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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Dec 4;66(Pt 1):o27. doi: 10.1107/S1600536809051447

N,N′-Bis(4-bromo­phen­yl)naphthalene-1,4-dicarboxamide N,N-dimethyl­acetamide disolvate

Lin-Hai Jing a,*
PMCID: PMC2980233  PMID: 21580134

Abstract

The title compound, C24H16Br2N2O2·2C4H9NO, crystallizes in an anti C=O orientation. The two amide groups are twisted away from the naphthalene ring system by 62.67 (8) and 75.93 (7)°. The crystal packing is stabilized by N—H⋯O and C—H⋯O hydrogen bonds. Each of the dimethyl­acetamide solvent mol­ecules is disordered over two positions, with occupancy ratios of 0.556 (7):0.444 (7) and 0.654 (7):0.346 (7).

Related literature

For the use of 1,4-naphthalene­dicarboxylic acid derivatives in the preparation of polymers, see: Fukuzumi et al. (1994); Tsukada et al. (1994). For the crystal structure of the 4-methyl­phenyl analog, see: Jing (2008).graphic file with name e-66-00o27-scheme1.jpg

Experimental

Crystal data

  • C24H16Br2N2O2·2C4H9NO

  • M r = 698.45

  • Triclinic, Inline graphic

  • a = 10.4589 (9) Å

  • b = 12.4485 (5) Å

  • c = 12.8439 (11) Å

  • α = 90.775 (2)°

  • β = 111.370 (4)°

  • γ = 92.944 (2)°

  • V = 1554.3 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 2.65 mm−1

  • T = 93 K

  • 0.47 × 0.33 × 0.17 mm

Data collection

  • Rigaku AFC10/Saturn724+ diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995) T min = 0.364, T max = 0.637

  • 12655 measured reflections

  • 6836 independent reflections

  • 5420 reflections with I > 2σ(I)

  • R int = 0.024

Refinement

  • R[F 2 > 2σ(F 2)] = 0.029

  • wR(F 2) = 0.065

  • S = 0.95

  • 6836 reflections

  • 509 parameters

  • 64 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.35 e Å−3

  • Δρmin = −0.73 e Å−3

Data collection: RAPID-AUTO (Rigaku, 2004); cell refinement: RAPID-AUTO; data reduction: RAPID-AUTO; 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: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809051447/ci2967sup1.cif

e-66-00o27-sup1.cif (30.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809051447/ci2967Isup2.hkl

e-66-00o27-Isup2.hkl (334.5KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1N⋯O4 0.84 (2) 2.03 (3) 2.865 (13) 170 (2)
N2—H2N⋯O3′i 0.81 (2) 2.00 (3) 2.797 (13) 171 (2)
C2—H2⋯O1i 0.95 2.50 3.423 (2) 163
C6—H6⋯O2ii 0.95 2.49 3.426 (2) 169
C14—H14⋯O4iii 0.95 2.55 3.48 (2) 167

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic.

Acknowledgments

The author thanks the Centre for Testing and Analysis, Cheng Du Branch, Chinese Academy of Sciences, for analytical support.

supplementary crystallographic information

Comment

1,4-Naphthalenedicarboxylic acid derivatives are a class of intermediates important for applications as monomers in the preparation of polymers (Fukuzumi et al., 1994; Tsukada et al., 1994). Previously, the author has reported the crystal structure of N,N'-bis(4-methylphenyl)-1,4-naphthalenedicarboxamide N,N-dimethylacetamide disolvate (Jing, 2008). The crystal structure of the title compound is now reported.

The naphthalene ring system is planar, with a maximum deviation of 0.030 (3) Å for atom C3. The two C═O groups exhibit an anti orientation. As a result of steric effects, the substituent groups at atoms C1 and C4 are twisted away from the plane of the naphthalene ring system (Fig. 1). The O1/N1/C1/C11 and O2/N2/C4/C18 planes form dihedral angles of 62.67 (8) and 75.93 (7)°, respectively, with the C1–C4/C9/C10 plane. The O1/N1/C1/C11 and C12–C17 planes are inclined at an angle of 16.21 (4)° while the O2/N2/C4/C18 and C19–C24 planes make a dihedral angle of 7.42 (3)°. The crystal packing is stabilized by N—H···O and C—H···O hydrogen bonds (Table 1).

Experimental

Naphthalene-1,4-dicarboxylic acid (2 mmol) and an excess of thionyl chloride (6 mmol) in dioxane (20 ml) were boiled under reflux for 6 h. The solution was distilled by reduced pressure and a yellow solid was obtained. p-Bromoaniline (4 mmol) in tetrahydrofuran (20 ml) was added to the yellow solid and boiled under reflux for 1 d. The solution was then cooled to ambient temperature and filtered to remove the tetrahydrofuran. The precipitate was dissolved in dimethylacetamide and allowed to stand for one month at ambient temperature, after which time colourless single crystals of the title compound suitable for X-ray diffraction were obtained.

