organic compounds
1-[(Butylamino)(phenyl)methyl]naphthalen-2-ol
aCollege of Chemistry and Chemical Engineering, Southeast University, Nanjing 211189, People's Republic of China
*Correspondence e-mail: nihmseu@hotmail.com
In the title compound, C21H23NO, obtained via a one-pot synthesis, an intramolecular O—H⋯N hydrogen bond stabilizes the molecular conformation. The dihedral angle between the fused ring system and the phenyl ring is 78.27 (5)°. The crystal packing is characterized by helical chains of molecules linked by C—H⋯O hydrogen bonds.
Related literature
For applications of Betti-type reactions, see: Zhao et al. (2004); Lu et al. (2002); Xu et al. (2004); Wang et al. (2005)
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear (Rigaku, 2005); cell CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.
Supporting information
10.1107/S1600536811000067/gw2088sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811000067/gw2088Isup2.hkl
benzaldehyde (1.59 g, 0.015 mol) and butan-1-amine (1.095 g, 0.015 mol) was added to 2-naphthol (2.16 g, 0.015 mol) without solvent under nitrogen. The temperature was raised to 120°C in one hour gradually and the mixture was stirred at this temperature for 10 h. The system was treated with 20 ml of ethanol 95% and cooled. The precipitate was filtered and washed with a small amount of ethanol 95%. The title compound was isolated using
(Petroleum ether: ethyl acetate-2:1). Single crystals suitable for X-ray were obtained from slow evaporation of ethyl acetate solution.H atoms bonded to O atoms were located in a difference map and refined with distance restraints of O—H = 0.82 Å, and with Uiso(H) = 1.368Ueq(O). Other H atoms were positioned geometrically and refined using a riding model, with C—H = 0.93–0.98 Å and Uiso(H) = 1.3–1.6Ueq(C). The structure does not contain a strong anomalous scatterer, therefore MERG 3 have been applied. 1459 Friedel pairs were merged.
Data collection: CrystalClear (Rigaku, 2005); cell
CrystalClear (Rigaku, 2005); data reduction: CrystalClear (Rigaku, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).C21H23NO | F(000) = 656 |
Mr = 305.40 | Dx = 1.148 Mg m−3 |
Orthorhombic, Pna21 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2c -2n | Cell parameters from 2229 reflections |
a = 10.842 (7) Å | θ = 2.4–27.4° |
b = 16.651 (7) Å | µ = 0.07 mm−1 |
c = 9.787 (6) Å | T = 293 K |
V = 1766.9 (17) Å3 | Prism, colorless |
Z = 4 | 0.30 × 0.25 × 0.15 mm |
Rigaku Mercury2 diffractometer | 3121 independent reflections |
Radiation source: fine-focus sealed tube | 1998 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.078 |
Detector resolution: 13.6612 pixels mm-1 | θmax = 25.0°, θmin = 2.4° |
CCD_Profile_fitting scans | h = −12→12 |
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −19→19 |
