Literature DB >> 22412487

(E)-2-({2-[(E)-(Hy-droxy-imino)-meth-yl]phen-oxy}meth-yl)-3-p-tolyl-acrylonitrile.

G Suresh, V Sabari, J Srinivasan, Bakthadoss Mannickam, S Aravindhan.   

Abstract

In the title compound, C(18)H(16)N(2)O(2), the hy-droxy-ethanimine group is essentially coplanar with the ring to which it is attached (C-C-N-O torsion angle = -176.9°). Mol-ecules are linked into cyclic centrosymmetric R(2) (2)(6) dimers via O-H⋯N hydrogen bonds.

Entities:  

Year:  2012        PMID: 22412487      PMCID: PMC3297297          DOI: 10.1107/S160053681200270X

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


Related literature

For the structures of other acrylate derivatives, see: Zhang et al. (2009 ▶); Wang et al. (2011 ▶); SakthiMurugesan et al. (2011 ▶); Govindan et al. (2011 ▶). For the use of oxime ligands in coordination chemistry, see: Chaudhuri (2003 ▶). For the biological activity of caffeic acids, see: Hwang et al. (2001 ▶); Altug et al. (2008 ▶); Ates et al. (2006 ▶); Atik et al. (2006 ▶); Padinchare et al. (2001 ▶).

Experimental

Crystal data

C18H16N2O2 M = 292.33 Triclinic, a = 8.4851 (2) Å b = 9.3900 (3) Å c = 10.0779 (3) Å α = 100.208 (2)° β = 90.725 (1)° γ = 105.206 (1)° V = 761.10 (4) Å3 Z = 2 Mo Kα radiation μ = 0.08 mm−1 T = 293 K 0.2 × 0.2 × 0.2 mm

Data collection

Oxford Diffraction Xcalibur-S diffractometer Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009 ▶) T min = 0.980, T max = 0.990 18160 measured reflections 4229 independent reflections 3031 reflections with I > 2σ(I) R int = 0.022

