supplementary materials


im2078 scheme

Acta Cryst. (2008). E64, o1725    [ doi:10.1107/S1600536808025026 ]

2-(6-Methyl-2-pyridyl)-1,1-diphenylethanol

W.-J. Gu and B.-X. Wang

Abstract top

The title compound, C20H19NO, was prepared from 2,6-lutidine and benzophenone. There are two symmetry-independent molecules in the asymmetric unit. Each molecule is involved in one intramolecular O-H...N hydrogen bond. In the crystal structure, helical chains are formed along the b axis by weak [pi]-[pi] interactions between neighbouring molecules [centroid-centroid distances between the pyridyl rings of the two independent molecules = 4.041 (3) and 4.051 (3) Å].

Comment top

There is a growing interest in the chemistry of metal-nitrido complexes, particularly those of late transition metals (Dehnicke et al., 2001). 2-(6-Methyl-pyridin-2-yl)-1,1-diphenyl-ethanol has been used as a multianionic chelating (N, O) ligand and coordinated with transition metals and main group elements, such as Ru, Os, Mo, B, Si etc. (Yip et al., 2003; Gibson et al., 2007). It can be prepared from 2,6-lutidine in moderate yield (Koning et al., 2000). During our studies, we obtained single crystals of the title compound report its crystal structure herein.

The crystal structure of title compound, C20H19NO, shows that all the bond lengths and angles have normal values. In an asymmetric unit there are two symmetry independent molecules I and II. Each molecule has one intramolecular O—H···N hydrogen bond (O1—H1A···N1, O2—H2A···N2)(Fig. 1).

Molecule I exhibits two benzene rings A (C2—C7) and B (C8—C13) as well as a pyridine ring C (N1/C15—C19) that are not coplanar with respect to each other. The dihedral angles between rings A and B, B and C, and C and A measure to 82.02 (6)°, 47.06 (6)°, and 85.87 (5)°, respectively.

Molecule II looks pretty much the same as molecule I, but the dihedral angles are significantly different. The angles between rings D(C22—C27) and E(C28—C33), E and F(N2/C35—C39), and F and D are 83.58 (6)°, 85.44 (5)°, and 49.70 (6)°, respectively.

In the crystal packing weak ππ interactions between neighbouring molecules I and II are observed, the distance of g1-g2 being 4.041 (3) and 4.051 (3) Å (g1 is center of mass of N1/C15—C19, g2 is center of mass of N2/C35—C39). Helical chains along the b axis are formed by these interactions (Fig. 2).

The additional weak intermolecular C18—H18···O2iii and C38—H38···O1iv (iii: -x,1 - y,-z; iv: 1 - x,1 - y,-z) hydrogen bonds play part an important role linking the helical chains to form the three-dimensional crystal structure.

Related literature top

For related literature, see: Berg & Holm (1985); Dehnicke et al. (2001); Gibson et al. (2007); Koning et al. (2000); Yip et al. (2003).

Experimental top

2-(6-Methyl-pyridin-2-yl)-1,1-diphenyl-ethanol was prepared from 2,6-lutidine and benzophenone according to a procedure described in the literature (Berg & Holm, 1985, yield: 60%). Colorless crystals were obtained by recrystallization from light petroleum-ethyl acetate(vol. ratio: 5:1) at room temperature.

1H-NMR (CDCl3, 400 MHz): δ = 8.1 (1 H, s, OH), 6.8–7.5 (13 H, 2 Ph + 3H), 3.7 (2 H, s, CH2), 2.5 (3 H, s, CH3).

Refinement top

The H atoms were placed in calculated positions except O—H atoms and included as part of a riding model, with C—H = 0.93–0.97 Å, and with Uequiv values set at 1.2–1.5 Uequiv of the parent atoms. The O—H atoms were located in the Fourier difference map and refined with a given isotropic thermal parameters 1.2 times the Uequiv for the parent atom.