Tmin = 0.856, Tmax = 1.000 | l = −11→11 |
14129 measured reflections |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.087 | H-atom parameters constrained |
wR(F2) = 0.134 | w = 1/[σ2(Fo2) + (0.0007P)2 + 1.9999P] where P = (Fo2 + 2Fc2)/3 |
S = 1.02 | (Δ/σ)max < 0.001 |
3121 reflections | Δρmax = 0.25 e Å−3 |
211 parameters | Δρmin = −0.13 e Å−3 |
2 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0043 (9) |
C21H23NO | V = 1766.9 (17) Å3 |
Mr = 305.40 | Z = 4 |
Orthorhombic, Pna21 | Mo Kα radiation |
a = 10.842 (7) Å | µ = 0.07 mm−1 |
b = 16.651 (7) Å | T = 293 K |
c = 9.787 (6) Å | 0.30 × 0.25 × 0.15 mm |
Rigaku Mercury2 diffractometer | 3121 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | 1998 reflections with I > 2σ(I) |
Tmin = 0.856, Tmax = 1.000 | Rint = 0.078 |
14129 measured reflections |
R[F2 > 2σ(F2)] = 0.087 | 2 restraints |
wR(F2) = 0.134 | H-atom parameters constrained |
S = 1.02 | Δρmax = 0.25 e Å−3 |
3121 reflections | Δρmin = −0.13 e Å−3 |
211 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
O1 | 0.2175 (3) | 0.0230 (2) | 0.4209 (4) | 0.0825 (11) | |
H1A | 0.2786 | 0.0483 | 0.3966 | 0.124* | |
N1 | 0.4017 (4) | 0.1176 (2) | 0.4649 (5) | 0.0718 (12) | |
H1D | 0.4572 | 0.1535 | 0.4201 | 0.086* | |
C1 | 0.1998 (4) | 0.1346 (3) | 0.5773 (5) | 0.0551 (12) | |
C2 | 0.1594 (4) | 0.0636 (3) | 0.5250 (5) | 0.0657 (14) | |
C3 | 0.0511 (5) | 0.0240 (3) | 0.5748 (5) | 0.0717 (16) | |
H3A | 0.0260 | −0.0245 | 0.5368 | 0.086* | |
C4 | −0.0136 (5) | 0.0574 (4) | 0.6767 (6) | 0.0748 (16) | |
H4A | −0.0832 | 0.0311 | 0.7097 | 0.090* | |
C5 | −0.0463 (5) | 0.1666 (4) | 0.8420 (6) | 0.0822 (18) | |
H5A | −0.1145 | 0.1397 | 0.8769 | 0.099* | |
C6 | −0.0147 (6) | 0.2386 (5) | 0.8958 (6) | 0.093 (2) | |
H6A | −0.0610 | 0.2609 | 0.9662 | 0.111* | |
C7 | 0.0874 (6) | 0.2788 (4) | 0.8448 (6) | 0.0899 (19) | |
H7A | 0.1090 | 0.3282 | 0.8822 | 0.108* | |
C8 | 0.1585 (5) | 0.2473 (4) | 0.7391 (5) | 0.0739 (16) | |
H8A | 0.2257 | 0.2758 | 0.7055 | 0.089* | |
C9 | 0.1277 (4) | 0.1714 (3) | 0.6832 (5) | 0.0601 (13) | |
C10 | 0.0212 (4) | 0.1313 (3) | 0.7350 (5) | 0.0646 (14) | |
C11 | 0.3145 (4) | 0.1767 (3) | 0.5238 (5) | 0.0566 (12) | |
H11A | 0.3552 | 0.2032 | 0.6009 | 0.068* | |
C12 | 0.2873 (4) | 0.2400 (3) | 0.4156 (5) | 0.0603 (12) | |
C13 | 0.1947 (6) | 0.2301 (4) | 0.3193 (6) | 0.094 (2) | |
H13A | 0.1443 | 0.1849 | 0.3231 | 0.113* | |
C14 | 0.1761 (6) | 0.2872 (5) | 0.2161 (7) | 0.113 (2) | |
H14A | 0.1128 | 0.2807 | 0.1530 | 0.136* | |
C15 | 0.2523 (6) | 0.3530 (4) | 0.2093 (7) | 0.098 (2) | |
H15A | 0.2425 | 0.3901 | 0.1390 | 0.118* | |
C16 | 0.3415 (6) | 0.3644 (4) | 0.3043 (6) | 0.097 (2) | |
H16A | 0.3908 | 0.4100 | 0.3015 | 0.116* | |
C17 | 0.3588 (5) | 0.3071 (3) | 0.4058 (6) | 0.0789 (16) | |
H17A | 0.4215 | 0.3148 | 0.4694 | 0.095* | |
