(6S)-2-tert-Butyl-6-[(4S,5R)-3,4-di­methyl-5-phenyloxazolidin-2-yl]phenol

The title compound, C₂₁H₂₇NO₂, exhibits hydrogen bonding between the phenolic H atom and the heterocyclic N atom. The absolute configuration of the mol­ecule is known from the synthetic procedure.

Related literature

For related structures and background to the use of chiral oxazolidines as templates in asymmetric synthesis, see: Agami & Couty (2004); Campbell et al. (2010); Koyanagi et al. (2010); Parrott & Hitchcock (2007); Parrott et al. (2008). The synthesis of the title compound is described by Parrott & Hitchcock (2007). The absolute configuration assignment is based on both optical activity measurements and on the known stereochemistry of the commercially obtained optically pure ephedrine from which it was prepared (Parrott & Hitchcock, 2007). For geometry checks using Mogul, see: Bruno et al. (2004). For ring puckering analysis, see: Boeyens (1978); Cremer & Pople (1975); Spek (2009). For a description of the Jmol toolkit for the preparation of enhanced figures, see: McMahon & Hanson (2008).

Experimental

Crystal data

• C₂₁H₂₇NO₂

• M_r = 325.44

• Monoclinic, P 2₁

• a = 8.3288 (8) Å

• b = 9.8657 (9) Å

• c = 11.4325 (11) Å

• β = 91.667 (1)°

• V = 939.00 (15) ų

• Z = 2

• Mo Kα radiation

• μ = 0.07 mm⁻¹

• T = 140 K

• 0.55 × 0.27 × 0.27 mm

Data collection

• Bruker SMART APEX CCD diffractometer

• Absorption correction: multi-scan (APEX2; Bruker, 2008) T_min = 0.687, T_max = 0.746

• 9040 measured reflections

• 2284 independent reflections

• 2191 reflections with I > 2σ(I)

• R_int = 0.017

Refinement

• R[F² > 2σ(F²)] = 0.028

• wR(F²) = 0.074

• S = 1.04

• 2284 reflections

• 221 parameters

• 1 restraint

• H atoms treated by a mixture of independent and constrained refinement

• Δρ_max = 0.21 e Å⁻³

• Δρ_min = −0.14 e Å⁻³

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
O20—H20⋯N3	0.90 (2)	1.79 (2)	2.6244 (16)	154.4 (19)

Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT; program(s) used to solve structure: SIR2004 (Burla et al., 2005); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999), publCIF (McMahon & Westrip, 2008) and Mercury (Macrae et al., 2008).

Supporting information

S1. Comment

Chiral oxazolidines are useful templates for conducting asymmetric syntheses (Agami & Couty, 2004). In order to explore the utility of these compounds in the catalytic asymmetric addition of diethylzinc to aldehydes, we prepared a series of oxazolidines from (1R,2S)-ephedrine, (1S,2S)-pseudoephedrine (Parrott & Hitchcock, 2007) and (1R,2S)-norephedrine (Parrott et al., 2008). In the course of synthesizing these oxazolidines, we were able to obtain crystals suitable for X-ray crystallographic analysis.

The title compound is structurally similar to two other oxazolidines published by Koyanagi et al. (2010) and Campbell et al. (2010). Despite these structural similarities, a Mogul geometry check (Bruno et al., 2004) reveals differences between the three structures. The C2—N3—C4 angle is found to be usual in the title compound (103.0 (1)°) and in Koyanagi et al. (106.0 (1)°), but not in Campbell et al. (106.2 (1)°), even though the last two angles are not significantly different. Another angle, C5—O1—C2, considered unusual in Mogul for both Koyanagi et al. and Campbell et al. (103.9 (1)° and 103.3 (1)°, respectively) is not unusual in the title compound (108.9 (1)°). These differences could be due to the difference in substituents on the N3 position in these compounds. The methyl substituent in the title compound occupies less space than the isopropyl substituent in the other two structures, allowing for more typical bond angles in the heterocycle of the title compound.

The difference in bond angles also appears in PLATON in the ring-puckering analysis of these compounds (Spek, 2009; Cremer & Pople, 1975; Boeyens, 1978). Koyanagi et al. and Campbell et al. report O1—C2—N3—C4—C5 ring conformations close to ¹E (Φ = 1.63 (17)° and -7.05 (19)°, respectively), with O1 as the flap apex, while the heterocycle conformation of the title compound is closer to an ³E conformation (Φ = 65.73 (20)°), resulting in N3 as the flap apex. Even with these differences, the distance between the hydrogen donor and acceptor in all three structures is virtually identical (2.6244 Å in the title compound compared to 2.6278 (16) Å and 2.6180 (17) Å in Koyanagi et al. and Campbell et al., respectively).