Refinement

R[F 2 > 2σ(F 2)] = 0.047 wR(F 2) = 0.151 S = 1.03 4229 reflections 201 parameters H-atom parameters constrained Δρmax = 0.24 e Å−3 Δρmin = −0.18 e Å−3 Data collection: CrysAlis PRO (Oxford Diffraction, 2009 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: PLATON (Spek, 2009 ▶). Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S160053681200270X/bt5756sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681200270X/bt5756Isup2.hkl Supplementary material file. DOI: 10.1107/S160053681200270X/bt5756Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C18H16N2O2Z = 2
Mr = 292.33F(000) = 308
Triclinic, P1Dx = 1.276 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 8.4851 (2) ÅCell parameters from 8725 reflections
b = 9.3900 (3) Åθ = 2.8–29.1°
c = 10.0779 (3) ŵ = 0.08 mm1
α = 100.208 (2)°T = 293 K
β = 90.725 (1)°Triclinic, colourless
γ = 105.206 (1)°0.2 × 0.2 × 0.2 mm
V = 761.10 (4) Å3
Oxford Diffraction Xcalibur-S diffractometer4229 independent reflections
Radiation source: fine-focus sealed tube3031 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.022
Detector resolution: 15.9948 pixels mm-1θmax = 29.6°, θmin = 2.1°
ω scansh = −11→11
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009)k = −12→12
Tmin = 0.980, Tmax = 0.990l = −13→13
18160 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)] = 0.047H-atom parameters constrained
wR(F2) = 0.151w = 1/[σ2(Fo2) + (0.0732P)2 + 0.135P] where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.001
4229 reflectionsΔρmax = 0.24 e Å3
201 parametersΔρmin = −0.18 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008)
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0173 (18)
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
C10.2633 (2)0.81093 (18)1.11597 (16)0.0584 (4)
H10.20240.85441.17910.070*
C20.22978 (17)0.64825 (16)1.09291 (13)0.0453 (3)
C30.13864 (19)0.57501 (19)1.18740 (15)0.0561 (4)
H30.10030.63181.25850.067*
C40.10362 (19)0.42252 (19)1.17926 (16)0.0589 (4)
H40.04030.37671.24250.071*
C50.1631 (2)0.33864 (18)1.07685 (16)0.0586 (4)
H50.14290.23561.07210.070*
C60.25320 (19)0.40619 (16)0.98021 (14)0.0532 (3)
H60.29380.34820.91150.064*
C70.28343 (16)0.55934 (15)0.98496 (12)0.0421 (3)
C80.3950 (2)0.53835 (16)0.76860 (13)0.0522 (3)
H8A0.30040.45350.73960.063*
H8B0.48740.50030.78660.063*
C90.43216 (17)0.63100 (15)0.66042 (12)0.0450 (3)
C100.29368 (19)0.66178 (18)0.60167 (15)0.0559 (4)
C110.58348 (17)0.67335 (15)0.61876 (13)0.0460 (3)
H110.66090.64330.66500.055*
C120.64990 (16)0.75770 (15)0.51448 (12)0.0435 (3)
C130.81374 (17)0.77192 (17)0.48925 (14)0.0495 (3)
H130.87460.72720.53800.059*
C140.88750 (18)0.85082 (17)0.39364 (15)0.0549 (4)
H140.99740.85890.37950.066*
C150.80160 (19)0.91823 (16)0.31820 (14)0.0536 (4)
C160.6389 (2)0.9040 (2)0.34270 (17)0.0634 (4)
H160.57870.94870.29330.076*
C170.56333 (19)0.8258 (2)0.43805 (17)0.0599 (4)
H170.45350.81820.45170.072*
C180.8817 (3)1.0064 (2)0.21478 (18)0.0740 (5)
H18A0.84240.95110.12580.111*
H18B0.99821.02320.22470.111*
H18C0.85581.10130.22780.111*
N10.36637 (16)0.89828 (13)1.05886 (12)0.0535 (3)
N20.1784 (2)0.6810 (2)0.55663 (18)0.0851 (5)
O10.37363 (18)1.04895 (13)1.10956 (14)0.0795 (4)
H1A0.44511.10351.07330.119*
O20.36281 (13)0.63175 (10)0.88863 (9)0.0495 (3)
U11U22U33U12U13U23
C10.0724 (10)0.0543 (9)0.0521 (8)0.0226 (7)0.0238 (7)0.0100 (7)
C20.0489 (7)0.0495 (7)0.0402 (6)0.0151 (6)0.0072 (5)0.0123 (5)
C30.0607 (8)0.0672 (10)0.0479 (7)0.0241 (7)0.0193 (6)0.0195 (7)
C40.0598 (9)0.0687 (10)0.0552 (8)0.0151 (7)0.0152 (7)0.0322 (8)
C50.0720 (10)0.0498 (8)0.0534 (8)0.0072 (7)0.0059 (7)0.0218 (7)
C60.0708 (9)0.0444 (8)0.0419 (7)0.0102 (7)0.0085 (6)0.0091 (6)
C70.0475 (6)0.0442 (7)0.0330 (6)0.0075 (5)0.0036 (5)0.0102 (5)
