Literature DB >> 21201933

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

Mark A Rodriguez, Thomas Zifer, Andrew L Vance, Bryan M Wong, Francois Leonard.   

Abstract

The crystal structure of the title compound, C(31)H(26)N(4)O(4), displays a trans conformation for the nitro-phenyl-diazenyl portion of the mol-ecule. Packing diagrams indicate that weak C-H⋯O hydrogen bonds, likely associated with a strong dipole moment present in the mol-ecule, dictate the arrangement of mol-ecules in the crystal structure.

Entities:  

Year:  2008        PMID: 21201933      PMCID: PMC2960836          DOI: 10.1107/S1600536808004108

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


Related literature

Simmons et al. (2007 ▶) describe the use of the title compound in the fabrication of carbon nanotubes with optically modulated electronic conduction. Sekkat et al. (1992 ▶) document the use of Disperse Red 1 for reversible photoisomerization in thin films. For related literature, see: Atassi et al. (1998 ▶); Becke (1993 ▶).

Experimental

Crystal data

C31H26N4O4 M = 518.56 Triclinic, a = 9.3161 (9) Å b = 10.6586 (10) Å c = 13.5328 (13) Å α = 101.134 (3)° β = 104.667 (4)° γ = 99.779 (3)° V = 1241.2 (2) Å3 Z = 2 Mo Kα radiation μ = 0.09 mm−1 T = 173 (2) K 0.20 × 0.08 × 0.06 mm

Data collection

Bruker SMART CCD area-detector diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 1999 ▶) T min = 0.982, T max = 0.994 9650 measured reflections 4824 independent reflections 2786 reflections with I > 2σ(I) R int = 0.050

