Literature DB >> 22065617

4,4'-Bipyridine-3-(thio-phen-3-yl)acrylic acid (1/2).

Palanisamy Rajakannu1, Firasat Hussain, Malaichamy Sathiyendiran.   

Abstract

In the title 1/2 adduct, C(10)H(8)N(2)·2C(7)H(6)O(2)S, the dihedral angle between the pyridine rings is 18.41 (11)°. In the thio-phene-acrylic acid mol-ecules, the dihedral angles between the respective thio-phene and acrylic acid units are 5.52 (17)° and 23.92 (9)°. In the crystal, the components are linked via O-H⋯N hydrogen-bonding inter-actions, forming units of two 3-thio-phene-acrylic acid mol-ecules and one 4,4'-bipyridine mol-ecule.

Entities:  

Year:  2011        PMID: 22065617      PMCID: PMC3201325          DOI: 10.1107/S1600536811035823

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


Related literature

For the synthesis and in vitro anti­bacterial activity of oxazolidines, see: Srivastava et al. (2008 ▶). For crystal engineering co-crystal and polymorph architectures, see: Friščić & MacGillivray (2009 ▶); Eccles et al. (2010 ▶). For the supra­molecular construction of mol­ecular ladders, see: Gao et al. (2004 ▶); MacGillivray et al. (2008 ▶); Friščić & MacGillivray (2005 ▶). For C—H⋯O hydrogen bonds in supra­molecular design, see: Desiraju (1996 ▶) and for C—H⋯π inter­actions in crystal engineering, see: Desiraju (2002 ▶).

Experimental

Crystal data

C10H8N2·2C7H6O2S M = 464.54 Triclinic, a = 7.3454 (5) Å b = 10.7319 (8) Å c = 15.0196 (11) Å α = 102.518 (6)° β = 103.648 (6)° γ = 94.892 (6)° V = 1111.54 (14) Å3 Z = 2 Cu Kα radiation μ = 2.46 mm−1 T = 293 K 0.37 × 0.15 × 0.10 mm

Data collection

Oxford Diffraction Xcalibur Sapphire3 diffractometer Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009 ▶) T min = 0.692, T max = 1.000 9038 measured reflections 4344 independent reflections 3498 reflections with I > 2σ(I) R int = 0.027