Refinement

Both dimethylacetamide molecules are disordered over two positions. The site-occupation factors for the disordered atoms were refined to 0.444 (7) and 0.556 (7), respectively, for the minor and major components of one of the dimethylacetamide molecules (with O3), and to 0.654 (7) and 0.346 (7), respectively, for the major and minor components of the other molecule. The corresponding distances in the major and minor disorder components were restrained to be the same. The Uij components of atoms O3, O3', C26, C27', C28', C31' and C32'were restrained to an approximate isotropic behaviour. N-bound H atoms were located in a difference Fourier map and refined isotropically (N–H = 0.84 (2) and 0.81 (2) Å). The C-bound H atoms were placed in calculated positions, with C–H = 0.95 or 0.98 Å, and refined using a riding model, with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

The asymmetric unit of the title compound. Displacement ellipsoids are drawn at the 50% probability level. All disorder components are shown. H atoms have been omitted for clarity.

Crystal data

C24H16Br2N2O2·2C4H9NO Z = 2
Mr = 698.45 F(000) = 712
Triclinic, P1 Dx = 1.492 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 10.4589 (9) Å Cell parameters from 4940 reflections
b = 12.4485 (5) Å θ = 3.2–27.5°
c = 12.8439 (11) Å µ = 2.65 mm1
α = 90.775 (2)° T = 93 K
β = 111.370 (4)° Prism, colourless
γ = 92.944 (2)° 0.47 × 0.33 × 0.17 mm
V = 1554.3 (2) Å3

Data collection

Rigaku AFC10/Saturn724+ diffractometer 6836 independent reflections
Radiation source: Rotating Anode 5420 reflections with I > 2σ(I)
graphite Rint = 0.024
Detector resolution: 28.5714 pixels mm-1 θmax = 27.5°, θmin = 3.2°
ω scans h = −11→13
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) k = −15→16
Tmin = 0.364, Tmax = 0.637 l = −16→14
12655 measured reflections