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SMART (Bruker, 2000); data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. A view of the title compound showing the atom-numbering scheme and displacement ellipsoids drawn at 30% probability level. Dashed lines indicate hydrogen bonds and all H atoms except those involved in hydrogen bonding have been omitted for clarity.
[Figure 2] Fig. 2. A view of the helical chain-like structure along the b axis. (i: x,1 + y,z; ii:x,-1 + y,z).
2-(6-Methyl-2-pyridyl)-1,1-diphenylethanol top
Crystal data top
C20H19NOF000 = 1232
Mr = 289.36Dx = 1.208 Mg m3
Monoclinic, P21/cMo Kα radiation
λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 9992 reflections
a = 13.466 (2) Åθ = 2.3–27.7º
b = 8.022 (1) ŵ = 0.07 mm1
c = 30.220 (3) ÅT = 291 (2) K
β = 102.874 (3)ºBloc, colourless
V = 3182.4 (7) Å30.30 × 0.26 × 0.24 mm
Z = 8
Data collection top
Bruker SMART APEX CCD
diffractometer
6247 independent reflections
Radiation source: sealed tube4901 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.039
T = 291(2) Kθmax = 26.0º
φ and ω scansθmin = 1.6º
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
h = 16→16
Tmin = 0.98, Tmax = 0.98k = 9→9
24109 measured reflectionsl = 36→37
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)] = 0.049H atoms treated by a mixture of
independent and constrained refinement
wR(F2) = 0.116  w = 1/[σ2(Fo2) + (0.05P)2 + 0.55P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
6247 reflectionsΔρmax = 0.12 e Å3
405 parametersΔρmin = 0.12 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
C20H19NOV = 3182.4 (7) Å3
Mr = 289.36Z = 8
Monoclinic, P21/cMo Kα
a = 13.466 (2) ŵ = 0.07 mm1
b = 8.022 (1) ÅT = 291 (2) K
c = 30.220 (3) Å0.30 × 0.26 × 0.24 mm
β = 102.874 (3)º
Data collection top
Bruker SMART APEX CCD
diffractometer
6247 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
4901 reflections with I > 2σ(I)
Tmin = 0.98, Tmax = 0.98Rint = 0.039
24109 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.049405 parameters
wR(F2) = 0.116H atoms treated by a mixture of
independent and constrained refinement
S = 1.03Δρmax = 0.12 e Å3
6247 reflectionsΔρmin = 0.12 e Å3
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.

Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane)

7.9264 (0.0081) x + 2.5384 (0.0055) y + 17.9519 (0.0173) z = 7.2409 (0.0023)

* 0.0041 (0.0011) C2 * -0.0032 (0.0012) C3 * 0.0016 (0.0013) C4 * -0.0007 (0.0013) C5 * 0.0017 (0.0013) C6 * -0.0033 (0.0012) C7

Rms deviation of fitted atoms = 0.0027

8.6157 (0.0075) x - 6.1646 (0.0038) y - 4.0922 (0.0231) z = 2.4746 (0.0072)

Angle to previous plane (with approximate e.s.d.) = 82.02 (0.06)

* -0.0038 (0.0011) C8 * 0.0059 (0.0011) C9 * -0.0038 (0.0013) C10 * -0.0004 (0.0014) C11 * 0.0025 (0.0014) C12 * -0.0004 (0.0012) C13

Rms deviation of fitted atoms = 0.0034

- 0.0031 (0.0098) x + 7.0734 (0.0030) y - 13.8930 (0.0198) z = 1.4744 (0.0034)

Angle to previous plane (with approximate e.s.d.) = 47.06 (0.06)

* 0.0019 (0.0011) N1 * 0.0034 (0.0011) C15 * -0.0039 (0.0012) C16 * -0.0005 (0.0014) C17 * 0.0056 (0.0014) C18 * -0.0064 (0.0012) C19

Rms deviation of fitted atoms = 0.0041

7.9264 (0.0081) x + 2.5384 (0.0055) y + 17.9519 (0.0173) z = 7.2409 (0.0023)

Angle to previous plane (with approximate e.s.d.) = 85.87 (0.05)

* 0.0041 (0.0011) C2 * -0.0032 (0.0012) C3 * 0.0016 (0.0013) C4 * -0.0007 (0.0013) C5 * 0.0017 (0.0013) C6 * -0.0033 (0.0012) C7

Rms deviation of fitted atoms = 0.0027

8.6502 (0.0076) x + 6.1357 (0.0039) y - 2.9169 (0.0234) z = 5.1262 (0.0059)

