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In the title compound, C20H14N2, the presence of adjacent phenyl rings causes an out-of-plane twist in the quinoxaline system of approximately 12°.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806017776/fl2028sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806017776/fl2028Isup2.hkl
Contains datablock I

CCDC reference: 610767

Key indicators

  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.044
  • wR factor = 0.112
  • Data-to-parameter ratio = 17.1

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT432_ALERT_2_C Short Inter X...Y Contact C6 .. C12 .. 3.19 Ang.
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 1 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: CrysAlis CCD (Oxford Diffraction, 2003); cell refinement: CrysAlis RED (Oxford Diffraction, 2003); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: PARST95 (Nardelli, 1995) and PLATON (Spek, 2003).

2,3-diphenylquinoxaline top
Crystal data top
C20H14N2F(000) = 592
Mr = 282.33Dx = 1.268 Mg m3
Monoclinic, P21/nMelting point: 398 K
Hall symbol: -P 2ynMo Kα radiation, λ = 0.71073 Å
a = 6.0306 (2) ÅCell parameters from 25 reflections
b = 10.9269 (5) Åθ = 6.5–13.8°
c = 22.5309 (8) ŵ = 0.08 mm1
β = 95.005 (3)°T = 100 K
V = 1479.03 (10) Å3Prism, light yellow
Z = 40.5 × 0.45 × 0.3 mm
Data collection top
Oxford Diffraction CrysAlisCCD
diffractometer
3413 independent reflections
Radiation source: fine-focus sealed tube2773 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.027
ω/2θ scansθmax = 27.6°, θmin = 2.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
h = 77
Tmin = 0.93, Tmax = 0.98k = 1414
16180 measured reflectionsl = 2929
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.044H-atom parameters constrained
wR(F2) = 0.112 w = 1/[σ2(Fo2) + (0.0404P)2 + 0.715P]
where P = (Fo2 + 2Fc2)/3
S = 1.13(Δ/σ)max < 0.001
3413 reflectionsΔρmax = 0.30 e Å3
200 parametersΔρmin = 0.17 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0092 (16)
Special details top

Experimental. To a glass vial, Benzil (0.50 mg, 2,38 mmol), 1,2-diamino benzene (0.26 mg, 2.40 mmol), molecular sieves (1 g) and manganese oxide (0.10 mg) as a catalyst was heated under microwave irradiation using domestic microwave M197DL. After one min the vial was cooled to room temperature. The solution was filtered and solid obtained was recrystallized from ethanol to give 2,3-diphenyl quinoxaline (0.570 mg, 76.49%).

