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Journal logoSTRUCTURAL
CHEMISTRY
ISSN: 2053-2296

5,5′-Di-tert-butyl-2,2′-di­hy­droxy-3,3′-methanediyl­dibenz­aldehyde and its allyl-protected dialcohol and di­aldehyde precursors

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aChemistry Department, Loughborough University, Leicestershire LE11 3TU, England
*Correspondence e-mail: v.mckee@lboro.ac.uk

(Received 9 August 2004; accepted 24 August 2004; online 9 October 2004)

5,5′-Di-tert-butyl-2,2′-di­hydroxy-3,3′-methanediyl­dibenz­alde­hyde, C23H28O4, (IV[link]), has been structurally characterized in two polymorphic forms. The tetragonal form, (in I41/a) has been reported previously but is redetermined and reinterpreted here, while the monoclinic form, (in C2/c) is reported for the first time. In both polymorphs, the mol­ecule lies on a crystallographic twofold axis. Two precursors in the synthesis of (IV), namely 2,2′-bis­(allyl­oxy)-5,5′-di-tert-butyl-3,3′-methanediyldi­benzene­methanol (C29H40O4) and 2,2′-bis­(allyl­oxy)-5,5′-di-tert-butyl-3,3′-methanediyl­dibenz­aldehyde (C29H36O4) have also been char­acterized.

Comment

The diphenolic di­aldehyde 5,5′-di-tert-butyl-2,2′-di­hydroxy- 3,3′-methanediyl­dibenz­aldehyde, (IV[link]), has been used to synthesize new polynucleating macrocycles by Schiff base condensation with di­amines (Barreira Fontecha et al., 2002[Barreira Fontecha, J., Goetz, S. & McKee, V. (2002). Angew. Chem. Int. Ed. 41, 4554-4556.]). Compound (IV[link]) was prepared in three steps from the known dialcohol analogue 5,5′-di-tert-butyl-2,2′-di­hydroxy-3,3′-methanediyldi­benzene­methanol, (I[link]) (Dhawan & Gutsche, 1983[Dhawan, B. & Gutsche, C. D. (1983). J. Org. Chem. 48, 1536-1539.]).

The structure of 2,2′-bis­(allyl­oxy)-5,5′-di-tert-butyl-3,3′-methanediyldi­benzene­methanol, (II[link]), is shown in Fig. 1[link]. The mol­ecule is non-planar, with the two aryl rings inclined at 78.84 (9)° with respect to one another and the tert-butyl groups lying on opposite sides of the mol­ecule. The apparent folding of the mol­ecule is actually due to rotation about the C12—C4 and C12—C13 bonds, and the conformation adopted is probably a consequence of the hydrogen-bonding network throughout the lattice. Hydro­gen bonding between alcohol groups generates eight-membered rings [graph-set notation R44(8)] and links the mol­ecules into a double chain running parallel to the a axis (Fig. 2[link] and Table 1[link]). The H atoms on the hydroxy groups are disordered, and these atoms were modelled with 50% occupancy of two equivalent positions. As a result there are two self-consistent hydrogen-bonding patterns, which have O—H⋯O directions running either anticlockwise (as in Fig. 2[link]) or clockwise around the same ring. The highest residual electron-density peak is 1.26 Å from atom C28 and 1.39 Å from atom C27, and may indicate a minor disorder of that allyl group.

[Scheme 1]

The dialcohol was oxidized using MnO2 to form the analogous di­aldehyde, 2,2′-bis­(allyl­oxy)-5,5′-di-tert-butyl-3,3′-methanediyl­dibenz­aldehyde, (III[link]). As Fig. 3[link] shows, the phenyl planes are inclined at 74.17 (5)° and the tert-butyl groups are on the same side of the mol­ecule. One of the allyl groups is disordered, and this disorder was modelled as a 70:30 occupancy of two conformations. Again, the mol­ecules are linked by hydrogen bonding into a double chain, in this case running parallel to c (Fig. 4[link]); however, the interactions are all of the type C—H⋯O=C (Table 2[link]). There is also some ππ stacking across the hydrogen-bonded chain involving the benz­aldehyde groups. The section incorporating atoms O1/C1/C2/C3/C7 overlaps the O4/C23/C16–C18 section of a neighbouring mol­ecule at (x, [1\over2] − y, [1\over2] + z). The planes of the interacting benz­aldehyde rings are inclined at 12.33 (7)°, while atoms O1 and C1 are 3.274 (2) and 3.357 (2) Å, respectively, from the mean plane of the interacting phenyl ring (Fig. 4[link]).

Compound (IV[link]) has been characterized in two polymorphic forms. We obtained the tetragonal form, (IVa) (space group I41/a), by recrystallization of the crude material from diethyl ether, while Masci et al. (2004[Masci, B., Levi Mortera, S., Seralessandri, L. & Thuery, P. (2004) Acta Cryst. C60, o107-o109.]) obtained the same polymorph by recrystallization from methanol. A second polymorph was formed as a side product in the synthesis of a macrocyclic complex; crystals of (IVb) in the monoclinic space group C2/c were obtained from a methanol solution containing 1,5-di­amino­pentan-3-ol and nickel(II) nitrate.

In the tetragonal form, (IVa), the asymmetric unit contains half of the mol­ecule, with a twofold axis passing through atom C12 (Fig. 5[link]), while in the monoclinic form, (IVb), the asymmetric unit contains two independent half mol­ecules, each having twofold symmetry (Fig. 6[link]). The molecular conformation and bond lengths are similar in the two polymorphs; the tert-butyl groups are on opposite sides of the linked aryl rings and the phenol H atoms are involved in intramolecular hydrogen bonds with the adjacent carbonyl groups (Tables 3[link] and 4[link]). In (IVb), there is additional intermolecular hydrogen bonding involving one of the carbonyl groups (C13=O3). Atom C13 forms a C—H⋯O=C hydrogen bond to atom O3 of a neighbouring mol­ecule at (−x, 2 − y, 1 − z), resulting in zigzag chains parallel to c. The second mol­ecule does not show a corresponding interaction. As in the precursors, the phenyl rings are inclined with respect to one another: in the tetragonal form, the phenyl rings are inclined at 61.48 (5)°, whereas in the monoclinic polymorph, the values are 73.58 (5) and 75.04 (5)°.

In form (IVa), the mol­ecules are packed as shown in Figs. 5[link] and 7[link]. In contrast to the previous report of this structure (Masci et al., 2004[Masci, B., Levi Mortera, S., Seralessandri, L. & Thuery, P. (2004) Acta Cryst. C60, o107-o109.]), we have identified ππ interactions (the most direct overlap being between the sections containing atoms O1/C1/C2/C7/C6; see Fig. 5[link]) linking the mol­ecules into sets of zigzag ribbons running parallel to either the a or the b axis. As can be seen in Fig. 5[link], π-stacked pairs of rings are parallel and related by inversion; the distance between the mean plane of the benz­aldehyde ring containing atoms O1 and C7 and the centroid of the neighbouring phenyl ring at (2 − x, 1 − y, −z) is 3.361 (4) Å.

In polymorph (IVb), the two independent mol­ecules form ABAB π-stacked columns parallel to the b axis (Fig. 8[link]). The relative rotation between adjacent layers prevents steric interference between successive tert-butyl groups (Fig. 6[link]). The benz­aldehyde rings are almost parallel [interplanar angle = 6.34 (10)°], with average interplanar separations of 3.48 and 3.32 Å between the ring containing atoms O1 and C7 and that containing O3 and C19 at (−x, y, [1 \over 2] − z) and (−x, 1 + y, [1\over2] − z), respectively. Again, the shortest ππ interactions are between the carbonyl groups and the phenyl rings of neighbouring mol­ecules in the stack.

[Figure 1]
Figure 1
A view of the structure of (II[link]). The H atoms on the two alcohol functions are disordered and only one position is shown for each. Displacement ellipsoids are drawn at the 50% probability level.
[Figure 2]
Figure 2
The hydrogen bonding in (II[link]), producing a double chain parallel to a. Only one of the two orientations of the hydrogen bonding within the R44(8) ring is shown. [Symmetry codes: (i) 1 + x, y, z; (ii) −x, 2 − y, −z; (iii) 1 − x, 2 − y, −z.]
[Figure 3]
Figure 3
A view of the structure of (III[link]), showing the disorder in one allyl group. Displacement ellipsoids are drawn at the 50% probability level.
[Figure 4]
Figure 4
The C—H⋯O=C hydrogen-bonded chain parallel to b in (III[link]). [Symmetry codes: (vi) x, [1\over 2] − y, [1\over 2] + z; (vii) x, [1\over 2] − y, −[1\over 2] + z.]
[Figure 5]
Figure 5
A view of the structure of polymorph (IVa); intramolecular hydrogen-bonding interactions between the phenol and aldehyde functions are shown as dashed lines. Dotted lines show interatomic distances in the range 3.42–3.47 Å in the ππ overlap region. Displacement ellipsoids are drawn at the 50% probability level. [Symmetry codes: (viii) 2 − x, [3\over 2] − y, z; (ix) 2 − x, 1 − y, −z.]
[Figure 6]
Figure 6
A view of the two independent mol­ecules in polymorph (IVb). A twofold axis passes through atoms C12 and C24. Displacement ellipsoids are drawn at the 30% probability level. [Symmetry code: (x) −x, y, [1\over2] − z.]
[Figure 7]
Figure 7
A unit-cell plot for polymorph (IVa), viewed down the a axis, showing the ππ-stacked ribbons running parallel to a and parallel to b. O atoms are shown as shaded circles. Dashed lines indicate the ππ overlapped sections.
[Figure 8]
Figure 8
A unit-cell plot for polymorph (IVb), projected down b, showing π-stacked columns parallel to b and inter- and intramolecular hydrogen bonding (dashed lines). O atoms are shown as shaded circles.

Experimental

Compound (I[link]) was synthesized according to the procedure of Dhawan & Gutsche (1983[Dhawan, B. & Gutsche, C. D. (1983). J. Org. Chem. 48, 1536-1539.]). For the synthesis of (II[link]), compound (I[link]) (10 g, 27 mmol), allyl ­bromide (7 g, 58 mmol), an­hydrous K2CO3 (7.42 g) and acetone (100 ml) were placed in a 250 ml three-necked round-bottomed flask fitted with a reflux condenser and a sealed stirrer unit, and were refluxed for 20 h with stirring. The reaction mixture was then poured into water (200 ml) and the aqueous layer was extracted three times with diethyl ether. The organic layer was washed with a 2 M sodium hydroxide solution and dried over an­hydrous K2CO3. The solvent was removed under vacuum, leaving a white solid, which was recrystallized from di­chloro­methane/n-­hexane; the yield was 9.0 g (74%). Colourless crystals suitable for X-­ray studies were obtained by slow evaporation of a solution of di­chloro­methane/pentane (1:5). Thin-layer chromatography (TLC) on silica gel (diethyl ether/petroleum ether 40/60, 45:55): RF = 0.68. Analysis calculated for (II[link])·0.5H2O: C 75.45, H 8.95%; found: C 75.64, H 9.06%. 1H NMR (CDCl3, p.p.m.): 7.24 (d, 2H, ArH), 7.01 (d, 2H, ArH), 6.07 (m, 2H, allyl =CH), 5.34 (dd, 2H, allyl =CH2), 5.30 (dd, 2H, allyl =CH2), 4.73 (d, 4H, CH2OH), 4.34 (d, 4H, allyl CH2), 4.70 (s, 4H, CH2OH), 4.07 (s, 2H, ArCH2Ar), 1.26 [s, 18H, C(CH3)3]. IR (KBr, cm−1): 3272 [s, ν(OH)], 3081 [w, ν(allyl =CH2)], 883 (m, 1,2,3,5 tetrasubstitution of Ar).