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)] = 0.029 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.065 H atoms treated by a mixture of independent and constrained refinement
S = 0.95 w = 1/[σ2(Fo2) + (0.0312P)2] where P = (Fo2 + 2Fc2)/3
6836 reflections (Δ/σ)max = 0.001
509 parameters Δρmax = 0.35 e Å3
64 restraints Δρmin = −0.72 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 Occ. (<1)
Br1 0.53236 (2) 0.112534 (16) 0.932514 (17) 0.02903 (7)
Br2 0.22415 (2) 1.394801 (16) 0.057404 (18) 0.03060 (7)
O1 0.32331 (13) 0.45436 (10) 0.48313 (11) 0.0177 (3)
O2 0.31551 (13) 1.04379 (10) 0.50572 (11) 0.0191 (3)
N1 0.34837 (17) 0.50996 (13) 0.66106 (14) 0.0168 (3)
H1N 0.348 (2) 0.5650 (19) 0.700 (2) 0.039 (7)*
N2 0.23601 (17) 0.99105 (13) 0.32026 (14) 0.0189 (4)
H2N 0.203 (2) 0.9395 (17) 0.2781 (19) 0.024 (6)*
C1 0.30036 (18) 0.63948 (14) 0.51685 (15) 0.0143 (4)
C2 0.39398 (19) 0.68975 (15) 0.47878 (16) 0.0171 (4)
H2 0.4670 0.6508 0.4729 0.021*
C3 0.38368 (19) 0.79752 (15) 0.44845 (16) 0.0172 (4)
H3 0.4495 0.8307 0.4222 0.021*
C4 0.27922 (18) 0.85564 (14) 0.45630 (15) 0.0145 (4)
C5 0.06363 (19) 0.86155 (15) 0.49518 (16) 0.0170 (4)
H5 0.0559 0.9348 0.4750 0.020*
C6 −0.03434 (19) 0.81135 (15) 0.52719 (16) 0.0183 (4)
H6 −0.1095 0.8499 0.5291 0.022*
C7 −0.02522 (19) 0.70304 (15) 0.55738 (16) 0.0178 (4)
H7 −0.0940 0.6690 0.5798 0.021*
C8 0.08240 (18) 0.64638 (15) 0.55463 (16) 0.0159 (4)
H8 0.0872 0.5731 0.5746 0.019*
C9 0.18715 (18) 0.69610 (14) 0.52222 (15) 0.0130 (4)
C10 0.17723 (18) 0.80569 (14) 0.49159 (15) 0.0136 (4)
C11 0.32325 (18) 0.52500 (14) 0.55106 (16) 0.0144 (4)
C12 0.38661 (19) 0.41416 (14) 0.71995 (16) 0.0153 (4)
C13 0.44442 (19) 0.42461 (15) 0.83616 (16) 0.0184 (4)
H13 0.4552 0.4937 0.8717 0.022*
C14 0.48654 (19) 0.33506 (15) 0.90073 (16) 0.0187 (4)
H14 0.5262 0.3420 0.9800 0.022*
C15 0.46910 (19) 0.23536 (15) 0.84642 (16) 0.0175 (4)
C16 0.40962 (18) 0.22272 (14) 0.73121 (16) 0.0158 (4)
H16 0.3972 0.1532 0.6962 0.019*
C17 0.36833 (18) 0.31242 (14) 0.66737 (16) 0.0145 (4)
H17 0.3278 0.3048 0.5882 0.017*
C18 0.27844 (18) 0.97352 (14) 0.43114 (16) 0.0147 (4)
C19 0.23255 (19) 1.08886 (15) 0.26482 (16) 0.0162 (4)
C20 0.27827 (18) 1.18916 (15) 0.31961 (16) 0.0169 (4)
H20 0.3117 1.1949 0.3990 0.020*
C21 0.27480 (19) 1.28043 (15) 0.25775 (16) 0.0180 (4)
H21 0.3053 1.3490 0.2944 0.022*
C22 0.2264 (2) 1.27038 (15) 0.14216 (17) 0.0195 (4)
C23 0.1782 (2) 1.17201 (15) 0.08598 (17) 0.0236 (5)
H23 0.1433 1.1669 0.0066 0.028*
C24 0.1820 (2) 1.08126 (15) 0.14807 (17) 0.0222 (4)
H24 0.1500 1.0132 0.1108 0.027*
O3 0.9394 (16) 0.1698 (9) 0.8232 (17) 0.021 (2) 0.444 (7)
N3 0.8990 (5) 0.3438 (4) 0.7831 (4) 0.0226 (14) 0.444 (7)
C25 1.0986 (17) 0.2599 (10) 0.7668 (15) 0.025 (2) 0.444 (7)
H25A 1.1649 0.3154 0.8142 0.030* 0.444 (7)
H25B 1.0762 0.2764 0.6879 0.030* 0.444 (7)
H25C 1.1387 0.1896 0.7810 0.030* 0.444 (7)
C26 0.9712 (6) 0.2573 (4) 0.7930 (4) 0.0205 (15) 0.444 (7)
C27 0.9413 (14) 0.4520 (8) 0.7573 (15) 0.024 (2) 0.444 (7)
H27A 0.9882 0.4942 0.8271 0.029* 0.444 (7)
H27B 0.8599 0.4881 0.7108 0.029* 0.444 (7)
H27C 1.0041 0.4454 0.7168 0.029* 0.444 (7)
