Literature DB >> 22719526

6-Chloro-2-phenyl-3-(2-phenyl-ethyn-yl)quinoxaline.

Xi-Lin Ouyang, Miao Ouyang, Shi-Wen Huang.   

Abstract

In the title compound, C(22)H(13)ClN(2), the quinoxaline ring system is close to planar [maximum deviation = 0.061 (2) Å]. The phenyl ring at the 2-position and the phenyl ring of the phenyl-ethynyl substituent make dihedral angles of 49.32 (7) and 11.99 (7) °, respectively, with the quinoxaline mean plane. The two phenyl rings are inclined to one another by 61.27 (9)°. In the crystal, mol-ecules are linked by C-H⋯π and π-π inter-actions [centroid-centroid distances = 3.6210 (12) and 3.8091 (12) Å].

Entities:  

Year:  2012        PMID: 22719526      PMCID: PMC3379328          DOI: 10.1107/S1600536812020776

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


Related literature

For the biological activity of quinoxaline derivatives, see: Rodrigo et al. (2002 ▶); Watkins et al. (2009 ▶); Sashidhara et al. (2009 ▶). For the crystal structures of quinoxaline derivatives, see: Hegedus et al. (2003 ▶); Naraso et al. (2006 ▶); Hassan et al. (2010 ▶); Ammermann et al. (2008 ▶); Daouda et al. (2011 ▶); Ramli et al. (2012 ▶).

Experimental

Crystal data

C22H13ClN2 M = 340.79 Triclinic, a = 8.8652 (13) Å b = 9.8591 (8) Å c = 10.9740 (17) Å α = 73.032 (15)° β = 81.036 (17)° γ = 64.374 (13)° V = 826.68 (19) Å3 Z = 2 Mo Kα radiation μ = 0.24 mm−1 T = 223 K 0.70 × 0.45 × 0.20 mm

Data collection

Rigaku Saturn diffractometer Absorption correction: multi-scan (REQAB; Jacobson, 1998 ▶) T min = 0.649, T max = 0.954 7504 measured reflections 3714 independent reflections 2855 reflections with I > 2σ(I) R int = 0.024