Refinement

R[F 2 > 2σ(F 2)] = 0.066 wR(F 2) = 0.123 S = 1.02 4824 reflections 353 parameters H-atom parameters constrained Δρmax = 0.21 e Å−3 Δρmin = −0.21 e Å−3 Data collection: SMART (Bruker, 1998 ▶); cell refinement: SMART; data reduction: SAINT-Plus (Bruker, 2001 ▶); program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: XSHELL (Bruker, 2000 ▶); molecular graphics: XSHELL and Mercury (Macrae et al., 2006 ▶); software used to prepare material for publication: SHELXTL. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808004108/fl2188sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808004108/fl2188Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C31H26N4O4Z = 2
Mr = 518.56F000 = 544
Triclinic, P1Dx = 1.388 Mg m3
Hall symbol: -P 1Mo Kα radiation λ = 0.71073 Å
a = 9.3161 (9) ÅCell parameters from 100 reflections
b = 10.6586 (10) Åθ = 1.6–26.0º
c = 13.5328 (13) ŵ = 0.09 mm1
α = 101.134 (3)ºT = 173 (2) K
β = 104.667 (4)ºIrregular, orange
γ = 99.779 (3)º0.20 × 0.08 × 0.06 mm
V = 1241.2 (2) Å3
Bruker SMART CCD area-detector diffractometer4824 independent reflections
Radiation source: fine-focus sealed tube2786 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.050
Detector resolution: 0 pixels mm-1θmax = 26.0º
T = 173(2) Kθmin = 1.6º
phi and ω scansh = −11→11
Absorption correction: multi-scan(SADABS; Sheldrick, 1999)k = −13→13
Tmin = 0.982, Tmax = 0.994l = −16→16
9650 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)] = 0.066H-atom parameters constrained
wR(F2) = 0.123  w = 1/[σ2(Fo2) + (0.0333P)2] where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.001
4824 reflectionsΔρmax = 0.21 e Å3
353 parametersΔρmin = −0.21 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 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
C10.4311 (4)0.4301 (3)1.1818 (2)0.0357 (8)
H10.35520.38781.11670.043*
C20.3871 (4)0.4647 (3)1.2740 (2)0.0380 (8)
H20.28230.44551.27050.046*
C30.5796 (3)0.4565 (3)1.1849 (2)0.0314 (8)
H30.60660.43321.12180.038*
C40.4936 (3)0.5249 (3)1.3672 (2)0.0330 (8)
H40.46240.54861.42850.040*
C50.6965 (3)0.5190 (3)1.2820 (2)0.0256 (7)
C60.6513 (3)0.5536 (3)1.3752 (2)0.0267 (7)
C70.8515 (3)0.5491 (3)1.2887 (2)0.0233 (7)
C80.7638 (3)0.6146 (3)1.4708 (2)0.0295 (8)
H80.73390.63711.53280.035*
C90.9635 (3)0.6111 (3)1.3845 (2)0.0262 (7)
C100.9183 (3)0.6438 (3)1.4782 (2)0.0271 (7)
C111.1225 (3)0.6452 (3)1.3946 (2)0.0308 (8)
H111.15600.62501.33390.037*
C121.0315 (4)0.7073 (3)1.5759 (2)0.0363 (8)
H121.00170.72921.63800.044*
C131.2262 (4)0.7058 (3)1.4892 (3)0.0385 (9)
H131.33130.72791.49380.046*
C141.1804 (4)0.7369 (3)1.5816 (3)0.0404 (9)
H141.25480.77851.64760.049*
C150.8955 (3)0.5179 (3)1.1890 (2)0.0262 (7)
C160.9915 (3)0.3710 (3)1.0822 (2)0.0283 (7)
H16A1.08230.43721.08560.034*
H16B0.90860.36721.01850.034*
C171.0292 (3)0.2372 (3)1.0778 (2)0.0306 (8)
H17A1.10230.22861.03640.037*
H17B1.08080.23341.15030.037*