Angle to previous plane (with approximate e.s.d.) = 49.02 (0.07)

* -0.0040 (0.0011) C22 * 0.0029 (0.0013) C23 * -0.0003 (0.0014) C24 * -0.0010 (0.0014) C25 * -0.0002 (0.0013) C26 * 0.0028 (0.0012) C27

Rms deviation of fitted atoms = 0.0024

- 8.0302 (0.0080) x + 2.4726 (0.0054) y + 25.8511 (0.0117) z = 4.4687 (0.0039)

Angle to previous plane (with approximate e.s.d.) = 83.58 (0.06)

* 0.0063 (0.0011) C28 * -0.0023 (0.0012) C29 * -0.0051 (0.0013) C30 * 0.0085 (0.0014) C31 * -0.0043 (0.0013) C32 * -0.0032 (0.0012) C33

Rms deviation of fitted atoms = 0.0053

- 0.0603 (0.0094) x + 7.0521 (0.0030) y - 14.0087 (0.0195) z = 4.9759 (0.0037)

Angle to previous plane (with approximate e.s.d.) = 85.44 (0.05)

* -0.0024 (0.0011) N2 * 0.0054 (0.0011) C35 * -0.0025 (0.0012) C36 * -0.0031 (0.0013) C37 * 0.0060 (0.0013) C38 * -0.0034 (0.0012) C39

Rms deviation of fitted atoms = 0.0040

8.6502 (0.0076) x + 6.1357 (0.0039) y - 2.9169 (0.0234) z = 5.1262 (0.0059)

Angle to previous plane (with approximate e.s.d.) = 49.70 (0.06)

* -0.0040 (0.0011) C22 * 0.0029 (0.0013) C23 * -0.0003 (0.0014) C24 * -0.0010 (0.0014) C25 * -0.0002 (0.0013) C26 * 0.0028 (0.0012) C27

