Literature DB >> 21587990

2,4,6-Triphenyl-aniline.

Onome Ugono1, Stephanie Cowin, Alicia M Beatty.   

Abstract

Individual mol-ecules of the title compound, C(24)H(19)N, do not participate in hydrogen-bonding inter-actions due to the steric bulk of the phenyl rings ortho to the amine. The dihedral angles between the central ring and the pendant rings are 68.26 (10), 55.28 (10) and 30.61 (11)°.

Entities:  

Year:  2010        PMID: 21587990      PMCID: PMC3006753          DOI: 10.1107/S160053681002338X

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


Related literature

The reaction of equimolar amounts of pyrazole-3,5-dicarb­oxy­lic acid (HPzDCA) and primary amines have yielded ammonium carboxyl­ate salts that adopt layered architectures, see: Ugono et al. (2009 ▶); Beatty et al. (2002a ▶,b ▶). For other amines that do not exhibit inter­molecular hydrogen bonding due to the bulky ortho phenyl groups, see: Cherian et al. (2005 ▶); Lonkin & Marshal (2004 ▶). For the preparation of 2,4,6-triphenyl­aniline, see: Basu et al. (2003 ▶); Paul & Clark (2003 ▶).

Experimental

Crystal data

C24H19N M = 321.40 Monoclinic, a = 10.735 (2) Å b = 14.792 (3) Å c = 11.911 (2) Å β = 113.02 (3)° V = 1740.7 (6) Å3 Z = 4 Mo Kα radiation μ = 0.07 mm−1 T = 100 K 0.50 × 0.50 × 0.25 mm

Data collection

Bruker SMART APEXII diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.966, T max = 0.983 44061 measured reflections 6695 independent reflections 5813 reflections with I > 2σ(I) R int = 0.027