Compound (III[link]) was synthesized by a method similar to that reported by Taniguchi (1984[Taniguchi, S. (1984). Bull. Chem. Soc. Jpn, 57, 2683-2684.]). Activated MnO2 (50 g) was added to a solution of (II[link]) (9 g, 20 mmol) in chloro­form (200 ml). The reaction mixture was refluxed for 19–20 h, after which time MnO2 was filtered off and the organic layer dried over an­hydrous MgSO4. The solvent was removed under vacuum, leaving a pale-yellow oil that crystallized under vacuum over a period of one week. The solid was then washed with cold methanol to remove the yellow impurities. Colourless crystals suitable for X-ray studies were obtained by slow evaporation of a diethyl ether solution of the product. The yield was 7.0 g (78%). TLC on silica gel (diethyl ether/petroleum ether 40/60, 30:70): RF = 0.50. Analysis calculated for (III[link])·0.5H2O: C 76.11, H 8.15%; found: C 76.08, H 8.15%. 1H NMR (CDCl3, p.p.m.): 10.4 (s, 2H, CHO), 7.75 (d, 2H, ArH), 7.30 (d, 2H, ArH), 6.06 (m, 2H, allyl =CH), 4.40 (dd, 2H, allyl =CH2), 4.44 (dd, 2H, allyl =CH2), 4.13 (s, 2H, ArCH2Ar), 1.26 [s, 18H, C(CH3)3]. IR (KBr, cm−1): 1660 [ν(C=O)], 3081 [w, ν(allyl =CH2)], 885 (m, 1,2,3,5 tetrasubstitution of Ar).

Compound (IV[link]) was obtained using the method described by Boss & Scheffold (1976[Boss, R. & Scheffold, R. (1976). Angew. Chem. 88, 578-579.]). To a solution of (III[link]) (7 g, 15.6 mmol) in ethanol (150 ml) were added 10% Pd on activated charcoal (1.5 g) and p-toluene­sulfonic acid (0.7 g) in water (5 ml). The stirred suspension was refluxed for 2 d, after which time the reaction mixture was filtered hot. On cooling, the product precipitated out as a pale-yellow powder, which was filtered off (yield 1 g). An additional portion of (IV[link]) (3 g) was obtained on concentration of the resulting filtrate. Pale-yellow crystals of (IVa) suitable for X-ray studies were obtained by slow evaporation from a solution of the product in diethyl ether. The yield was 4 g (70%). TLC on silica gel (diethyl ether/petroleum ether 40/60, 30:70): RF = 0.64. Analysis calculated: C 74.97, H 7.66%; found: C 74.51, H 7.86%. 1H NMR (CDCl3, p.p.m.): 11.19 (s, 2H, Ar—OH), 9.86 (s, 2H, CHO), 7.64 (d, 2H, ArH), 7.37 (d, 2H, ArH), 4.03 (s, 2H, ArCH2Ar), 1.26 [s, 18H, C(CH3)3]. IR (KBr, cm−1): 1658 [ν(C=O)], 1270 [s, ν(ArOH)], 1216 (s).

Compound (II)[link]

Crystal data
  • C29H40O4

  • Mr = 452.61

  • Triclinic, [P\overline 1]

  • a = 10.6025 (11) Å

  • b = 11.9199 (12) Å

  • c = 12.4180 (13) Å

  • α = 64.611 (2)°

  • β = 82.672 (2)°

  • γ = 66.330 (2)°

  • V = 1296.7 (2) Å3

  • Z = 2

  • Dx = 1.159 Mg m−3

  • Mo Kα radiation

  • Cell parameters from 2476 reflections

  • θ = 2.3–27.2°

  • μ = 0.08 mm−1

  • T = 150 (2) K

  • Block, colourless

  • 0.29 × 0.17 × 0.12 mm

Data collection
  • Bruker SMART 1000 CCD area-detector diffractometer

  • φ and ω scans

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2001[Sheldrick, G. M. (2001). SHELXTL (Version 6.12) and SADABS (Version 6.12). Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.938, Tmax = 1.000

  • 9408 measured reflections

  • 4565 independent reflections

  • 3085 reflections with I > 2σ(I)

  • Rint = 0.025

  • θmax = 25.0°

  • h = −12 → 12

  • k = −14 → 14

  • l = −14 → 14

Refinement
  • Refinement on F2

  • R[F2 > 2σ(F2)] = 0.057

  • wR(F2) = 0.173

  • S = 1.04

  • 4565 reflections

  • 310 parameters

  • H-atom parameters constrained

  • w = 1/[σ2(Fo2) + (0.0843P)2 + 0.7234P] where P = (Fo2 + 2Fc2)/3

  • (Δ/σ)max < 0.001

  • Δρmax = 0.69 e Å−3

  • Δρmin = −0.22 e Å−3

Table 1
Hydrogen-bonding geometry (Å, °) for (II)[link]

D—H⋯A D—H H⋯A DA D—H⋯A
O1—H1OA⋯O4i 0.83 1.93 2.744 (3) 166
O1—H1OB⋯O4iv 0.82 1.99 2.749 (2) 155
O4—H4OA⋯O1iv 0.91 1.85 2.749 (2) 167
O4—H4OB⋯O1v 0.84 1.90 2.744 (3) 177
Symmetry codes: (i) 1+x,y,z; (iv) -x,1-y,-z; (v) x-1,y,z.

Compound (III)[link]

Crystal data
  • C29H36O4

  • Mr = 448.58

  • Monoclinic, P21/c

  • a = 16.2931 (10) Å

  • b = 10.1951 (6) Å

  • c = 16.4318 (10) Å

  • β = 108.367 (1)°

  • V = 2590.4 (3) Å3

  • Z = 4

  • Dx = 1.150 Mg m−3

  • Mo Kα radiation

  • Cell parameters from 7890 reflections

  • θ = 2.4–23.3°

  • μ = 0.08 mm−1

  • T = 150 (2) K

  • Block, colourless

  • 0.26 × 0.16 × 0.14 mm

Data collection
  • Bruker SMART 1000 CCD area-detector diffractometer

  • ω scans

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2001[Sheldrick, G. M. (2001). SHELXTL (Version 6.12) and SADABS (Version 6.12). Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.900, Tmax = 1.000

  • 17 928 measured reflections

  • 4559 independent reflections

  • 3620 reflections with I > 2σ(I)

  • Rint = 0.020

  • θmax = 25.0°

  • h = −19 → 19

  • k = −12 → 12

  • l = −19 → 19

Refinement
  • Refinement on F2

  • R[F2 > 2σ(F2)] = 0.043

  • wR(F2) = 0.123

  • S = 1.02

  • 4559 reflections

  • 317 parameters

  • H-atom parameters constrained

  • w = 1/[σ2(Fo2) + (0.058P)2 + 1.0861P] where P = (Fo2 + 2Fc2)/3

  • (Δ/σ)max = 0.001

  • Δρmax = 0.29 e Å−3

  • Δρmin = −0.18 e Å−3

Table 2
Hydrogen-bonding geometry (Å, °) for (III)[link]

D—H⋯A D—H H⋯A DA D—H⋯A
C5—H5⋯O1vii 0.95 2.46 3.406 (2) 171
C14—H14⋯O4vi 0.95 2.62 3.560 (2) 170
Symmetry codes: (vi) [x,{\script{1\over 2}}-y,{\script{1\over 2}}+z]; (vii) [x,{\script{1\over 2}}-y,-{\script{1\over 2}}+z].

Polymorph (IVa)

Crystal data
  • C23H28O4

  • Mr = 368.45

  • Tetragonal, I41/a

  • a = 12.7930 (7) Å

  • c = 24.158 (2) Å

  • V = 3953.7 (4) Å3

  • Z = 8

  • Dx = 1.238 Mg m−3

  • Mo Kα radiation

  • Cell parameters from 3205 reflections

  • θ = 2.8–22.8°

  • μ = 0.08 mm−1

  • T = 150 (2) K

  • Tablet, yellow

  • 0.28 × 0.20 × 0.05 mm

Data collection
  • Bruker SMART 1000 CCD area-detector diffractometer

  • φ and ω scans

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2001[Sheldrick, G. M. (2001). SHELXTL (Version 6.12) and SADABS (Version 6.12). Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.931, Tmax = 1.000

  • 19 093 measured reflections

  • 1736 independent reflections

  • 1203 reflections with I > 2σ(I)

  • Rint = 0.056

  • θmax = 25.0°

  • h = −15 → 15

  • k = −15 → 15

  • l = −28 → 28

Refinement
  • Refinement on F2

  • R[F2 > 2σ(F2)] = 0.043

  • wR(F2) = 0.120

  • S = 1.04

  • 1736 reflections

  • 125 parameters

  • H-atom parameters constrained

  • w = 1/[σ2(Fo2) + (0.0446P)2 + 4.6694P] where P = (Fo2 + 2Fc2)/3

  • (Δ/σ)max < 0.001

  • Δρmax = 0.19 e Å−3

  • Δρmin = −0.21 e Å−3

Table 3
Hydrogen-bonding geometry (Å, °) for (IVa)

D—H⋯A D—H H⋯A DA D—H⋯A
O2—H2⋯O1 0.92 (2) 1.80 (2) 2.645 (2) 151 (2)

Polymorph (IVb)

Crystal data
  • C23H28O4

  • Mr = 368.45

  • Monoclinic, C2/c

  • a = 26.809 (2) Å

  • b = 8.4543 (7) Å

  • c = 21.3720 (18) Å

  • β = 120.618 (1)°

  • V = 4168.7 (6) Å3

  • Z = 8

  • Dx = 1.174 Mg m−3

  • Mo Kα radiation

  • Cell parameters from 3051 reflections

  • θ = 2.6–25.6°

  • μ = 0.08 mm−1

  • T = 153 (2) K

  • Tablet, light brown

  • 0.48 × 0.38 × 0.16 mm

Data collection
  • Bruker SMART 1000 CCD area-detector diffractometer

  • φ and ω scans

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2001[Sheldrick, G. M. (2001). SHELXTL (Version 6.12) and SADABS (Version 6.12). Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.919, Tmax = 1.000

  • 14 739 measured reflections

  • 3668 independent reflections

  • 2235 reflections with I > 2σ(I)

  • Rint = 0.049

  • θmax = 25.0°

  • h = −31 → 31

  • k = −10 → 10

  • l = −25 → 25

Refinement
  • Refinement on F2

  • R[F2 > 2σ(F2)] = 0.047

  • wR(F2) = 0.132

  • S = 1.01

  • 3668 reflections

  • 251 parameters

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

  • w = 1/[σ2(Fo2) + (0.0393P)2 + 4.8718P] where P = (Fo2 + 2Fc2)/3

  • (Δ/σ)max < 0.001

  • Δρmax = 0.20 e Å−3

  • Δρmin = −0.18 e Å−3

Table 4
Hydrogen-bonding geometry (Å, °) for (IVb)

D—H⋯A D—H H⋯A DA D—H⋯A
O2—H2⋯O1 0.94 (2) 1.81 (2) 2.625 (3) 144 (2)
O4—H4⋯O3 0.88 (2) 1.85 (2) 2.631 (2) 147 (2)
C13—H13⋯O3ii 0.95 2.57 3.454 (3) 156
Symmetry code: (ii) -x,2-y,1-z.

Except as described below, H atoms bonded to C atoms were placed at calculated positions and refined using a riding model. The constrained C—H distances were 0.95, 0.98, 0.99 and 0.99 Å for aryl, methyl, methyl­ene and ethyl­ene H atoms, respectively. The Uiso(H) values were set at 1.2Ueq(C) for methyl­ene and aryl H atoms, and at 1.5Ueq(C) for tert-butyl H atoms. For (II[link]), the disordered H atoms bonded to atoms O1 and O4 were located from difference maps and were not further refined; their Uiso(H) values were fixed at 0.04 Å2. The Uiso(H) values of the tert-butyl H atoms were fixed at 0.05 Å2, and those of the H atoms on atoms C27 and C24 at 0.04 Å2. For (IVa), H atoms bonded to O atoms were placed at calculated positions, with a constrained O—H distance of 0.84 Å and with Uiso(H) set at 1.5Ueq of the carrier O atom. In (IVb), the Uiso values for the tert-butyl H atoms were fixed at 0.05 Å2, while the phenol H atoms were located from difference maps and their positions refined, with Uiso(H) values fixed at 0.05 Å2.