About the Jmol enhanced figure:

We are reporting three related structures containing Jmol enhanced figures, one in this paper and the other two in other papers in this Journal (Campbell et al., 2010; Koyanagi et al., 2010). The Jmol enhanced figures were created to illustrate a range of author convenience versus end user experience, ranging from a purely GUI driven experience for the author resulting in a less functional figure for the end user to a more sophisticated use of the Jmol scripting by the author resulting in a more polished and versatile figure for the end user. The buttons, check boxes and radio buttons in the three examples visually appear to be identical; however, the underlying code they execute results in significantly different overall responses by the Jmol visualizer.

The Jmol enhanced figure included with this paper required substantial author hand-coding of Jmol scripts. To generate this enhanced figure, substantial author familiarity with Jmol script coding is required and generation of the figure is significantly more time-consuming. Strictly authoring with the Jmol toolkit GUI, without text editing any code, provides a relatively quick and easy means to prepare a decent enhanced figure, and is often sufficient. For advanced users, hand-coding Jmol scripts provides a much more versatile figure for the end-user. In particular, the orientation information of the structure can be eliminated from all radio buttons, buttons, and check boxes. This becomes a major advantage when the end-user toggles the figure to rotate or changes the orientation from the location dictated in the script. When a new option is selected, the figure will only change in the areas being highlighted. Another advantage of stripping the script of lines not related to the defined option is the ability to see more than one option at a time. For instance, in this enhanced figure, the thermal ellipse color may be viewed even when the atom style is not in the ellipse mode.

Related literature

For related structures and background to the use of chiral oxazolidines as templates in asymmetric synthesis, see: Agami & Couty (2004); Campbell et al. (2010); Koyanagi et al. (2010); Parrott & Hitchcock (2007); Parrott et al. (2008). The synthesis of the title compound is described by Parrott & Hitchcock (2007). The absolute configuration assignment is based on both optical activity measurements and on the known stereochemistry of the commercially obtained optically pure ephedrine from which it was prepared (Parrott & Hitchcock, 2007). For geometry checks using Mogul, see: Bruno et al. (2004). For ring puckering analysis, see: Boeyens (1978); Cremer & Pople (1975); Spek (2009). For a description of the Jmol toolkit for the preparation of enhanced figures, see: McMahon & Hanson (2008).

S2. Experimental

The title compound was synthesized as previously reported (Parrott & Hitchcock, 2007). Single crystals were grown by vapor diffusion of hexane into a methylene chloride solution of the title compound.

S3. Refinement

All non-H atoms were refined anisotropically without disorder. The absolute configuration assignment is based on both optical activity measurements and on the known stereochemistry of the commercially obtained optically pure ephedrine from which it was prepared (Parrott & Hitchcock, 2007). All H atoms were initially identified through difference Fourier syntheses and then, except for the O–H hydrogen atom, removed and included in the refinement in the riding-model approximation (C–H = 0.95, 0.98, and 1.00 Å for Ar–H, CH₃ and CH; U_iso(H) = 1.2U_eq(C) except for methyl groups, where U_iso(H) = 1.5U_eq(C)). The OH H atom was freely refined isotropically. In the absence of significant anomalous scattering effects, Friedel pairs were merged.

Computing details

Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT (Bruker, 2008); program(s) used to solve structure: SIR2004 (Burla et al., 2005); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999), publCIF (McMahon & Westrip, 2008) and Mercury (Macrae et al., 2008).

Figures

Fig. 1. The molecular structure of the title compound with the atomic numbering scheme. The intramolecular H-bonding is denoted by the dashed line and the ^3E heterocycle conformation is shown. Displacement ellipsoids are drawn at the 50% probability level and H-atoms are shown as spheres of arbitrary size.

Fig. 2. The enhanced Jmol figure of the title compound. This is the third in a series of three Jmol figures intended to illustrate some versatility of the program. See also: Campbell et al. (2010); Koyanagi et al. (2010). In this Jmol, all interactive features are defined by text editing or hand writing the scripts. Most script artifacts are resolved by using this method and the orientation of the molecule only depends upon the end-user's preference.