Refinement

R[F 2 > 2σ(F 2)] = 0.045 wR(F 2) = 0.132 S = 1.05 4344 reflections 291 parameters H-atom parameters constrained Δρmax = 0.24 e Å−3 Δρmin = −0.32 e Å−3 Data collection: CrysAlis PRO (Oxford Diffraction 2009) ▶; cell refinement: CrysAlis RED (Oxford Diffraction, 2009) ▶; data reduction: CrysAlis RED ▶; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶) and PLATON (Spek, 2009 ▶). Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811035823/si2368sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811035823/si2368Isup2.hkl Supplementary material file. DOI: 10.1107/S1600536811035823/si2368Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C10H8N2·2C7H6O2SZ = 2
Mr = 464.54F(000) = 484
Triclinic, P1Dx = 1.388 Mg m3
Hall symbol: -P 1Cu Kα radiation, λ = 1.54184 Å
a = 7.3454 (5) ÅCell parameters from 3251 reflections
b = 10.7319 (8) Åθ = 3.1–72.9°
c = 15.0196 (11) ŵ = 2.46 mm1
α = 102.518 (6)°T = 293 K
β = 103.648 (6)°Plate, white
γ = 94.892 (6)°0.37 × 0.15 × 0.10 mm
V = 1111.54 (14) Å3
Xcalibur, Sapphire3 diffractometer4344 independent reflections
Radiation source: fine-focus sealed tube3498 reflections with I > 2σ(I)
graphiteRint = 0.027
Detector resolution: 15.9853 pixels mm-1θmax = 72.1°, θmin = 3.1°
ω scansh = −8→9
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009)k = −13→12
Tmin = 0.692, Tmax = 1.000l = −18→13
9038 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.045Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.132H-atom parameters constrained
S = 1.05w = 1/[σ2(Fo2) + (0.0658P)2 + 0.2003P] where P = (Fo2 + 2Fc2)/3
4344 reflections(Δ/σ)max < 0.001
291 parametersΔρmax = 0.24 e Å3
0 restraintsΔρmin = −0.32 e Å3
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
C10.0548 (3)0.0002 (2)−0.17354 (15)0.0547 (5)
H10.0689−0.0528−0.13160.066*
C20.1988 (3)0.08388 (19)−0.17968 (13)0.0439 (4)
C30.1338 (3)0.1521 (2)−0.25031 (15)0.0542 (5)
H30.21200.2136−0.26450.065*
C4−0.0525 (3)0.1183 (2)−0.29432 (16)0.0611 (6)
H4−0.11720.1531−0.34200.073*
C50.3899 (3)0.09887 (19)−0.12014 (13)0.0447 (4)
H50.40970.0504−0.07530.054*
C60.5392 (3)0.1746 (2)−0.12320 (14)0.0479 (4)
H60.52620.2230−0.16810.058*
C70.7262 (3)0.18356 (19)−0.05652 (14)0.0467 (4)
C80.2956 (3)0.2219 (2)0.08555 (15)0.0559 (5)
H80.23250.13940.07620.067*
C90.4852 (3)0.2485 (2)0.13424 (15)0.0508 (5)
H90.54590.18500.15740.061*
C100.5840 (3)0.36980 (18)0.14838 (13)0.0429 (4)
C110.4821 (3)0.4604 (2)0.11311 (16)0.0571 (5)
H110.54120.54370.12130.069*
C120.2929 (3)0.4253 (2)0.06605 (17)0.0610 (6)
H120.22730.48720.04320.073*
C130.7889 (3)0.40367 (18)0.19703 (13)0.0430 (4)
C140.8822 (3)0.3308 (2)0.25474 (15)0.0537 (5)
H140.81630.25930.26460.064*
C151.0737 (3)0.3656 (2)0.29725 (16)0.0575 (5)
H151.13400.31490.33470.069*
C161.0874 (3)0.5381 (2)0.23340 (17)0.0595 (6)
H161.15650.61040.22630.071*
C170.8972 (3)0.5096 (2)0.18718 (16)0.0556 (5)
H170.84170.56140.14940.067*
C181.2549 (3)0.6734 (2)0.52895 (16)0.0584 (5)
H181.24720.58560.50260.070*
C191.1052 (3)0.7401 (2)0.51574 (13)0.0475 (4)
C201.1585 (3)0.8722 (2)0.56515 (17)0.0614 (6)
H201.07460.93240.56520.074*
C211.3461 (3)0.9011 (2)0.61250 (18)0.0660 (6)
H211.40530.98300.64770.079*
C220.9150 (3)0.6807 (2)0.46025 (13)0.0490 (5)
H220.89560.59180.43620.059*
C230.7683 (3)0.7418 (2)0.44109 (15)0.0548 (5)
H230.78570.83030.46680.066*
C240.5778 (3)0.6803 (2)0.38173 (15)0.0549 (5)
O10.7640 (2)0.11251 (16)−0.00462 (11)0.0637 (4)
O20.8489 (2)0.27837 (16)−0.05983 (12)0.0645 (4)
H20.95100.2794−0.02270.097*
O30.4670 (2)0.74129 (19)0.34314 (14)0.0809 (6)
O40.5423 (2)0.55602 (16)0.37539 (13)0.0650 (4)
H4A0.43250.52890.34500.098*
S1−0.15372 (8)0.00362 (7)−0.25123 (4)0.0671 (2)
S21.45740 (8)0.76787 (7)0.59882 (5)0.0697 (2)
N10.1992 (2)0.30804 (19)0.05151 (13)0.0568 (5)
N21.1767 (2)0.46765 (18)0.28753 (13)0.0552 (4)
U11U22U33U12U13U23
C10.0390 (10)0.0657 (13)0.0557 (12)0.0000 (9)0.0023 (8)0.0207 (10)
C20.0382 (10)0.0472 (10)0.0429 (9)0.0050 (8)0.0058 (7)0.0098 (8)
C30.0474 (11)0.0583 (12)0.0553 (12)0.0055 (9)0.0045 (9)0.0213 (10)
C40.0512 (12)0.0715 (14)0.0548 (12)0.0142 (11)−0.0025 (9)0.0193 (11)
C50.0378 (10)0.0497 (10)0.0448 (10)0.0062 (8)0.0048 (8)0.0147 (8)