For all determinations, data collection: SMART (Bruker, 1998[Bruker (1998). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SMART; data reduction: SAINT (Bruker, 1998[Bruker (1998). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.]); program(s) used to solve structure: SHELXTL (Sheldrick, 2001[Sheldrick, G. M. (2001). SHELXTL (Version 6.12) and SADABS (Version 6.12). Bruker AXS Inc., Madison, Wisconsin, USA.]); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Supporting information


Comment top

The diphenolic dialdehyde 5,5'-di-tert-butyl-2,2'-dihydroxy- 3,3'-methanediyldibenzaldehyde, (IV), has been used to synthesize new polynucleating macrocycles by Schiff base condensation with diamines (Barreira Fontecha et al., 2002). Compound (IV) was prepared in three steps from the known dialcohol analogue 5,5'-di-tert-butyl-2,2'-dihydroxy- 3,3'-methanediyldibenzenemethanol, (I) (Dhawan & Gutsche, 1983).

The structure of 2,2'-bis(allyloxy)-5,5'-di-tert-butyl-3,3'-methanediyldibenzenemethanol, (II), is shown in Fig. 1. The molecule is non-planar, with the two aryl rings inclined at 78.84 (9)° with respect to one another and the tert-butyl groups lying on opposite sides of the molecule. The apparent folding of the molecule is actually due to rotation about the C12—C4 and C12—C13 bonds, and the conformation adopted is probably a consequence of the hydrogen-bonding network throughout the lattice. Hydrogen bonding between alcohol groups generates eight-membered rings [graph set notation R44(8)] and links the molecules into a double chain running parallel to the a axis (Fig. 2 and Table 1). The H atoms on the hydroxy groups are disordered, and these atoms were modelled with 50% occupancy of two equivalent positions. The highest residual electron density peak (0.69 e Å−3) is 1.26 (s.u.?) Å from C28 and 1.39 (s.u.?) Å from C27, and may indicate a minor disorder of that allyl group.

The dialcohol was oxidized using MnO2 to form the analogous dialdehyde 2,2'-bis(allyloxy)-5,5'-di-tert-butyl-3,3'-methanediyldibenzaldehyde, (III). As Fig. 3 shows, the phenyl planes are inclined at 74.17 (5)° and the tert-butyl groups are on the same side of the molecule. One of the allyl groups is disordered, and this disorder was modelled as 70:30 occupancy of two conformations. Again, the molecules are linked by hydrogen bonding into a double chain, in this case running parallel to c (Fig. 4); however, the interactions are all of the type C—H····OC (Table 2). There is also some ππ stacking across the hydrogen-bonded chain involving the benzaldehyde groups. The section incorporating atoms O1, C1, C2, C3 and C7 overlaps the O4/C23/C16–C18 section of a neighbouring molecule under symmetry operation (x, 0.5 − y, 0.5 + z). The planes of the interacting benzaldehyde rings are inclined at 12.33 (7)°, while atoms O1 and C1 are 3.274 (2) and 3.357 (2) Å, respectively, from the mean plane of the interacting phenyl ring (Fig. 4).

Compound (IV) has been characterized in two polymorphic forms. We obtained the tetragonal form, (IVa) (space group I41/a), by recrystallization of the crude material from diethyl ether, while Masci et al. (2004) obtained the same polymorph by recrystallization from methanol. A second polymorph was formed as a side product in the synthesis of a macrocyclic complex; crystals of (IVb) in the monoclinic space group C2/c were obtained from a methanol solution containing 1,5-diaminopentan-3-ol and nickel(II) nitrate.

In the tetragonal form, (IVa), the asymmetric unit contains half of the molecule, with a twofold axis passing through C12 (Fig. 5), while in the monoclinic form, (IVb), the asymmetric unit contains two independent half molecules, each having twofold symmetry (Fig. 6). The molecular conformation and bond lengths are similar in the two polymorphs; the tert-butyl groups are on opposite sides of the linked aryl rings and the phenol H atoms are involved in intramolecular hydrogen bonds with the adjacent carbonyl groups (Tables 3 and 4). In (IVb), there is additional intermolecular hydrogen bonding involving one of the carbonyl groups (C13O3). Atom C13 forms a C—H····OC hydrogen bond to atom O3 of a neighbouring molecule at (-x, 2 − y, 1 − z), resulting in zigzag chains parallel to c. The second molecule does not show a corresponding interaction. As in the precursors, the phenyl rings are inclined with respect to one another. In the tetragonal form, the phenyl rings are inclined at 61.48 (5)°, whereas in the monoclinic polymorph, the values are 73.58 (5) and 75.04 (5)°.

In form (IVa), the molecules are packed as shown in Figs. 5 and 7. In contrast to the previous report of this structure (Masci et al., 2004), we have identified ππ interactions (the most direct overlap being between the sections containing atoms O1, C1, C2, C7 and C6; see Fig. 5) linking the molecules into sets of zigzag ribbons running parallel to either the a or the b axis. π stacked pairs of rings are parallel and related by inversion; the distance between the mean plane of the benzaldehyde ring containing atoms O1 and C7 and the centroid of the neighbouring phenyl ring at (2 − x, 1 − y, −z) is 3.361 (4) Å.

In polymorph (IVb), the two independent molecules form ABAB π stacked columns parallel to the b axis (Fig. 8). The relative rotation between adjacent layers prevents steric interference between successive tert-butyl groups (Fig. 6). The benzaldehyde rings are almost parallel [interplanar angle 6.3 (s.u.?)°], with average interplanar separations of 3.48 and 3.32 Å between the ring containing atoms O1 and C7 and that containing O3 and C19 at (-x, y, 0.5 − z) and (-x, 1 + y, 0.5 − z), respectively. Again, the shortest ππ interactions are between the carbonyl groups and the phenyl rings of neighbouring molecules in the stack.

Experimental top

Compound (I) was synthesized according to the procedure of Dhawan & Gutsche (1982).

For the synthesis of (II), compound (I) (10 g, 27 mmol), allylbromide (7 g, 58 mmol), anhydrous K2CO3 (7.42 g) and acetone (100 ml) were placed in a 250 ml three-necked round-bottomed flask fitted with a reflux condenser and sealed stirrer unit, and were refluxed for 20 h with stirring. The reaction mixture was then poured into water (200 ml) and the aqueous layer was extracted three times with diethyl ether. The organic layer was washed with a 2M sodium hydroxide solution and dried over anhydrous K2CO3. The solvent was removed under vacuum, leaving a white solid, which was recrystallized from dichloromethane/n-hexane. The yield was 9.0 g (74%). Colourless crystals suitable for X-ray studies were obtained by slow evaporation of a solution of dichloromethane/ pentane (1:5). Thin-layer chromatography (TLC) on silica gel (diethylether/pet–ether 40/60, 45:55) Rf = 0.68. Analysis calculated for (II)·0.5H2O: C 75.45, H 8.95%; found: C 75.64, H 9.06%. 1H NMR (CDCl3, p.p.m.): 7.24 (d, 2, ArH), 7.01 (d, 2, ArH), 6.07 (m, 2, allyl CH), 5.34 (dd, 2, allyl CH2), 5.30 (dd, 2, allyl CH2), 4.73 (d, 4, CH2OH), 4.34 (d, 4, allyl CH2), 4.70 (s, 4, CH2OH), 4.07 (s, 2, ArCH2Ar), 1.26 (s, 18, C(CH3)3). IR (KBr, cm−1): 3272 (s, νOH), 3081 (w, νallyl CH2), 883 (m, 1,2,3,5 tetrasubstitution of Ar).

Compound (III) was synthesized by a method similar to that reported by Taniguchi (1984). Activated MnO2 (50 g) was added to a solution of (II) (9 g, 20 mmol) in chloroform (200 ml). The reaction mixture was refluxed for 19–20 h, after which time MnO2 was filtered off and the organic layer was dried over anhydrous MgSO4. The solvent was removed under vacuum, leaving a pale-yellow oil that crystallized under vacuum over a week. The solid was then washed with cold methanol to remove the yellow impurities. Colourless crystals suitable for X-ray studies were obtained by slow evaporation of a diethyl ether solution of the product. The yield is 7.0 g (78%). TLC on silica gel (diethylether/ pet–ether 40/60, 30:70) Rf = 0.50. Analysis calculated for (III)·0.5H2O: C 76.11, H 8.15%; found: C 76.08, H 8.15%. 1H NMR (CDCl3, p.p.m.): 10.4 (s, 2,CHO), 7.75 (d, 2, ArH), 7.30 (d, 2, ArH), 6.06 (m, 2, allyl CH), 4.40 (dd, 2, allyl CH2), 4.44 (dd, 2, allyl CH2), 4.13 (s, 2, ArCH2Ar), 1.26 (s, 18, C(CH3)3). IR (KBr, cm−1): 1660 (νCO), 3081 (w, νallyl CH2), 885 (m, 1,2,3,5 tetrasubstitution of Ar).

Compound (IV) was obtained using the method described by Boss & Scheffold (1976). To a solution of (III) (7 g, 15.6 mmol) in ethanol (150 ml) were added 10% Pd on activated charcoal (1.5 g) and p-toluenesulfonic acid (0.7 g) in water (5 ml). The stirred suspension was refluxed for 2 d, after which time the reaction mixture was filtered hot. On cooling, the product precipitated out as a pale-yellow powder, which was filtered off (yield 1 g). An additional portion of (IV) (3 g) was obtained on concentration of the resulting filtrate. Pale-yellow crystals of (IVa) suitable for X-ray studies were obtained by slow evaporation from a solution of the product in diethyl ether. The yield was 4 g (70%). TLC on silica gel (diethylether/pet–ether 40/60, 30:70) Rf = 0.64. Analysis calculated: C 74.97, H 7.66%; found: C 74.51, H 7.86%. 1H NMR (CDCl3, p.p.m.): 11.19 (s, 2H, Ar–OH), 9.86 (s, 2, CHO), 7.64 (d, 2, ArH), 7.37 (d, 2, ArH), 4.03 (s, 2, ArCH2Ar), 1.26 [s, 18, C(CH3)3]. IR (KBr, cm−1): 1658 (νCO), 1270 (s, ν(ArOH)), 1216 (s).

##AUTHOR: Would "tablet" be better than "block" for the crystal shape of IVa, ## given that there is one dimensions much smaller than the other two?

Refinement top

Except as described below, H atoms bonded to C atoms were placed at calculated positions and refined using a riding model. The constrained C—H distances were 0.95, 0.98, 0.99 and 0.99 Å for aryl, methyl, methylene and ethylene atoms, respectively. The Uiso(H) values were set at 1.2Ueq(C) for methylene and aryl atoms, and 1.5Ueq(C) for tert-butyl atoms. For (II), the disordered H atoms bonded to atoms O1 and O4 were located from difference maps and were not further refined; their Uiso(H) values were fixed at 0.04 Å2. The Uiso(H) values of the tert-butyl H atoms were fixed at 0.05 Å2, and those of the H atoms on atoms C27 and C24 at 0.04 Å2. For (IVa), H atoms bonded to O atoms were placed at calculated positions, with a constrained O—H distance of 0.84 Å and with Uiso(H) set at 1.5Ueq of the carrier O atom. In (IVb), the Uiso values for the tert-butyl H atoms were fixed at 0.05 Å2, while the phenol H atoms were located from difference maps and their positions were refined, with Uiso(H) values fixed at 0.05 Å2.

