Literature DB >> 21581239

(E)-4-[(4-Nitro-phen-yl)diazen-yl]phenyl anthracene-9-carboxyl-ate.

Mark A Rodriguez, Jessica L Nichol, Thomas Zifer, Andrew L Vance, Bryan M Wong, François Léonard.   

Abstract

In the title compound, C(27)H(17)N(3)O(4), the azo group displays a trans conformation and the dihedral angles between the central benzene ring and the pendant anthracene and nitro-benzene rings are 82.94 (7) and 7.30 (9)°, respectively. In the crystal structure, weak C-H⋯O hydrogen bonds, likely associated with a dipole moment present on the mol-ecule, help to consolidate the packing.

Entities:  

Year:  2008        PMID: 21581239      PMCID: PMC2959833          DOI: 10.1107/S1600536808034958

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

This structure is similar to the perviously reported compound (E)-2-{Eth­yl[4-(4-nitro­phenyl­diazen­yl)phen­yl]amino}ethyl anthracene-9-carboxyl­ate (Rodriguez, et al., 2008 ▶). For general background, see: Atassi et al. (1998 ▶); Becke (1993 ▶).

Experimental

Crystal data

C27H17N3O4 M = 447.44 Monoclinic, a = 13.525 (2) Å b = 8.6011 (14) Å c = 18.956 (3) Å β = 109.322 (3)° V = 2080.9 (6) Å3 Z = 4 Mo Kα radiation μ = 0.10 mm−1 T = 173 (2) K 0.20 × 0.18 × 0.05 mm

Data collection

Bruker SMART CCD area-detector diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 1999 ▶) T min = 0.980, T max = 0.995 14511 measured reflections 3665 independent reflections 2752 reflections with I > 2σ(I) R int = 0.038