C180.8293 (4)0.0686 (3)1.1033 (2)0.0326 (8)
H18A0.90520.09191.17390.039*
H18B0.8035−0.02831.07770.039*
C190.6864 (4)0.1132 (3)1.1141 (2)0.0384 (9)
H19A0.71240.20811.14540.058*
H19B0.64280.06701.15950.058*
H19C0.61170.09341.04430.058*
C200.8434 (3)0.0764 (3)0.9246 (2)0.0252 (7)
C210.9076 (3)0.1361 (3)0.8559 (2)0.0271 (7)
H210.98500.21480.88460.032*
C220.8607 (3)0.0830 (3)0.7490 (2)0.0274 (7)
H220.90830.12380.70530.033*
C230.7442 (3)−0.0300 (3)0.7038 (2)0.0248 (7)
C240.6742 (3)−0.0860 (3)0.7695 (2)0.0275 (7)
H240.5922−0.16140.73940.033*
C250.7210 (3)−0.0349 (3)0.8769 (2)0.0259 (7)
H250.6704−0.07500.91950.031*
C260.6993 (3)−0.0968 (3)0.4302 (2)0.0248 (7)
C270.7983 (3)−0.1047 (3)0.3689 (2)0.0271 (7)
H270.9051−0.07330.40090.033*
C280.7414 (3)−0.1583 (3)0.2614 (2)0.0270 (7)
H280.8081−0.16630.21900.032*
C290.5850 (3)−0.1999 (3)0.2170 (2)0.0255 (7)
C300.4844 (3)−0.1891 (3)0.2755 (2)0.0303 (8)
H300.3775−0.21720.24270.036*
C310.5424 (3)−0.1365 (3)0.3829 (2)0.0298 (7)
H310.4751−0.12740.42460.036*
N10.8986 (3)0.1256 (2)1.03191 (18)0.0281 (6)
N20.6851 (3)−0.0883 (2)0.59401 (18)0.0278 (6)
N30.7671 (3)−0.0435 (2)0.54054 (18)0.0281 (6)
N40.5237 (3)−0.2560 (2)0.10309 (19)0.0333 (7)
O10.9436 (2)0.40590 (19)1.17640 (14)0.0297 (5)
O20.8885 (3)0.5849 (2)1.12621 (17)0.0432 (6)
O30.6111 (3)−0.2485 (2)0.04881 (16)0.0490 (7)
O40.3869 (3)−0.3075 (2)0.06570 (16)0.0461 (6)
U11U22U33U12U13U23
C10.030 (2)0.0329 (19)0.036 (2)0.0005 (16)0.0081 (16)−0.0016 (16)
C20.030 (2)0.035 (2)0.046 (2)0.0021 (16)0.0162 (17)0.0015 (17)
C30.036 (2)0.0261 (18)0.0289 (18)0.0055 (15)0.0106 (16)−0.0005 (14)
C40.036 (2)0.0326 (19)0.035 (2)0.0098 (16)0.0191 (17)0.0063 (16)
C50.0308 (19)0.0178 (16)0.0267 (18)0.0049 (14)0.0099 (15)0.0010 (13)
C60.0305 (19)0.0233 (17)0.0282 (18)0.0062 (14)0.0133 (15)0.0046 (14)
C70.0281 (18)0.0186 (16)0.0264 (17)0.0059 (13)0.0135 (14)0.0054 (13)
C80.040 (2)0.0282 (18)0.0238 (17)0.0098 (15)0.0150 (16)0.0049 (14)
C90.0315 (19)0.0203 (16)0.0285 (18)0.0071 (14)0.0084 (15)0.0096 (14)
C100.0320 (19)0.0227 (17)0.0256 (18)0.0058 (14)0.0084 (15)0.0045 (14)
C110.0299 (19)0.0324 (19)0.0326 (19)0.0089 (15)0.0110 (16)0.0100 (15)
C120.043 (2)0.036 (2)0.0251 (18)0.0072 (17)0.0068 (16)0.0028 (15)
C130.029 (2)0.036 (2)0.047 (2)0.0041 (16)0.0076 (17)0.0102 (17)
C140.044 (2)0.035 (2)0.032 (2)0.0020 (17)0.0012 (17)0.0036 (16)
C150.0232 (18)0.0212 (17)0.0312 (19)0.0026 (14)0.0074 (15)0.0027 (14)
C160.0292 (18)0.0356 (19)0.0184 (16)0.0067 (15)0.0081 (14)0.0021 (14)
C170.0261 (18)0.0376 (19)0.0230 (17)0.0103 (15)0.0047 (14)−0.0035 (15)
C180.043 (2)0.0314 (19)0.0253 (18)0.0130 (16)0.0100 (16)0.0077 (15)
C190.046 (2)0.035 (2)0.036 (2)0.0086 (17)0.0176 (17)0.0064 (16)
C200.0260 (18)0.0265 (18)0.0263 (18)0.0137 (14)0.0094 (15)0.0052 (14)
C210.0234 (17)0.0249 (17)0.0292 (18)0.0042 (14)0.0072 (14)0.0000 (14)
C220.0256 (18)0.0321 (18)0.0276 (18)0.0088 (15)0.0114 (14)0.0076 (15)