C60.0390 (10)0.0518 (11)0.0511 (11)0.0052 (8)0.0018 (8)0.0200 (9)
C70.0358 (9)0.0512 (11)0.0511 (10)0.0048 (8)0.0049 (8)0.0163 (9)
C80.0430 (11)0.0567 (12)0.0597 (12)−0.0069 (9)0.0073 (9)0.0086 (10)
C90.0421 (10)0.0491 (11)0.0569 (11)0.0014 (8)0.0065 (9)0.0130 (9)
C100.0351 (9)0.0489 (10)0.0400 (9)0.0028 (8)0.0049 (7)0.0074 (8)
C110.0437 (11)0.0502 (11)0.0701 (13)0.0020 (9)−0.0004 (10)0.0178 (10)
C120.0426 (11)0.0653 (14)0.0701 (14)0.0101 (10)0.0000 (10)0.0208 (11)
C130.0338 (9)0.0472 (10)0.0422 (9)0.0030 (7)0.0039 (7)0.0065 (8)
C140.0396 (10)0.0610 (12)0.0590 (12)0.0026 (9)0.0047 (9)0.0224 (10)
C150.0415 (11)0.0663 (14)0.0609 (13)0.0078 (10)0.0005 (9)0.0220 (11)
C160.0406 (11)0.0591 (13)0.0695 (14)−0.0079 (9)0.0010 (10)0.0165 (11)
C170.0422 (11)0.0544 (12)0.0629 (13)−0.0014 (9)−0.0013 (9)0.0186 (10)
C180.0406 (11)0.0641 (13)0.0612 (13)0.0030 (9)0.0058 (9)0.0059 (10)
C190.0372 (10)0.0588 (12)0.0421 (9)0.0004 (8)0.0040 (7)0.0121 (9)
C200.0439 (12)0.0593 (13)0.0700 (14)0.0058 (10)−0.0008 (10)0.0101 (11)
C210.0461 (12)0.0624 (14)0.0716 (15)−0.0046 (10)−0.0014 (10)0.0021 (11)
C220.0390 (10)0.0576 (12)0.0453 (10)−0.0037 (9)0.0036 (8)0.0140 (9)
C230.0406 (11)0.0612 (13)0.0559 (12)−0.0025 (9)0.0000 (9)0.0182 (10)
C240.0371 (10)0.0682 (14)0.0571 (12)−0.0024 (9)0.0027 (9)0.0248 (10)
O10.0460 (8)0.0779 (11)0.0686 (10)0.0059 (7)−0.0012 (7)0.0399 (9)
O20.0389 (8)0.0669 (10)0.0806 (11)−0.0046 (7)−0.0068 (7)0.0324 (8)
O30.0477 (9)0.0871 (12)0.0997 (13)−0.0059 (9)−0.0160 (9)0.0502 (11)
O40.0359 (8)0.0668 (10)0.0792 (11)−0.0008 (7)−0.0064 (7)0.0169 (8)
S10.0359 (3)0.0853 (4)0.0685 (4)−0.0024 (3)−0.0014 (2)0.0156 (3)
S20.0343 (3)0.0880 (5)0.0729 (4)0.0059 (3)−0.0003 (2)0.0073 (3)
N10.0350 (9)0.0705 (12)0.0563 (10)−0.0002 (8)0.0024 (7)0.0110 (9)
N20.0359 (9)0.0640 (11)0.0558 (10)0.0012 (8)0.0006 (7)0.0089 (8)
C1—C21.361 (3)C13—C141.392 (3)
C1—S11.701 (2)C14—C151.382 (3)
C1—H10.9300C14—H140.9300
C2—C31.430 (3)C15—N21.332 (3)
C2—C51.451 (3)C15—H150.9300
C3—C41.351 (3)C16—N21.328 (3)
C3—H30.9300C16—C171.380 (3)
C4—S11.703 (3)C16—H160.9300
C4—H40.9300C17—H170.9300
C5—C61.324 (3)C18—C191.362 (3)
C5—H50.9300C18—S21.699 (2)
C6—C71.478 (3)C18—H180.9300
C6—H60.9300C19—C201.423 (3)
C7—O11.207 (2)C19—C221.456 (3)
C7—O21.318 (2)C20—C211.367 (3)
C8—N11.328 (3)C20—H200.9300
C8—C91.385 (3)C21—S21.705 (3)
C8—H80.9300C21—H210.9300
C9—C101.383 (3)C22—C231.315 (3)
C9—H90.9300C22—H220.9300
C10—C111.395 (3)C23—C241.479 (3)
C10—C131.485 (2)C23—H230.9300
C11—C121.380 (3)C24—O31.208 (3)
C11—H110.9300C24—O41.315 (3)
C12—N11.330 (3)O2—H20.8200
C12—H120.9300O4—H4A0.8200
C13—C171.386 (3)
C2—C1—S1112.31 (16)C15—C14—C13119.4 (2)
C2—C1—H1123.8C15—C14—H14120.3
S1—C1—H1123.8C13—C14—H14120.3
C1—C2—C3110.97 (18)N2—C15—C14123.6 (2)
C1—C2—C5122.51 (18)N2—C15—H15118.2
C3—C2—C5126.52 (18)C14—C15—H15118.2
C4—C3—C2113.3 (2)N2—C16—C17123.3 (2)
C4—C3—H3123.4N2—C16—H16118.3
C2—C3—H3123.4C17—C16—H16118.3
C3—C4—S1111.33 (17)C16—C17—C13120.1 (2)
C3—C4—H4124.3C16—C17—H17120.0
S1—C4—H4124.3C13—C17—H17120.0
C6—C5—C2126.60 (18)C19—C18—S2112.62 (18)
C6—C5—H5116.7C19—C18—H18123.7
C2—C5—H5116.7S2—C18—H18123.7
C5—C6—C7121.21 (18)C18—C19—C20111.27 (19)
C5—C6—H6119.4C18—C19—C22123.4 (2)
C7—C6—H6119.4C20—C19—C22125.35 (19)
O1—C7—O2123.23 (18)C21—C20—C19112.8 (2)
O1—C7—C6124.35 (18)C21—C20—H20123.6
O2—C7—C6112.42 (17)C19—C20—H20123.6
N1—C8—C9123.5 (2)C20—C21—S2111.29 (18)
N1—C8—H8118.3C20—C21—H21124.4
C9—C8—H8118.3S2—C21—H21124.4
C10—C9—C8119.7 (2)C23—C22—C19125.7 (2)
C10—C9—H9120.1C23—C22—H22117.1
C8—C9—H9120.1C19—C22—H22117.1
C9—C10—C11116.67 (18)C22—C23—C24124.9 (2)
C9—C10—C13122.63 (18)C22—C23—H23117.6
C11—C10—C13120.69 (18)C24—C23—H23117.6
C12—C11—C10119.5 (2)O3—C24—O4124.2 (2)
C12—C11—H11120.3O3—C24—C23121.6 (2)
C10—C11—H11120.2O4—C24—C23114.25 (18)
N1—C12—C11123.6 (2)C7—O2—H2109.5
N1—C12—H12118.2C24—O4—H4A109.5
C11—C12—H12118.2C1—S1—C492.12 (11)
C17—C13—C14116.54 (18)C18—S2—C2191.96 (11)
C17—C13—C10121.64 (18)C8—N1—C12117.01 (18)
C14—C13—C10121.82 (18)C16—N2—C15117.01 (18)
D—H···AD—HH···AD···AD—H···A
O2—H2···N1i0.821.862.668 (2)168.
O4—H4A···N2ii0.821.872.684 (2)174.
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
O2—H2⋯N1i0.821.862.668 (2)168
O4—H4A⋯N2ii0.821.872.684 (2)174