Refinement

R[F 2 > 2σ(F 2)] = 0.043 wR(F 2) = 0.100 S = 1.03 3665 reflections 307 parameters H-atom parameters constrained Δρmax = 0.39 e Å−3 Δρmin = −0.16 e Å−3 Data collection: SMART (Bruker, 2001 ▶); cell refinement: SMART (Bruker, 2001 ▶); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: XSHELL (Bruker, 2001 ▶); software used to prepare material for publication: SHELXTL. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808034958/hb2827sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808034958/hb2827Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C27H17N3O4F000 = 928
Mr = 447.44Dx = 1.428 Mg m3
Monoclinic, P21/cMo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 100 reflections
a = 13.525 (2) Åθ = 1.6–25.0º
b = 8.6011 (14) ŵ = 0.10 mm1
c = 18.956 (3) ÅT = 173 (2) K
β = 109.322 (3)ºPlate, red
V = 2080.9 (6) Å30.20 × 0.18 × 0.05 mm
Z = 4
Bruker SMART CCD area-detector diffractometer3665 independent reflections
Radiation source: fine-focus sealed tube2752 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.038
Detector resolution: 0 pixels mm-1θmax = 25.0º
T = 173(2) Kθmin = 1.6º
φ and ω scansh = −16→16
Absorption correction: multi-scan(SADABS; Sheldrick, 1999)k = −10→10
Tmin = 0.980, Tmax = 0.995l = −21→22
14511 measured reflections
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.043H-atom parameters constrained
wR(F2) = 0.100  w = 1/[σ2(Fo2) + (0.0388P)2 + 0.7361P] where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.001
3665 reflectionsΔρmax = 0.39 e Å3
307 parametersΔρmin = −0.16 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Geometry. All e.s.d.'s, except the e.s.d. in the dihedral angle between two least-square (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.
xyzUiso*/Ueq
N10.69229 (14)1.52655 (19)0.65761 (9)0.0352 (4)
N20.44775 (13)1.12430 (19)0.43308 (9)0.0350 (4)
N30.48826 (13)1.08369 (18)0.38663 (9)0.0333 (4)
O10.78660 (13)1.5368 (2)0.66951 (9)0.0581 (5)
O20.64573 (13)1.60250 (18)0.69126 (8)0.0486 (4)
O30.26778 (10)0.69438 (15)0.15211 (7)0.0304 (3)
O40.10043 (11)0.77469 (17)0.12517 (8)0.0416 (4)
C10.63159 (15)1.4180 (2)0.59981 (10)0.0272 (4)
C20.52768 (15)1.3952 (2)0.59086 (11)0.0322 (5)
H20.49571.44760.62180.039*
C30.47087 (16)1.2945 (2)0.53590 (11)0.0334 (5)
H30.39931.27490.52950.040*
C40.51755 (15)1.2218 (2)0.49006 (10)0.0289 (5)
C50.62352 (16)1.2433 (2)0.50109 (11)0.0307 (5)
H50.65561.19070.47030.037*
C60.68173 (16)1.3411 (2)0.55702 (11)0.0304 (5)
H60.75451.35550.56600.037*
C70.42162 (15)0.9862 (2)0.32817 (10)0.0298 (5)
C80.31857 (16)0.9475 (2)0.31890 (11)0.0326 (5)
H80.28600.98740.35240.039*
C90.26266 (16)0.8502 (2)0.26061 (11)0.0316 (5)
H90.19240.82180.25430.038*
C100.31210 (15)0.7960 (2)0.21211 (10)0.0273 (4)
C110.41510 (15)0.8342 (2)0.22141 (11)0.0296 (5)
H110.44800.79490.18790.036*
C120.46943 (16)0.9293 (2)0.27953 (11)0.0318 (5)
H120.54010.95600.28620.038*
C130.16358 (15)0.6938 (2)0.11132 (11)0.0281 (4)
C140.14418 (14)0.5854 (2)0.04656 (10)0.0258 (4)
C150.09289 (14)0.6443 (2)−0.02570 (11)0.0265 (4)
C160.05487 (14)0.8006 (2)−0.04087 (12)0.0313 (5)
H160.06260.8699−0.00040.038*
C170.00814 (16)0.8515 (2)−0.11171 (12)0.0383 (5)
H17−0.01590.9559−0.12010.046*