(6S)-2-tert-Butyl-6-[(4S/i>,5R)-3,4-dimethyl- 5-phenyloxazolidin-2-yl]phenol

Crystal data

C21H27NO2	F(000) = 352
Mr = 325.44	Dx = 1.151 Mg m^−3
Monoclinic, P21	Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2yb	Cell parameters from 5731 reflections
a = 8.3288 (8) Å	θ = 2.5–3.4°
b = 9.8657 (9) Å	µ = 0.07 mm^−1
c = 11.4325 (11) Å	T = 140 K
β = 91.667 (1)°	Rod, colourless
V = 939.00 (15) Å^3	0.55 × 0.27 × 0.27 mm
Z = 2

Data collection

Bruker SMART APEX CCD diffractometer	2191 reflections with I > 2σ(I)
Graphite monochromator	Rint = 0.017
ω scans	θmax = 27.5°, θmin = 1.8°
Absorption correction: multi-scan (APEX2; Bruker, 2008)	h = −10→10
Tmin = 0.687, Tmax = 0.746	k = −12→12
9040 measured reflections	l = −14→14
2284 independent reflections

Refinement

Refinement on F^2	Primary atom site location: structure-invariant direct methods
Least-squares matrix: full	Secondary atom site location: difference Fourier map
R[F^2 > 2σ(F^2)] = 0.028	Hydrogen site location: inferred from neighbouring sites
wR(F^2) = 0.074	H atoms treated by a mixture of independent and constrained refinement
S = 1.04	w = 1/[σ^2(Fo^2) + (0.0485P)^2 + 0.090P] where P = (Fo^2 + 2Fc^2)/3
2284 reflections	(Δ/σ)max < 0.001
221 parameters	Δρmax = 0.21 e Å^−3
1 restraint	Δρmin = −0.14 e Å^−3

Special details

Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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 (Ų)

	x	y	z	Uiso*/Ueq
O1	0.99692 (12)	0.27815 (11)	0.41600 (9)	0.0248 (2)
O20	0.65433 (12)	0.17836 (11)	0.28853 (9)	0.0213 (2)
N3	0.79655 (14)	0.40974 (12)	0.33736 (10)	0.0202 (2)
C16	0.75996 (15)	0.03243 (13)	0.14241 (11)	0.0174 (3)
C14	0.91785 (16)	0.22492 (14)	0.21866 (11)	0.0185 (3)
C19	1.04036 (16)	0.19395 (15)	0.14295 (12)	0.0204 (3)
H19	1.1354	0.2472	0.1438	0.025*
C2	0.94417 (16)	0.33629 (15)	0.30751 (12)	0.0210 (3)
H2	1.0265	0.4016	0.2795	0.025*
C6	0.87041 (16)	0.27789 (16)	0.60254 (12)	0.0233 (3)
C15	0.77689 (15)	0.14637 (14)	0.21694 (11)	0.0177 (3)
C4	0.84147 (17)	0.47509 (15)	0.45020 (13)	0.0241 (3)
H4	0.9104	0.5556	0.4342	0.029*
C21	0.61341 (16)	−0.06087 (14)	0.14940 (12)	0.0189 (3)
C23	0.60832 (17)	−0.12120 (14)	0.27378 (12)	0.0221 (3)
H23A	0.515	−0.1811	0.2791	0.033*
H23B	0.6	−0.0477	0.3309	0.033*
H23C	0.7067	−0.1731	0.2903	0.033*
C8	0.71138 (18)	0.08617 (17)	0.66066 (14)	0.0280 (3)
H8	0.6469	0.0099	0.6402	0.034*
C22	0.62164 (19)	−0.17981 (16)	0.06338 (13)	0.0273 (3)
H22A	0.526	−0.2368	0.0706	0.041*
H22B	0.718	−0.2338	0.0813	0.041*
H22C	0.6261	−0.1448	−0.0167	0.041*
C17	0.88590 (16)	0.00653 (14)	0.06749 (11)	0.0199 (3)
H17	0.8768	−0.0681	0.0152	0.024*
C13	0.7473 (2)	0.50590 (16)	0.24528 (14)	0.0285 (3)
H13A	0.6492	0.5527	0.2679	0.043*
H13B	0.7267	0.4568	0.1718	0.043*
H13C	0.833	0.5724	0.2345	0.043*
C9	0.74020 (19)	0.11793 (18)	0.77790 (14)	0.0316 (4)
H9	0.6968	0.0629	0.8374	0.038*
C5	0.94712 (16)	0.36461 (16)	0.51019 (12)	0.0242 (3)
H5	1.0446	0.4091	0.546	0.029*
C18	1.02423 (16)	0.08575 (15)	0.06636 (12)	0.0215 (3)
H18	1.1069	0.0657	0.0135	0.026*
C11	0.89769 (18)	0.30989 (18)	0.72035 (13)	0.0284 (3)
H11	0.9612	0.3866	0.7412	0.034*
C24	0.45695 (17)	0.01669 (16)	0.11992 (14)	0.0257 (3)
H24A	0.3653	−0.0452	0.1249	0.039*
H24B	0.4612	0.0534	0.0404	0.039*
H24C	0.4447	0.0912	0.1757	0.039*
C10	0.8326 (2)	0.23041 (19)	0.80740 (14)	0.0323 (4)
H10	0.8516	0.2532	0.8874	0.039*
C12	0.69710 (19)	0.52203 (17)	0.51714 (14)	0.0301 (3)
H12A	0.6389	0.5915	0.4717	0.045*
H12B	0.7333	0.5601	0.5926	0.045*
H12C	0.6259	0.4448	0.5304	0.045*
C7	0.77616 (17)	0.16510 (16)	0.57324 (13)	0.0244 (3)
H7	0.7564	0.1424	0.4934	0.029*
H20	0.680 (2)	0.258 (3)	0.3212 (18)	0.040 (5)*