Rms deviation of fitted atoms = 0.0024

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
C10.55525 (11)0.30363 (18)0.12015 (5)0.0333 (3)
C20.52945 (10)0.15683 (18)0.14763 (5)0.0333 (3)
C30.46070 (12)0.1698 (2)0.17575 (5)0.0432 (4)
H30.42570.26920.17670.052*
C40.44374 (14)0.0364 (3)0.20236 (6)0.0552 (5)
H40.39810.04740.22120.066*
C50.49408 (16)0.1119 (3)0.20098 (7)0.0631 (5)
H50.48230.20140.21870.076*
C60.56142 (15)0.1273 (2)0.17356 (7)0.0606 (5)
H60.59590.22740.17280.073*
C70.57882 (12)0.0055 (2)0.14681 (6)0.0458 (4)
H70.62440.00720.12800.055*
C80.64575 (11)0.40377 (18)0.14754 (5)0.0364 (3)
C90.67094 (12)0.4062 (2)0.19461 (6)0.0428 (4)
H90.63390.34160.21080.051*
C100.75135 (13)0.5046 (2)0.21792 (7)0.0546 (5)
H100.76650.50630.24950.065*
C110.80791 (14)0.5984 (2)0.19495 (8)0.0640 (6)
H110.86160.66300.21070.077*
C120.78427 (14)0.5961 (3)0.14796 (9)0.0674 (6)
H120.82240.65930.13200.081*
C130.70373 (13)0.4996 (2)0.12451 (7)0.0517 (4)
H130.68850.49920.09290.062*
C140.46541 (11)0.42749 (19)0.10506 (5)0.0381 (3)
H14A0.44630.47080.13200.046*
H14B0.48890.52070.08970.046*
C150.37153 (11)0.35434 (19)0.07395 (5)0.0395 (3)
C160.27485 (13)0.3698 (2)0.08237 (6)0.0511 (4)
H160.26490.42060.10870.061*
C170.19352 (14)0.3071 (3)0.05024 (8)0.0628 (5)
H170.12770.31580.05480.075*
C180.20984 (15)0.2327 (3)0.01190 (7)0.0642 (5)
H180.15520.19170.00980.077*
C190.30793 (15)0.2184 (2)0.00548 (6)0.0542 (5)
C200.3320 (2)0.1393 (3)0.03588 (7)0.0780 (7)
H20A0.36010.22150.05270.117*
H20B0.27080.09440.05460.117*
H20C0.38060.05120.02680.117*
C210.06735 (10)0.80270 (18)0.12103 (5)0.0333 (3)
C220.00363 (11)0.90017 (18)0.14826 (5)0.0356 (3)
C230.07527 (13)1.0013 (2)0.12473 (7)0.0519 (4)
H230.08841.00600.09320.062*
C240.13383 (15)1.0943 (3)0.14768 (9)0.0668 (6)
H240.18631.16040.13160.080*
C250.11486 (15)1.0896 (3)0.19424 (8)0.0659 (6)
H250.15441.15240.20970.079*
C260.03709 (15)0.9914 (3)0.21801 (7)0.0578 (5)
H260.02410.98790.24950.069*
C270.02182 (12)0.8979 (2)0.19507 (6)0.0424 (4)
H270.07440.83260.21140.051*
C280.12469 (11)0.65852 (18)0.14885 (5)0.0350 (3)
C290.07775 (13)0.5045 (2)0.14868 (6)0.0471 (4)
H290.01350.48760.13020.057*
C300.12589 (15)0.3745 (2)0.17595 (7)0.0566 (5)
H300.09390.27160.17540.068*
C310.22188 (17)0.3991 (3)0.20394 (7)0.0643 (6)
H310.25330.31320.22260.077*
C320.26986 (14)0.5481 (3)0.20410 (6)0.0576 (5)
H320.33460.56330.22240.069*
C330.22213 (12)0.6781 (2)0.17688 (6)0.0453 (4)
H330.25550.77980.17730.054*
C340.14015 (11)0.92662 (19)0.10486 (5)0.0382 (3)
H34A0.10011.01870.08950.046*
H34B0.18680.97160.13130.046*
C350.20135 (12)0.85435 (19)0.07364 (5)0.0396 (3)
C360.30642 (13)0.8702 (2)0.08174 (6)0.0502 (4)
H360.34280.92190.10790.060*
C370.35558 (15)0.8070 (3)0.04974 (7)0.0596 (5)
H370.42600.81550.05420.072*