C18−0.00531 (17)0.7513 (3)−0.17329 (12)0.0426 (6)
H18−0.03910.7882−0.22270.051*
C190.02967 (16)0.6035 (2)−0.16205 (12)0.0381 (5)
H190.02060.5375−0.20390.046*
C200.07981 (14)0.5446 (2)−0.08895 (11)0.0287 (5)
C210.11527 (14)0.3921 (2)−0.07705 (11)0.0296 (5)
H210.10700.3269−0.11910.036*
C220.16242 (14)0.3316 (2)−0.00585 (11)0.0256 (4)
C230.19358 (15)0.1725 (2)0.00493 (12)0.0309 (5)
H230.18210.1069−0.03730.037*
C240.23912 (15)0.1134 (2)0.07422 (12)0.0345 (5)
H240.25970.00730.08030.041*
C250.25608 (15)0.2095 (2)0.13743 (12)0.0339 (5)
H250.28860.16770.18600.041*
C260.22641 (15)0.3615 (2)0.12975 (11)0.0312 (5)
H260.23760.42360.17320.037*
C270.17899 (14)0.4293 (2)0.05797 (11)0.0260 (4)
U11U22U33U12U13U23
N10.0431 (11)0.0312 (10)0.0275 (10)−0.0035 (8)0.0066 (8)−0.0032 (8)
N20.0409 (10)0.0305 (10)0.0359 (10)0.0027 (8)0.0158 (9)0.0012 (8)
N30.0388 (10)0.0277 (9)0.0353 (10)0.0021 (8)0.0148 (9)0.0029 (8)
O10.0400 (10)0.0717 (12)0.0571 (11)−0.0170 (9)0.0088 (8)−0.0273 (9)
O20.0602 (11)0.0453 (9)0.0393 (9)0.0034 (8)0.0155 (8)−0.0165 (8)
O30.0253 (7)0.0304 (8)0.0328 (8)−0.0026 (6)0.0060 (6)−0.0102 (6)
O40.0307 (8)0.0404 (9)0.0486 (9)0.0042 (7)0.0062 (7)−0.0176 (7)
C10.0340 (11)0.0229 (10)0.0210 (10)−0.0012 (8)0.0040 (9)0.0008 (8)
C20.0352 (12)0.0302 (11)0.0306 (11)0.0052 (9)0.0102 (9)−0.0003 (9)
C30.0295 (11)0.0335 (11)0.0348 (12)−0.0004 (9)0.0074 (9)0.0016 (9)
C40.0348 (12)0.0224 (10)0.0241 (10)−0.0027 (9)0.0023 (9)0.0017 (8)
C50.0401 (12)0.0276 (11)0.0263 (11)0.0024 (9)0.0135 (9)−0.0016 (9)
C60.0308 (11)0.0299 (11)0.0309 (11)−0.0023 (9)0.0106 (9)0.0009 (9)
C70.0351 (12)0.0226 (10)0.0253 (11)−0.0047 (9)0.0013 (9)0.0003 (8)
C80.0467 (13)0.0280 (11)0.0246 (11)0.0042 (9)0.0137 (10)0.0006 (9)
C90.0327 (12)0.0317 (11)0.0296 (11)−0.0027 (9)0.0094 (9)−0.0003 (9)
C100.0343 (11)0.0202 (10)0.0236 (10)−0.0005 (8)0.0045 (9)−0.0015 (8)
C110.0316 (11)0.0270 (10)0.0282 (11)−0.0010 (9)0.0071 (9)−0.0018 (9)
C120.0314 (11)0.0301 (11)0.0303 (11)−0.0035 (9)0.0056 (9)−0.0022 (9)
C130.0271 (11)0.0222 (10)0.0337 (11)−0.0021 (8)0.0083 (9)−0.0007 (9)
C140.0212 (10)0.0246 (10)0.0304 (11)−0.0045 (8)0.0069 (8)−0.0032 (8)
C150.0202 (10)0.0244 (10)0.0343 (11)−0.0031 (8)0.0083 (9)−0.0007 (9)
C160.0266 (11)0.0249 (10)0.0408 (13)−0.0026 (8)0.0091 (9)−0.0020 (9)
C170.0350 (12)0.0281 (11)0.0482 (14)0.0031 (9)0.0092 (11)0.0068 (10)
C180.0461 (14)0.0416 (13)0.0358 (13)0.0042 (11)0.0076 (11)0.0094 (10)
C190.0422 (13)0.0392 (13)0.0316 (12)0.0006 (10)0.0105 (10)−0.0004 (10)
C200.0256 (10)0.0289 (11)0.0318 (11)−0.0015 (8)0.0097 (9)−0.0010 (9)
C210.0295 (11)0.0299 (11)0.0301 (11)−0.0036 (9)0.0108 (9)−0.0062 (9)
C220.0213 (10)0.0237 (10)0.0319 (11)−0.0034 (8)0.0091 (9)−0.0039 (8)
C230.0319 (11)0.0251 (10)0.0378 (12)−0.0008 (9)0.0142 (10)−0.0050 (9)
C240.0336 (12)0.0227 (10)0.0466 (14)−0.0001 (9)0.0123 (10)0.0022 (10)
C250.0313 (11)0.0308 (11)0.0353 (12)−0.0014 (9)0.0053 (9)0.0056 (9)
C260.0319 (11)0.0280 (11)0.0314 (12)−0.0040 (9)0.0071 (9)−0.0009 (9)
C270.0209 (10)0.0248 (10)0.0316 (11)−0.0044 (8)0.0078 (8)−0.0019 (8)
N1—O11.223 (2)C12—H120.9500
N1—O21.223 (2)C13—C141.494 (3)
N1—C11.467 (2)C14—C151.409 (3)
N2—N31.231 (2)C14—C271.416 (3)
N2—C41.445 (2)C15—C161.434 (3)
N3—C71.443 (2)C15—C201.437 (3)
O3—C131.365 (2)C16—C171.354 (3)