C230.0248 (17)0.0263 (17)0.0204 (17)0.0071 (14)0.0052 (14)0.0003 (13)
C240.0282 (18)0.0263 (17)0.0242 (17)0.0053 (14)0.0061 (14)0.0007 (14)
C250.0292 (18)0.0249 (17)0.0242 (17)0.0075 (14)0.0095 (14)0.0046 (14)
C260.0329 (19)0.0179 (16)0.0247 (17)0.0092 (14)0.0085 (15)0.0048 (13)
C270.0248 (17)0.0273 (17)0.0256 (18)0.0035 (14)0.0053 (14)0.0033 (14)
C280.0268 (18)0.0322 (18)0.0250 (18)0.0079 (15)0.0095 (14)0.0104 (14)
C290.0332 (19)0.0233 (17)0.0178 (16)0.0077 (14)0.0045 (14)0.0032 (13)
C300.0271 (18)0.0328 (19)0.0285 (18)0.0077 (15)0.0050 (15)0.0056 (15)
C310.0293 (19)0.0346 (19)0.0268 (18)0.0101 (15)0.0096 (15)0.0070 (15)
N10.0309 (16)0.0331 (15)0.0189 (14)0.0075 (12)0.0072 (12)0.0028 (12)
N20.0308 (15)0.0296 (15)0.0245 (15)0.0111 (12)0.0093 (12)0.0049 (12)
N30.0306 (16)0.0308 (15)0.0218 (14)0.0083 (12)0.0070 (12)0.0037 (12)
N40.0376 (18)0.0333 (16)0.0253 (16)0.0071 (14)0.0045 (14)0.0064 (13)
O10.0383 (13)0.0302 (12)0.0231 (12)0.0128 (10)0.0121 (10)0.0043 (10)
O20.0657 (17)0.0346 (14)0.0456 (15)0.0187 (12)0.0329 (13)0.0194 (12)
O30.0528 (16)0.0625 (17)0.0281 (13)0.0052 (13)0.0163 (12)0.0045 (12)
O40.0316 (14)0.0597 (16)0.0327 (14)0.0039 (12)−0.0035 (11)0.0011 (12)
C1—C31.352 (4)C18—N11.460 (3)
C1—C21.411 (4)C18—C191.519 (4)
C1—H10.9500C18—H18A0.9900
C2—C41.350 (4)C18—H18B0.9900
C2—H20.9500C19—H19A0.9800
C3—C51.431 (4)C19—H19B0.9800
C3—H30.9500C19—H19C0.9800
C4—C61.421 (4)C20—N11.373 (3)
C4—H40.9500C20—C251.413 (4)
C5—C71.400 (4)C20—C211.416 (4)
C5—C61.431 (4)C21—C221.373 (4)
C6—C81.397 (4)C21—H210.9500
C7—C91.399 (4)C22—C231.392 (4)
C7—C151.500 (4)C22—H220.9500
C8—C101.394 (4)C23—C241.392 (4)
C8—H80.9500C23—N21.418 (3)
C9—C111.429 (4)C24—C251.376 (4)
C9—C101.433 (4)C24—H240.9500
C10—C121.422 (4)C25—H250.9500
C11—C131.354 (4)C26—C271.391 (4)
C11—H110.9500C26—C311.391 (4)
C12—C141.349 (4)C26—N31.423 (3)
C12—H120.9500C27—C281.381 (4)
C13—C141.418 (4)C27—H270.9500
C13—H130.9500C28—C291.384 (4)
C14—H140.9500C28—H280.9500
C15—O21.207 (3)C29—C301.378 (4)
C15—O11.341 (3)C29—N41.463 (3)
C16—O11.457 (3)C30—C311.379 (4)
C16—C171.519 (4)C30—H300.9500
C16—H16A0.9900C31—H310.9500
C16—H16B0.9900N2—N31.275 (3)
C17—N11.457 (3)N4—O41.229 (3)
C17—H17A0.9900N4—O31.230 (3)
C17—H17B0.9900
C3—C1—C2120.9 (3)N1—C18—C19114.1 (3)
C3—C1—H1119.5N1—C18—H18A108.7
C2—C1—H1119.5C19—C18—H18A108.7
C4—C2—C1120.2 (3)N1—C18—H18B108.7
C4—C2—H2119.9C19—C18—H18B108.7
C1—C2—H2119.9H18A—C18—H18B107.6
C1—C3—C5120.9 (3)C18—C19—H19A109.5
C1—C3—H3119.6C18—C19—H19B109.5
C5—C3—H3119.6H19A—C19—H19B109.5
C2—C4—C6121.2 (3)C18—C19—H19C109.5
C2—C4—H4119.4H19A—C19—H19C109.5
C6—C4—H4119.4H19B—C19—H19C109.5
C7—C5—C6119.2 (3)N1—C20—C25122.4 (3)
C7—C5—C3122.8 (3)N1—C20—C21121.0 (3)
C6—C5—C3118.0 (3)C25—C20—C21116.6 (3)
C8—C6—C4122.4 (3)C22—C21—C20121.7 (3)
C8—C6—C5118.9 (3)C22—C21—H21119.2
C4—C6—C5118.8 (3)C20—C21—H21119.2
C9—C7—C5121.6 (3)C21—C22—C23120.8 (3)
C9—C7—C15120.1 (3)C21—C22—H22119.6