Computing details top

For all compounds, data collection: SMART (Bruker, 1998); cell refinement: SMART; data reduction: SAINT (Bruker, 1998); program(s) used to solve structure: SHELXTL (Sheldrick, 2001); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. A view of the structure of (II). The H atoms on the two alcohol functions are disordered, and only one position is shown. Displacement ellipsoids are drawn at the 50% probability level.
[Figure 2] Fig. 2. The hydrogen bonding in (II), leading to a double chain parallel to a. [Symmetry codes: (i) 1 + x, y, z; (ii) −x, 2 − y, −z; (iii) = 1 − x, 2 − y, −z.]
[Figure 3] Fig. 3. A view of the structure of (III), showing the disorder in one allyl group. Displacement ellipsoids are drawn at the 50% probability level.
[Figure 4] Fig. 4. The C—H···OC hydrogen-bonded chain parallel to b in (III). [Symmetry codes: (i) x, 0.5 − y, 0.5 + z; (ii) x, 0.5 − y, −0.5 + z.]
[Figure 5] Fig. 5. A view of the structure of (IVa); intramolecular hydrogen-bonding interactions between the phenol and aldehyde functions are shown as dashed lines. Dotted lines show interatomic distances in the range 3.42–3.47 Å in the ππ overlap region. Displacement ellipsoids are drawn at the 50% probability level. [Symmetry codes: (i) 2 − x, 1.5 − y, z, (ii) 2 − x, 1 − y, −z.]
[Figure 6] Fig. 6. A view of the two independent molecules in (IVb). A twofold axis passes through atoms C12 and C24. Displacement ellipsoids are drawn at the 30% probability level. [Symmetry code: (i) −x, y, 0.5 − z.]
[Figure 7] Fig. 7. A unit cell plot for (IVa), viewed down the a axis, showing the ππ stacked ribbons running parallel to a and parallel to b. O atoms are shown as shaded circles. Dashed lines indicate the ππ overlapped sections.
[Figure 8] Fig. 8. A unit-cell plot for (IVb), projected down b, showing π stacked columns parallel to b and inter- and intramolecular hydrogen bonding (dashed lines). O atoms are shown as shaded circles.
(II) 2,2'-bis(allyloxy)-5,5'-di-tert-butyl-3,3'-methanediyldibenzenemethanol top
Crystal data top
C29H40O4Z = 2
Mr = 452.61F(000) = 492
Triclinic, P1Dx = 1.159 Mg m3
a = 10.6025 (11) ÅMo Kα radiation, λ = 0.71073 Å
b = 11.9199 (12) ÅCell parameters from 2476 reflections
c = 12.4180 (13) Åθ = 2.3–27.2°
α = 64.611 (2)°µ = 0.08 mm1
β = 82.672 (2)°T = 150 K
γ = 66.330 (2)°Block, colourless
V = 1296.7 (2) Å30.29 × 0.17 × 0.12 mm
Data collection top
Bruker SMART 1000 CCD area-detector
diffractometer
4565 independent reflections
Radiation source: normal-focus sealed tube3085 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.025
ϕ and ω scansθmax = 25.0°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2001)
h = 1212
Tmin = 0.938, Tmax = 1.000k = 1414
9408 measured reflectionsl = 1414
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)] = 0.057Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.173H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0843P)2 + 0.7234P]
where P = (Fo2 + 2Fc2)/3
4565 reflections(Δ/σ)max < 0.001
310 parametersΔρmax = 0.69 e Å3
0 restraintsΔρmin = 0.22 e Å3
Crystal data top
C29H40O4γ = 66.330 (2)°
Mr = 452.61V = 1296.7 (2) Å3
Triclinic, P1Z = 2
a = 10.6025 (11) ÅMo Kα radiation
b = 11.9199 (12) ŵ = 0.08 mm1
c = 12.4180 (13) ÅT = 150 K
α = 64.611 (2)°0.29 × 0.17 × 0.12 mm
β = 82.672 (2)°
Data collection top
Bruker SMART 1000 CCD area-detector
diffractometer
4565 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2001)
3085 reflections with I > 2σ(I)
Tmin = 0.938, Tmax = 1.000Rint = 0.025
9408 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0570 restraints
wR(F2) = 0.173H-atom parameters constrained
S = 1.04Δρmax = 0.69 e Å3
4565 reflectionsΔρmin = 0.22 e Å3
310 parameters
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O10.34147 (18)0.45442 (18)0.04311 (17)0.0350 (5)
C10.2100 (3)0.4894 (3)0.0094 (2)0.0274 (6)
H1A0.19180.56820.08740.033*
H1B0.13560.51310.04340.033*
C20.2132 (2)0.3708 (2)0.0259 (2)0.0223 (5)
C30.1642 (2)0.2774 (2)0.0588 (2)0.0221 (5)
O20.10499 (17)0.29559 (17)0.15977 (15)0.0272 (4)
C40.1704 (2)0.1654 (2)0.0439 (2)0.0221 (5)
C50.2330 (2)0.1468 (2)0.0561 (2)0.0231 (5)
H50.23920.07030.06640.028*
C60.2872 (2)0.2354 (2)0.1417 (2)0.0227 (5)
C70.2738 (2)0.3479 (2)0.1249 (2)0.0245 (6)
H70.30720.41140.18310.029*
C80.3584 (3)0.2077 (3)0.2485 (2)0.0293 (6)
C90.2579 (3)0.1980 (4)0.3195 (3)0.0512 (9)
H9A0.30380.17990.38730.077*
H9B0.17720.28320.34880.077*
H9C0.22840.12480.26770.077*
C100.4841 (3)0.0739 (3)0.2021 (3)0.0471 (8)
H10A0.53040.05560.26970.071*
H10B0.45400.00100.15060.071*
H10C0.54830.07970.15630.071*
C110.4082 (4)0.3183 (4)0.3318 (3)0.0555 (9)
H11A0.45360.29680.39830.083*
H11B0.47370.32430.28750.083*
H11C0.32910.40470.36290.083*
C120.1130 (2)0.0662 (2)0.1340 (2)0.0232 (5)
H12A0.15720.03210.21350.028*
H12B0.13960.01140.11310.028*
C130.0424 (2)0.1213 (2)0.1433 (2)0.0223 (5)
C140.0995 (2)0.1238 (2)0.2502 (2)0.0239 (6)
H140.03930.09360.31610.029*
C150.2413 (3)0.1690 (2)0.2644 (2)0.0255 (6)
C160.3253 (3)0.2084 (2)0.1666 (2)0.0266 (6)
H160.42230.23780.17410.032*
C170.2736 (2)0.2066 (2)0.0586 (2)0.0235 (5)
C180.1309 (2)0.1654 (2)0.0469 (2)0.0227 (5)
O30.07517 (17)0.15992 (17)0.05911 (14)0.0262 (4)
C190.3047 (3)0.1796 (3)0.3797 (2)0.0291 (6)
C200.4174 (4)0.1242 (5)0.4156 (3)0.0669 (11)
H20A0.45610.13200.48920.100*
H20B0.37850.02920.42880.100*
H20C0.49030.17550.35180.100*
C210.1966 (3)0.1030 (4)0.4847 (2)0.0553 (9)
H21A0.24120.11300.55600.083*
H21B0.12480.13990.46460.083*
H21C0.15480.00740.50030.083*
C220.3634 (4)0.3278 (3)0.3585 (3)0.0570 (10)
H22A0.40370.33660.43140.086*
H22B0.43480.38010.29330.086*
H22C0.28930.36170.33700.086*
C230.3723 (3)0.2521 (2)0.0429 (2)0.0273 (6)
H23A0.32070.22070.10370.033*
H23B0.44110.21040.01250.033*
O40.44276 (18)0.39600 (17)0.09784 (16)0.0323 (5)
C240.0170 (4)0.3774 (4)0.3440 (3)0.0750 (13)
H24A0.04510.41170.27830.090*
H24B0.01340.40270.40860.090*
C250.1415 (4)0.2974 (4)0.3455 (3)0.0510 (9)
H250.19910.26630.41340.061*
C260.2058 (3)0.2478 (3)0.2528 (2)0.0358 (7)
H26A0.28110.27960.21850.043*
H26B0.24610.14810.28940.043*
C270.2187 (4)0.3605 (4)0.3517 (3)0.0665 (11)
H27A0.28850.43380.33930.080*
H27B0.22380.34800.42140.080*
C280.1153 (3)0.2768 (3)0.2729 (3)0.0437 (8)
H280.04680.20430.28740.052*
C290.0998 (3)0.2897 (3)0.1610 (2)0.0325 (6)
H29A0.02140.31660.16600.039*
H29B0.18450.35980.15080.039*
H1OA0.39730.43540.00600.040*0.50
H1OB0.34560.51270.05940.040*0.50
H4OA0.39600.43490.07820.040*0.50
H4OB0.50730.41320.05270.040*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0306 (10)0.0334 (11)0.0489 (12)0.0147 (9)0.0023 (9)0.0206 (9)
C10.0243 (13)0.0265 (14)0.0338 (14)0.0101 (11)0.0010 (11)0.0141 (12)
C20.0192 (12)0.0231 (13)0.0248 (13)0.0069 (10)0.0009 (10)0.0107 (11)
C30.0172 (12)0.0281 (13)0.0210 (12)0.0062 (10)0.0015 (10)0.0126 (11)
O20.0252 (9)0.0351 (10)0.0263 (9)0.0119 (8)0.0055 (7)0.0179 (8)
C40.0169 (12)0.0262 (13)0.0240 (13)0.0081 (10)0.0000 (10)0.0110 (11)
C50.0211 (12)0.0227 (13)0.0254 (13)0.0073 (10)0.0010 (10)0.0105 (11)
C60.0186 (12)0.0250 (13)0.0205 (12)0.0056 (10)0.0006 (10)0.0081 (10)
C70.0241 (13)0.0251 (13)0.0243 (13)0.0118 (11)0.0024 (10)0.0084 (11)
C80.0322 (14)0.0328 (15)0.0253 (14)0.0130 (12)0.0070 (11)0.0153 (12)
C90.0503 (19)0.075 (2)0.0376 (17)0.0219 (18)0.0052 (15)0.0346 (17)
C100.0416 (18)0.0493 (19)0.0433 (18)0.0079 (15)0.0106 (14)0.0241 (16)
C110.079 (3)0.057 (2)0.0386 (18)0.0352 (19)0.0284 (17)0.0254 (16)
C120.0222 (13)0.0219 (13)0.0234 (13)0.0077 (11)0.0018 (10)0.0084 (10)
C130.0229 (13)0.0175 (12)0.0252 (13)0.0085 (10)0.0021 (10)0.0073 (10)
C140.0247 (13)0.0230 (13)0.0213 (13)0.0105 (11)0.0010 (10)0.0055 (10)
C150.0280 (14)0.0212 (13)0.0247 (13)0.0109 (11)0.0048 (11)0.0069 (11)