O3—C101.402 (2)C16—H160.9500
O4—C131.196 (2)C17—C181.413 (3)
C1—C21.373 (3)C17—H170.9500
C1—C61.385 (3)C18—C191.349 (3)
C2—C31.377 (3)C18—H180.9500
C2—H20.9500C19—C201.420 (3)
C3—C41.381 (3)C19—H190.9500
C3—H30.9500C20—C211.389 (3)
C4—C51.391 (3)C21—C221.389 (3)
C5—C61.378 (3)C21—H210.9500
C5—H50.9500C22—C231.426 (3)
C6—H60.9500C22—C271.429 (3)
C7—C121.379 (3)C23—C241.352 (3)
C7—C81.387 (3)C23—H230.9500
C8—C91.393 (3)C24—C251.411 (3)
C8—H80.9500C24—H240.9500
C9—C101.384 (3)C25—C261.361 (3)
C9—H90.9500C25—H250.9500
C10—C111.385 (3)C26—C271.423 (3)
C11—C121.374 (3)C26—H260.9500
C11—H110.9500
O1—N1—O2123.42 (18)O3—C13—C14109.61 (15)
O1—N1—C1118.41 (17)C15—C14—C27121.42 (17)
O2—N1—C1118.17 (18)C15—C14—C13118.08 (16)
N3—N2—C4111.35 (17)C27—C14—C13120.48 (17)
N2—N3—C7113.66 (17)C14—C15—C16124.09 (18)
C13—O3—C10123.10 (14)C14—C15—C20118.80 (17)
C2—C1—C6122.62 (18)C16—C15—C20117.09 (17)
C2—C1—N1118.71 (17)C17—C16—C15121.37 (19)
C6—C1—N1118.67 (17)C17—C16—H16119.3
C1—C2—C3118.39 (19)C15—C16—H16119.3
C1—C2—H2120.8C16—C17—C18120.84 (19)
C3—C2—H2120.8C16—C17—H17119.6
C2—C3—C4120.25 (19)C18—C17—H17119.6
C2—C3—H3119.9C19—C18—C17120.1 (2)
C4—C3—H3119.9C19—C18—H18119.9
C3—C4—C5120.56 (18)C17—C18—H18119.9
C3—C4—N2114.30 (17)C18—C19—C20121.3 (2)
C5—C4—N2125.14 (18)C18—C19—H19119.3
C6—C5—C4119.65 (18)C20—C19—H19119.3
C6—C5—H5120.2C21—C20—C19121.55 (18)
C4—C5—H5120.2C21—C20—C15119.19 (18)
C5—C6—C1118.43 (18)C19—C20—C15119.26 (18)
C5—C6—H6120.8C22—C21—C20122.30 (18)
C1—C6—H6120.8C22—C21—H21118.8
C12—C7—C8120.27 (18)C20—C21—H21118.8
C12—C7—N3114.06 (17)C21—C22—C23121.17 (17)
C8—C7—N3125.67 (18)C21—C22—C27119.68 (17)
C7—C8—C9120.27 (18)C23—C22—C27119.15 (18)
C7—C8—H8119.9C24—C23—C22121.19 (19)
C9—C8—H8119.9C24—C23—H23119.4
C10—C9—C8118.32 (19)C22—C23—H23119.4
C10—C9—H9120.8C23—C24—C25119.90 (19)
C8—C9—H9120.8C23—C24—H24120.0
C9—C10—C11121.49 (18)C25—C24—H24120.0
C9—C10—O3125.30 (17)C26—C25—C24120.85 (19)
C11—C10—O3113.16 (16)C26—C25—H25119.6
C12—C11—C10119.47 (18)C24—C25—H25119.6
C12—C11—H11120.3C25—C26—C27121.29 (19)
C10—C11—H11120.3C25—C26—H26119.4
C11—C12—C7120.18 (19)C27—C26—H26119.4
C11—C12—H12119.9C14—C27—C26123.82 (17)
C7—C12—H12119.9C14—C27—C22118.54 (17)
O4—C13—O3123.49 (17)C26—C27—C22117.60 (17)
O4—C13—C14126.81 (18)
D—H···AD—HH···AD···AD—H···A
C26—H26···O2i0.952.543.273 (3)134
C17—H17···O4ii0.952.573.509 (3)169
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C26—H26⋯O2i0.952.543.273 (3)134
C17—H17⋯O4ii0.952.573.509 (3)169

Symmetry codes: (i) ; (ii) .

  2 in total

1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

2.  (E)-2-{Eth-yl[4-(4-nitro-phenyl-diazen-yl)phen-yl]amino}ethyl anthracene-9-carboxyl-ate.

Authors:  Mark A Rodriguez; Thomas Zifer; Andrew L Vance; Bryan M Wong; Francois Leonard
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2008-02-15
  2 in total
  1 in total

1.  Electronic Properties of Vinylene-Linked Heterocyclic Conducting Polymers: Predictive Design and Rational Guidance from DFT Calculations.

Authors:  Bryan M Wong; Joseph G Cordaro
Journal:  J Phys Chem C Nanomater Interfaces       Date:  2011-07-13       Impact factor: 4.126

  1 in total

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