Refinement

R[F 2 > 2σ(F 2)] = 0.048 wR(F 2) = 0.128 S = 1.07 3714 reflections 227 parameters H-atom parameters constrained Δρmax = 0.27 e Å−3 Δρmin = −0.37 e Å−3 Data collection: CrystalClear (Rigaku, 2002 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: CrystalStructure (Rigaku, 2002 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812020776/su2414sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812020776/su2414Isup2.hkl Supplementary material file. DOI: 10.1107/S1600536812020776/su2414Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C22H13ClN2Z = 2
Mr = 340.79F(000) = 352
Triclinic, P1Dx = 1.369 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71075 Å
a = 8.8652 (13) ÅCell parameters from 3874 reflections
b = 9.8591 (8) Åθ = 3.2–27.5°
c = 10.9740 (17) ŵ = 0.24 mm1
α = 73.032 (15)°T = 223 K
β = 81.036 (17)°Block, yellow
γ = 64.374 (13)°0.70 × 0.45 × 0.20 mm
V = 826.68 (19) Å3
Rigaku Saturn diffractometer3714 independent reflections
Radiation source: fine-focus sealed tube2855 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.024
Detector resolution: 14.63 pixels mm-1θmax = 27.5°, θmin = 3.2°
ω scansh = −11→9
Absorption correction: multi-scan (REQAB; Jacobson, 1998)k = −12→12
Tmin = 0.649, Tmax = 0.954l = −14→10
7504 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)] = 0.048Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.128H-atom parameters constrained
S = 1.07w = 1/[σ2(Fo2) + (0.0712P)2] where P = (Fo2 + 2Fc2)/3
3714 reflections(Δ/σ)max < 0.001
227 parametersΔρmax = 0.27 e Å3
0 restraintsΔρmin = −0.37 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
Cl1−0.11370 (6)0.42900 (6)1.28280 (4)0.05093 (18)
N10.47258 (16)0.32096 (14)0.93213 (12)0.0299 (3)
N20.26481 (16)0.16607 (15)0.94729 (12)0.0314 (3)
C10.05364 (19)0.40009 (19)1.17229 (15)0.0344 (4)
C20.1450 (2)0.49110 (19)1.15630 (15)0.0349 (4)
H20.11210.56801.20120.042*
C30.28190 (19)0.46636 (18)1.07482 (15)0.0326 (4)
H30.34460.52551.06430.039*
C40.32946 (18)0.35241 (17)1.00641 (14)0.0286 (3)
C50.22960 (19)0.26891 (18)1.01856 (14)0.0298 (3)
C60.0918 (2)0.29202 (19)1.10582 (15)0.0338 (4)
H60.02760.23391.11780.041*
C70.51048 (19)0.21689 (17)0.86690 (14)0.0292 (3)
C80.40000 (18)0.14242 (17)0.87130 (14)0.0288 (3)
C90.67530 (19)0.17448 (17)0.79653 (15)0.0308 (3)
C100.8145 (2)0.14816 (19)0.85823 (17)0.0379 (4)
H100.80260.15690.94260.045*
C110.9711 (2)0.1090 (2)0.79661 (19)0.0456 (5)
H111.06490.08990.83960.055*
C120.9889 (2)0.0981 (2)0.6723 (2)0.0485 (5)
H121.09470.07140.63050.058*
C130.8506 (2)0.1266 (2)0.60934 (18)0.0459 (5)
H130.86280.12090.52410.055*
C140.6945 (2)0.16343 (19)0.67054 (16)0.0366 (4)
H140.60160.18100.62740.044*
C150.43695 (19)0.03324 (18)0.79721 (15)0.0322 (4)