C80.0743 (9)0.0423 (7)0.0355 (6)0.0098 (6)0.0139 (6)0.0035 (5)
C90.0583 (8)0.0414 (7)0.0322 (6)0.0099 (6)0.0098 (5)0.0037 (5)
C100.0535 (8)0.0653 (10)0.0487 (8)0.0125 (7)0.0183 (6)0.0147 (7)
C110.0536 (7)0.0481 (7)0.0361 (6)0.0132 (6)0.0034 (5)0.0078 (5)
C120.0467 (7)0.0444 (7)0.0368 (6)0.0085 (5)0.0052 (5)0.0059 (5)
C130.0479 (7)0.0519 (8)0.0467 (7)0.0115 (6)0.0030 (5)0.0064 (6)
C140.0498 (7)0.0533 (8)0.0547 (8)0.0060 (6)0.0144 (6)0.0031 (7)
C150.0655 (9)0.0440 (7)0.0430 (7)0.0021 (6)0.0115 (6)0.0042 (6)
C160.0644 (9)0.0693 (11)0.0619 (9)0.0150 (8)0.0042 (7)0.0307 (8)
C170.0475 (7)0.0738 (11)0.0657 (9)0.0170 (7)0.0114 (7)0.0310 (8)
C180.0942 (13)0.0603 (10)0.0604 (10)0.0033 (9)0.0250 (9)0.0171 (8)
N10.0721 (8)0.0417 (6)0.0470 (6)0.0179 (6)0.0113 (6)0.0043 (5)
N20.0583 (9)0.1209 (15)0.0875 (11)0.0292 (9)0.0200 (8)0.0404 (11)
O10.1108 (11)0.0418 (6)0.0846 (9)0.0226 (6)0.0388 (8)0.0032 (6)
O20.0706 (6)0.0383 (5)0.0342 (4)0.0058 (4)0.0158 (4)0.0051 (4)
C1—N11.2541 (19)C10—N21.143 (2)
C1—C21.454 (2)C11—C121.4578 (18)
C1—H10.9300C11—H110.9300
C2—C31.3963 (19)C12—C131.3923 (19)
C2—C71.4063 (17)C12—C171.396 (2)
C3—C41.371 (2)C13—C141.376 (2)
C3—H30.9300C13—H130.9300
C4—C51.369 (2)C14—C151.382 (2)
C4—H40.9300C14—H140.9300
C5—C61.385 (2)C15—C161.382 (2)
C5—H50.9300C15—C181.504 (2)
C6—C71.3850 (19)C16—C171.376 (2)
C6—H60.9300C16—H160.9300
C7—O21.3670 (15)C17—H170.9300
C8—O21.4371 (15)C18—H18A0.9600
C8—C91.4985 (19)C18—H18B0.9600
C8—H8A0.9700C18—H18C0.9600
C8—H8B0.9700N1—O11.4013 (15)
C9—C111.3371 (19)O1—H1A0.8200
C9—C101.427 (2)
N1—C1—C2126.24 (13)C9—C11—C12132.12 (13)
N1—C1—H1116.9C9—C11—H11113.9
C2—C1—H1116.9C12—C11—H11113.9
C3—C2—C7117.57 (13)C13—C12—C17117.22 (13)
C3—C2—C1116.91 (12)C13—C12—C11117.23 (12)
C7—C2—C1125.51 (12)C17—C12—C11125.54 (12)
C4—C3—C2122.44 (14)C14—C13—C12121.36 (13)
C4—C3—H3118.8C14—C13—H13119.3
C2—C3—H3118.8C12—C13—H13119.3
C5—C4—C3119.14 (13)C13—C14—C15121.31 (13)
C5—C4—H4120.4C13—C14—H14119.3
C3—C4—H4120.4C15—C14—H14119.3
C4—C5—C6120.48 (14)C16—C15—C14117.50 (14)
C4—C5—H5119.8C16—C15—C18120.80 (16)
C6—C5—H5119.8C14—C15—C18121.69 (15)
C7—C6—C5120.58 (13)C17—C16—C15121.93 (15)
C7—C6—H6119.7C17—C16—H16119.0
C5—C6—H6119.7C15—C16—H16119.0
O2—C7—C6123.63 (12)C16—C17—C12120.67 (14)
O2—C7—C2116.70 (11)C16—C17—H17119.7
C6—C7—C2119.66 (12)C12—C17—H17119.7
O2—C8—C9108.34 (11)C15—C18—H18A109.5
O2—C8—H8A110.0C15—C18—H18B109.5
C9—C8—H8A110.0H18A—C18—H18B109.5
O2—C8—H8B110.0C15—C18—H18C109.5
C9—C8—H8B110.0H18A—C18—H18C109.5
H8A—C8—H8B108.4H18B—C18—H18C109.5
C11—C9—C10123.51 (12)C1—N1—O1111.61 (12)
C11—C9—C8121.38 (13)N1—O1—H1A109.5
C10—C9—C8115.02 (12)C7—O2—C8116.51 (10)
N2—C10—C9176.93 (17)
N1—C1—C2—C3165.75 (16)C8—C9—C11—C12177.74 (13)
N1—C1—C2—C7−13.2 (3)C9—C11—C12—C13−174.78 (14)
C7—C2—C3—C41.3 (2)C9—C11—C12—C175.4 (2)
C1—C2—C3—C4−177.81 (15)C17—C12—C13—C140.5 (2)
C2—C3—C4—C51.6 (2)C11—C12—C13—C14−179.33 (12)
C3—C4—C5—C6−2.0 (2)C12—C13—C14—C15−0.4 (2)
C4—C5—C6—C7−0.5 (2)C13—C14—C15—C160.3 (2)
C5—C6—C7—O2−175.94 (13)C13—C14—C15—C18179.17 (14)
C5—C6—C7—C23.5 (2)C14—C15—C16—C17−0.2 (2)
C3—C2—C7—O2175.69 (12)C18—C15—C16—C17−179.07 (16)
C1—C2—C7—O2−5.3 (2)C15—C16—C17—C120.2 (3)
C3—C2—C7—C6−3.8 (2)C13—C12—C17—C16−0.4 (2)
C1—C2—C7—C6175.23 (14)C11—C12—C17—C16179.43 (15)
O2—C8—C9—C11108.86 (14)C2—C1—N1—O1−176.87 (15)
O2—C8—C9—C10−74.60 (16)C6—C7—O2—C88.7 (2)
C11—C9—C10—N2156 (3)C2—C7—O2—C8−170.73 (12)
C8—C9—C10—N2−21 (3)C9—C8—O2—C7162.41 (12)
C10—C9—C11—C121.5 (2)
D—H···AD—HH···AD···AD—H···A
O1—H1A···N1i0.822.102.795 (2)143
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
O1—H1A⋯N1i0.822.102.795 (2)143

Symmetry code: (i) .

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