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The title compound, C21H17N, was synthesized by the p-toluene­sulfonic acid-assisted Schiff base reaction between 9-fluorenone and 3,4-di­methyl­aniline. The crystal structure has been determined at 100 K.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536804015089/lh6231sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536804015089/lh6231Isup2.hkl
Contains datablock I

CCDC reference: 245340

Key indicators

  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.054
  • wR factor = 0.147
  • Data-to-parameter ratio = 18.5

checkCIF/PLATON results

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No errors found in this datablock

Computing details top

Data collection: SMART (1997-1999); cell refinement: SMART; data reduction: SAINT-Plus (1997–1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

N-9H-Fluoren-9-ylidene-3,4-dimethyaniline top
Crystal data top
C21H17NZ = 2
Mr = 283.36F(000) = 300
Triclinic, P1Dx = 1.251 Mg m3
Hall symbol: -P 1Melting point: 355.8 K
a = 8.476 (3) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.870 (3) ÅCell parameters from 6350 reflections
c = 10.376 (4) Åθ = 2.3–28.4°
α = 78.886 (6)°µ = 0.07 mm1
β = 79.375 (6)°T = 100 K
γ = 89.483 (6)°Parallelepiped, orange
V = 752.1 (5) Å30.40 × 0.34 × 0.10 mm
Data collection top
Bruker SMART APEX
diffractometer
3722 independent reflections
Radiation source: sealed tube3472 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.035
/w scansθmax = 28.5°, θmin = 2.0°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
h = 1111
Tmin = 0.967, Tmax = 0.995k = 1111
7401 measured reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.054Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.147H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0842P)2 + 0.226P]
where P = (Fo2 + 2Fc2)/3
3722 reflections(Δ/σ)max < 0.001
201 parametersΔρmax = 0.49 e Å3
0 restraintsΔρmin = 0.28 e Å3
Special details top

Experimental. All hydrogen atoms were included in calculated positions with C—H distances of 0.95 Å and 0.98 Å (for aromatic and methyl H atoms respectively) and were included in the refinement in riding motion approximation with Uiso = 1.2Ueq of the carrier atom. Other details are mentioned above in the text.