C28 0.7799 (19) 0.3420 (14) 0.8162 (18) 0.024 (3) 0.444 (7)
H28A 0.7246 0.2743 0.7893 0.029* 0.444 (7)
H28B 0.7242 0.4026 0.7837 0.029* 0.444 (7)
H28C 0.8107 0.3478 0.8980 0.029* 0.444 (7)
O3' 0.9084 (13) 0.1781 (7) 0.8283 (14) 0.0227 (19) 0.556 (7)
N3' 0.9840 (5) 0.3352 (3) 0.7788 (3) 0.0245 (12) 0.556 (7)
C25' 0.7828 (18) 0.3251 (12) 0.8320 (16) 0.040 (4) 0.556 (7)
H25D 0.7252 0.2693 0.8500 0.048* 0.556 (7)
H25E 0.7272 0.3612 0.7646 0.048* 0.556 (7)
H25F 0.8198 0.3778 0.8946 0.048* 0.556 (7)
C26' 0.8982 (4) 0.2748 (4) 0.8120 (3) 0.0197 (12) 0.556 (7)
C27' 0.9802 (11) 0.4515 (7) 0.7669 (13) 0.036 (3) 0.556 (7)
H27D 0.9253 0.4673 0.6894 0.043* 0.556 (7)
H27E 1.0740 0.4832 0.7864 0.043* 0.556 (7)
H27F 0.9387 0.4821 0.8169 0.043* 0.556 (7)
C28' 1.0974 (13) 0.2903 (8) 0.7562 (12) 0.034 (3) 0.556 (7)
H28D 1.1842 0.3113 0.8174 0.041* 0.556 (7)
H28E 1.1003 0.3177 0.6858 0.041* 0.556 (7)
H28F 1.0841 0.2116 0.7501 0.041* 0.556 (7)
O4 0.3394 (12) 0.6785 (6) 0.8119 (18) 0.0205 (19) 0.654 (7)
N4 0.2121 (3) 0.8208 (3) 0.8085 (2) 0.0229 (10) 0.654 (7)
C29 0.4147 (11) 0.8427 (10) 0.7597 (11) 0.028 (3) 0.654 (7)
H29A 0.4752 0.8870 0.8243 0.033* 0.654 (7)
H29B 0.3635 0.8896 0.7000 0.033* 0.654 (7)
H29C 0.4701 0.7967 0.7327 0.033* 0.654 (7)
C30 0.3170 (4) 0.7747 (3) 0.7932 (3) 0.0205 (10) 0.654 (7)
C31 0.1860 (9) 0.9350 (5) 0.7976 (8) 0.0283 (17) 0.654 (7)
H31A 0.2042 0.9679 0.8717 0.034* 0.654 (7)
H31B 0.0898 0.9430 0.7499 0.034* 0.654 (7)
H31C 0.2465 0.9706 0.7639 0.034* 0.654 (7)
C32 0.1180 (15) 0.7532 (12) 0.8495 (11) 0.030 (2) 0.654 (7)
H32A 0.1453 0.6787 0.8559 0.036* 0.654 (7)
H32B 0.0231 0.7554 0.7965 0.036* 0.654 (7)
H32C 0.1243 0.7814 0.9229 0.036* 0.654 (7)
O4' 0.312 (2) 0.6646 (12) 0.810 (3) 0.019 (3) 0.346 (7)
N4' 0.2828 (6) 0.8424 (5) 0.7762 (4) 0.0184 (18) 0.346 (7)
C29' 0.142 (3) 0.748 (2) 0.858 (2) 0.034 (5) 0.346 (7)
H29D 0.1246 0.6751 0.8791 0.041* 0.346 (7)
H29E 0.0585 0.7721 0.8007 0.041* 0.346 (7)
H29F 0.1708 0.7969 0.9235 0.041* 0.346 (7)
C30' 0.2524 (8) 0.7475 (5) 0.8120 (5) 0.022 (2) 0.346 (7)
C31' 0.2132 (17) 0.9405 (10) 0.7792 (16) 0.023 (3) 0.346 (7)
H31D 0.1200 0.9215 0.7765 0.028* 0.346 (7)
H31E 0.2084 0.9836 0.7147 0.028* 0.346 (7)
H31F 0.2647 0.9823 0.8484 0.028* 0.346 (7)
C32' 0.4106 (17) 0.854 (2) 0.746 (2) 0.019 (4) 0.346 (7)
H32D 0.4930 0.8586 0.8142 0.023* 0.346 (7)
H32E 0.4078 0.9197 0.7038 0.023* 0.346 (7)
H32F 0.4132 0.7915 0.6995 0.023* 0.346 (7)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Br1 0.04347 (14) 0.01313 (10) 0.01985 (11) 0.00236 (9) −0.00130 (10) 0.00551 (8)
Br2 0.05477 (16) 0.01552 (11) 0.02162 (12) 0.00101 (10) 0.01403 (11) 0.00613 (8)
O1 0.0235 (7) 0.0134 (7) 0.0165 (7) 0.0034 (5) 0.0073 (6) 0.0003 (5)
O2 0.0257 (7) 0.0144 (7) 0.0169 (7) 0.0017 (6) 0.0075 (6) −0.0002 (5)
N1 0.0254 (9) 0.0102 (8) 0.0142 (8) 0.0058 (7) 0.0059 (7) 0.0008 (6)
N2 0.0279 (10) 0.0105 (8) 0.0154 (9) −0.0011 (7) 0.0050 (8) −0.0003 (7)
C1 0.0167 (9) 0.0128 (9) 0.0113 (9) 0.0024 (7) 0.0023 (8) 0.0013 (7)
C2 0.0178 (10) 0.0165 (10) 0.0185 (10) 0.0055 (8) 0.0078 (8) 0.0022 (8)
C3 0.0172 (10) 0.0175 (10) 0.0186 (10) 0.0008 (8) 0.0089 (8) 0.0018 (8)