C160.4708 (2)−0.06017 (18)0.73719 (15)0.0339 (4)
C170.5261 (2)−0.17824 (18)0.66936 (15)0.0324 (4)
C180.6633 (2)−0.1962 (2)0.58335 (16)0.0397 (4)
H180.7119−0.12410.56380.048*
C190.7275 (2)−0.3183 (2)0.52727 (17)0.0434 (4)
H190.8201−0.32990.46990.052*
C200.6561 (2)−0.4245 (2)0.55506 (17)0.0420 (4)
H200.7017−0.50930.51790.050*
C210.5186 (2)−0.4060 (2)0.63702 (17)0.0399 (4)
H210.4698−0.47770.65470.048*
C220.4516 (2)−0.28344 (19)0.69351 (16)0.0364 (4)
H220.3562−0.27050.74810.044*
U11U22U33U12U13U23
Cl10.0412 (3)0.0698 (3)0.0470 (3)−0.0267 (2)0.0169 (2)−0.0255 (2)
N10.0286 (6)0.0311 (7)0.0339 (7)−0.0147 (6)0.0008 (6)−0.0106 (6)
N20.0298 (7)0.0338 (7)0.0353 (7)−0.0166 (6)−0.0003 (6)−0.0103 (6)
C10.0287 (8)0.0418 (9)0.0311 (8)−0.0133 (7)0.0021 (7)−0.0102 (7)
C20.0334 (8)0.0378 (9)0.0358 (9)−0.0136 (7)0.0004 (7)−0.0151 (7)
C30.0332 (8)0.0334 (8)0.0358 (8)−0.0158 (7)−0.0027 (7)−0.0112 (7)
C40.0255 (7)0.0310 (8)0.0307 (8)−0.0131 (7)−0.0008 (6)−0.0075 (7)
C50.0287 (8)0.0306 (8)0.0309 (8)−0.0127 (7)−0.0032 (6)−0.0070 (7)
C60.0306 (8)0.0387 (9)0.0356 (8)−0.0181 (7)0.0014 (7)−0.0092 (7)
C70.0277 (8)0.0296 (8)0.0308 (8)−0.0129 (6)−0.0011 (6)−0.0062 (6)
C80.0272 (7)0.0281 (8)0.0325 (8)−0.0115 (6)−0.0018 (7)−0.0089 (7)
C90.0287 (8)0.0277 (8)0.0386 (8)−0.0145 (7)0.0044 (7)−0.0100 (7)
C100.0348 (9)0.0410 (9)0.0446 (9)−0.0194 (8)0.0025 (8)−0.0164 (8)
C110.0289 (8)0.0484 (11)0.0660 (12)−0.0191 (8)0.0024 (9)−0.0207 (9)
C120.0356 (9)0.0501 (11)0.0656 (12)−0.0230 (9)0.0192 (9)−0.0254 (10)
C130.0480 (10)0.0495 (11)0.0443 (10)−0.0244 (9)0.0154 (9)−0.0195 (9)
C140.0358 (9)0.0390 (9)0.0380 (9)−0.0177 (8)0.0043 (7)−0.0130 (7)
C150.0297 (8)0.0339 (8)0.0372 (9)−0.0161 (7)−0.0002 (7)−0.0105 (7)
C160.0333 (8)0.0340 (9)0.0372 (9)−0.0165 (7)−0.0018 (7)−0.0082 (7)
C170.0331 (8)0.0313 (8)0.0343 (8)−0.0132 (7)−0.0034 (7)−0.0096 (7)
C180.0445 (10)0.0375 (9)0.0411 (9)−0.0212 (8)0.0023 (8)−0.0107 (8)
C190.0442 (10)0.0480 (10)0.0386 (9)−0.0195 (9)0.0078 (8)−0.0157 (8)
C200.0511 (10)0.0369 (9)0.0404 (9)−0.0144 (8)−0.0025 (8)−0.0182 (8)
C210.0454 (10)0.0386 (9)0.0447 (10)−0.0219 (8)−0.0052 (8)−0.0140 (8)
C220.0357 (9)0.0385 (9)0.0406 (9)−0.0177 (8)−0.0005 (7)−0.0143 (8)
Cl1—C11.7401 (16)C11—C121.378 (3)
N1—C71.3168 (18)C11—H110.9400
N1—C41.3621 (18)C12—C131.383 (3)
N2—C81.3216 (19)C12—H120.9400
N2—C51.3602 (19)C13—C141.384 (2)
C1—C61.359 (2)C13—H130.9400
C1—C21.408 (2)C14—H140.9400
C2—C31.366 (2)C15—C161.194 (2)
C2—H20.9400C16—C171.431 (2)
C3—C41.410 (2)C17—C181.398 (2)
C3—H30.9400C17—C221.400 (2)
C4—C51.417 (2)C18—C191.373 (2)
C5—C61.408 (2)C18—H180.9400
C6—H60.9400C19—C201.384 (2)
C7—C81.445 (2)C19—H190.9400
C7—C91.488 (2)C20—C211.375 (2)
C8—C151.432 (2)C20—H200.9400