C380.29968 (16)0.7313 (3)0.01125 (7)0.0600 (5)
H380.33200.68990.01060.072*
C390.19560 (14)0.7175 (2)0.00542 (6)0.0482 (4)
C400.12872 (14)0.6369 (3)0.03596 (6)0.0563 (5)
H40A0.08930.54960.02650.084*
H40B0.17070.59090.05480.084*
H40C0.08380.71900.05280.084*
N10.38751 (11)0.28000 (18)0.03621 (5)0.0465 (3)
N20.14697 (11)0.77822 (18)0.03610 (4)0.0443 (3)
O10.58575 (9)0.24349 (15)0.08070 (4)0.0458 (3)
H1A0.5263 (15)0.224 (2)0.0571 (7)0.055*
O20.00304 (8)0.73711 (15)0.08224 (4)0.0461 (3)
H2A0.0333 (14)0.704 (2)0.0597 (7)0.055*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0323 (7)0.0332 (8)0.0356 (8)0.0010 (6)0.0103 (6)0.0029 (6)
C20.0291 (7)0.0338 (8)0.0351 (7)0.0038 (6)0.0027 (6)0.0047 (6)
C30.0417 (8)0.0466 (9)0.0436 (9)0.0030 (7)0.0146 (7)0.0015 (7)
C40.0530 (10)0.0646 (12)0.0495 (10)0.0135 (9)0.0148 (8)0.0080 (9)
C50.0647 (12)0.0560 (12)0.0610 (12)0.0183 (10)0.0023 (10)0.0204 (9)
C60.0569 (11)0.0378 (10)0.0798 (14)0.0043 (8)0.0008 (10)0.0102 (9)
C70.0401 (8)0.0391 (9)0.0561 (10)0.0027 (7)0.0065 (7)0.0017 (8)
C80.0307 (7)0.0302 (8)0.0489 (9)0.0009 (6)0.0102 (6)0.0020 (6)
C90.0385 (8)0.0392 (9)0.0494 (9)0.0045 (7)0.0068 (7)0.0033 (7)
C100.0436 (9)0.0513 (11)0.0611 (11)0.0020 (8)0.0049 (8)0.0105 (9)
C110.0385 (9)0.0465 (11)0.0987 (17)0.0098 (8)0.0023 (10)0.0058 (11)
C120.0469 (10)0.0524 (12)0.1050 (18)0.0139 (9)0.0211 (11)0.0117 (11)
C130.0443 (9)0.0479 (10)0.0662 (11)0.0051 (8)0.0193 (8)0.0040 (9)
C140.0393 (8)0.0325 (8)0.0418 (8)0.0032 (6)0.0075 (6)0.0001 (6)
C150.0403 (8)0.0361 (8)0.0392 (8)0.0003 (7)0.0028 (6)0.0067 (7)
C160.0428 (9)0.0538 (11)0.0550 (11)0.0043 (8)0.0069 (8)0.0088 (8)
C170.0388 (9)0.0658 (13)0.0780 (14)0.0004 (9)0.0004 (9)0.0173 (11)
C180.0563 (12)0.0600 (12)0.0630 (13)0.0040 (9)0.0149 (10)0.0084 (10)
C190.0618 (11)0.0499 (10)0.0410 (9)0.0058 (8)0.0094 (8)0.0105 (8)
C200.0978 (17)0.0816 (16)0.0469 (11)0.0147 (13)0.0000 (11)0.0097 (11)
C210.0297 (7)0.0333 (8)0.0354 (8)0.0033 (6)0.0039 (6)0.0029 (6)
C220.0314 (7)0.0322 (8)0.0436 (8)0.0046 (6)0.0089 (6)0.0031 (6)
C230.0426 (9)0.0504 (10)0.0614 (11)0.0094 (8)0.0088 (8)0.0026 (9)
C240.0529 (11)0.0522 (11)0.0984 (17)0.0163 (9)0.0234 (11)0.0044 (11)
C250.0562 (11)0.0584 (12)0.0924 (16)0.0027 (10)0.0364 (11)0.0182 (11)
C260.0574 (11)0.0637 (12)0.0583 (11)0.0056 (9)0.0255 (9)0.0131 (10)
C270.0399 (8)0.0429 (9)0.0448 (9)0.0023 (7)0.0107 (7)0.0035 (7)
C280.0368 (7)0.0336 (8)0.0365 (8)0.0025 (6)0.0126 (6)0.0010 (6)
C290.0468 (9)0.0380 (9)0.0607 (11)0.0035 (7)0.0208 (8)0.0030 (8)
C300.0602 (11)0.0348 (9)0.0875 (14)0.0008 (8)0.0433 (11)0.0106 (9)
C310.0749 (13)0.0558 (12)0.0683 (13)0.0251 (10)0.0294 (11)0.0240 (10)
C320.0510 (10)0.0640 (12)0.0543 (11)0.0131 (9)0.0043 (8)0.0124 (9)
C330.0422 (9)0.0409 (9)0.0497 (10)0.0003 (7)0.0039 (7)0.0012 (7)