C4 0.0158 (9) 0.0129 (9) 0.0139 (9) 0.0018 (7) 0.0041 (8) 0.0015 (7)
C5 0.0186 (10) 0.0135 (9) 0.0181 (10) 0.0041 (8) 0.0051 (8) 0.0022 (7)
C6 0.0148 (10) 0.0201 (10) 0.0206 (10) 0.0043 (8) 0.0068 (8) 0.0000 (8)
C7 0.0174 (10) 0.0191 (10) 0.0193 (10) 0.0000 (8) 0.0096 (8) 0.0007 (8)
C8 0.0157 (10) 0.0144 (9) 0.0159 (10) 0.0011 (7) 0.0037 (8) 0.0028 (7)
C9 0.0160 (9) 0.0128 (9) 0.0096 (9) 0.0025 (7) 0.0037 (8) −0.0009 (7)
C10 0.0143 (9) 0.0135 (9) 0.0116 (9) 0.0017 (7) 0.0031 (8) 0.0001 (7)
C11 0.0116 (9) 0.0142 (9) 0.0169 (10) 0.0024 (7) 0.0043 (8) 0.0023 (7)
C12 0.0159 (10) 0.0132 (9) 0.0174 (10) 0.0041 (7) 0.0062 (8) 0.0036 (7)
C13 0.0227 (10) 0.0130 (9) 0.0181 (10) 0.0024 (8) 0.0057 (8) −0.0013 (7)
C14 0.0223 (10) 0.0179 (10) 0.0121 (9) 0.0009 (8) 0.0018 (8) 0.0012 (7)
C15 0.0200 (10) 0.0121 (9) 0.0192 (10) 0.0039 (8) 0.0051 (8) 0.0054 (8)
C16 0.0173 (10) 0.0117 (9) 0.0189 (10) 0.0002 (7) 0.0074 (8) 0.0010 (7)
C17 0.0161 (10) 0.0151 (9) 0.0130 (9) 0.0021 (7) 0.0058 (8) 0.0009 (7)
C18 0.0127 (9) 0.0145 (9) 0.0193 (10) 0.0031 (7) 0.0083 (8) 0.0038 (7)
C19 0.0191 (10) 0.0135 (9) 0.0164 (10) 0.0025 (8) 0.0065 (8) 0.0040 (7)
C20 0.0176 (10) 0.0169 (10) 0.0150 (10) 0.0015 (8) 0.0043 (8) 0.0013 (7)
C21 0.0213 (10) 0.0128 (9) 0.0197 (10) −0.0001 (8) 0.0073 (9) −0.0003 (7)
C22 0.0257 (11) 0.0135 (9) 0.0204 (10) 0.0026 (8) 0.0094 (9) 0.0061 (8)
C23 0.0352 (12) 0.0186 (10) 0.0154 (10) 0.0018 (9) 0.0074 (9) 0.0020 (8)
C24 0.0328 (12) 0.0121 (9) 0.0186 (10) −0.0015 (8) 0.0062 (9) −0.0011 (8)
O3 0.023 (5) 0.017 (3) 0.022 (3) 0.002 (2) 0.004 (3) −0.001 (2)
N3 0.024 (3) 0.017 (3) 0.023 (2) −0.006 (2) 0.006 (2) 0.0007 (18)
C25 0.027 (4) 0.026 (5) 0.025 (4) −0.003 (4) 0.014 (3) −0.007 (4)
C26 0.019 (3) 0.029 (4) 0.009 (2) −0.001 (2) 0.000 (2) −0.0051 (19)
C27 0.026 (5) 0.019 (4) 0.022 (4) −0.004 (3) 0.004 (5) 0.000 (3)
C28 0.017 (5) 0.022 (4) 0.036 (6) 0.001 (3) 0.011 (4) −0.011 (5)
O3' 0.028 (5) 0.014 (2) 0.022 (2) 0.001 (2) 0.004 (3) −0.0015 (18)
N3' 0.028 (3) 0.024 (2) 0.0216 (18) −0.0096 (17) 0.0109 (17) −0.0037 (14)
C25' 0.036 (5) 0.040 (6) 0.047 (7) −0.002 (4) 0.018 (4) 0.001 (4)
C26' 0.019 (3) 0.022 (3) 0.0159 (19) −0.0001 (18) 0.0043 (17) −0.0034 (17)
C27' 0.044 (6) 0.027 (3) 0.029 (4) −0.013 (3) 0.007 (5) 0.009 (3)
C28' 0.022 (3) 0.050 (6) 0.028 (4) −0.005 (4) 0.007 (3) −0.008 (4)
O4 0.023 (4) 0.015 (2) 0.018 (2) 0.002 (2) 0.001 (4) −0.003 (2)
N4 0.0200 (17) 0.0206 (19) 0.0267 (16) 0.0044 (13) 0.0065 (13) −0.0019 (12)
C29 0.036 (4) 0.029 (4) 0.017 (3) 0.000 (3) 0.009 (3) −0.004 (3)
C30 0.022 (2) 0.022 (3) 0.0114 (16) 0.0008 (18) −0.0018 (15) −0.0035 (14)
C31 0.021 (3) 0.020 (2) 0.040 (4) 0.006 (2) 0.007 (3) −0.005 (2)
C32 0.021 (4) 0.047 (4) 0.024 (3) 0.000 (3) 0.011 (3) 0.006 (3)
O4' 0.018 (7) 0.014 (4) 0.020 (4) 0.003 (5) 0.001 (6) −0.008 (5)
N4' 0.020 (3) 0.015 (3) 0.018 (3) 0.005 (2) 0.004 (2) −0.003 (2)
C29' 0.018 (8) 0.040 (9) 0.041 (9) −0.013 (6) 0.010 (6) −0.019 (7)
C30' 0.021 (4) 0.025 (5) 0.012 (3) −0.004 (4) −0.002 (3) −0.001 (3)
C31' 0.018 (6) 0.020 (4) 0.032 (5) 0.008 (4) 0.008 (4) 0.002 (3)
C32' 0.008 (5) 0.027 (6) 0.022 (7) −0.005 (4) 0.005 (4) 0.006 (4)