C9—C101.389 (2)C21—C221.378 (2)
C9—C141.397 (2)C21—H210.9400
C10—C111.389 (2)C22—H220.9400
C10—H100.9400
C7—N1—C4118.09 (11)C12—C11—C10119.90 (17)
C8—N2—C5117.11 (12)C12—C11—H11120.1
C6—C1—C2122.68 (14)C10—C11—H11120.1
C6—C1—Cl1119.67 (12)C11—C12—C13119.87 (16)
C2—C1—Cl1117.65 (12)C11—C12—H12120.1
C3—C2—C1119.21 (14)C13—C12—H12120.1
C3—C2—H2120.4C12—C13—C14120.66 (17)
C1—C2—H2120.4C12—C13—H13119.7
C2—C3—C4120.20 (13)C14—C13—H13119.7
C2—C3—H3119.9C13—C14—C9119.90 (16)
C4—C3—H3119.9C13—C14—H14120.0
N1—C4—C3119.84 (12)C9—C14—H14120.0
N1—C4—C5120.75 (13)C16—C15—C8178.49 (18)
C3—C4—C5119.39 (13)C15—C16—C17174.90 (17)
N2—C5—C6119.21 (12)C18—C17—C22118.90 (14)
N2—C5—C4121.04 (13)C18—C17—C16120.00 (13)
C6—C5—C4119.75 (13)C22—C17—C16120.97 (14)
C1—C6—C5118.58 (13)C19—C18—C17120.41 (14)
C1—C6—H6120.7C19—C18—H18119.8
C5—C6—H6120.7C17—C18—H18119.8
N1—C7—C8120.60 (12)C18—C19—C20120.15 (15)
N1—C7—C9116.64 (12)C18—C19—H19119.9
C8—C7—C9122.65 (12)C20—C19—H19119.9
N2—C8—C15116.82 (12)C21—C20—C19119.98 (14)
N2—C8—C7122.04 (12)C21—C20—H20120.0
C15—C8—C7121.08 (13)C19—C20—H20120.0
C10—C9—C14118.97 (14)C20—C21—C22120.73 (14)
C10—C9—C7118.40 (14)C20—C21—H21119.6
C14—C9—C7122.62 (15)C22—C21—H21119.6
C9—C10—C11120.69 (16)C21—C22—C17119.76 (15)
C9—C10—H10119.7C21—C22—H22120.1
C11—C10—H10119.7C17—C22—H22120.1
C6—C1—C2—C3−2.8 (3)N1—C7—C9—C1044.3 (2)
Cl1—C1—C2—C3176.92 (13)C8—C7—C9—C10−132.03 (16)
C1—C2—C3—C40.9 (3)N1—C7—C9—C14−134.37 (16)
C7—N1—C4—C3−178.15 (14)C8—C7—C9—C1449.3 (2)
C7—N1—C4—C53.5 (2)C14—C9—C10—C11−1.0 (2)
C2—C3—C4—N1−175.48 (15)C7—C9—C10—C11−179.69 (14)
C2—C3—C4—C52.9 (2)C9—C10—C11—C120.9 (3)
C8—N2—C5—C6−176.75 (14)C10—C11—C12—C130.1 (3)
C8—N2—C5—C43.1 (2)C11—C12—C13—C14−1.1 (3)
N1—C4—C5—N2−6.4 (2)C12—C13—C14—C91.0 (3)
C3—C4—C5—N2175.30 (14)C10—C9—C14—C130.0 (2)
N1—C4—C5—C6173.49 (14)C7—C9—C14—C13178.65 (14)
C3—C4—C5—C6−4.8 (2)N2—C8—C15—C16−108 (6)
C2—C1—C6—C50.8 (3)C7—C8—C15—C1670 (6)
Cl1—C1—C6—C5−178.91 (12)C8—C15—C16—C17−23 (7)
N2—C5—C6—C1−177.12 (15)C15—C16—C17—C18−56.4 (18)
C4—C5—C6—C13.0 (2)C15—C16—C17—C22119.5 (18)
C4—N1—C7—C82.0 (2)C22—C17—C18—C19−2.4 (3)
C4—N1—C7—C9−174.41 (13)C16—C17—C18—C19173.60 (16)
C5—N2—C8—C15179.58 (14)C17—C18—C19—C200.3 (3)
C5—N2—C8—C72.5 (2)C18—C19—C20—C211.3 (3)
N1—C7—C8—N2−5.3 (2)C19—C20—C21—C22−0.8 (3)
C9—C7—C8—N2170.89 (15)C20—C21—C22—C17−1.3 (3)
N1—C7—C8—C15177.74 (14)C18—C17—C22—C212.9 (3)
C9—C7—C8—C15−6.1 (2)C16—C17—C22—C21−173.08 (15)
D—H···AD—HH···AD···AD—H···A
C14—H14···Cg2i0.943.003.845 (2)151
Table 1

Hydrogen-bond geometry (Å, °)

Cg2 is the centroid of the C17–C22 ring.

D—H⋯AD—HH⋯ADAD—H⋯A
C14—H14⋯Cg2i0.943.003.845 (2)151

Symmetry code: (i) .

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