C15—N2—C17—C24 −64.1 (3)
C10—C1—C6—C5 179.5 (3) N2—C17—C18—C23 −125.1 (3)
C2—C1—C6—C7 178.7 (3) C24—C17—C18—C23 111.7 (3)
C10—C1—C6—C7 −0.4 (4) N2—C17—C18—C19 53.0 (3)
C4—C5—C6—C1 1.3 (6) C24—C17—C18—C19 −70.1 (3)
C4—C5—C6—C7 −178.8 (4) C23—C18—C19—C20 3.0 (4)
C1—C6—C7—C8 −1.7 (5) C17—C18—C19—C20 −175.2 (3)
C5—C6—C7—C8 178.4 (3) C18—C19—C20—C21 −1.1 (5)
C6—C7—C8—C9 1.9 (5) C19—C20—C21—C22 −1.7 (5)
C11—O—C9—C10 0.5 (4) C19—C20—C21—F1 177.2 (3)
C11—O—C9—C8 −179.8 (3) C20—C21—C22—C23 2.4 (5)
C7—C8—C9—C10 0.1 (5) F1—C21—C22—C23 −176.5 (2)
C7—C8—C9—O −179.7 (3) C19—C18—C23—C22 −2.3 (4)
O—C9—C10—C1 177.5 (2) C17—C18—C23—C22 175.9 (3)
C8—C9—C10—C1 −2.2 (4) C21—C22—C23—C18 −0.3 (4)
C6—C1—C10—C9 2.3 (4) N2—C17—C24—C29 −40.4 (4)
C2—C1—C10—C9 −176.8 (3) C18—C17—C24—C29 83.1 (3)
C9—O—C11—C12 −172.2 (3) N2—C17—C24—C25 140.3 (3)
C13—N1—C12—C11 89.7 (3) C18—C17—C24—C25 −96.2 (3)
C16—N1—C12—C11 −149.9 (3) C29—C24—C25—C26 0.3 (4)
O—C11—C12—N1 −64.6 (4) C17—C24—C25—C26 179.6 (3)
C12—N1—C13—C14 176.5 (2) C24—C25—C26—C27 0.7 (4)
C16—N1—C13—C14 55.2 (3) C25—C26—C27—C28 −1.3 (5)
C15—N2—C14—C13 60.2 (3) C25—C26—C27—F2 179.1 (3)
C17—N2—C14—C13 −176.6 (2) C26—C27—C28—C29 0.8 (5)
N1—C13—C14—N2 −59.4 (3) F2—C27—C28—C29 −179.6 (3)
C14—N2—C15—C16 −61.4 (3) C25—C24—C29—C28 −0.8 (5)
C17—N2—C15—C16 174.6 (2) C17—C24—C29—C28 179.9 (3)
C12—N1—C16—C15 −178.1 (3) C27—C28—C29—C24 0.3 (5)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB6811).

References

  1. Dai, Z.-H., Zhong, Y. & Wu, B. (2012). Acta Cryst. E68, o1077. [DOI] [PMC free article] [PubMed]
  2. Dayananda, A. S., Yathirajan, H. S. & Flörke, U. (2012). Acta Cryst. E68, o968. [DOI] [PMC free article] [PubMed]
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  6. Wu, B., Zhou, L. & Cai, H.-H. (2008). Chin. Chem. Lett. 19, 1163–1166.

Associated Data

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

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812024129/hb6811sup1.cif

e-68-o1974-sup1.cif (23.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812024129/hb6811Isup2.hkl

e-68-o1974-Isup2.hkl (222.5KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812024129/hb6811Isup3.cml

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


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