C340.0397 (8)0.0325 (8)0.0428 (8)0.0022 (6)0.0100 (6)0.0030 (6)
C350.0454 (8)0.0351 (8)0.0398 (8)0.0023 (7)0.0129 (7)0.0083 (7)
C360.0449 (9)0.0533 (10)0.0542 (10)0.0025 (8)0.0150 (8)0.0075 (8)
C370.0516 (10)0.0627 (12)0.0719 (13)0.0062 (9)0.0295 (10)0.0160 (10)
C380.0701 (13)0.0600 (12)0.0604 (12)0.0077 (10)0.0368 (10)0.0079 (10)
C390.0636 (11)0.0471 (10)0.0393 (9)0.0075 (8)0.0228 (8)0.0078 (7)
C400.0629 (11)0.0618 (12)0.0479 (10)0.0086 (9)0.0201 (9)0.0079 (9)
N10.0483 (8)0.0476 (8)0.0400 (8)0.0026 (6)0.0021 (6)0.0045 (6)
N20.0500 (8)0.0452 (8)0.0385 (7)0.0026 (6)0.0118 (6)0.0039 (6)
O10.0480 (6)0.0527 (7)0.0404 (6)0.0015 (5)0.0181 (5)0.0076 (5)
O20.0388 (6)0.0544 (7)0.0406 (6)0.0086 (5)0.0007 (5)0.0098 (5)
Geometric parameters (Å, °) top
C1—O11.4286 (17)C21—C221.529 (2)
C1—C21.525 (2)C21—C281.533 (2)
C1—C81.538 (2)C21—C341.550 (2)
C1—C141.553 (2)C22—C271.381 (2)
C2—C71.387 (2)C22—C231.399 (2)
C2—C31.393 (2)C23—C241.379 (3)
C3—C41.388 (2)C23—H230.9300
C3—H30.9300C24—C251.373 (3)
C4—C51.375 (3)C24—H240.9300
C4—H40.9300C25—C261.378 (3)
C5—C61.363 (3)C25—H250.9300
C5—H50.9300C26—C271.385 (2)
C6—C71.389 (3)C26—H260.9300
C6—H60.9300C27—H270.9300
C7—H70.9300C28—C291.387 (2)
C8—C91.387 (2)C28—C331.403 (2)
C8—C131.388 (2)C29—C301.396 (3)
C9—C101.398 (2)C29—H290.9300
C9—H90.9300C30—C311.392 (3)
C10—C111.365 (3)C30—H300.9300
C10—H100.9300C31—C321.358 (3)
C11—C121.384 (3)C31—H310.9300
C11—H110.9300C32—C331.394 (2)
C12—C131.391 (3)C32—H320.9300
C12—H120.9300C33—H330.9300
C13—H130.9300C34—C351.501 (2)
C14—C151.515 (2)C34—H34A0.9700
C14—H14A0.9700C34—H34B0.9700
C14—H14B0.9700C35—N21.351 (2)
C15—N11.346 (2)C35—C361.387 (2)
C15—C161.387 (2)C36—C371.384 (3)
C16—C171.386 (3)C36—H360.9300
C16—H160.9300C37—C381.377 (3)
C17—C181.364 (3)C37—H370.9300
C17—H170.9300C38—C391.377 (3)
C18—C191.382 (3)C38—H380.9300
C18—H180.9300C39—N21.340 (2)
C19—N11.346 (2)C39—C401.514 (3)
C19—C201.500 (3)C40—H40A0.9600
C20—H20A0.9600C40—H40B0.9600
C20—H20B0.9600C40—H40C0.9600
C20—H20C0.9600O1—H1A0.96 (2)
C21—O21.4334 (17)O2—H2A0.96 (2)
O1—C1—C2109.66 (11)C22—C21—C28111.41 (12)
O1—C1—C8106.55 (11)O2—C21—C34109.08 (12)
C2—C1—C8111.07 (12)C22—C21—C34108.18 (11)
O1—C1—C14108.72 (12)C28—C21—C34112.34 (12)
C2—C1—C14113.37 (12)C27—C22—C23118.02 (15)
C8—C1—C14107.20 (12)C27—C22—C21123.47 (14)
C7—C2—C3117.55 (15)C23—C22—C21118.48 (14)
C7—C2—C1119.86 (13)C24—C23—C22120.83 (18)
C3—C2—C1122.52 (14)C24—C23—H23119.6
C4—C3—C2120.90 (16)C22—C23—H23119.6
C4—C3—H3119.5C25—C24—C23120.24 (19)
C2—C3—H3119.5C25—C24—H24119.9
C5—C4—C3120.25 (17)C23—C24—H24119.9
C5—C4—H4119.9C24—C25—C26119.75 (17)
C3—C4—H4119.9C24—C25—H25120.1
C6—C5—C4119.74 (17)C26—C25—H25120.1
C6—C5—H5120.1C25—C26—C27120.15 (19)
C4—C5—H5120.1C25—C26—H26119.9
C5—C6—C7120.37 (18)C27—C26—H26119.9