C160.0221 (13)0.0248 (13)0.0305 (14)0.0099 (11)0.0051 (11)0.0096 (11)
C170.0243 (13)0.0193 (12)0.0270 (13)0.0096 (10)0.0004 (10)0.0083 (11)
C180.0270 (13)0.0193 (12)0.0240 (13)0.0104 (11)0.0032 (10)0.0101 (10)
O30.0289 (10)0.0273 (10)0.0230 (9)0.0096 (8)0.0028 (7)0.0128 (8)
C190.0291 (14)0.0295 (14)0.0248 (14)0.0112 (12)0.0075 (11)0.0098 (11)
C200.073 (3)0.116 (3)0.054 (2)0.069 (3)0.0407 (19)0.052 (2)
C210.0484 (19)0.069 (2)0.0240 (16)0.0070 (17)0.0065 (14)0.0137 (16)
C220.085 (3)0.0399 (19)0.0326 (17)0.0137 (18)0.0187 (17)0.0165 (15)
C230.0232 (13)0.0263 (14)0.0327 (14)0.0091 (11)0.0001 (11)0.0125 (11)
O40.0310 (10)0.0283 (10)0.0362 (11)0.0106 (8)0.0063 (8)0.0108 (8)
C240.066 (3)0.093 (3)0.059 (2)0.001 (2)0.001 (2)0.051 (2)
C250.062 (2)0.061 (2)0.0325 (17)0.0170 (18)0.0015 (15)0.0259 (16)
C260.0363 (16)0.0427 (17)0.0277 (14)0.0124 (13)0.0020 (12)0.0155 (13)
C270.082 (3)0.081 (3)0.0354 (19)0.037 (2)0.0150 (19)0.0131 (19)
C280.0496 (19)0.0470 (19)0.0339 (16)0.0201 (16)0.0041 (14)0.0156 (14)
C290.0355 (15)0.0301 (15)0.0281 (14)0.0122 (12)0.0003 (12)0.0089 (12)
Geometric parameters (Å, º) top
O1—C11.440 (3)C15—C191.535 (3)
O1—H1OA0.8329C16—C171.388 (3)
O1—H1OB0.8200C16—H160.9500
C1—C21.500 (3)C17—C181.399 (3)
C1—H1A0.9900C17—C231.508 (3)
C1—H1B0.9900C18—O31.389 (3)
C2—C31.391 (3)O3—C291.464 (3)
C2—C71.395 (3)C19—C201.520 (4)
C3—O21.392 (3)C19—C221.529 (4)
C3—C41.399 (3)C19—C211.539 (4)
O2—C261.436 (3)C20—H20A0.9800
C4—C51.392 (3)C20—H20B0.9800
C4—C121.513 (3)C20—H20C0.9800
C5—C61.393 (3)C21—H21A0.9800
C5—H50.9500C21—H21B0.9800
C6—C71.394 (3)C21—H21C0.9800
C6—C81.536 (3)C22—H22A0.9800
C7—H70.9500C22—H22B0.9800
C8—C111.529 (4)C22—H22C0.9800
C8—C91.533 (4)C23—O41.437 (3)
C8—C101.534 (4)C23—H23A0.9900
C9—H9A0.9800C23—H23B0.9900
C9—H9B0.9800O4—H4OA0.9127
C9—H9C0.9800O4—H4OB0.8446
C10—H10A0.9800C24—C251.278 (5)
C10—H10B0.9800C24—H24A0.9500
C10—H10C0.9800C24—H24B0.9500
C11—H11A0.9800C25—C261.483 (4)
C11—H11B0.9800C25—H250.9500
C11—H11C0.9800C26—H26A0.9900
C12—C131.519 (3)C26—H26B0.9900
C12—H12A0.9900C27—C281.309 (4)
C12—H12B0.9900C27—H27A0.9500
C13—C181.393 (3)C27—H27B0.9500
C13—C141.394 (3)C28—C291.498 (4)
C14—C151.395 (3)C28—H280.9500
C14—H140.9500C29—H29A0.9900
C15—C161.393 (3)C29—H29B0.9900
C1—O1—H1OA103.6C17—C16—C15122.9 (2)
C1—O1—H1OB114.1C17—C16—H16118.5
H1OA—O1—H1OB114.6C15—C16—H16118.5
O1—C1—C2108.52 (19)C16—C17—C18118.5 (2)
O1—C1—H1A110.0C16—C17—C23119.3 (2)
C2—C1—H1A110.0C18—C17—C23122.2 (2)
O1—C1—H1B110.0O3—C18—C13119.1 (2)
C2—C1—H1B110.0O3—C18—C17120.2 (2)
H1A—C1—H1B108.4C13—C18—C17120.6 (2)
C3—C2—C7118.4 (2)C18—O3—C29116.10 (18)
C3—C2—C1121.8 (2)C20—C19—C22110.3 (3)
C7—C2—C1119.7 (2)C20—C19—C15111.0 (2)
C2—C3—O2120.1 (2)C22—C19—C15108.2 (2)
C2—C3—C4121.4 (2)C20—C19—C21108.2 (3)
O2—C3—C4118.5 (2)C22—C19—C21106.8 (3)
C3—O2—C26112.68 (18)C15—C19—C21112.2 (2)
C5—C4—C3117.8 (2)C19—C20—H20A109.5
C5—C4—C12120.8 (2)C19—C20—H20B109.5
C3—C4—C12121.4 (2)H20A—C20—H20B109.5
C4—C5—C6122.9 (2)C19—C20—H20C109.5
C4—C5—H5118.5H20A—C20—H20C109.5
C6—C5—H5118.5H20B—C20—H20C109.5
C5—C6—C7116.9 (2)C19—C21—H21A109.5
C5—C6—C8120.6 (2)C19—C21—H21B109.5
C7—C6—C8122.5 (2)H21A—C21—H21B109.5
C6—C7—C2122.5 (2)C19—C21—H21C109.5
C6—C7—H7118.8H21A—C21—H21C109.5
C2—C7—H7118.8H21B—C21—H21C109.5
C11—C8—C9108.9 (2)C19—C22—H22A109.5
C11—C8—C10108.2 (2)C19—C22—H22B109.5
C9—C8—C10109.3 (2)H22A—C22—H22B109.5
C11—C8—C6111.8 (2)C19—C22—H22C109.5
C9—C8—C6109.7 (2)H22A—C22—H22C109.5
C10—C8—C6108.9 (2)H22B—C22—H22C109.5
C8—C9—H9A109.5O4—C23—C17112.0 (2)
C8—C9—H9B109.5O4—C23—H23A109.2
H9A—C9—H9B109.5C17—C23—H23A109.2
C8—C9—H9C109.5O4—C23—H23B109.2
H9A—C9—H9C109.5C17—C23—H23B109.2
H9B—C9—H9C109.5H23A—C23—H23B107.9
C8—C10—H10A109.5C23—O4—H4OA109.5
C8—C10—H10B109.5C23—O4—H4OB104.6
H10A—C10—H10B109.5H4OA—O4—H4OB93.5
C8—C10—H10C109.5C25—C24—H24A120.0
H10A—C10—H10C109.5C25—C24—H24B120.0
H10B—C10—H10C109.5H24A—C24—H24B120.0
C8—C11—H11A109.5C24—C25—C26127.1 (3)
C8—C11—H11B109.5C24—C25—H25116.5
H11A—C11—H11B109.5C26—C25—H25116.5
C8—C11—H11C109.5O2—C26—C25110.4 (2)
H11A—C11—H11C109.5O2—C26—H26A109.6
H11B—C11—H11C109.5C25—C26—H26A109.6
C4—C12—C13115.50 (19)O2—C26—H26B109.6
C4—C12—H12A108.4C25—C26—H26B109.6
C13—C12—H12A108.4H26A—C26—H26B108.1
C4—C12—H12B108.4C28—C27—H27A120.0
C13—C12—H12B108.4C28—C27—H27B120.0
H12A—C12—H12B107.5H27A—C27—H27B120.0
C18—C13—C14118.5 (2)C27—C28—C29123.2 (3)
C18—C13—C12120.8 (2)C27—C28—H28118.4
C14—C13—C12120.6 (2)C29—C28—H28118.4
C13—C14—C15122.8 (2)O3—C29—C28108.9 (2)
C13—C14—H14118.6O3—C29—H29A109.9
C15—C14—H14118.6C28—C29—H29A109.9
C16—C15—C14116.6 (2)O3—C29—H29B109.9
C16—C15—C19120.6 (2)C28—C29—H29B109.9
C14—C15—C19122.8 (2)H29A—C29—H29B108.3
O1—C1—C2—C394.7 (3)C18—C13—C14—C150.2 (4)
O1—C1—C2—C781.6 (3)C12—C13—C14—C15177.7 (2)
C7—C2—C3—O2179.0 (2)C13—C14—C15—C162.0 (4)
C1—C2—C3—O22.7 (3)C13—C14—C15—C19176.4 (2)
C7—C2—C3—C42.3 (3)C14—C15—C16—C171.4 (4)
C1—C2—C3—C4178.5 (2)C19—C15—C16—C17177.0 (2)
C2—C3—O2—C2683.1 (3)C15—C16—C17—C181.0 (4)
C4—C3—O2—C2698.2 (3)C15—C16—C17—C23179.5 (2)
C2—C3—C4—C52.8 (3)C14—C13—C18—O3178.3 (2)
O2—C3—C4—C5178.4 (2)C12—C13—C18—O30.8 (3)
C2—C3—C4—C12178.0 (2)C14—C13—C18—C172.3 (3)
O2—C3—C4—C120.7 (3)C12—C13—C18—C17175.2 (2)
C3—C4—C5—C61.0 (3)C16—C17—C18—O3178.8 (2)
C12—C4—C5—C6179.9 (2)C23—C17—C18—O32.7 (3)
C4—C5—C6—C71.3 (3)C16—C17—C18—C132.9 (3)
C4—C5—C6—C8178.5 (2)C23—C17—C18—C13178.6 (2)
C5—C6—C7—C21.9 (3)C13—C18—O3—C29112.4 (2)
C8—C6—C7—C2177.8 (2)C17—C18—O3—C2971.6 (3)
C3—C2—C7—C60.2 (3)C16—C15—C19—C2046.1 (3)
C1—C2—C7—C6176.2 (2)C14—C15—C19—C20135.6 (3)
C5—C6—C8—C11179.2 (2)C16—C15—C19—C2275.1 (3)
C7—C6—C8—C111.0 (3)C14—C15—C19—C22103.2 (3)
C5—C6—C8—C958.4 (3)C16—C15—C19—C21167.3 (3)
C7—C6—C8—C9121.9 (3)C14—C15—C19—C2114.4 (4)
C5—C6—C8—C1061.3 (3)C16—C17—C23—O475.1 (3)
C7—C6—C8—C10118.5 (3)C18—C17—C23—O4103.3 (3)
C5—C4—C12—C13114.7 (2)C3—O2—C26—C25166.8 (2)
C3—C4—C12—C1366.2 (3)C24—C25—C26—O23.8 (5)
C4—C12—C13—C1863.8 (3)C18—O3—C29—C28145.7 (2)
C4—C12—C13—C14118.7 (2)C27—C28—C29—O3129.3 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1OB···O4i0.821.992.749 (2)155
O1—H1OA···O4ii0.831.932.744 (3)166
O4—H4OA···O1i0.911.852.749 (2)167
O4—H4OB···O1iii0.841.902.744 (3)177
Symmetry codes: (i) x, y+1, z; (ii) x+1, y, z; (iii) x1, y, z.
(III) 2,2'-bis(allyloxy)-5,5'-di-tert-butyl-3,3'-methanediyldibenzaldehyde top
Crystal data top
C29H36O4F(000) = 968
Mr = 448.58Dx = 1.150 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 16.2931 (10) ÅCell parameters from 7890 reflections
b = 10.1951 (6) Åθ = 2.4–23.3°
c = 16.4318 (10) ŵ = 0.08 mm1
β = 108.367 (1)°T = 150 K
V = 2590.4 (3) Å3Block, pale yellow
Z = 40.26 × 0.16 × 0.14 mm
Data collection top
Bruker SMART 1000 CCD area-detector
diffractometer
4559 independent reflections
Radiation source: normal-focus sealed tube3620 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.020
ω scansθmax = 25.0°, θmin = 1.3°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2001)
h = 1919
Tmin = 0.900, Tmax = 1.000k = 1212
17928 measured reflectionsl = 1919
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)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.123H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.058P)2 + 1.0861P]
where P = (Fo2 + 2Fc2)/3
4559 reflections(Δ/σ)max = 0.001
317 parametersΔρmax = 0.29 e Å3
0 restraintsΔρmin = 0.18 e Å3
Crystal data top
C29H36O4V = 2590.4 (3) Å3
Mr = 448.58Z = 4
Monoclinic, P21/cMo Kα radiation
a = 16.2931 (10) ŵ = 0.08 mm1
b = 10.1951 (6) ÅT = 150 K
c = 16.4318 (10) Å0.26 × 0.16 × 0.14 mm
β = 108.367 (1)°
Data collection top
Bruker SMART 1000 CCD area-detector
diffractometer
4559 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2001)
3620 reflections with I > 2σ(I)
Tmin = 0.900, Tmax = 1.000Rint = 0.020
17928 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.123H-atom parameters constrained