Atomic displacement parameters (Ų)

	U^11	U^22	U^33	U^12	U^13	U^23
O1	0.0234 (5)	0.0272 (5)	0.0237 (5)	0.0053 (4)	−0.0006 (4)	−0.0053 (4)
O20	0.0187 (4)	0.0178 (5)	0.0278 (5)	−0.0037 (4)	0.0079 (4)	−0.0053 (4)
N3	0.0219 (5)	0.0147 (5)	0.0239 (6)	−0.0007 (4)	0.0028 (4)	−0.0002 (4)
C16	0.0189 (6)	0.0150 (6)	0.0183 (6)	0.0009 (5)	−0.0004 (5)	0.0027 (5)
C14	0.0196 (6)	0.0160 (6)	0.0201 (6)	−0.0004 (5)	0.0022 (5)	0.0015 (5)
C19	0.0175 (6)	0.0212 (7)	0.0227 (6)	−0.0013 (5)	0.0028 (5)	0.0050 (5)
C2	0.0182 (6)	0.0191 (6)	0.0259 (7)	−0.0040 (5)	0.0032 (5)	−0.0010 (5)
C6	0.0200 (6)	0.0257 (7)	0.0242 (7)	0.0065 (6)	−0.0015 (5)	−0.0031 (6)
C15	0.0181 (6)	0.0156 (6)	0.0195 (6)	0.0014 (5)	0.0031 (5)	0.0016 (5)
C4	0.0251 (7)	0.0172 (6)	0.0303 (7)	−0.0042 (5)	0.0023 (5)	−0.0051 (5)
C21	0.0204 (6)	0.0154 (6)	0.0210 (6)	−0.0019 (5)	0.0015 (5)	0.0003 (5)
C23	0.0251 (7)	0.0179 (7)	0.0236 (7)	−0.0022 (5)	0.0037 (5)	0.0032 (5)
C8	0.0248 (7)	0.0253 (7)	0.0338 (8)	0.0065 (6)	−0.0008 (6)	0.0030 (6)
C22	0.0336 (8)	0.0199 (7)	0.0286 (7)	−0.0052 (6)	0.0033 (6)	−0.0057 (6)
C17	0.0253 (6)	0.0176 (6)	0.0168 (6)	0.0032 (5)	0.0003 (5)	0.0014 (5)
C13	0.0336 (8)	0.0194 (7)	0.0328 (8)	0.0022 (6)	0.0040 (6)	0.0046 (6)
C9	0.0305 (8)	0.0345 (9)	0.0298 (7)	0.0155 (7)	0.0038 (6)	0.0080 (7)
C5	0.0196 (6)	0.0255 (7)	0.0275 (7)	−0.0007 (6)	−0.0011 (5)	−0.0086 (6)
C18	0.0205 (6)	0.0256 (7)	0.0186 (6)	0.0047 (6)	0.0058 (5)	0.0033 (5)
C11	0.0265 (7)	0.0315 (8)	0.0267 (7)	0.0098 (6)	−0.0050 (5)	−0.0075 (6)
C24	0.0216 (7)	0.0204 (7)	0.0349 (8)	−0.0012 (6)	−0.0027 (5)	0.0016 (6)
C10	0.0349 (8)	0.0378 (9)	0.0238 (7)	0.0176 (7)	−0.0036 (6)	−0.0032 (7)
C12	0.0319 (8)	0.0247 (7)	0.0339 (8)	0.0047 (6)	0.0043 (6)	−0.0062 (7)
C7	0.0230 (7)	0.0253 (7)	0.0248 (7)	0.0042 (6)	−0.0016 (5)	−0.0021 (6)