Refinement

R[F 2 > 2σ(F 2)] = 0.043 wR(F 2) = 0.125 S = 1.02 6695 reflections 226 parameters H-atom parameters constrained Δρmax = 0.48 e Å−3 Δρmin = −0.23 e Å−3 Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: X-SEED (Barbour, 2001 ▶); software used to prepare material for publication: SHELXL97 and PLATON (Spek, 2009 ▶). Crystal structure: contains datablocks I, New_Global_Publ_Block. DOI: 10.1107/S160053681002338X/hg2686sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S160053681002338X/hg2686Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C24H19NF(000) = 680
Mr = 321.40Dx = 1.226 Mg m3
Monoclinic, P21/cMelting point = 395–398 K
Hall symbol: -P 2ybcMo Kα radiation, λ = 0.71073 Å
a = 10.735 (2) ÅCell parameters from 6695 reflections
b = 14.792 (3) Åθ = 2.1–33.9°
c = 11.911 (2) ŵ = 0.07 mm1
β = 113.02 (3)°T = 100 K
V = 1740.7 (6) Å3Prism, colorless
Z = 40.50 × 0.50 × 0.25 mm
Bruker SMART APEXII diffractometer6695 independent reflections
Radiation source: fine-focus sealed tube5813 reflections with I > 2σ(I)
graphiteRint = 0.027
ω scansθmax = 33.9°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996)h = −16→16
Tmin = 0.966, Tmax = 0.983k = −23→23
44061 measured reflectionsl = −18→18
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.125H-atom parameters constrained
S = 1.02w = 1/[σ2(Fo2) + (0.0697P)2 + 0.5511P] where P = (Fo2 + 2Fc2)/3
6695 reflections(Δ/σ)max = 0.001
226 parametersΔρmax = 0.48 e Å3
0 restraintsΔρmin = −0.23 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
N1−0.03946 (8)0.31892 (6)0.10628 (7)0.02312 (15)
H1A−0.03090.35320.16930.028*
H1B−0.10860.28170.07600.028*
C10.05584 (7)0.32362 (5)0.05479 (6)0.01365 (13)
C20.16729 (8)0.38320 (5)0.10276 (7)0.01385 (13)
C30.26324 (8)0.38694 (5)0.05077 (7)0.01493 (13)
H30.33760.42720.08420.018*
C40.25338 (7)0.33322 (5)−0.04924 (7)0.01409 (13)
C50.14616 (7)0.27160 (5)−0.09177 (7)0.01405 (13)
H50.13990.2322−0.15670.017*
C60.04796 (7)0.26577 (5)−0.04244 (6)0.01310 (13)
C70.18451 (8)0.44422 (5)0.20775 (7)0.01407 (13)
C80.29191 (8)0.43079 (5)0.32071 (7)0.01645 (14)
H80.35170.38120.33140.020*
C90.31156 (8)0.48981 (6)0.41751 (7)0.01874 (15)
H90.38370.47960.49410.022*
C100.22601 (9)0.56362 (6)0.40238 (7)0.01889 (15)
H100.24040.60420.46810.023*
C110.11933 (9)0.57760 (6)0.29049 (7)0.01905 (15)
H110.06090.62800.27970.023*
C120.09793 (9)0.51788 (5)0.19407 (7)0.01751 (14)
H120.02390.52730.11840.021*
C130.34837 (8)0.34425 (5)−0.11131 (7)0.01444 (13)
C140.48238 (8)0.37311 (6)−0.04755 (7)0.01809 (14)
H140.51460.38290.03800.022*
C150.56863 (8)0.38749 (6)−0.10796 (8)0.02019 (15)
H150.65890.4071−0.06330.024*
C160.52351 (9)0.37333 (6)−0.23338 (8)0.02020 (15)
H160.58190.3842−0.27470.024*
C170.39142 (9)0.34296 (6)−0.29744 (8)0.01904 (15)
H170.36030.3318−0.38260.023*
C180.30489 (8)0.32897 (5)−0.23725 (7)0.01613 (14)
H180.21500.3088−0.28210.019*
C19−0.06390 (7)0.19929 (5)−0.09729 (6)0.01294 (12)
C20−0.19933 (8)0.22763 (5)−0.14897 (7)0.01598 (14)
H20−0.22060.2894−0.14330.019*
C21−0.30318 (8)0.16641 (5)−0.20861 (7)0.01793 (14)
H21−0.39440.1866−0.24310.022*
C22−0.27334 (8)0.07567 (5)−0.21765 (7)0.01761 (14)
H22−0.34380.0339−0.25870.021*
C23−0.13918 (8)0.04676 (5)−0.16595 (7)0.01747 (14)
H23−0.1184−0.0151−0.17150.021*
C24−0.03506 (8)0.10781 (5)−0.10612 (7)0.01537 (13)
H240.05590.0872−0.07120.018*
U11U22U33U12U13U23
N10.0255 (3)0.0285 (4)0.0204 (3)−0.0110 (3)0.0144 (3)−0.0100 (3)
C10.0160 (3)0.0130 (3)0.0116 (3)−0.0006 (2)0.0051 (2)0.0004 (2)
C20.0169 (3)0.0120 (3)0.0117 (3)−0.0010 (2)0.0047 (2)−0.0007 (2)