Symmetry codes: (i) ; (ii) .

  8 in total

1.  Supramolecular construction of molecular ladders in the solid state.

Authors:  Xiuchun Gao; Tomislav Friscić; Leonard R MacGillivray
Journal:  Angew Chem Int Ed Engl       Date:  2004-01       Impact factor: 15.336

2.  Synthesis and in vitro antibacterial activities of novel oxazolidinones.

Authors:  Brijesh Kumar Srivastava; Mukul R Jain; Manish Solanki; Rina Soni; Darshan Valani; Sunil Gupta; Bhupendra Mishra; Vijay Takale; Prashant Kapadnis; Harilal Patel; Purvi Pandya; Jayendra Z Patel; Pankaj R Patel
Journal:  Eur J Med Chem       Date:  2007-05-27       Impact factor: 6.514

3.  A short history of SHELX.

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

4.  Engineering cocrystal and polymorph architecture via pseudoseeding.

Authors:  Tomislav Friscić; Leonard R Macgillivray
Journal:  Chem Commun (Camb)       Date:  2009-01-14       Impact factor: 6.222

5.  The C-h···o hydrogen bond:  structural implications and supramolecular design.

Authors:  G R Desiraju
Journal:  Acc Chem Res       Date:  1996-09       Impact factor: 22.384

6.  Supramolecular control of reactivity in the solid state: from templates to ladderanes to metal-organic frameworks.

Authors:  Leonard R MacGillivray; Giannis S Papaefstathiou; Tomislav Friscić; Tamara D Hamilton; Dejan-Kresimir Bucar; Qianli Chu; Dushyant B Varshney; Ivan G Georgiev
Journal:  Acc Chem Res       Date:  2008-02-19       Impact factor: 22.384

Review 7.  Hydrogen bridges in crystal engineering: interactions without borders.

Authors:  Gautam R Desiraju
Journal:  Acc Chem Res       Date:  2002-07       Impact factor: 22.384

8.  Structure validation in chemical crystallography.

Authors:  Anthony L Spek
Journal:  Acta Crystallogr D Biol Crystallogr       Date:  2009-01-20
  8 in total

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