C18 | 0.4708 (5) | 0.0719 (4) | 0.5698 (7) | 0.0921 (19) | |
H18A | 0.4145 | 0.0401 | 0.6248 | 0.111* | |
H18B | 0.5153 | 0.1083 | 0.6294 | 0.111* | |
C19 | 0.5652 (6) | 0.0146 (5) | 0.4899 (8) | 0.127 (3) | |
H19A | 0.5187 | −0.0218 | 0.4321 | 0.152* | |
H19B | 0.6169 | 0.0472 | 0.4312 | 0.152* | |
C20 | 0.6390 (7) | −0.0296 (5) | 0.5756 (10) | 0.162 (4) | |
H20A | 0.5881 | −0.0654 | 0.6297 | 0.194* | |
H20B | 0.6816 | 0.0064 | 0.6377 | 0.194* | |
C21 | 0.7336 (6) | −0.0788 (5) | 0.4962 (9) | 0.153 (4) | |
H21A | 0.7833 | −0.1090 | 0.5589 | 0.230* | |
H21B | 0.7854 | −0.0434 | 0.4441 | 0.230* | |
H21C | 0.6916 | −0.1149 | 0.4355 | 0.230* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.079 (2) | 0.084 (2) | 0.085 (3) | −0.017 (2) | 0.006 (2) | −0.019 (2) |
N1 | 0.053 (2) | 0.076 (3) | 0.086 (3) | −0.001 (2) | 0.009 (2) | −0.003 (3) |
C1 | 0.045 (3) | 0.070 (3) | 0.050 (3) | −0.004 (2) | −0.003 (2) | 0.003 (3) |
C2 | 0.057 (3) | 0.075 (4) | 0.065 (4) | −0.001 (3) | −0.002 (3) | −0.001 (3) |
C3 | 0.060 (3) | 0.075 (4) | 0.080 (4) | −0.010 (3) | −0.002 (3) | 0.009 (3) |
C4 | 0.053 (3) | 0.091 (4) | 0.080 (4) | −0.007 (3) | 0.000 (3) | 0.028 (3) |
C5 | 0.065 (4) | 0.110 (5) | 0.072 (4) | 0.021 (4) | −0.002 (3) | 0.022 (4) |
C6 | 0.075 (4) | 0.128 (6) | 0.075 (5) | 0.031 (4) | 0.010 (4) | −0.002 (4) |
C7 | 0.100 (5) | 0.095 (5) | 0.074 (4) | 0.024 (4) | −0.016 (4) | −0.013 (4) |
C8 | 0.073 (4) | 0.090 (4) | 0.058 (4) | 0.008 (3) | −0.014 (3) | −0.002 (3) |
C9 | 0.050 (3) | 0.074 (4) | 0.057 (3) | 0.001 (3) | −0.014 (2) | 0.013 (3) |
C10 | 0.053 (3) | 0.087 (4) | 0.054 (3) | 0.016 (3) | −0.004 (3) | 0.006 (3) |
C11 | 0.047 (3) | 0.064 (3) | 0.059 (3) | −0.003 (2) | −0.004 (2) | −0.010 (3) |
C12 | 0.059 (3) | 0.067 (3) | 0.055 (3) | −0.008 (3) | −0.002 (3) | −0.013 (3) |
C13 | 0.108 (5) | 0.103 (5) | 0.072 (4) | −0.042 (4) | −0.023 (4) | 0.017 (4) |
C14 | 0.109 (5) | 0.146 (7) | 0.085 (5) | −0.022 (5) | −0.038 (4) | 0.034 (5) |
C15 | 0.125 (6) | 0.104 (5) | 0.066 (4) | −0.002 (5) | 0.003 (4) | 0.028 (4) |
C16 | 0.119 (6) | 0.084 (5) | 0.088 (5) | −0.025 (4) | 0.000 (4) | 0.008 (4) |
C17 | 0.080 (4) | 0.075 (4) | 0.082 (4) | −0.021 (3) | −0.012 (3) | 0.010 (4) |
C18 | 0.076 (4) | 0.086 (4) | 0.115 (5) | 0.009 (3) | −0.012 (4) | −0.005 (4) |
C19 | 0.077 (5) | 0.151 (7) | 0.152 (8) | 0.026 (4) | −0.008 (5) | 0.026 (6) |
C20 | 0.136 (8) | 0.188 (10) | 0.161 (9) | 0.033 (7) | −0.001 (7) | −0.012 (8) |
C21 | 0.105 (6) | 0.109 (6) | 0.245 (11) | 0.032 (5) | 0.032 (6) | −0.047 (6) |
O1—C2 | 1.375 (6) | C11—H11A | 0.9800 |
O1—H1A | 0.8200 | C12—C17 | 1.363 (6) |
N1—C18 | 1.481 (6) | C12—C13 | 1.387 (6) |
N1—C11 | 1.483 (5) | C13—C14 | 1.402 (8) |
N1—H1D | 0.9548 | C13—H13A | 0.9300 |
C1—C2 | 1.362 (6) | C14—C15 | 1.374 (8) |
C1—C9 | 1.435 (7) | C14—H14A | 0.9300 |
