Literature DB >> 24427027

(E)-3-(4-Bromo-5-methyl-thio-phen-2-yl)acrylo-nitrile.

Gamal A El-Hiti1, Keith Smith2, Asim A Balakit3, Ali Masmali1, Benson M Kariuki2.   

Abstract

In the title structure, C8H6BrNS, the molecules are planar with the exception of the methyl H atoms. In the crystal, molecules are linked by intermolecular C-H⋯N interactions to form ribbons parallel to the b axis. Groups of ribbons are arranged in a herringbone pattern to form a layered structure parallel to the ab plane.

Entities:  

Year:  2013        PMID: 24427027      PMCID: PMC3884493          DOI: 10.1107/S1600536813019752

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


Related literature

For related structures and their applications, see: Perner et al. (2003 ▶); Kose (2004 ▶); Chandra et al. (2006 ▶); Zhao et al. (2009 ▶); Pu et al. (2010 ▶); Dinçalp et al. (2011 ▶).

Experimental

Crystal data

C8H6BrNS M = 228.11 Orthorhombic, a = 6.1347 (5) Å b = 7.1124 (3) Å c = 19.8245 (13) Å V = 864.99 (10) Å3 Z = 4 Mo Kα radiation μ = 4.92 mm−1 T = 150 K 0.40 × 0.30 × 0.10 mm

Data collection

Nonius KappaCCD diffractometer Absorption correction: empirical (using intensity measurements) (DENZO/SCALEPACK; Otwinowski & Minor, 1997 ▶) T min = 0.243, T max = 0.639 3294 measured reflections 1910 independent reflections 1769 reflections with I > 2σ(I) R int = 0.060