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
N10.17433 (12)0.46338 (11)0.67607 (10)0.0192 (2)
C10.04904 (13)0.25424 (13)0.90276 (11)0.0185 (2)
H1B0.03350.19570.86250.022*
C20.16822 (14)0.18367 (13)1.00806 (11)0.0202 (2)
H2A0.16720.07591.03990.024*
C30.28873 (14)0.27017 (14)1.06676 (12)0.0216 (3)
H3A0.36900.22051.13850.026*
C40.29349 (14)0.42875 (14)1.02188 (11)0.0204 (2)
H4A0.37570.48741.06230.024*
C50.23586 (14)0.78863 (13)0.86896 (11)0.0201 (2)
H5A0.32860.78050.93740.024*
C60.18410 (15)0.93022 (14)0.78815 (12)0.0219 (3)
H6A0.24261.01950.80150.026*
C70.04821 (14)0.94273 (13)0.68831 (12)0.0213 (3)
H7A0.01471.04050.63480.026*
C80.03990 (14)0.81344 (13)0.66552 (11)0.0190 (2)
H8A0.13260.82220.59700.023*
C90.05504 (13)0.51429 (12)0.74783 (11)0.0158 (2)
C100.05363 (13)0.41135 (13)0.85820 (11)0.0161 (2)
C110.17535 (13)0.49860 (12)0.91689 (11)0.0164 (2)
C120.14870 (13)0.65976 (13)0.84713 (11)0.0168 (2)
C130.01134 (13)0.67170 (12)0.74549 (11)0.0162 (2)
C140.27151 (13)0.56591 (12)0.56911 (11)0.0181 (2)
C150.40697 (13)0.63838 (13)0.59043 (11)0.0182 (2)
H15A0.43220.62070.67750.022*
C160.50606 (13)0.73612 (13)0.48654 (11)0.0183 (2)
C170.47049 (13)0.76004 (13)0.35730 (11)0.0188 (2)
C180.33727 (14)0.68383 (14)0.33679 (12)0.0205 (2)
H18A0.31360.69820.24930.025*
C190.23786 (14)0.58724 (14)0.44088 (12)0.0209 (2)
H19A0.14760.53620.42450.025*
C200.65200 (15)0.81173 (15)0.51315 (13)0.0260 (3)
H20A0.65920.77980.60760.039*
H20B0.64320.92370.49170.039*
H20C0.74850.78100.45740.039*
C210.57716 (15)0.86252 (15)0.24221 (13)0.0270 (3)
H21A0.52810.87470.16250.040*
H21B0.68240.81620.22440.040*
H21C0.59040.96340.26480.040*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0174 (5)0.0174 (5)0.0217 (5)0.0023 (3)0.0009 (4)0.0039 (4)
C10.0185 (5)0.0173 (5)0.0202 (5)0.0028 (4)0.0039 (4)0.0046 (4)
C20.0239 (6)0.0164 (5)0.0200 (5)0.0002 (4)0.0051 (4)0.0022 (4)
C30.0225 (6)0.0227 (6)0.0180 (5)0.0017 (4)0.0004 (4)0.0036 (4)
C40.0206 (5)0.0218 (6)0.0187 (5)0.0026 (4)0.0011 (4)0.0063 (4)
C50.0204 (5)0.0208 (6)0.0206 (5)0.0049 (4)0.0033 (4)0.0088 (4)
C60.0249 (6)0.0177 (5)0.0267 (6)0.0072 (4)0.0085 (5)0.0095 (4)
C70.0248 (6)0.0148 (5)0.0252 (6)0.0018 (4)0.0070 (4)0.0041 (4)
C80.0185 (5)0.0176 (5)0.0214 (5)0.0015 (4)0.0041 (4)0.0049 (4)
C90.0155 (5)0.0152 (5)0.0178 (5)0.0016 (4)0.0046 (4)0.0044 (4)
C100.0157 (5)0.0172 (5)0.0166 (5)0.0014 (4)0.0043 (4)0.0054 (4)
C110.0172 (5)0.0168 (5)0.0169 (5)0.0021 (4)0.0046 (4)0.0063 (4)
C120.0176 (5)0.0170 (5)0.0172 (5)0.0023 (4)0.0043 (4)0.0062 (4)
C130.0158 (5)0.0162 (5)0.0183 (5)0.0030 (4)0.0045 (4)0.0062 (4)
C140.0168 (5)0.0150 (5)0.0212 (5)0.0048 (4)0.0001 (4)0.0043 (4)
C150.0196 (5)0.0174 (5)0.0180 (5)0.0043 (4)0.0017 (4)0.0067 (4)
C160.0172 (5)0.0158 (5)0.0224 (5)0.0037 (4)0.0019 (4)0.0068 (4)
C170.0175 (5)0.0157 (5)0.0216 (5)0.0055 (4)0.0004 (4)0.0030 (4)
C180.0199 (5)0.0218 (5)0.0201 (5)0.0052 (4)0.0054 (4)0.0035 (4)
C190.0170 (5)0.0210 (5)0.0249 (6)0.0016 (4)0.0052 (4)0.0039 (4)
C200.0240 (6)0.0246 (6)0.0303 (6)0.0040 (5)0.0048 (5)0.0073 (5)
C210.0232 (6)0.0262 (6)0.0267 (6)0.0015 (5)0.0003 (5)0.0020 (5)
Geometric parameters (Å, º) top
N1—C91.2745 (15)C9—C131.4982 (15)
N1—C141.4229 (15)C10—C111.4035 (15)