C1—C11 | 1.520 (6) | C15—C16 | 1.355 (8) |
C2—C3 | 1.431 (6) | C15—H15A | 0.9300 |
C3—C4 | 1.340 (7) | C16—C17 | 1.390 (8) |
C3—H3A | 0.9300 | C16—H16A | 0.9300 |
C4—C10 | 1.409 (7) | C17—H17A | 0.9300 |
C4—H4A | 0.9300 | C18—C19 | 1.603 (8) |
C5—C6 | 1.353 (8) | C18—H18A | 0.9700 |
C5—C10 | 1.406 (8) | C18—H18B | 0.9700 |
C5—H5A | 0.9300 | C19—C20 | 1.373 (9) |
C6—C7 | 1.386 (8) | C19—H19A | 0.9700 |
C6—H6A | 0.9300 | C19—H19B | 0.9700 |
C7—C8 | 1.393 (7) | C20—C21 | 1.526 (9) |
C7—H7A | 0.9300 | C20—H20A | 0.9700 |
C8—C9 | 1.417 (7) | C20—H20B | 0.9700 |
C8—H8A | 0.9300 | C21—H21A | 0.9600 |
C9—C10 | 1.427 (6) | C21—H21B | 0.9600 |
C11—C12 | 1.523 (6) | C21—H21C | 0.9600 |
C2—O1—H1A | 109.5 | C17—C12—C11 | 120.4 (5) |
C18—N1—C11 | 113.2 (4) | C13—C12—C11 | 122.0 (5) |
C18—N1—H1D | 108.8 | C12—C13—C14 | 120.8 (6) |
C11—N1—H1D | 99.4 | C12—C13—H13A | 119.6 |
C2—C1—C9 | 117.8 (5) | C14—C13—H13A | 119.6 |
C2—C1—C11 | 122.3 (4) | C15—C14—C13 | 119.4 (6) |
C9—C1—C11 | 119.8 (4) | C15—C14—H14A | 120.3 |
C1—C2—O1 | 123.9 (5) | C13—C14—H14A | 120.3 |
C1—C2—C3 | 122.4 (5) | C16—C15—C14 | 120.4 (6) |
O1—C2—C3 | 113.7 (5) | C16—C15—H15A | 119.8 |
C4—C3—C2 | 119.5 (5) | C14—C15—H15A | 119.8 |
C4—C3—H3A | 120.2 | C15—C16—C17 | 119.4 (6) |
C2—C3—H3A | 120.2 | C15—C16—H16A | 120.3 |
C3—C4—C10 | 121.6 (5) | C17—C16—H16A | 120.3 |
C3—C4—H4A | 119.2 | C12—C17—C16 | 122.3 (6) |
C10—C4—H4A | 119.2 | C12—C17—H17A | 118.8 |
C6—C5—C10 | 121.9 (6) | C16—C17—H17A | 118.8 |
C6—C5—H5A | 119.1 | N1—C18—C19 | 106.9 (5) |
C10—C5—H5A | 119.1 | N1—C18—H18A | 110.3 |
C5—C6—C7 | 119.3 (6) | C19—C18—H18A | 110.3 |
C5—C6—H6A | 120.3 | N1—C18—H18B | 110.3 |
C7—C6—H6A | 120.3 | C19—C18—H18B | 110.3 |
C6—C7—C8 | 121.8 (6) | H18A—C18—H18B | 108.6 |
C6—C7—H7A | 119.1 | C20—C19—C18 | 113.2 (7) |
C8—C7—H7A | 119.1 | C20—C19—H19A | 108.9 |
C7—C8—C9 | 119.5 (6) | C18—C19—H19A | 108.9 |
C7—C8—H8A | 120.2 | C20—C19—H19B | 108.9 |
C9—C8—H8A | 120.2 | C18—C19—H19B | 108.9 |
C8—C9—C10 | 118.0 (5) | H19A—C19—H19B | 107.8 |
C8—C9—C1 | 122.1 (5) | C19—C20—C21 | 111.6 (8) |
C10—C9—C1 | 119.9 (5) | C19—C20—H20A | 109.3 |
C5—C10—C4 | 121.9 (6) | C21—C20—H20A | 109.3 |
C5—C10—C9 | 119.4 (6) | C19—C20—H20B | 109.3 |
C4—C10—C9 | 118.8 (5) | C21—C20—H20B | 109.3 |
N1—C11—C1 | 110.4 (4) | H20A—C20—H20B | 108.0 |
N1—C11—C12 | 108.2 (4) | C20—C21—H21A | 109.5 |
C1—C11—C12 | 113.6 (4) | C20—C21—H21B | 109.5 |
N1—C11—H11A | 108.1 | H21A—C21—H21B | 109.5 |
C1—C11—H11A | 108.1 | C20—C21—H21C | 109.5 |
C12—C11—H11A | 108.1 | H21A—C21—H21C | 109.5 |
C17—C12—C13 | 117.5 (5) | H21B—C21—H21C | 109.5 |
Experimental details
Crystal data | |
Chemical formula | C21H23NO |
Mr | 305.40 |
Crystal system, space group | Orthorhombic, Pna21 |
Temperature (K) | 293 |
a, b, c (Å) | 10.842 (7), 16.651 (7), 9.787 (6) |