C30.0165 (3)0.0133 (3)0.0141 (3)−0.0019 (2)0.0050 (2)−0.0016 (2)
C40.0147 (3)0.0134 (3)0.0139 (3)−0.0009 (2)0.0053 (2)−0.0010 (2)
C50.0153 (3)0.0124 (3)0.0139 (3)−0.0006 (2)0.0052 (2)−0.0015 (2)
C60.0146 (3)0.0112 (3)0.0123 (3)−0.0006 (2)0.0040 (2)−0.0001 (2)
C70.0177 (3)0.0130 (3)0.0113 (3)−0.0022 (2)0.0054 (2)−0.0006 (2)
C80.0166 (3)0.0180 (3)0.0134 (3)−0.0012 (2)0.0045 (2)−0.0003 (2)
C90.0196 (3)0.0231 (4)0.0123 (3)−0.0046 (3)0.0049 (3)−0.0016 (3)
C100.0253 (4)0.0192 (3)0.0140 (3)−0.0058 (3)0.0095 (3)−0.0039 (3)
C110.0268 (4)0.0151 (3)0.0165 (3)0.0002 (3)0.0098 (3)−0.0012 (2)
C120.0229 (3)0.0148 (3)0.0132 (3)0.0011 (3)0.0052 (3)0.0004 (2)
C130.0153 (3)0.0125 (3)0.0155 (3)−0.0007 (2)0.0060 (2)−0.0011 (2)
C140.0154 (3)0.0195 (3)0.0182 (3)−0.0013 (2)0.0054 (3)−0.0018 (3)
C150.0159 (3)0.0192 (3)0.0262 (4)−0.0002 (3)0.0090 (3)−0.0002 (3)
C160.0214 (4)0.0173 (3)0.0264 (4)0.0023 (3)0.0142 (3)0.0026 (3)
C170.0245 (4)0.0166 (3)0.0186 (3)0.0012 (3)0.0112 (3)0.0001 (3)
C180.0181 (3)0.0144 (3)0.0158 (3)−0.0012 (2)0.0065 (3)−0.0017 (2)
C190.0153 (3)0.0117 (3)0.0117 (3)−0.0009 (2)0.0052 (2)0.0001 (2)
C200.0162 (3)0.0129 (3)0.0166 (3)0.0004 (2)0.0041 (2)0.0001 (2)
C210.0162 (3)0.0162 (3)0.0178 (3)−0.0010 (2)0.0028 (3)0.0006 (2)
C220.0189 (3)0.0152 (3)0.0167 (3)−0.0041 (2)0.0048 (3)−0.0012 (2)
C230.0204 (3)0.0123 (3)0.0204 (3)−0.0017 (2)0.0088 (3)−0.0018 (2)
C240.0168 (3)0.0124 (3)0.0176 (3)−0.0007 (2)0.0075 (3)−0.0006 (2)
N1—C11.3850 (11)C12—H120.9500
N1—H1A0.8800C13—C181.4040 (11)
N1—H1B0.8800C13—C141.4050 (11)
C1—C21.4142 (11)C14—C151.3933 (12)
C1—C61.4156 (10)C14—H140.9500
C2—C31.3951 (11)C15—C161.3944 (13)
C2—C71.4939 (11)C15—H150.9500
C3—C41.4010 (11)C16—C171.3960 (13)
C3—H30.9500C16—H160.9500
C4—C51.3987 (10)C17—C181.3930 (12)
C4—C131.4841 (11)C17—H170.9500
C5—C61.3959 (11)C18—H180.9500
C5—H50.9500C19—C241.4012 (11)
C6—C191.4907 (10)C19—C201.4030 (11)
C7—C121.3997 (11)C20—C211.3958 (11)
C7—C81.4020 (12)C20—H200.9500
C8—C91.3950 (11)C21—C221.3939 (12)
C8—H80.9500C21—H210.9500
C9—C101.3923 (13)C22—C231.3938 (12)
C9—H90.9500C22—H220.9500
C10—C111.3916 (13)C23—C241.3962 (11)
C10—H100.9500C23—H230.9500
C11—C121.3949 (11)C24—H240.9500
C11—H110.9500
C1—N1—H1A120.0C7—C12—H12119.7
C1—N1—H1B120.0C18—C13—C14117.95 (8)
H1A—N1—H1B120.0C18—C13—C4120.56 (7)
N1—C1—C2120.47 (7)C14—C13—C4121.46 (7)
N1—C1—C6120.92 (7)C15—C14—C13120.93 (8)
C2—C1—C6118.53 (7)C15—C14—H14119.5
C3—C2—C1120.01 (7)C13—C14—H14119.5
C3—C2—C7118.45 (7)C14—C15—C16120.51 (8)
C1—C2—C7121.53 (7)C14—C15—H15119.7
C2—C3—C4122.11 (7)C16—C15—H15119.7
C2—C3—H3118.9C15—C16—C17119.14 (8)
C4—C3—H3118.9C15—C16—H16120.4
C5—C4—C3117.09 (7)C17—C16—H16120.4
C5—C4—C13121.31 (7)C18—C17—C16120.38 (8)
C3—C4—C13121.54 (7)C18—C17—H17119.8
C6—C5—C4122.53 (7)C16—C17—H17119.8
C6—C5—H5118.7C17—C18—C13121.06 (8)
C4—C5—H5118.7C17—C18—H18119.5
C5—C6—C1119.59 (7)C13—C18—H18119.5
C5—C6—C19117.89 (6)C24—C19—C20118.49 (7)
C1—C6—C19122.51 (7)C24—C19—C6120.41 (7)
C12—C7—C8118.77 (7)C20—C19—C6120.94 (7)
C12—C7—C2120.91 (7)C21—C20—C19120.92 (7)
C8—C7—C2120.26 (7)C21—C20—H20119.5
C9—C8—C7120.42 (8)C19—C20—H20119.5
C9—C8—H8119.8C22—C21—C20120.14 (7)
C7—C8—H8119.8C22—C21—H21119.9
C10—C9—C8120.33 (8)C20—C21—H21119.9
C10—C9—H9119.8C23—C22—C21119.36 (7)
C8—C9—H9119.8C23—C22—H22120.3
C11—C10—C9119.64 (7)C21—C22—H22120.3
C11—C10—H10120.2C22—C23—C24120.65 (7)
C9—C10—H10120.2C22—C23—H23119.7
C10—C11—C12120.22 (8)C24—C23—H23119.7
C10—C11—H11119.9C23—C24—C19120.44 (7)
C12—C11—H11119.9C23—C24—H24119.8
C11—C12—C7120.61 (8)C19—C24—H24119.8
C11—C12—H12119.7
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