Geometric parameters (Å, º)

O1—C2	1.4243 (17)	C23—H23C	0.98
O1—C5	1.4441 (17)	C8—C7	1.388 (2)
O20—C15	1.3638 (15)	C8—C9	1.391 (2)
O20—H20	0.90 (2)	C8—H8	0.95
N3—C13	1.4667 (19)	C22—H22A	0.98
N3—C2	1.4756 (18)	C22—H22B	0.98
N3—C4	1.4805 (18)	C22—H22C	0.98
C16—C17	1.3970 (18)	C17—C18	1.393 (2)
C16—C15	1.4151 (18)	C17—H17	0.95
C16—C21	1.5327 (18)	C13—H13A	0.98
C14—C19	1.3911 (18)	C13—H13B	0.98
C14—C15	1.4064 (18)	C13—H13C	0.98
C14—C2	1.5081 (19)	C9—C10	1.387 (3)
C19—C18	1.385 (2)	C9—H9	0.95
C19—H19	0.95	C5—H5	1
C2—H2	1	C18—H18	0.95
C6—C11	1.396 (2)	C11—C10	1.389 (2)
C6—C7	1.397 (2)	C11—H11	0.95
C6—C5	1.515 (2)	C24—H24A	0.98
C4—C12	1.516 (2)	C24—H24B	0.98
C4—C5	1.548 (2)	C24—H24C	0.98
C4—H4	1	C10—H10	0.95
C21—C22	1.5338 (19)	C12—H12A	0.98
C21—C24	1.540 (2)	C12—H12B	0.98
C21—C23	1.5433 (18)	C12—H12C	0.98
C23—H23A	0.98	C7—H7	0.95
C23—H23B	0.98
C2—O1—C5	108.87 (11)	C21—C22—H22B	109.5
C15—O20—H20	106.2 (13)	H22A—C22—H22B	109.5
C13—N3—C2	111.67 (11)	C21—C22—H22C	109.5
C13—N3—C4	113.71 (12)	H22A—C22—H22C	109.5
C2—N3—C4	102.96 (11)	H22B—C22—H22C	109.5
C17—C16—C15	116.81 (12)	C18—C17—C16	122.63 (13)
C17—C16—C21	122.37 (12)	C18—C17—H17	118.7
C15—C16—C21	120.75 (11)	C16—C17—H17	118.7
C19—C14—C15	119.83 (12)	N3—C13—H13A	109.5
C19—C14—C2	118.96 (12)	N3—C13—H13B	109.5
C15—C14—C2	121.05 (11)	H13A—C13—H13B	109.5
C18—C19—C14	120.22 (13)	N3—C13—H13C	109.5
C18—C19—H19	119.9	H13A—C13—H13C	109.5
C14—C19—H19	119.9	H13B—C13—H13C	109.5
O1—C2—N3	103.56 (10)	C10—C9—C8	119.59 (15)
O1—C2—C14	109.16 (12)	C10—C9—H9	120.2
N3—C2—C14	114.06 (11)	C8—C9—H9	120.2
O1—C2—H2	110	O1—C5—C6	108.80 (12)
N3—C2—H2	110	O1—C5—C4	104.91 (11)
C14—C2—H2	110	C6—C5—C4	117.42 (11)
C11—C6—C7	119.09 (14)	O1—C5—H5	108.5
C11—C6—C5	119.00 (14)	C6—C5—H5	108.5
C7—C6—C5	121.90 (13)	C4—C5—H5	108.5
O20—C15—C14	120.21 (12)	C19—C18—C17	119.46 (12)
O20—C15—C16	118.81 (12)	C19—C18—H18	120.3
C14—C15—C16	120.97 (11)	C17—C18—H18	120.3
N3—C4—C12	112.88 (12)	C10—C11—C6	120.52 (15)
N3—C4—C5	101.85 (11)	C10—C11—H11	119.7
C12—C4—C5	116.12 (13)	C6—C11—H11	119.7
N3—C4—H4	108.5	C21—C24—H24A	109.5
C12—C4—H4	108.5	C21—C24—H24B	109.5