S = 1.02Δρmax = 0.29 e Å3
4559 reflectionsΔρmin = 0.18 e Å3
317 parameters
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O10.63607 (10)0.33380 (15)1.08524 (9)0.0608 (4)
O40.86478 (9)0.34770 (14)0.45857 (8)0.0534 (4)
C10.67472 (13)0.38088 (19)1.04065 (11)0.0462 (5)
H10.71230.45261.06280.055*
C20.66705 (10)0.33351 (16)0.95351 (10)0.0342 (4)
C30.70349 (10)0.40326 (15)0.90068 (10)0.0317 (4)
C40.69296 (9)0.36070 (15)0.81739 (10)0.0288 (3)
C50.64915 (9)0.24344 (16)0.79061 (10)0.0310 (4)
H50.64290.21280.73440.037*
C60.61386 (9)0.16860 (16)0.84255 (10)0.0323 (4)
C70.62221 (10)0.21718 (17)0.92370 (10)0.0351 (4)
H70.59690.17040.95980.042*
C80.56911 (11)0.03898 (18)0.80846 (12)0.0428 (4)
C90.52995 (14)0.0256 (2)0.87163 (14)0.0608 (6)
H9A0.50150.10780.84710.091*
H9B0.48740.03360.88280.091*
H9C0.57580.04410.92550.091*
C100.49717 (13)0.0616 (2)0.72365 (12)0.0570 (5)
H10A0.46900.02210.70220.085*
H10B0.52190.09890.68160.085*
H10C0.45440.12260.73280.085*
C110.63634 (14)0.0536 (2)0.79162 (18)0.0707 (7)
H11A0.60870.13700.76890.106*
H11B0.68300.06940.84540.106*
H11C0.66030.01340.74980.106*
C120.72087 (10)0.44424 (16)0.75498 (11)0.0342 (4)
H12A0.75190.52180.78610.041*
H12B0.66840.47640.71040.041*
C130.77824 (9)0.37788 (14)0.71076 (9)0.0272 (3)
C140.83411 (9)0.27642 (14)0.74857 (9)0.0273 (3)
H140.83500.24630.80360.033*
C150.88930 (9)0.21633 (15)0.70929 (10)0.0291 (3)
C160.88543 (10)0.26107 (15)0.62858 (10)0.0307 (3)
H160.92250.22300.60050.037*
C170.82869 (10)0.36046 (15)0.58740 (10)0.0302 (3)
C180.77561 (9)0.41923 (14)0.62884 (10)0.0285 (3)
C190.94943 (10)0.10569 (16)0.75587 (11)0.0358 (4)
C201.00889 (12)0.05833 (19)0.70575 (12)0.0476 (5)
H20A1.04590.01260.73750.071*
H20B1.04510.13130.69840.071*
H20C0.97370.02610.64940.071*
C211.00683 (11)0.1551 (2)0.84346 (11)0.0465 (5)
H21A0.97030.18660.87670.070*
H21B1.04330.22710.83520.070*
H21C1.04350.08330.87440.070*
C220.89451 (13)0.00976 (18)0.76842 (14)0.0501 (5)
H22A0.85630.01970.80040.075*
H22B0.93250.07950.80050.075*
H22C0.85960.04340.71230.075*
C230.82405 (11)0.40009 (17)0.49972 (11)0.0392 (4)
H230.78690.47080.47410.047*
O20.74638 (8)0.52087 (11)0.92911 (7)0.0401 (3)
C240.84626 (18)0.7420 (2)0.93001 (16)0.0698 (7)
H24A0.78580.74400.90090.084*
H24B0.87960.81980.93500.084*
C250.88268 (15)0.6348 (2)0.96244 (14)0.0573 (5)
H250.94320.63750.99100.069*
C260.83900 (13)0.50676 (19)0.95959 (15)0.0577 (6)
H26A0.85720.44640.92130.069*
H26B0.85680.46781.01770.069*
O30.71578 (7)0.51227 (10)0.58584 (7)0.0357 (3)
C270.6204 (3)0.8014 (4)0.5349 (3)0.0694 (10)0.70
H27A0.64450.81790.49020.083*0.70
H27B0.56820.84360.53440.083*0.70
C280.6583 (3)0.7218 (4)0.5960 (3)0.0572 (9)0.70
H280.63120.70920.63890.069*0.70
C290.73933 (12)0.64767 (16)0.60730 (12)0.0444 (4)0.70
H29A0.77040.68340.56920.053*0.70
H29B0.77760.65450.66740.053*0.70
C27'0.6173 (11)0.7853 (16)0.5874 (11)0.113 (5)0.30
H27C0.62300.76730.64560.136*0.30
H27D0.57240.84110.55450.136*0.30
C28'0.6708 (5)0.7338 (8)0.5528 (7)0.0506 (19)0.30
H28'0.66620.75060.49470.061*0.30
C29'0.73933 (12)0.64767 (16)0.60730 (12)0.0444 (4)0.30
H29C0.79510.66720.59770.053*0.30
H29D0.74620.66350.66850.053*0.30
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0847 (10)0.0650 (9)0.0419 (7)0.0187 (8)0.0331 (7)0.0085 (7)
O40.0657 (9)0.0631 (9)0.0403 (7)0.0012 (7)0.0293 (7)0.0014 (6)
C10.0606 (12)0.0427 (10)0.0356 (9)0.0168 (9)0.0158 (9)0.0044 (8)
C20.0355 (8)0.0363 (9)0.0302 (8)0.0101 (7)0.0093 (7)0.0024 (7)
C30.0300 (8)0.0286 (8)0.0345 (8)0.0064 (7)0.0072 (7)0.0006 (7)
C40.0233 (7)0.0316 (8)0.0324 (8)0.0063 (6)0.0100 (6)0.0023 (7)
C50.0253 (8)0.0377 (9)0.0292 (8)0.0035 (7)0.0077 (6)0.0024 (7)
C60.0225 (7)0.0363 (9)0.0365 (9)0.0022 (6)0.0070 (7)0.0021 (7)
C70.0303 (8)0.0409 (9)0.0358 (9)0.0062 (7)0.0128 (7)0.0090 (7)
C80.0337 (9)0.0420 (10)0.0498 (10)0.0076 (8)0.0092 (8)0.0008 (8)
C90.0595 (13)0.0555 (13)0.0609 (13)0.0213 (10)0.0099 (10)0.0109 (10)
C100.0489 (11)0.0653 (13)0.0498 (11)0.0255 (10)0.0056 (9)0.0017 (10)
C110.0572 (13)0.0431 (12)0.109 (2)0.0097 (10)0.0217 (13)0.0260 (12)
C120.0342 (8)0.0317 (9)0.0400 (9)0.0062 (7)0.0165 (7)0.0034 (7)
C130.0243 (7)0.0261 (8)0.0309 (8)0.0034 (6)0.0084 (6)0.0014 (6)
C140.0255 (7)0.0292 (8)0.0276 (7)0.0019 (6)0.0089 (6)0.0010 (6)
C150.0252 (7)0.0295 (8)0.0329 (8)0.0017 (6)0.0095 (6)0.0010 (6)
C160.0295 (8)0.0321 (8)0.0336 (8)0.0019 (7)0.0144 (7)0.0047 (7)
C170.0316 (8)0.0294 (8)0.0293 (8)0.0065 (6)0.0091 (7)0.0014 (6)
C180.0257 (7)0.0254 (8)0.0314 (8)0.0034 (6)0.0046 (6)0.0002 (6)
C190.0335 (8)0.0368 (9)0.0401 (9)0.0075 (7)0.0158 (7)0.0050 (7)
C200.0442 (10)0.0514 (11)0.0510 (11)0.0208 (9)0.0204 (9)0.0065 (9)
C210.0377 (9)0.0572 (12)0.0416 (10)0.0153 (9)0.0085 (8)0.0071 (9)
C220.0515 (11)0.0352 (10)0.0674 (13)0.0097 (8)0.0244 (10)0.0117 (9)
C230.0450 (10)0.0392 (9)0.0340 (9)0.0080 (8)0.0135 (8)0.0002 (7)
O20.0458 (7)0.0293 (6)0.0416 (7)0.0021 (5)0.0086 (5)0.0048 (5)
C240.0963 (18)0.0447 (12)0.0846 (17)0.0022 (12)0.0518 (15)0.0034 (12)
C250.0648 (13)0.0463 (12)0.0629 (13)0.0108 (10)0.0232 (11)0.0115 (10)
C260.0475 (11)0.0402 (11)0.0708 (14)0.0048 (9)0.0022 (10)0.0021 (10)
O30.0379 (6)0.0285 (6)0.0364 (6)0.0024 (5)0.0055 (5)0.0039 (5)
C270.060 (2)0.0344 (18)0.103 (3)0.0072 (17)0.011 (2)0.008 (2)
C280.076 (3)0.0338 (18)0.074 (3)0.0125 (16)0.041 (2)0.0073 (19)
C290.0538 (11)0.0277 (9)0.0513 (11)0.0033 (8)0.0161 (9)0.0038 (8)
C27'0.145 (12)0.088 (9)0.138 (13)0.024 (8)0.091 (11)0.042 (9)
C28'0.060 (5)0.036 (4)0.063 (5)0.004 (4)0.029 (4)0.010 (4)
C29'0.0538 (11)0.0277 (9)0.0513 (11)0.0033 (8)0.0161 (9)0.0038 (8)
Geometric parameters (Å, º) top
O1—C11.206 (2)C16—H160.9500
O4—C231.211 (2)C17—C181.394 (2)
C1—C21.479 (2)C17—C231.475 (2)
C1—H10.9500C18—O31.3839 (18)
C2—C31.392 (2)C19—C221.531 (2)
C2—C71.398 (2)C19—C211.534 (2)
C3—O21.3923 (19)C19—C201.534 (2)
C3—C41.394 (2)C20—H20A0.9800
C4—C51.391 (2)C20—H20B0.9800
C4—C121.509 (2)C20—H20C0.9800
C5—C61.397 (2)C21—H21A0.9800
C5—H50.9500C21—H21B0.9800
C6—C71.388 (2)C21—H21C0.9800
C6—C81.528 (2)C22—H22A0.9800
C7—H70.9500C22—H22B0.9800
C8—C91.528 (3)C22—H22C0.9800
C8—C101.530 (3)C23—H230.9500
C8—C111.535 (3)O2—C261.440 (2)
C9—H9A0.9800C26—C251.481 (3)
C9—H9B0.9800C26—H26A0.9900
C9—H9C0.9800C26—H26B0.9900
C10—H10A0.9800C25—C241.277 (3)
C10—H10B0.9800C25—H250.9500
C10—H10C0.9800C24—H24A0.9500
C11—H11A0.9800C24—H24B0.9500
C11—H11B0.9800O3—C291.446 (2)
C11—H11C0.9800C29—C281.481 (5)
C12—C131.513 (2)C29—H29A0.9900
C12—H12A0.9900C29—H29B0.9900
C12—H12B0.9900C28—C271.289 (6)
C13—C141.389 (2)C28—H280.9500
C13—C181.398 (2)C27—H27A0.9500
C14—C151.402 (2)C27—H27B0.9500
C14—H140.9500C28'—C27'1.291 (17)
C15—C161.385 (2)C28'—H28'0.9500
C15—C191.531 (2)C27'—H27C0.9500
C16—C171.395 (2)C27'—H27D0.9500
O1—C1—C2123.87 (19)C18—C17—C16119.59 (14)
O1—C1—H1118.1C18—C17—C23120.72 (15)
C2—C1—H1118.1C16—C17—C23119.67 (14)
C3—C2—C7119.57 (15)O3—C18—C17119.40 (13)
C3—C2—C1120.97 (16)O3—C18—C13120.08 (13)
C7—C2—C1119.45 (16)C17—C18—C13120.35 (14)
C2—C3—O2119.90 (14)C22—C19—C15108.93 (13)
C2—C3—C4120.58 (15)C22—C19—C21109.61 (15)
O2—C3—C4119.40 (14)C15—C19—C21109.38 (14)
C5—C4—C3118.05 (14)C22—C19—C20108.97 (15)
C5—C4—C12120.31 (14)C15—C19—C20112.11 (14)
C3—C4—C12121.42 (14)C21—C19—C20107.81 (14)
C4—C5—C6123.05 (14)C19—C20—H20A109.5
C4—C5—H5118.5C19—C20—H20B109.5
C6—C5—H5118.5H20A—C20—H20B109.5
C7—C6—C5117.22 (15)C19—C20—H20C109.5
C7—C6—C8123.49 (15)H20A—C20—H20C109.5
C5—C6—C8119.29 (15)H20B—C20—H20C109.5
C6—C7—C2121.42 (15)C19—C21—H21A109.5
C6—C7—H7119.3C19—C21—H21B109.5
C2—C7—H7119.3H21A—C21—H21B109.5
C6—C8—C9112.13 (16)C19—C21—H21C109.5
C6—C8—C10110.10 (15)H21A—C21—H21C109.5
C9—C8—C10108.64 (15)H21B—C21—H21C109.5
C6—C8—C11108.22 (14)C19—C22—H22A109.5
C9—C8—C11109.38 (18)C19—C22—H22B109.5
C10—C8—C11108.31 (18)H22A—C22—H22B109.5