C5—C6—H6119.8C22—C27—C26121.00 (16)
C7—C6—H6119.8C22—C27—H27119.5
C2—C7—C6121.17 (16)C26—C27—H27119.5
C2—C7—H7119.4C29—C28—C33117.78 (15)
C6—C7—H7119.4C29—C28—C21119.76 (14)
C9—C8—C13118.06 (15)C33—C28—C21122.37 (13)
C9—C8—C1122.85 (13)C28—C29—C30120.78 (17)
C13—C8—C1119.07 (14)C28—C29—H29119.6
C8—C9—C10120.65 (16)C30—C29—H29119.6
C8—C9—H9119.7C31—C30—C29119.95 (17)
C10—C9—H9119.7C31—C30—H30120.0
C11—C10—C9120.83 (19)C29—C30—H30120.0
C11—C10—H10119.6C32—C31—C30120.22 (17)
C9—C10—H10119.6C32—C31—H31119.9
C10—C11—C12119.17 (17)C30—C31—H31119.9
C10—C11—H11120.4C31—C32—C33120.01 (18)
C12—C11—H11120.4C31—C32—H32120.0
C11—C12—C13120.33 (18)C33—C32—H32120.0
C11—C12—H12119.8C32—C33—C28121.25 (16)
C13—C12—H12119.8C32—C33—H33119.4
C8—C13—C12120.95 (18)C28—C33—H33119.4
C8—C13—H13119.5C35—C34—C21115.16 (12)
C12—C13—H13119.5C35—C34—H34A108.5
C15—C14—C1114.95 (12)C21—C34—H34A108.5
C15—C14—H14A108.5C35—C34—H34B108.5
C1—C14—H14A108.5C21—C34—H34B108.5
C15—C14—H14B108.5H34A—C34—H34B107.5
C1—C14—H14B108.5N2—C35—C36122.03 (15)
H14A—C14—H14B107.5N2—C35—C34115.57 (13)
N1—C15—C16121.93 (15)C36—C35—C34122.35 (15)
N1—C15—C14115.37 (13)C37—C36—C35118.10 (18)
C16—C15—C14122.62 (15)C37—C36—H36121.0
C17—C16—C15117.81 (18)C35—C36—H36121.0
C17—C16—H16121.1C38—C37—C36119.67 (18)
C15—C16—H16121.1C38—C37—H37120.2
C18—C17—C16120.15 (19)C36—C37—H37120.2
C18—C17—H17119.9C37—C38—C39119.50 (17)
C16—C17—H17119.9C37—C38—H38120.2
C17—C18—C19119.70 (18)C39—C38—H38120.2
C17—C18—H18120.2N2—C39—C38121.49 (18)
C19—C18—H18120.2N2—C39—C40115.73 (16)
N1—C19—C18120.77 (18)C38—C39—C40122.77 (16)
N1—C19—C20116.34 (18)C39—C40—H40A109.5
C18—C19—C20122.87 (18)C39—C40—H40B109.5
C19—C20—H20A109.5H40A—C40—H40B109.5
C19—C20—H20B109.5C39—C40—H40C109.5
H20A—C20—H20B109.5H40A—C40—H40C109.5
C19—C20—H20C109.5H40B—C40—H40C109.5
H20A—C20—H20C109.5C19—N1—C15119.63 (16)
H20B—C20—H20C109.5C39—N2—C35119.21 (15)
O2—C21—C22106.24 (11)C1—O1—H1A109.3 (11)
O2—C21—C28109.39 (12)C21—O2—H2A109.5 (11)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O1—H1A···N10.96 (2)1.89 (2)2.724 (2)144 (2)
O2—H2A···N20.96 (2)1.92 (2)2.718 (2)139 (2)
C18—H18···O2i0.932.703.518 (2)147
C38—H38···O1ii0.932.653.472 (2)147
Symmetry codes: (i) −x, −y+1, −z; (ii) −x+1, −y+1, −z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O1—H1A···N10.96 (2)1.89 (2)2.724 (2)144 (2)
O2—H2A···N20.96 (2)1.92 (2)2.718 (2)139 (2)
C18—H18···O2i0.932.703.518 (2)147
C38—H38···O1ii0.932.653.472 (2)147
Symmetry codes: (i) −x, −y+1, −z; (ii) −x+1, −y+1, −z.
Acknowledgements top

We thank the Natural Science Foundation of the Jiangsu Higher Education Institutions of China (grant No. 07KJD150101) for financial support.

references
References top

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