C5—C4—H4	108.5	H24A—C24—H24B	109.5
C16—C21—C22	112.05 (11)	C21—C24—H24C	109.5
C16—C21—C24	111.12 (11)	H24A—C24—H24C	109.5
C22—C21—C24	107.05 (12)	H24B—C24—H24C	109.5
C16—C21—C23	108.84 (11)	C9—C10—C11	120.18 (15)
C22—C21—C23	107.38 (12)	C9—C10—H10	119.9
C24—C21—C23	110.34 (11)	C11—C10—H10	119.9
C21—C23—H23A	109.5	C4—C12—H12A	109.5
C21—C23—H23B	109.5	C4—C12—H12B	109.5
H23A—C23—H23B	109.5	H12A—C12—H12B	109.5
C21—C23—H23C	109.5	C4—C12—H12C	109.5
H23A—C23—H23C	109.5	H12A—C12—H12C	109.5
H23B—C23—H23C	109.5	H12B—C12—H12C	109.5
C7—C8—C9	120.51 (16)	C8—C7—C6	120.11 (14)
C7—C8—H8	119.7	C8—C7—H7	119.9
C9—C8—H8	119.7	C6—C7—H7	119.9
C21—C22—H22A	109.5
C15—C14—C19—C18	−0.3 (2)	C17—C16—C21—C24	−121.31 (14)
C2—C14—C19—C18	175.24 (12)	C15—C16—C21—C24	61.85 (16)
C5—O1—C2—N3	−29.88 (13)	C17—C16—C21—C23	116.99 (14)
C5—O1—C2—C14	−151.74 (11)	C15—C16—C21—C23	−59.85 (16)
C13—N3—C2—O1	164.76 (12)	C15—C16—C17—C18	1.39 (19)
C4—N3—C2—O1	42.40 (13)	C21—C16—C17—C18	−175.57 (12)
C13—N3—C2—C14	−76.72 (15)	C7—C8—C9—C10	0.9 (2)
C4—N3—C2—C14	160.91 (11)	C2—O1—C5—C6	132.44 (12)
C19—C14—C2—O1	−95.64 (14)	C2—O1—C5—C4	6.00 (14)
C15—C14—C2—O1	79.84 (15)	C11—C6—C5—O1	142.27 (13)
C19—C14—C2—N3	149.09 (13)	C7—C6—C5—O1	−36.26 (17)
C15—C14—C2—N3	−35.44 (17)	C11—C6—C5—C4	−98.86 (15)
C19—C14—C15—O20	−178.14 (12)	C7—C6—C5—C4	82.61 (17)
C2—C14—C15—O20	6.42 (19)	N3—C4—C5—O1	19.92 (13)
C19—C14—C15—C16	2.55 (19)	C12—C4—C5—O1	142.96 (13)
C2—C14—C15—C16	−172.88 (13)	N3—C4—C5—C6	−101.00 (13)
C17—C16—C15—O20	177.65 (12)	C12—C4—C5—C6	22.04 (18)
C21—C16—C15—O20	−5.34 (18)	C14—C19—C18—C17	−1.3 (2)
C17—C16—C15—C14	−3.03 (18)	C16—C17—C18—C19	0.8 (2)
C21—C16—C15—C14	173.98 (12)	C7—C6—C11—C10	0.3 (2)
C13—N3—C4—C12	76.22 (16)	C5—C6—C11—C10	−178.31 (13)
C2—N3—C4—C12	−162.80 (12)	C8—C9—C10—C11	−0.8 (2)
C13—N3—C4—C5	−158.56 (12)	C6—C11—C10—C9	0.2 (2)
C2—N3—C4—C5	−37.58 (13)	C9—C8—C7—C6	−0.4 (2)
C17—C16—C21—C22	−1.61 (18)	C11—C6—C7—C8	−0.2 (2)
C15—C16—C21—C22	−178.45 (12)	C5—C6—C7—C8	178.33 (13)

Hydrogen-bond geometry (Å, º)

D—H···A	D—H	H···A	D···A	D—H···A
O20—H20···N3	0.90 (2)	1.79 (2)	2.6244 (16)	154.4 (19)