C8—C9—H9A109.5C19—C22—H22C109.5
C8—C9—H9B109.5H22A—C22—H22C109.5
H9A—C9—H9B109.5H22B—C22—H22C109.5
C8—C9—H9C109.5O4—C23—C17123.79 (17)
H9A—C9—H9C109.5O4—C23—H23118.1
H9B—C9—H9C109.5C17—C23—H23118.1
C8—C10—H10A109.5C3—O2—C26113.02 (12)
C8—C10—H10B109.5O2—C26—C25111.32 (17)
H10A—C10—H10B109.5O2—C26—H26A109.4
C8—C10—H10C109.5C25—C26—H26A109.4
H10A—C10—H10C109.5O2—C26—H26B109.4
H10B—C10—H10C109.5C25—C26—H26B109.4
C8—C11—H11A109.5H26A—C26—H26B108.0
C8—C11—H11B109.5C24—C25—C26125.9 (2)
H11A—C11—H11B109.5C24—C25—H25117.1
C8—C11—H11C109.5C26—C25—H25117.1
H11A—C11—H11C109.5C25—C24—H24A120.0
H11B—C11—H11C109.5C25—C24—H24B120.0
C4—C12—C13115.99 (13)H24A—C24—H24B120.0
C4—C12—H12A108.3C18—O3—C29116.08 (12)
C13—C12—H12A108.3O3—C29—C28107.39 (19)
C4—C12—H12B108.3O3—C29—H29A110.2
C13—C12—H12B108.3C28—C29—H29A110.2
H12A—C12—H12B107.4O3—C29—H29B110.2
C14—C13—C18118.18 (14)C28—C29—H29B110.2
C14—C13—C12122.38 (13)H29A—C29—H29B108.5
C18—C13—C12119.44 (13)C27—C28—C29127.5 (6)
C13—C14—C15122.99 (14)C27—C28—H28116.3
C13—C14—H14118.5C29—C28—H28116.3
C15—C14—H14118.5C28—C27—H27A120.0
C16—C15—C14117.04 (14)C28—C27—H27B120.0
C16—C15—C19123.37 (14)H27A—C27—H27B120.0
C14—C15—C19119.59 (13)C27'—C28'—H28'121.3
C15—C16—C17121.81 (14)C28'—C27'—H27C120.0
C15—C16—H16119.1C28'—C27'—H27D120.0
C17—C16—H16119.1H27C—C27'—H27D120.0
O1—C1—C2—C3170.72 (16)C13—C14—C15—C161.0 (2)
O1—C1—C2—C79.0 (3)C13—C14—C15—C19179.52 (14)
C7—C2—C3—O2178.41 (13)C14—C15—C16—C170.7 (2)
C1—C2—C3—O21.3 (2)C19—C15—C16—C17178.78 (14)
C7—C2—C3—C42.3 (2)C15—C16—C17—C181.6 (2)
C1—C2—C3—C4177.39 (14)C15—C16—C17—C23177.01 (14)
C2—C3—C4—C53.3 (2)C16—C17—C18—O3176.18 (13)
O2—C3—C4—C5179.43 (13)C23—C17—C18—O32.4 (2)
C2—C3—C4—C12171.27 (14)C16—C17—C18—C130.8 (2)
O2—C3—C4—C124.8 (2)C23—C17—C18—C13177.74 (14)
C3—C4—C5—C61.5 (2)C14—C13—C18—O3174.56 (13)
C12—C4—C5—C6173.22 (14)C12—C13—C18—O35.5 (2)
C4—C5—C6—C71.4 (2)C14—C13—C18—C170.7 (2)
C4—C5—C6—C8178.22 (14)C12—C13—C18—C17179.24 (14)
C5—C6—C7—C22.5 (2)C16—C15—C19—C22116.42 (17)
C8—C6—C7—C2177.14 (14)C14—C15—C19—C2263.02 (19)
C3—C2—C7—C60.7 (2)C16—C15—C19—C21123.80 (16)
C1—C2—C7—C6179.59 (15)C14—C15—C19—C2156.76 (19)
C7—C6—C8—C93.7 (2)C16—C15—C19—C204.3 (2)
C5—C6—C8—C9176.71 (15)C14—C15—C19—C20176.29 (15)
C7—C6—C8—C10124.76 (18)C18—C17—C23—O4175.62 (16)
C5—C6—C8—C1055.6 (2)C16—C17—C23—O43.0 (3)
C7—C6—C8—C11117.05 (19)C2—C3—O2—C26100.36 (18)
C5—C6—C8—C1162.6 (2)C4—C3—O2—C2683.54 (18)
C5—C4—C12—C1356.86 (19)C3—O2—C26—C25161.55 (16)
C3—C4—C12—C13128.65 (15)O2—C26—C25—C2410.7 (3)
C4—C12—C13—C1429.0 (2)C17—C18—O3—C29101.49 (17)
C4—C12—C13—C18150.97 (14)C13—C18—O3—C2983.16 (18)
C18—C13—C14—C151.7 (2)C18—O3—C29—C28149.5 (2)
C12—C13—C14—C15178.28 (14)O3—C29—C28—C27105.6 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C5—H5···O1i0.952.463.406 (2)171
C14—H14···O4ii0.952.623.560 (2)170
Symmetry codes: (i) x, y+1/2, z1/2; (ii) x, y+1/2, z+1/2.
(IVa) 5,5'-di-tert-butyl-2,2'-dihydroxy-3,3'-methanediyldibenzaldehyde top
Crystal data top
C23H28O4Dx = 1.238 Mg m3
Mr = 368.45Mo Kα radiation, λ = 0.71073 Å
Tetragonal, I41/aCell parameters from 3205 reflections
a = 12.7930 (7) Åθ = 2.8–22.8°
c = 24.158 (2) ŵ = 0.08 mm1
V = 3953.7 (4) Å3T = 150 K
Z = 8Block ## AUTHOR: Tablet?, yellow
F(000) = 15840.28 × 0.20 × 0.05 mm
Data collection top
Bruker SMART 1000 CCD area-detector
diffractometer
1736 independent reflections
Radiation source: normal-focus sealed tube1203 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.056
ϕ and ω scansθmax = 25.0°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2001)
h = 1515
Tmin = 0.931, Tmax = 1.000k = 1515
19093 measured reflectionsl = 2828
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)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.120H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0446P)2 + 4.6694P]
where P = (Fo2 + 2Fc2)/3
1736 reflections(Δ/σ)max < 0.001
125 parametersΔρmax = 0.19 e Å3
0 restraintsΔρmin = 0.21 e Å3
Crystal data top
C23H28O4Z = 8
Mr = 368.45Mo Kα radiation
Tetragonal, I41/aµ = 0.08 mm1
a = 12.7930 (7) ÅT = 150 K
c = 24.158 (2) Å0.28 × 0.20 × 0.05 mm
V = 3953.7 (4) Å3
Data collection top
Bruker SMART 1000 CCD area-detector
diffractometer
1736 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2001)
1203 reflections with I > 2σ(I)
Tmin = 0.931, Tmax = 1.000Rint = 0.056
19093 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.120H-atom parameters constrained
S = 1.04Δρmax = 0.19 e Å3
1736 reflectionsΔρmin = 0.21 e Å3
125 parameters
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O10.91517 (13)0.36217 (12)0.07535 (7)0.0529 (5)
C11.00238 (18)0.38549 (17)0.05825 (10)0.0448 (6)
H11.04060.33320.03900.054*
C21.05164 (16)0.48672 (16)0.06515 (9)0.0359 (5)
C30.99989 (15)0.56794 (16)0.09323 (9)0.0359 (5)
O20.90144 (11)0.55533 (13)0.11373 (7)0.0472 (4)
H20.8850 (17)0.4864 (18)0.1065 (9)0.040*
C41.05026 (15)0.66379 (15)0.10117 (8)0.0332 (5)
C51.14976 (15)0.67573 (16)0.07960 (8)0.0342 (5)
H51.18400.74080.08510.041*
C61.20321 (15)0.59785 (15)0.05009 (8)0.0332 (5)
C71.15190 (16)0.50302 (16)0.04417 (9)0.0364 (5)
H71.18600.44760.02530.044*
C81.31390 (16)0.61729 (16)0.02875 (9)0.0379 (5)
C91.3448 (2)0.5401 (2)0.01681 (11)0.0575 (7)
H9A1.41610.55540.02930.086*
H9B1.29640.54690.04810.086*
H9C1.34180.46870.00220.086*
C101.39030 (18)0.6054 (2)0.07729 (11)0.0560 (7)
H10A1.37130.65440.10680.084*
H10B1.46150.62040.06460.084*
H10C1.38700.53370.09150.084*
C111.3234 (2)0.72779 (19)0.00507 (9)0.0584 (7)
H11A1.30390.77880.03350.088*
H11B1.27680.73500.02690.088*
H11C1.39580.74030.00660.088*
C121.00000.750000.13460 (9)0.0367 (7)
H12A0.94610.71860.15890.044*0.50
H12B1.05390.78140.15890.044*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0454 (10)0.0437 (10)0.0695 (12)0.0126 (7)0.0040 (8)0.0090 (8)
C10.0448 (14)0.0360 (13)0.0535 (14)0.0042 (10)0.0042 (11)0.0074 (10)
C20.0349 (11)0.0302 (11)0.0425 (12)0.0024 (9)0.0028 (9)0.0062 (9)
C30.0276 (11)0.0394 (12)0.0408 (12)0.0022 (9)0.0014 (9)0.0069 (9)
O20.0334 (9)0.0452 (10)0.0629 (11)0.0046 (7)0.0061 (7)0.0008 (8)
C40.0335 (11)0.0312 (11)0.0350 (11)0.0047 (9)0.0025 (9)0.0020 (9)
C50.0345 (11)0.0293 (11)0.0390 (12)0.0003 (9)0.0015 (9)0.0029 (9)
C60.0303 (11)0.0304 (11)0.0388 (12)0.0016 (8)0.0005 (9)0.0038 (9)
C70.0378 (12)0.0285 (11)0.0428 (12)0.0042 (9)0.0001 (9)0.0014 (9)
C80.0330 (11)0.0328 (11)0.0478 (12)0.0013 (9)0.0046 (10)0.0002 (10)
C90.0472 (14)0.0562 (16)0.0691 (18)0.0016 (12)0.0199 (13)0.0177 (13)
C100.0350 (13)0.0681 (17)0.0649 (17)0.0004 (12)0.0030 (12)0.0025 (14)
C110.0546 (16)0.0455 (14)0.0750 (18)0.0014 (11)0.0242 (14)0.0121 (13)
C120.0348 (16)0.0377 (17)0.0377 (16)0.0049 (13)0.0000.000
Geometric parameters (Å, º) top
O1—C11.227 (3)C8—C91.530 (3)
C1—C21.450 (3)C8—C111.530 (3)
C1—H10.9500C8—C101.534 (3)
C2—C71.395 (3)C9—H9A0.9800
C2—C31.406 (3)C9—H9B0.9800
C3—O21.363 (2)C9—H9C0.9800
C3—C41.399 (3)C10—H10A0.9800
O2—H20.92 (2)C10—H10B0.9800
C4—C51.384 (3)C10—H10C0.9800
C4—C121.511 (3)C11—H11A0.9800
C5—C61.403 (3)C11—H11B0.9800
C5—H50.9500C11—H11C0.9800
C6—C71.387 (3)C12—C4i1.510 (3)
C6—C81.527 (3)C12—H12A0.9900
C7—H70.9500C12—H12B0.9900
O1—C1—C2125.0 (2)C9—C8—C10108.7 (2)
O1—C1—H1117.5C11—C8—C10109.05 (19)
C2—C1—H1117.5C8—C9—H9A109.5
C7—C2—C3119.83 (19)C8—C9—H9B109.5
C7—C2—C1119.4 (2)H9A—C9—H9B109.5
C3—C2—C1120.7 (2)C8—C9—H9C109.5
O2—C3—C4118.67 (19)H9A—C9—H9C109.5
O2—C3—C2121.52 (19)H9B—C9—H9C109.5
C4—C3—C2119.81 (18)C8—C10—H10A109.5
C3—O2—H2104.7 (14)C8—C10—H10B109.5
C5—C4—C3117.98 (19)H10A—C10—H10B109.5
C5—C4—C12120.80 (19)C8—C10—H10C109.5
C3—C4—C12121.16 (19)H10A—C10—H10C109.5
C4—C5—C6124.13 (19)H10B—C10—H10C109.5
C4—C5—H5117.9C8—C11—H11A109.5
C6—C5—H5117.9C8—C11—H11B109.5
C7—C6—C5116.30 (19)H11A—C11—H11B109.5
C7—C6—C8123.13 (18)C8—C11—H11C109.5