C5—C7—C15118.2 (3)C23—C22—H22119.6
C10—C8—C6122.2 (3)C22—C23—C24118.4 (3)
C10—C8—H8118.9C22—C23—N2124.4 (3)
C6—C8—H8118.9C24—C23—N2117.1 (3)
C7—C9—C11123.4 (3)C25—C24—C23121.6 (3)
C7—C9—C10119.1 (3)C25—C24—H24119.2
C11—C9—C10117.5 (3)C23—C24—H24119.2
C8—C10—C12121.6 (3)C24—C25—C20120.8 (3)
C8—C10—C9118.9 (3)C24—C25—H25119.6
C12—C10—C9119.5 (3)C20—C25—H25119.6
C13—C11—C9121.1 (3)C27—C26—C31120.1 (3)
C13—C11—H11119.5C27—C26—N3116.6 (3)
C9—C11—H11119.5C31—C26—N3123.3 (3)
C14—C12—C10121.0 (3)C28—C27—C26120.0 (3)
C14—C12—H12119.5C28—C27—H27120.0
C10—C12—H12119.5C26—C27—H27120.0
C11—C13—C14121.0 (3)C27—C28—C29118.5 (3)
C11—C13—H13119.5C27—C28—H28120.8
C14—C13—H13119.5C29—C28—H28120.8
C12—C14—C13120.0 (3)C30—C29—C28122.6 (3)
C12—C14—H14120.0C30—C29—N4118.6 (3)
C13—C14—H14120.0C28—C29—N4118.8 (3)
O2—C15—O1123.0 (3)C29—C30—C31118.5 (3)
O2—C15—C7124.5 (3)C29—C30—H30120.8
O1—C15—C7112.4 (3)C31—C30—H30120.8
O1—C16—C17107.3 (2)C30—C31—C26120.3 (3)
O1—C16—H16A110.3C30—C31—H31119.9
C17—C16—H16A110.3C26—C31—H31119.9
O1—C16—H16B110.3C20—N1—C17120.5 (2)
C17—C16—H16B110.3C20—N1—C18121.5 (2)
H16A—C16—H16B108.5C17—N1—C18118.0 (2)
N1—C17—C16115.0 (2)N3—N2—C23113.5 (2)
N1—C17—H17A108.5N2—N3—C26112.1 (2)
C16—C17—H17A108.5O4—N4—O3122.8 (3)
N1—C17—H17B108.5O4—N4—C29118.6 (3)
C16—C17—H17B108.5O3—N4—C29118.6 (3)
H17A—C17—H17B107.5C15—O1—C16115.4 (2)
D—H···AD—HH···AD···AD—H···A
C1—H1···O3i0.952.563.230 (4)128
C3—H3···O4i0.952.653.570 (4)163
C16—H16B···O4i0.992.613.462 (4)144
C21—H21···O2ii0.952.313.176 (4)152
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C1—H1⋯O3i0.952.563.230 (4)128
C3—H3⋯O4i0.952.653.570 (4)163
C16—H16B⋯O4i0.992.613.462 (4)144
C21—H21⋯O2ii0.952.313.176 (4)152

Symmetry codes: (i) ; (ii) .

  2 in total

1.  Optically modulated conduction in chromophore-functionalized single-wall carbon nanotubes.

Authors:  J M Simmons; I In; V E Campbell; T J Mark; F Léonard; P Gopalan; M A Eriksson
Journal:  Phys Rev Lett       Date:  2007-02-22       Impact factor: 9.161

2.  A short history of SHELX.

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

  2 in total
  3 in total

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

Authors:  Mark A Rodriguez; Jessica L Nichol; Thomas Zifer; Andrew L Vance; Bryan M Wong; François Léonard
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2008-11-08

2.  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

3.  (E)-7-[(4-Nitro-phen-yl)diazen-yl]-3a-(p-tol-yl)-2,3,3a,4-tetra-hydro-1H-benzo[d]pyrrolo-[1,2-a]imidazol-1-one 0.58-dimethyl sulfoxide 0.42-aceto-nitrile solvate: crystal structure, Hirshfeld analysis and DFT estimation of the energy of inter-molecular inter-actions.

Authors:  Vyacheslav S Grinev; Natalya V Babkina; Alevtina Yu Yegorova
Journal:  Acta Crystallogr E Crystallogr Commun       Date:  2017-09-29
  3 in total

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