Geometric parameters (Å, °)

Br1—C15 1.9013 (18) C25—C26 1.487 (16)
Br2—C22 1.9014 (18) C25—H25A 0.98
O1—C11 1.231 (2) C25—H25B 0.98
O2—C18 1.227 (2) C25—H25C 0.98
N1—C11 1.357 (2) C27—H27A 0.98
N1—C12 1.417 (2) C27—H27B 0.98
N1—H1N 0.84 (2) C27—H27C 0.98
N2—C18 1.353 (2) C28—H28A 0.98
N2—C19 1.414 (2) C28—H28B 0.98
N2—H2N 0.81 (2) C28—H28C 0.98
C1—C2 1.372 (2) O3'—C26' 1.229 (8)
C1—C9 1.431 (2) N3'—C26' 1.330 (6)
C1—C11 1.502 (2) N3'—C28' 1.457 (13)
C2—C3 1.401 (2) N3'—C27' 1.458 (8)
C2—H2 0.95 C25'—C26' 1.488 (14)
C3—C4 1.374 (3) C25'—H25D 0.98
C3—H3 0.95 C25'—H25E 0.98
C4—C10 1.422 (3) C25'—H25F 0.98
C4—C18 1.507 (2) C27'—H27D 0.98
C5—C6 1.363 (3) C27'—H27E 0.98
C5—C10 1.422 (2) C27'—H27F 0.98
C5—H5 0.95 C28'—H28D 0.98
C6—C7 1.406 (3) C28'—H28E 0.98
C6—H6 0.95 C28'—H28F 0.98
C7—C8 1.369 (3) O4—C30 1.242 (8)
C7—H7 0.95 N4—C30 1.337 (5)
C8—C9 1.423 (3) N4—C31 1.460 (7)
C8—H8 0.95 N4—C32 1.503 (11)
C9—C10 1.423 (2) C29—C30 1.479 (11)
C12—C13 1.393 (3) C29—H29A 0.98
C12—C17 1.398 (3) C29—H29B 0.98
C13—C14 1.391 (2) C29—H29C 0.98
C13—H13 0.95 C30—O4 1.242 (8)
C14—C15 1.386 (3) C31—H31A 0.98
C14—H14 0.95 C31—H31B 0.98
C15—C16 1.384 (3) C31—H31C 0.98
C16—C17 1.386 (2) C32—H32A 0.98
C16—H16 0.95 C32—H32B 0.98
C17—H17 0.95 C32—H32C 0.98
C19—C24 1.397 (3) O4'—C30' 1.236 (13)
C19—C20 1.397 (3) N4'—C30' 1.338 (9)
C20—C21 1.390 (2) N4'—C31' 1.461 (11)
C20—H20 0.95 N4'—C32' 1.525 (16)
C21—C22 1.384 (3) C29'—C30' 1.468 (18)
C21—H21 0.95 C29'—H29D 0.98
C22—C23 1.386 (3) C29'—H29E 0.98
C23—C24 1.385 (3) C29'—H29F 0.98
C23—H23 0.95 C31'—H31D 0.98
C24—H24 0.95 C31'—H31E 0.98
O3—C26 1.231 (10) C31'—H31F 0.98
N3—C26 1.328 (8) C32'—H32D 0.98
N3—C28 1.455 (16) C32'—H32E 0.98
N3—C27 1.476 (10) C32'—H32F 0.98
C11—N1—C12 127.23 (16) C21—C22—Br2 119.34 (15)
C11—N1—H1N 116.2 (16) C23—C22—Br2 118.80 (15)
C12—N1—H1N 116.3 (16) C24—C23—C22 118.63 (19)
C18—N2—C19 129.45 (17) C24—C23—H23 120.7
C18—N2—H2N 117.0 (15) C22—C23—H23 120.7
C19—N2—H2N 113.5 (15) C23—C24—C19 120.67 (18)
C2—C1—C9 119.96 (16) C23—C24—H24 119.7
C2—C1—C11 116.99 (15) C19—C24—H24 119.7
C9—C1—C11 123.05 (15) C26—N3—C28 120.6 (9)
C1—C2—C3 121.09 (16) C26—N3—C27 124.9 (8)
C1—C2—H2 119.5 C28—N3—C27 113.7 (10)
C3—C2—H2 119.5 O3—C26—N3 123.8 (9)
C4—C3—C2 120.59 (17) O3—C26—C25 114.8 (9)
C4—C3—H3 119.7 N3—C26—C25 121.3 (7)
C2—C3—H3 119.7 C26'—N3'—C28' 122.0 (6)
C3—C4—C10 120.19 (16) C26'—N3'—C27' 124.8 (7)
C3—C4—C18 118.68 (16) C28'—N3'—C27' 113.1 (7)
C10—C4—C18 121.09 (15) C26'—C25'—H25D 109.6
C6—C5—C10 120.79 (16) C26'—C25'—H25E 109.5
C6—C5—H5 119.6 H25D—C25'—H25E 109.5
C10—C5—H5 119.6 C26'—C25'—H25F 109.3
C5—C6—C7 120.67 (16) H25D—C25'—H25F 109.5