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
N10.7349 (2)0.79330 (11)0.18973 (5)0.0191 (3)
C20.5488 (2)0.83953 (13)0.16342 (6)0.0180 (3)
C30.4405 (2)0.94333 (13)0.18815 (6)0.0175 (3)
N40.5096 (2)0.98709 (11)0.24124 (5)0.0184 (3)
C50.6961 (2)0.93603 (13)0.27012 (6)0.0185 (3)
C60.8142 (2)0.84227 (13)0.24330 (6)0.0184 (3)
C71.0153 (2)0.79688 (14)0.27257 (7)0.0206 (3)
H71.09570.73400.25470.025*
C81.0928 (3)0.84432 (14)0.32675 (7)0.0225 (3)
H81.22790.81440.34630.027*
C90.9731 (3)0.93757 (14)0.35382 (7)0.0229 (3)
H91.02870.96920.39150.028*
C100.7784 (3)0.98275 (14)0.32639 (7)0.0217 (3)
H100.69921.04500.34500.026*
C110.2511 (2)1.00973 (13)0.15553 (6)0.0180 (3)
C120.0850 (2)1.05899 (13)0.18797 (7)0.0195 (3)
H120.09421.04930.23000.023*
C130.0932 (3)1.12187 (14)0.15923 (7)0.0235 (3)
H130.20731.15310.18150.028*
C140.1052 (3)1.13922 (14)0.09807 (8)0.0269 (4)
H140.22851.18120.07840.032*
C150.0633 (3)1.09510 (15)0.06561 (7)0.0266 (4)
H150.05761.10940.02390.032*
C160.2404 (3)1.03005 (14)0.09405 (7)0.0230 (3)
H160.35450.99930.07160.028*
C170.4574 (2)0.77395 (13)0.10864 (6)0.0191 (3)
C180.2414 (3)0.72696 (14)0.10354 (7)0.0223 (3)
H180.14510.74210.13390.027*
C190.1673 (3)0.65773 (14)0.05379 (7)0.0245 (3)
H190.02110.62450.05070.029*
C200.3059 (3)0.63694 (14)0.00873 (7)0.0257 (4)
H200.25460.58980.02510.031*
C210.5196 (3)0.68520 (15)0.01330 (7)0.0259 (4)
H210.61380.67200.01770.031*
C220.5958 (3)0.75273 (14)0.06318 (7)0.0229 (3)
H220.74280.78470.06640.027*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0192 (6)0.0170 (6)0.0211 (6)0.0017 (5)0.0013 (5)0.0008 (5)
C20.0181 (7)0.0175 (7)0.0187 (7)0.0014 (6)0.0031 (6)0.0007 (5)
C30.0186 (7)0.0166 (7)0.0177 (7)0.0011 (6)0.0033 (6)0.0012 (5)
N40.0194 (6)0.0167 (6)0.0192 (6)0.0005 (5)0.0023 (5)0.0011 (5)
C50.0209 (7)0.0158 (7)0.0189 (7)0.0021 (6)0.0018 (6)0.0023 (5)
C60.0205 (7)0.0153 (7)0.0195 (7)0.0028 (6)0.0025 (6)0.0016 (5)
C70.0210 (7)0.0171 (7)0.0236 (8)0.0002 (6)0.0018 (6)0.0018 (6)
C80.0221 (8)0.0206 (7)0.0238 (8)0.0014 (6)0.0033 (6)0.0064 (6)
C90.0279 (8)0.0210 (7)0.0191 (7)0.0046 (6)0.0025 (6)0.0006 (6)
C100.0263 (8)0.0189 (7)0.0200 (7)0.0012 (6)0.0024 (6)0.0003 (6)
C110.0178 (7)0.0144 (7)0.0215 (7)0.0016 (5)0.0004 (6)0.0004 (5)
C120.0207 (7)0.0161 (7)0.0219 (7)0.0030 (6)0.0022 (6)0.0000 (6)
C130.0191 (7)0.0191 (7)0.0328 (9)0.0004 (6)0.0042 (6)0.0012 (6)
C140.0240 (8)0.0210 (8)0.0344 (9)0.0034 (6)0.0051 (7)0.0031 (7)
C150.0339 (9)0.0239 (8)0.0210 (8)0.0026 (7)0.0026 (7)0.0023 (6)
C160.0257 (8)0.0209 (7)0.0226 (8)0.0026 (6)0.0028 (6)0.0014 (6)
C170.0219 (7)0.0162 (7)0.0186 (7)0.0036 (6)0.0014 (6)0.0002 (6)
C180.0217 (8)0.0218 (8)0.0233 (8)0.0027 (6)0.0011 (6)0.0017 (6)
C190.0219 (8)0.0212 (7)0.0293 (8)0.0017 (6)0.0039 (6)0.0026 (6)
C200.0318 (9)0.0217 (8)0.0222 (8)0.0045 (7)0.0058 (6)0.0043 (6)
C210.0301 (8)0.0274 (8)0.0202 (8)0.0056 (7)0.0025 (6)0.0031 (6)
C220.0221 (8)0.0228 (8)0.0236 (8)0.0024 (6)0.0013 (6)0.0008 (6)
