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In the structure of the title compound, C15H13N, the dihedral angle between the five- and the six-membered rings of the indole system is 1.19 (5)° and the phenyl ring makes a dihedral angle of 46.09 (5)° with the indole ring system.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807012962/nc2030sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807012962/nc2030Isup2.hkl
Contains datablock I

CCDC reference: 643063

Key indicators

  • Single-crystal X-ray study
  • T = 294 K
  • Mean [sigma](C-C)= 0.002 Å
  • R factor = 0.060
  • wR factor = 0.157
  • Data-to-parameter ratio = 18.3

checkCIF/PLATON results

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No errors found in this datablock

Computing details top

Data collection: CrystalClear (Rigaku/MSC, 2005); cell refinement: CrystalClear; data reduction: CrystalClear; 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: WinGX (Farrugia, 1999).

1-Methyl-2-phenyl-1H-indole top
Crystal data top
C15H13NF(000) = 880
Mr = 207.26Dx = 1.234 Mg m3
Orthorhombic, PbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 9521 reflections
a = 8.1957 (1) Åθ = 2.4–30.5°
b = 15.8652 (3) ŵ = 0.07 mm1
c = 17.1653 (3) ÅT = 294 K
V = 2231.94 (6) Å3Prism, colorless
Z = 80.35 × 0.20 × 0.15 mm
Data collection top
Rigaku R-AXIS RAPID-S
diffractometer
2146 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.080
Graphite monochromatorθmax = 30.5°, θmin = 2.4°
ω scansh = 1111
60316 measured reflectionsk = 2220
3414 independent reflectionsl = 2424
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)] = 0.061H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.157 w = 1/[σ2(Fo2) + (0.0597P)2 + 0.2662P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
3414 reflectionsΔρmax = 0.14 e Å3
187 parametersΔρmin = 0.16 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0054 (11)
Special details top