C1—C101.3837 (16)C11—C121.4714 (16)
C1—C21.3953 (16)C12—C131.4090 (16)
C1—H1B0.9500C14—C191.3890 (17)
C2—C31.3928 (16)C14—C151.3937 (16)
C2—H2A0.9500C15—C161.3922 (16)
C3—C41.3966 (17)C15—H15A0.9500
C3—H3A0.9500C16—C171.4045 (17)
C4—C111.3864 (16)C16—C201.5061 (16)
C4—H4A0.9500C17—C181.3911 (17)
C5—C121.3880 (15)C17—C211.5059 (16)
C5—C61.3933 (17)C18—C191.3897 (16)
C5—H5A0.9500C18—H18A0.9500
C6—C71.3893 (18)C19—H19A0.9500
C6—H6A0.9500C20—H20A0.9800
C7—C81.3975 (16)C20—H20B0.9800
C7—H7A0.9500C20—H20C0.9800
C8—C131.3902 (16)C21—H21A0.9800
C8—H8A0.9500C21—H21B0.9800
C9—C101.4888 (15)C21—H21C0.9800
C9—N1—C14119.74 (10)C5—C12—C11129.79 (10)
C10—C1—C2118.56 (10)C13—C12—C11109.39 (10)
C10—C1—H1B120.7C8—C13—C12120.44 (10)
C2—C1—H1B120.7C8—C13—C9131.69 (10)
C3—C2—C1120.44 (11)C12—C13—C9107.86 (9)
C3—C2—H2A119.8C19—C14—C15119.39 (11)
C1—C2—H2A119.8C19—C14—N1120.24 (10)
C2—C3—C4121.04 (11)C15—C14—N1120.24 (10)
C2—C3—H3A119.5C16—C15—C14121.25 (11)
C4—C3—H3A119.5C16—C15—H15A119.4
C11—C4—C3118.44 (11)C14—C15—H15A119.4
C11—C4—H4A120.8C15—C16—C17119.39 (11)
C3—C4—H4A120.8C15—C16—C20119.78 (11)
C12—C5—C6118.42 (11)C17—C16—C20120.81 (11)
C12—C5—H5A120.8C18—C17—C16118.73 (10)
C6—C5—H5A120.8C18—C17—C21120.55 (11)
C7—C6—C5120.97 (11)C16—C17—C21120.70 (11)
C7—C6—H6A119.5C19—C18—C17121.75 (11)
C5—C6—H6A119.5C19—C18—H18A119.1
C6—C7—C8120.93 (11)C17—C18—H18A119.1
C6—C7—H7A119.5C14—C19—C18119.45 (11)
C8—C7—H7A119.5C14—C19—H19A120.3
C13—C8—C7118.41 (11)C18—C19—H19A120.3
C13—C8—H8A120.8C16—C20—H20A109.5
C7—C8—H8A120.8C16—C20—H20B109.5
N1—C9—C10121.98 (10)H20A—C20—H20B109.5
N1—C9—C13132.58 (10)C16—C20—H20C109.5
C10—C9—C13105.44 (9)H20A—C20—H20C109.5
C1—C10—C11121.07 (10)H20B—C20—H20C109.5
C1—C10—C9129.78 (10)C17—C21—H21A109.5
C11—C10—C9109.14 (10)C17—C21—H21B109.5
C4—C11—C10120.44 (10)H21A—C21—H21B109.5
C4—C11—C12131.40 (10)C17—C21—H21C109.5
C10—C11—C12108.16 (10)H21A—C21—H21C109.5
C5—C12—C13120.82 (11)H21B—C21—H21C109.5
C10—C1—C2—C30.09 (17)C7—C8—C13—C120.18 (16)
C1—C2—C3—C40.09 (18)C7—C8—C13—C9179.54 (11)
C2—C3—C4—C110.16 (17)C5—C12—C13—C80.35 (16)
C12—C5—C6—C70.23 (17)C11—C12—C13—C8179.52 (10)
C5—C6—C7—C80.41 (18)C5—C12—C13—C9179.85 (9)
C6—C7—C8—C130.19 (17)C11—C12—C13—C90.01 (12)
C14—N1—C9—C10178.03 (9)N1—C9—C13—C82.0 (2)
C14—N1—C9—C130.52 (19)C10—C9—C13—C8179.26 (11)
C2—C1—C10—C110.16 (16)N1—C9—C13—C12178.56 (12)
C2—C1—C10—C9178.89 (10)C10—C9—C13—C120.16 (11)
N1—C9—C10—C10.25 (18)C9—N1—C14—C1992.47 (14)
C13—C9—C10—C1179.14 (11)C9—N1—C14—C1591.52 (13)
N1—C9—C10—C11178.60 (10)C19—C14—C15—C162.33 (17)
C13—C9—C10—C110.29 (11)N1—C14—C15—C16178.37 (9)
C3—C4—C11—C100.42 (17)C14—C15—C16—C171.15 (16)
C3—C4—C11—C12179.19 (11)C14—C15—C16—C20179.64 (10)
C1—C10—C11—C40.42 (16)C15—C16—C17—C180.53 (16)
C9—C10—C11—C4179.39 (9)C20—C16—C17—C18177.95 (11)
C1—C10—C11—C12179.27 (10)C15—C16—C17—C21178.75 (10)
C9—C10—C11—C120.30 (12)C20—C16—C17—C210.27 (16)
C6—C5—C12—C130.14 (16)C16—C17—C18—C191.04 (17)
C6—C5—C12—C11179.70 (11)C21—C17—C18—C19179.26 (11)
C4—C11—C12—C50.7 (2)C15—C14—C19—C181.80 (17)
C10—C11—C12—C5179.65 (11)N1—C14—C19—C18177.84 (10)
C4—C11—C12—C13179.45 (11)C17—C18—C19—C140.13 (17)
C10—C11—C12—C130.20 (12)
 

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