Geometric parameters (Å, º) top
N1—C21.3228 (18)C12—H120.9500
N1—C61.3678 (19)C13—C141.386 (2)
C2—C31.445 (2)C13—H130.9500
C2—C171.491 (2)C14—C151.389 (2)
C3—N41.3213 (19)C14—H140.9500
C3—C111.492 (2)C15—C161.392 (2)
N4—C51.3683 (19)C15—H150.9500
C5—C61.413 (2)C16—H160.9500
C5—C101.416 (2)C17—C181.396 (2)
C6—C71.419 (2)C17—C221.396 (2)
C7—C81.370 (2)C18—C191.393 (2)
C7—H70.9500C18—H180.9500
C8—C91.417 (2)C19—C201.389 (2)
C8—H80.9500C19—H190.9500
C9—C101.370 (2)C20—C211.388 (2)
C9—H90.9500C20—H200.9500
C10—H100.9500C21—C221.389 (2)
C11—C121.399 (2)C21—H210.9500
C11—C161.399 (2)C22—H220.9500
C12—C131.387 (2)
C2—N1—C6117.61 (13)C11—C12—H12119.7
N1—C2—C3121.43 (13)C14—C13—C12120.19 (15)
N1—C2—C17115.18 (13)C14—C13—H13119.9
C3—C2—C17123.34 (13)C12—C13—H13119.9
N4—C3—C2121.04 (13)C13—C14—C15119.91 (15)
N4—C3—C11115.94 (13)C13—C14—H14120.0
C2—C3—C11122.99 (12)C15—C14—H14120.0
C3—N4—C5117.65 (13)C14—C15—C16120.15 (15)
N4—C5—C6121.09 (13)C14—C15—H15119.9
N4—C5—C10119.22 (13)C16—C15—H15119.9
C6—C5—C10119.60 (13)C15—C16—C11120.26 (15)
N1—C6—C5120.71 (13)C15—C16—H16119.9
N1—C6—C7119.49 (13)C11—C16—H16119.9
C5—C6—C7119.80 (13)C18—C17—C22119.46 (14)
C8—C7—C6119.55 (14)C18—C17—C2121.35 (13)
C8—C7—H7120.2C22—C17—C2119.07 (13)
C6—C7—H7120.2C19—C18—C17119.85 (14)
C7—C8—C9120.58 (14)C19—C18—H18120.1
C7—C8—H8119.7C17—C18—H18120.1
C9—C8—H8119.7C20—C19—C18120.37 (15)
C10—C9—C8120.89 (14)C20—C19—H19119.8
C10—C9—H9119.6C18—C19—H19119.8
C8—C9—H9119.6C21—C20—C19119.86 (14)
C9—C10—C5119.58 (14)C21—C20—H20120.1
C9—C10—H10120.2C19—C20—H20120.1
C5—C10—H10120.2C20—C21—C22120.09 (15)
C12—C11—C16118.90 (13)C20—C21—H21120.0
C12—C11—C3118.84 (13)C22—C21—H21120.0
C16—C11—C3122.16 (13)C21—C22—C17120.36 (15)
C13—C12—C11120.51 (14)C21—C22—H22119.8
C13—C12—H12119.7C17—C22—H22119.8
C6—N1—C2—C34.1 (2)C2—C3—C11—C12146.09 (14)
C6—N1—C2—C17173.67 (12)N4—C3—C11—C16140.78 (14)
N1—C2—C3—N47.6 (2)C2—C3—C11—C1637.4 (2)
C17—C2—C3—N4169.90 (13)C16—C11—C12—C133.1 (2)
N1—C2—C3—C11170.49 (13)C3—C11—C12—C13179.68 (13)
C17—C2—C3—C1112.0 (2)C11—C12—C13—C141.7 (2)
C2—C3—N4—C54.3 (2)C12—C13—C14—C151.0 (2)
C11—C3—N4—C5173.93 (12)C13—C14—C15—C162.1 (2)
C3—N4—C5—C61.8 (2)C14—C15—C16—C110.6 (2)
C3—N4—C5—C10178.34 (13)C12—C11—C16—C152.0 (2)
C2—N1—C6—C52.1 (2)C3—C11—C16—C15178.41 (14)
C2—N1—C6—C7178.91 (13)N1—C2—C17—C18123.30 (15)
N4—C5—C6—N15.3 (2)C3—C2—C17—C1854.4 (2)
C10—C5—C6—N1178.20 (13)N1—C2—C17—C2252.69 (19)
N4—C5—C6—C7175.72 (13)C3—C2—C17—C22129.63 (15)
C10—C5—C6—C70.8 (2)C22—C17—C18—C191.1 (2)
N1—C6—C7—C8178.82 (13)C2—C17—C18—C19174.86 (13)
C5—C6—C7—C80.2 (2)C17—C18—C19—C201.1 (2)
C6—C7—C8—C90.4 (2)C18—C19—C20—C210.1 (2)
C7—C8—C9—C100.3 (2)C19—C20—C21—C220.9 (2)
C8—C9—C10—C50.3 (2)C20—C21—C22—C170.9 (2)
N4—C5—C10—C9175.75 (14)C18—C17—C22—C210.1 (2)
C6—C5—C10—C90.8 (2)C2—C17—C22—C21175.93 (14)
N4—C3—C11—C1235.69 (19)
 

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