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
N10.69104 (15)0.02624 (8)0.89841 (7)0.0567 (3)
C10.53523 (18)0.00878 (10)0.87075 (8)0.0549 (4)
C20.5352 (2)0.06949 (10)0.83742 (9)0.0609 (4)
C30.69556 (19)0.10341 (10)0.84393 (8)0.0569 (4)
C40.79057 (18)0.04153 (9)0.88152 (8)0.0555 (4)
C50.9566 (2)0.05257 (12)0.89561 (10)0.0654 (4)
C61.0257 (2)0.12777 (12)0.87299 (10)0.0686 (4)
C70.9331 (2)0.19096 (12)0.83734 (10)0.0687 (5)
C80.7701 (2)0.17938 (11)0.82203 (10)0.0660 (4)
C90.39997 (18)0.06971 (10)0.87645 (9)0.0558 (4)
C100.3649 (2)0.11392 (11)0.94430 (10)0.0640 (4)
C110.2400 (2)0.17240 (12)0.94654 (12)0.0749 (5)
C120.1473 (2)0.18728 (13)0.88119 (14)0.0817 (6)
C130.1767 (2)0.14149 (13)0.81421 (13)0.0788 (5)
C140.3015 (2)0.08343 (12)0.81145 (10)0.0661 (4)
C150.7471 (2)0.10365 (11)0.93398 (13)0.0857 (6)
H20.436 (2)0.0944 (11)0.8168 (11)0.078 (5)*
H51.022 (2)0.0094 (12)0.9197 (11)0.084 (6)*
H61.145 (3)0.1378 (11)0.8848 (10)0.080 (5)*
H70.990 (2)0.2451 (13)0.8220 (11)0.093 (6)*
H80.704 (2)0.2244 (11)0.7958 (10)0.084 (5)*
H100.4287 (19)0.1048 (10)0.9903 (10)0.066 (5)*
H110.221 (2)0.2038 (11)0.9944 (12)0.091 (6)*
H120.056 (3)0.2288 (13)0.8838 (11)0.094 (6)*
H130.110 (2)0.1520 (12)0.7689 (12)0.092 (6)*
H140.325 (2)0.0523 (10)0.7642 (11)0.077 (5)*
H15A0.86030.11200.92190.129*
H15B0.68460.15010.91420.129*
H15C0.73370.10020.98940.129*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0539 (7)0.0554 (7)0.0609 (7)0.0034 (6)0.0056 (5)0.0012 (5)
C10.0519 (8)0.0618 (9)0.0511 (7)0.0022 (7)0.0023 (6)0.0028 (6)
C20.0562 (9)0.0666 (10)0.0598 (9)0.0058 (7)0.0027 (7)0.0064 (7)
C30.0574 (8)0.0597 (9)0.0535 (8)0.0038 (7)0.0027 (6)0.0001 (6)
C40.0542 (8)0.0579 (8)0.0543 (8)0.0013 (7)0.0004 (6)0.0041 (6)
C50.0550 (9)0.0717 (11)0.0694 (10)0.0031 (8)0.0048 (7)0.0020 (8)
C60.0579 (10)0.0780 (12)0.0699 (10)0.0059 (9)0.0010 (8)0.0054 (8)
C70.0704 (11)0.0681 (11)0.0676 (10)0.0086 (8)0.0077 (8)0.0013 (8)
C80.0697 (11)0.0635 (10)0.0649 (10)0.0019 (8)0.0044 (8)0.0060 (8)
C90.0514 (8)0.0605 (9)0.0555 (8)0.0034 (7)0.0004 (6)0.0068 (6)
C100.0662 (10)0.0669 (10)0.0590 (9)0.0032 (8)0.0019 (7)0.0050 (7)
C110.0721 (11)0.0679 (11)0.0845 (13)0.0033 (9)0.0142 (9)0.0012 (9)
C120.0601 (11)0.0700 (12)0.1148 (17)0.0052 (9)0.0056 (10)0.0186 (11)
C130.0603 (10)0.0846 (13)0.0914 (14)0.0021 (9)0.0139 (9)0.0234 (11)
C140.0611 (9)0.0756 (11)0.0616 (10)0.0066 (8)0.0071 (7)0.0083 (8)
C150.0698 (11)0.0658 (11)0.1215 (17)0.0031 (9)0.0204 (11)0.0194 (10)
Geometric parameters (Å, º) top
N1—C41.3804 (19)C9—C101.390 (2)
N1—C11.3904 (19)C9—C141.394 (2)
N1—C151.446 (2)C9—C11.474 (2)
C1—C21.367 (2)C10—C111.382 (2)
C2—H20.969 (18)C10—H100.959 (17)
C3—C81.403 (2)C11—H110.973 (19)
C3—C41.409 (2)C12—C111.375 (3)
C3—C21.424 (2)C12—H120.99 (2)
C4—C51.393 (2)C13—C121.381 (3)
C5—C61.377 (2)C13—H130.96 (2)
C5—H50.962 (19)C14—C131.377 (3)
C6—C71.398 (3)C14—H140.969 (17)
C6—H61.01 (2)C15—H15A0.9600
C7—H71.01 (2)C15—H15B0.9600
C8—C71.374 (3)C15—H15C0.9600
C8—H81.004 (18)
C4—N1—C1108.42 (12)C3—C8—H8119.7 (10)
C4—N1—C15124.21 (14)C10—C9—C14118.18 (16)
C1—N1—C15127.24 (14)C10—C9—C1122.83 (14)
C2—C1—N1108.89 (14)C14—C9—C1118.99 (14)
C2—C1—C9128.57 (14)C11—C10—C9121.02 (17)
N1—C1—C9122.51 (14)C11—C10—H10118.9 (10)
C1—C2—C3108.08 (14)C9—C10—H10120.1 (10)
C1—C2—H2121.5 (11)C12—C11—C10120.1 (2)
C3—C2—H2130.3 (11)C12—C11—H11120.6 (12)
C8—C3—C4118.71 (15)C10—C11—H11119.2 (12)
C8—C3—C2134.88 (15)C11—C12—C13119.50 (19)
C4—C3—C2106.41 (14)C11—C12—H12119.3 (12)
N1—C4—C5129.70 (15)C13—C12—H12121.1 (11)
N1—C4—C3108.19 (14)C14—C13—C12120.65 (19)
C5—C4—C3122.11 (15)C14—C13—H13120.6 (12)
C6—C5—C4117.52 (17)C12—C13—H13118.8 (12)
C6—C5—H5120.6 (11)C13—C14—C9120.45 (18)
C4—C5—H5121.9 (11)C13—C14—H14121.0 (10)
C5—C6—C7121.44 (17)C9—C14—H14118.5 (10)
C5—C6—H6118.6 (10)N1—C15—H15A109.5
C7—C6—H6120.0 (10)N1—C15—H15B109.5
C8—C7—C6121.03 (17)H15A—C15—H15B109.5
C8—C7—H7120.9 (11)N1—C15—H15C109.5
C6—C7—H7118.0 (11)H15A—C15—H15C109.5
C7—C8—C3119.17 (16)H15B—C15—H15C109.5
C7—C8—H8121.1 (10)
C4—N1—C1—C20.64 (17)N1—C4—C5—C6179.45 (15)
C15—N1—C1—C2176.48 (16)C3—C4—C5—C61.5 (2)
C4—N1—C1—C9177.49 (13)C4—C5—C6—C70.1 (3)
C15—N1—C1—C91.7 (2)C5—C6—C7—C81.5 (3)
C1—N1—C4—C5178.07 (15)C3—C8—C7—C61.1 (3)
C15—N1—C4—C52.1 (3)C10—C9—C1—C2135.81 (18)
C1—N1—C4—C31.11 (16)C14—C9—C1—C243.6 (2)
C15—N1—C4—C3177.11 (15)C10—C9—C1—N146.4 (2)
N1—C1—C2—C30.08 (17)C14—C9—C1—N1134.12 (16)
C9—C1—C2—C3178.07 (14)C10—C9—C14—C132.2 (2)
C8—C3—C2—C1179.38 (17)C1—C9—C14—C13178.35 (15)
C4—C3—C2—C10.75 (17)C14—C9—C10—C112.5 (2)
C8—C3—C4—N1178.97 (13)C1—C9—C10—C11178.03 (15)
C2—C3—C4—N11.14 (16)C9—C10—C11—C120.4 (3)
C8—C3—C4—C51.8 (2)C14—C13—C12—C112.4 (3)
C2—C3—C4—C5178.11 (15)C13—C12—C11—C102.1 (3)
C4—C3—C8—C70.4 (2)C9—C14—C13—C120.3 (3)
C2—C3—C8—C7179.42 (17)
 

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