V (Å3) | 1766.9 (17) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.07 |
Crystal size (mm) | 0.30 × 0.25 × 0.15 |
Data collection | |
Diffractometer | Rigaku Mercury2 diffractometer |
Absorption correction | Multi-scan (CrystalClear; Rigaku, 2005) |
Tmin, Tmax | 0.856, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 14129, 3121, 1998 |
Rint | 0.078 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.087, 0.134, 1.02 |
No. of reflections | 3121 |
No. of parameters | 211 |
No. of restraints | 2 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.25, −0.13 |
Computer programs: CrystalClear (Rigaku, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
Acknowledgements
This work was supported by a start-up grant to the author.
References
Lu, J., Xu, X. N., Wang, C. D., He, J. G., Hu, Y. F. & Hu, H. W. (2002). Tetrahedron Lett. 43, 8367–8369. Web of Science CrossRef CAS Google Scholar
Rigaku (2005). CrystalClear. Rigaku Corporation, Tokyo, Japan. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Wang, X. Y., Dong, Y. M., Sun, J. W., Xu, X. N., Li, R. & Hu, Y. F. (2005). J. Org. Chem. 70, 1897–1900. Web of Science CrossRef PubMed CAS Google Scholar
Xu, X. N., Lu, J., Dong, Y. M., Li, R., Ge, Z. M. & Hu, Y. F. (2004). Tetrahedron Asymmetry, 15, 475–479. Web of Science CrossRef CSD CAS Google Scholar
Zhao, H., Li, Y. H., Wang, X. S., Qu, Z. R., Wang, L. Z., Xiong, R. G., Abrahams, B. F. & Xue, Z. L. (2004). Chem. Eur. J. 10, 2386–2390. Web of Science CSD CrossRef PubMed CAS Google Scholar
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Over one hundred years ago, Betti developed a straightforward synthesis involving the condensation of 2-naphthol, ammonia and equivalents of benzaldehyde, followed by the addition of HCl and KOH to yield 1-(a-aminobenzyl)-2-naphthol. This product which possesses an asymmetric carbon center is known as a Betti base (Zhao & Li et al. 2004). Betti-type reaction is an important method to synthesize chiral ligands and by this method many unnatural homochiral amino-phenol compounds have been obtained (Lu et al. 2002; Xu et al. 2004; Wang et al. 2005). Here we report the synthesis and crystal structure of the title compound (Fig. 1), obtained by a three-component condensation reaction of 2-naphthol, benzaldehyde and butan-1-amine under solvent-free condition.
Molecules of the title compound have normal geometric parameters. The bond lengths and angles are within their normal ranges. The rings A (C1–C10) and B (C12–C17) are, of course, planar and the dihedral angle between them is A/B = 78.27 (5). As can be seen from the packing diagram (Fig. 2), the intramolecular O—H···N hydrogen bond seems to be effective in the stabilization of the crystal structure. Dipole–dipole and van der Waals interactions are effective in the molecular packing.