C5—C6—H6 119.7 H25E—C25'—H25F 109.5
C7—C6—H6 119.7 O3'—C26'—N3' 123.7 (7)
C8—C7—C6 120.29 (17) O3'—C26'—C25' 116.7 (9)
C8—C7—H7 119.9 N3'—C26'—C25' 119.5 (8)
C6—C7—H7 119.9 N3'—C27'—H27D 109.5
C7—C8—C9 120.74 (16) N3'—C27'—H27E 109.5
C7—C8—H8 119.6 H27D—C27'—H27E 109.5
C9—C8—H8 119.6 N3'—C27'—H27F 109.5
C8—C9—C10 118.71 (15) H27D—C27'—H27F 109.5
C8—C9—C1 122.53 (16) H27E—C27'—H27F 109.5
C10—C9—C1 118.74 (15) N3'—C28'—H28D 109.5
C4—C10—C5 121.84 (16) N3'—C28'—H28E 109.5
C4—C10—C9 119.35 (15) H28D—C28'—H28E 109.5
C5—C10—C9 118.80 (15) N3'—C28'—H28F 109.4
O1—C11—N1 125.01 (17) H28D—C28'—H28F 109.5
O1—C11—C1 120.76 (16) H28E—C28'—H28F 109.5
N1—C11—C1 114.18 (16) C30—N4—C31 125.5 (5)
C13—C12—C17 119.83 (16) C30—N4—C32 118.6 (7)
C13—C12—N1 116.77 (17) C31—N4—C32 115.7 (7)
C17—C12—N1 123.41 (17) O4—C30—N4 122.4 (8)
C14—C13—C12 120.73 (18) O4—C30—N4 122.4 (8)
C14—C13—H13 119.6 O4—C30—C29 118.9 (9)
C12—C13—H13 119.6 O4—C30—C29 118.9 (9)
C15—C14—C13 118.27 (18) N4—C30—C29 118.6 (6)
C15—C14—H14 120.9 C30'—N4'—C31' 124.2 (8)
C13—C14—H14 120.9 C30'—N4'—C32' 118.4 (11)
C16—C15—C14 122.03 (17) C31'—N4'—C32' 116.8 (11)
C16—C15—Br1 118.91 (14) C30'—C29'—H29D 109.5
C14—C15—Br1 119.05 (15) C30'—C29'—H29E 109.4
C15—C16—C17 119.36 (17) H29D—C29'—H29E 109.5
C15—C16—H16 120.3 C30'—C29'—H29F 109.5
C17—C16—H16 120.3 H29D—C29'—H29F 109.5
C16—C17—C12 119.76 (17) H29E—C29'—H29F 109.5
C16—C17—H17 120.1 O4'—C30'—N4' 124.1 (16)
C12—C17—H17 120.1 O4'—C30'—C29' 120.9 (18)
O2—C18—N2 125.32 (17) N4'—C30'—C29' 115.0 (12)
O2—C18—C4 121.85 (17) N4'—C31'—H31D 109.5
N2—C18—C4 112.82 (16) N4'—C31'—H31E 109.5
C24—C19—C20 119.70 (17) H31D—C31'—H31E 109.5
C24—C19—N2 116.18 (17) N4'—C31'—H31F 109.5
C20—C19—N2 124.11 (17) H31D—C31'—H31F 109.5
C21—C20—C19 119.86 (18) H31E—C31'—H31F 109.5
C21—C20—H20 120.1 N4'—C32'—H32D 109.5
C19—C20—H20 120.1 N4'—C32'—H32E 109.5
C22—C21—C20 119.26 (18) H32D—C32'—H32E 109.5
C22—C21—H21 120.4 N4'—C32'—H32F 109.5
C20—C21—H21 120.4 H32D—C32'—H32F 109.5
C21—C22—C23 121.86 (17) H32E—C32'—H32F 109.5
C9—C1—C2—C3 2.3 (3) C13—C12—C17—C16 −0.9 (3)
C11—C1—C2—C3 −177.90 (18) N1—C12—C17—C16 179.49 (16)
C1—C2—C3—C4 0.1 (3) C19—N2—C18—O2 4.7 (3)
C2—C3—C4—C10 −2.3 (3) C19—N2—C18—C4 −174.05 (17)
C2—C3—C4—C18 175.41 (18) C3—C4—C18—O2 −102.4 (2)
C10—C5—C6—C7 0.0 (3) C10—C4—C18—O2 75.2 (2)
C5—C6—C7—C8 −0.2 (3) C3—C4—C18—N2 76.3 (2)
C6—C7—C8—C9 0.5 (3) C10—C4—C18—N2 −106.0 (2)
C7—C8—C9—C10 −0.6 (3) C18—N2—C19—C24 −179.70 (19)
C7—C8—C9—C1 −179.19 (18) C18—N2—C19—C20 1.6 (3)
C2—C1—C9—C8 176.20 (17) C24—C19—C20—C21 −0.8 (3)
C11—C1—C9—C8 −3.6 (3) N2—C19—C20—C21 177.91 (17)