Refinement

R[F 2 > 2σ(F 2)] = 0.048 wR(F 2) = 0.120 S = 1.05 1910 reflections 102 parameters H-atom parameters constrained Δρmax = 0.74 e Å−3 Δρmin = −1.12 e Å−3 Absolute structure: Flack (1983 ▶), 699 Friedel pairs Absolute structure parameter: 0.03 (2) Data collection: COLLECT (Nonius, 2000 ▶); cell refinement: DENZO and SCALEPACK (Otwinowski & Minor, 1997 ▶); data reduction: DENZO and SCALEPACK; 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, 2012 ▶); software used to prepare material for publication: WinGX (Farrugia, 2012 ▶) and CHEMDRAW Ultra (Cambridge Soft, 2001 ▶). Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536813019752/hg5330sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813019752/hg5330Isup2.hkl Click here for additional data file. Supplementary material file. DOI: 10.1107/S1600536813019752/hg5330Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C8H6BrNSF(000) = 448
Mr = 228.11Dx = 1.752 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 1769 reflections
a = 6.1347 (5) Åθ = 3.0–28.4°
b = 7.1124 (3) ŵ = 4.92 mm1
c = 19.8245 (13) ÅT = 150 K
V = 864.99 (10) Å3Plate, yellow
Z = 40.40 × 0.30 × 0.10 mm
Nonius KappaCCD diffractometer1910 independent reflections
Radiation source: fine-focus sealed tube1769 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.060
CCD scansθmax = 27.4°, θmin = 3.0°
Absorption correction: empirical (using intensity measurements) (DENZO/SCALEPACK; Otwinowski & Minor, 1997)h = −4→7
Tmin = 0.243, Tmax = 0.639k = −9→7
3294 measured reflectionsl = −25→20
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.048w = 1/[σ2(Fo2) + (0.0412P)2 + 2.3854P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.120(Δ/σ)max < 0.001
S = 1.05Δρmax = 0.74 e Å3
1910 reflectionsΔρmin = −1.12 e Å3
102 parametersExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.030 (3)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983), 699 Friedel pairs
Secondary atom site location: difference Fourier mapAbsolute structure parameter: 0.03 (2)
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
C1−0.4336 (10)−0.1420 (8)0.7590 (3)0.0265 (11)
C2−0.2429 (10)−0.1841 (9)0.7200 (3)0.0264 (12)
H2−0.1959−0.30790.71590.032*
C3−0.1322 (9)−0.0462 (8)0.6895 (3)0.0258 (12)
H3−0.18240.07640.69460.031*
C40.0617 (10)−0.0763 (7)0.6489 (3)0.0235 (11)
C50.1860 (10)0.0569 (8)0.6186 (3)0.0222 (11)
H50.15530.18490.62030.027*
C60.3668 (10)−0.0199 (8)0.5843 (3)0.0241 (12)
C70.3838 (8)−0.2120 (7)0.5887 (2)0.0191 (11)
C80.5528 (11)−0.3400 (7)0.5583 (3)0.0264 (12)
H8A0.5059−0.37910.51420.040*
H8B0.5713−0.44850.58650.040*
H8C0.6888−0.27410.55460.040*
N1−0.5883 (9)−0.1203 (8)0.7912 (3)0.0331 (11)
S10.1701 (3)−0.2987 (2)0.63524 (7)0.0246 (3)
Br10.57000 (10)0.12692 (8)0.53635 (3)0.0319 (2)
U11U22U33U12U13U23
C10.022 (3)0.028 (3)0.030 (3)−0.001 (3)0.000 (2)0.000 (2)
C20.024 (3)0.027 (3)0.029 (3)0.003 (2)0.001 (2)−0.005 (2)
C30.023 (3)0.025 (3)0.029 (3)0.006 (2)−0.002 (2)−0.003 (2)
C40.016 (2)0.025 (3)0.030 (3)0.003 (2)−0.002 (2)−0.001 (2)
C50.023 (3)0.018 (2)0.026 (3)0.004 (2)−0.006 (2)−0.006 (2)
C60.025 (3)0.024 (3)0.023 (3)−0.001 (2)−0.001 (2)−0.004 (2)
C70.021 (3)0.019 (2)0.017 (2)0.002 (2)−0.0057 (19)0.0017 (19)
C80.032 (3)0.019 (3)0.028 (3)0.002 (2)0.002 (2)0.003 (2)
N10.031 (3)0.031 (2)0.038 (3)−0.008 (3)0.002 (2)−0.004 (2)
S10.0240 (7)0.0207 (6)0.0291 (7)0.0007 (6)0.0021 (6)−0.0004 (5)
Br10.0332 (3)0.0259 (3)0.0368 (3)−0.0021 (3)0.0065 (3)0.0040 (2)
C1—N11.154 (8)C5—H50.9300
C1—C21.434 (8)C6—C71.373 (7)
C2—C31.338 (8)C6—Br11.884 (6)
C2—H20.9300C7—C81.506 (8)
C3—C41.452 (8)C7—S11.717 (5)
C3—H30.9300C8—H8A0.9600
C4—C51.356 (8)C8—H8B0.9600
C4—S11.737 (5)C8—H8C0.9600
C5—C61.412 (8)
N1—C1—C2175.6 (7)C7—C6—C5114.5 (5)
C3—C2—C1120.3 (5)C7—C6—Br1122.3 (4)
C3—C2—H2119.8C5—C6—Br1123.3 (4)
C1—C2—H2119.8C6—C7—C8128.9 (5)
C2—C3—C4123.9 (5)C6—C7—S1109.5 (4)
C2—C3—H3118.0C8—C7—S1121.6 (4)
C4—C3—H3118.0C7—C8—H8A109.5
C5—C4—C3127.1 (5)C7—C8—H8B109.5
C5—C4—S1110.6 (4)H8A—C8—H8B109.5
C3—C4—S1122.3 (4)C7—C8—H8C109.5
C4—C5—C6112.6 (5)H8A—C8—H8C109.5
C4—C5—H5123.7H8B—C8—H8C109.5
C6—C5—H5123.7C7—S1—C492.8 (3)
D—H···AD—HH···AD···AD—H···A
C3—H3···N1i0.932.593.501 (8)166
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
C3—H3⋯N1i 0.932.593.501 (8)166

Symmetry code: (i) .

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