C2—C1—C9—C10 −2.4 (3) C19—C20—C21—C22 −0.3 (3)
C11—C1—C9—C10 177.81 (17) C20—C21—C22—C23 1.5 (3)
C3—C4—C10—C5 −176.67 (18) C20—C21—C22—Br2 −179.05 (13)
C18—C4—C10—C5 5.7 (3) C21—C22—C23—C24 −1.5 (3)
C3—C4—C10—C9 2.1 (3) Br2—C22—C23—C24 179.00 (15)
C18—C4—C10—C9 −175.54 (17) C22—C23—C24—C19 0.4 (3)
C6—C5—C10—C4 178.69 (18) C20—C19—C24—C23 0.7 (3)
C6—C5—C10—C9 −0.1 (3) N2—C19—C24—C23 −178.07 (18)
C8—C9—C10—C4 −178.42 (17) C28—N3—C26—O3 4.5 (17)
C1—C9—C10—C4 0.2 (3) C27—N3—C26—O3 174.0 (15)
C8—C9—C10—C5 0.4 (3) C28—N3—C26—C25 −175.8 (13)
C1—C9—C10—C5 179.02 (17) C27—N3—C26—C25 −6.4 (13)
C12—N1—C11—O1 3.9 (3) C28'—N3'—C26'—O3' 1.5 (13)
C12—N1—C11—C1 −173.45 (16) C27'—N3'—C26'—O3' −175.2 (12)
C2—C1—C11—O1 −61.0 (2) C28'—N3'—C26'—C25' −179.0 (12)
C9—C1—C11—O1 118.8 (2) C27'—N3'—C26'—C25' 4.3 (12)
C2—C1—C11—N1 116.43 (19) O4—O4—C30—N4 0(3)
C9—C1—C11—N1 −63.8 (2) O4—O4—C30—C29 0(4)
C11—N1—C12—C13 162.24 (18) C31—N4—C30—O4 174.5 (12)
C11—N1—C12—C17 −18.1 (3) C32—N4—C30—O4 −0.1 (13)
C17—C12—C13—C14 1.1 (3) C31—N4—C30—O4 174.5 (12)
N1—C12—C13—C14 −179.22 (16) C32—N4—C30—O4 −0.1 (13)
C12—C13—C14—C15 −0.2 (3) C31—N4—C30—C29 −1.6 (9)
C13—C14—C15—C16 −1.0 (3) C32—N4—C30—C29 −176.2 (9)
C13—C14—C15—Br1 177.59 (14) C31'—N4'—C30'—O4' −180 (2)
C14—C15—C16—C17 1.3 (3) C32'—N4'—C30'—O4' −9(2)
Br1—C15—C16—C17 −177.35 (13) C31'—N4'—C30'—C29' −0.9 (17)
C15—C16—C17—C12 −0.3 (3) C32'—N4'—C30'—C29' 170.0 (16)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1N···O4 0.84 (2) 2.03 (3) 2.865 (13) 170 (2)
N2—H2N···O3'i 0.81 (2) 2.00 (3) 2.797 (13) 171 (2)
C2—H2···O1i 0.95 2.50 3.423 (2) 163
C6—H6···O2ii 0.95 2.49 3.426 (2) 169
C14—H14···O4iii 0.95 2.55 3.48 (2) 167

Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x, −y+2, −z+1; (iii) −x+1, −y+1, −z+2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CI2967).

References

  1. Fukuzumi, T., Tajiri, T., Tsukada, H. & Yoshida, J. (1994). Jpn Patent JP 06298919.
  2. Higashi, T. (1995). ABSCOR Rigaku Corporation, Tokyo, Japan.
  3. Jing, L.-H. (2008). Acta Cryst. E64, o2379. [DOI] [PMC free article] [PubMed]
  4. Rigaku (2004). RAPID-AUTO Rigaku/MSC Inc., The Woodlands, Texas, USA.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. Tsukada, H., Tajiri, T., Fukuzumi, T. & Yoshida, J. (1994). Jpn Patent JP 06298918.

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/S1600536809051447/ci2967sup1.cif

e-66-00o27-sup1.cif (30.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809051447/ci2967Isup2.hkl

e-66-00o27-Isup2.hkl (334.5KB, hkl)

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


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