C5—C6—C8120.51 (18)H11A—C11—H11C109.5
C6—C7—C2121.9 (2)H11B—C11—H11C109.5
C6—C7—H7119.0C4i—C12—C4115.4 (2)
C2—C7—H7119.0C4i—C12—H12A108.4
C6—C8—C9112.16 (18)C4—C12—H12A108.4
C6—C8—C11110.52 (17)C4i—C12—H12B108.4
C9—C8—C11107.88 (19)C4—C12—H12B108.4
C6—C8—C10108.48 (19)H12A—C12—H12B107.5
O1—C1—C2—C7179.3 (2)C4—C5—C6—C8178.80 (19)
O1—C1—C2—C30.1 (4)C5—C6—C7—C21.6 (3)
C7—C2—C3—O2179.23 (19)C8—C6—C7—C2178.56 (19)
C1—C2—C3—O21.5 (3)C3—C2—C7—C60.0 (3)
C7—C2—C3—C41.6 (3)C1—C2—C7—C6179.3 (2)
C1—C2—C3—C4177.7 (2)C7—C6—C8—C921.4 (3)
O2—C3—C4—C5179.34 (18)C5—C6—C8—C9161.8 (2)
C2—C3—C4—C51.4 (3)C7—C6—C8—C11141.8 (2)
O2—C3—C4—C123.6 (3)C5—C6—C8—C1141.4 (3)
C2—C3—C4—C12175.65 (19)C7—C6—C8—C1098.7 (2)
C3—C4—C5—C60.2 (3)C5—C6—C8—C1078.1 (2)
C12—C4—C5—C6177.35 (19)C5—C4—C12—C4i81.9 (2)
C4—C5—C6—C71.7 (3)C3—C4—C12—C4i101.1 (2)
Symmetry code: (i) x+2, y+3/2, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H2···O10.92 (2)1.80 (2)2.645 (2)151 (2)
(IVb) 2,2'–Dihydroxy–5,5'–di–tert–butyl–3,3'– methanediyldibenzaldehyde top
Crystal data top
C23H28O4F(000) = 1584
Mr = 368.45Dx = 1.174 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 26.809 (2) ÅCell parameters from 3051 reflections
b = 8.4543 (7) Åθ = 2.6–25.6°
c = 21.3720 (18) ŵ = 0.08 mm1
β = 120.618 (1)°T = 153 K
V = 4168.7 (6) Å3Tablet, light brown
Z = 80.48 × 0.38 × 0.16 mm
Data collection top
Bruker SMART 1000 CCD area-detector
diffractometer
3668 independent reflections
Radiation source: normal-focus sealed tube2235 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.049
ϕ and ω scansθmax = 25.0°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2001)
h = 3131
Tmin = 0.919, Tmax = 1.000k = 1010
14739 measured reflectionsl = 2525
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)] = 0.047Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.132H atoms treated by a mixture of independent and constrained refinement
S = 1.01 w = 1/[σ2(Fo2) + (0.0393P)2 + 4.8718P]
where P = (Fo2 + 2Fc2)/3
3668 reflections(Δ/σ)max < 0.001
251 parametersΔρmax = 0.20 e Å3
0 restraintsΔρmin = 0.18 e Å3
Crystal data top
C23H28O4V = 4168.7 (6) Å3
Mr = 368.45Z = 8
Monoclinic, C2/cMo Kα radiation
a = 26.809 (2) ŵ = 0.08 mm1
b = 8.4543 (7) ÅT = 153 K
c = 21.3720 (18) Å0.48 × 0.38 × 0.16 mm
β = 120.618 (1)°
Data collection top
Bruker SMART 1000 CCD area-detector
diffractometer
3668 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2001)
2235 reflections with I > 2σ(I)
Tmin = 0.919, Tmax = 1.000Rint = 0.049
14739 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0470 restraints
wR(F2) = 0.132H atoms treated by a mixture of independent and constrained refinement
S = 1.01Δρmax = 0.20 e Å3
3668 reflectionsΔρmin = 0.18 e Å3
251 parameters
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O10.12612 (7)0.3427 (2)0.17034 (10)0.0614 (5)
C10.07491 (11)0.3578 (3)0.12349 (14)0.0472 (6)
H10.06600.42170.08250.057*
C20.02703 (9)0.2858 (3)0.12591 (12)0.0347 (5)
C30.03676 (9)0.1916 (3)0.18513 (12)0.0352 (5)
C40.00989 (10)0.1207 (3)0.18602 (12)0.0338 (5)
C50.06496 (10)0.1474 (3)0.12771 (12)0.0356 (6)
H50.09660.09720.12780.043*
C60.07678 (9)0.2444 (3)0.06828 (12)0.0350 (5)
C70.02974 (9)0.3110 (3)0.06866 (12)0.0367 (6)
H70.03600.37570.02900.044*
O20.09102 (7)0.1694 (2)0.24251 (9)0.0448 (4)
H20.1181 (10)0.220 (3)0.2342 (13)0.050*
C80.13972 (10)0.2741 (3)0.00882 (13)0.0424 (6)
C90.14402 (11)0.3823 (3)0.05135 (13)0.0528 (7)
H9A0.12530.48380.03020.079*
H9B0.18490.40020.08770.079*
H9C0.12460.33210.07460.079*
C100.16911 (11)0.1174 (3)0.02543 (15)0.0604 (8)
H10A0.20940.13710.06350.091*
H10B0.16840.04860.01190.091*
H10C0.14850.06590.04680.091*
C110.17152 (10)0.3556 (3)0.04259 (14)0.0526 (7)
H11A0.15240.45620.06450.079*
H11B0.17070.28720.08010.079*
H11C0.21180.37570.00480.079*
C120.00000.0212 (4)0.25000.0396 (8)
H12A0.03410.04770.23500.048*0.50
H12B0.03410.04770.26500.048*0.50
O30.04622 (7)0.8544 (2)0.48082 (9)0.0523 (5)
C130.00570 (11)0.8664 (3)0.43552 (13)0.0432 (6)
H130.02840.93210.44750.052*
C140.03482 (9)0.7891 (3)0.36593 (12)0.0342 (5)
C150.00390 (9)0.6939 (3)0.34339 (12)0.0326 (5)
C160.03278 (9)0.6202 (2)0.27591 (12)0.0315 (5)
C170.09193 (9)0.6446 (3)0.23255 (12)0.0342 (5)
H170.11170.59280.18680.041*
C180.12444 (9)0.7414 (3)0.25209 (12)0.0348 (5)
C190.09454 (9)0.8120 (3)0.31941 (12)0.0358 (5)
H190.11490.87820.33480.043*
O40.05409 (7)0.6738 (2)0.38596 (9)0.0417 (4)
H40.0659 (10)0.725 (3)0.4270 (13)0.050*
C200.18896 (10)0.7661 (3)0.19921 (13)0.0430 (6)
C210.19675 (12)0.8506 (4)0.13167 (15)0.0688 (9)
H21A0.17720.95350.14560.103*
H21B0.23820.86630.09710.103*
H21C0.17990.78630.10900.103*
C220.21941 (11)0.6067 (4)0.17775 (18)0.0700 (9)
H22A0.26090.62270.14370.105*
H22B0.21400.55220.22130.105*
H22C0.20300.54240.15450.105*
C230.21703 (11)0.8669 (4)0.23221 (16)0.0645 (8)
H23A0.19790.97030.24610.097*
H23B0.21300.81370.27530.097*
H23C0.25820.88140.19640.097*
C240.00000.5208 (4)0.25000.0362 (8)
H24A0.02770.45180.29020.043*0.50
H24B0.02770.45180.20980.043*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0376 (11)0.0847 (15)0.0625 (12)0.0085 (10)0.0259 (10)0.0015 (11)
C10.0446 (16)0.0551 (17)0.0491 (15)0.0064 (13)0.0290 (14)0.0014 (13)
C20.0363 (13)0.0363 (13)0.0377 (13)0.0013 (10)0.0234 (11)0.0038 (10)
C30.0356 (13)0.0336 (13)0.0373 (13)0.0014 (10)0.0193 (11)0.0060 (11)
C40.0412 (14)0.0278 (12)0.0365 (13)0.0002 (10)0.0227 (11)0.0057 (10)
C50.0376 (13)0.0333 (13)0.0411 (14)0.0068 (10)0.0238 (12)0.0078 (11)
C60.0371 (13)0.0377 (13)0.0334 (13)0.0020 (10)0.0202 (11)0.0052 (10)
C70.0405 (14)0.0394 (14)0.0353 (13)0.0013 (11)0.0230 (12)0.0003 (11)
O20.0366 (10)0.0507 (11)0.0447 (10)0.0028 (8)0.0189 (8)0.0008 (8)
C80.0352 (13)0.0547 (16)0.0392 (14)0.0014 (12)0.0203 (11)0.0043 (12)
C90.0445 (15)0.072 (2)0.0403 (15)0.0080 (14)0.0204 (12)0.0077 (14)
C100.0465 (16)0.068 (2)0.0548 (17)0.0080 (14)0.0174 (14)0.0129 (15)
C110.0404 (15)0.0721 (19)0.0497 (16)0.0072 (13)0.0262 (13)0.0012 (14)
C120.049 (2)0.0293 (18)0.042 (2)0.0000.0250 (17)0.000
O30.0485 (11)0.0675 (13)0.0395 (10)0.0082 (9)0.0214 (9)0.0079 (9)
C130.0490 (16)0.0464 (15)0.0411 (14)0.0042 (12)0.0280 (13)0.0036 (12)
C140.0397 (13)0.0352 (13)0.0329 (12)0.0042 (10)0.0223 (11)0.0003 (10)
C150.0332 (13)0.0332 (13)0.0363 (13)0.0021 (10)0.0214 (11)0.0048 (10)
C160.0379 (13)0.0267 (12)0.0373 (13)0.0019 (10)0.0246 (11)0.0015 (10)
C170.0386 (13)0.0309 (13)0.0389 (13)0.0076 (10)0.0239 (11)0.0026 (10)
C180.0345 (13)0.0361 (13)0.0393 (13)0.0040 (10)0.0228 (11)0.0004 (11)
C190.0398 (13)0.0332 (13)0.0429 (14)0.0011 (10)0.0273 (12)0.0003 (11)
O40.0357 (9)0.0492 (11)0.0382 (9)0.0016 (8)0.0175 (8)0.0007 (8)
C200.0340 (13)0.0520 (16)0.0455 (14)0.0022 (11)0.0221 (12)0.0032 (12)
C210.0496 (17)0.097 (2)0.0554 (18)0.0130 (16)0.0237 (15)0.0161 (17)
C220.0390 (16)0.071 (2)0.093 (2)0.0143 (15)0.0291 (16)0.0139 (18)
C230.0382 (15)0.085 (2)0.070 (2)0.0089 (15)0.0274 (14)0.0112 (17)
C240.0411 (19)0.0281 (17)0.046 (2)0.0000.0270 (16)0.000
Geometric parameters (Å, º) top
O1—C11.226 (3)O3—C131.230 (3)
C1—C21.445 (3)C13—C141.437 (3)
C1—H10.9500C13—H130.9500
C2—C71.401 (3)C14—C191.403 (3)
C2—C31.403 (3)C14—C151.405 (3)
C3—O21.356 (3)C15—O41.354 (3)
C3—C41.396 (3)C15—C161.389 (3)
C4—C51.382 (3)C16—C171.385 (3)
C4—C121.509 (3)C16—C241.510 (3)
C5—C61.406 (3)C17—C181.405 (3)
C5—H50.9500C17—H170.9500
C6—C71.377 (3)C18—C191.377 (3)
C6—C81.530 (3)C18—C201.524 (3)
C7—H70.9500C19—H190.9500
O2—H20.94 (2)O4—H40.88 (2)
C8—C101.524 (4)C20—C221.520 (4)
C8—C111.533 (3)C20—C231.527 (3)
C8—C91.534 (3)C20—C211.526 (4)
C9—H9A0.9800C21—H21A0.9800
C9—H9B0.9800C21—H21B0.9800
C9—H9C0.9800C21—H21C0.9800
C10—H10A0.9800C22—H22A0.9800
C10—H10B0.9800C22—H22B0.9800
C10—H10C0.9800C22—H22C0.9800
C11—H11A0.9800C23—H23A0.9800
C11—H11B0.9800C23—H23B0.9800
C11—H11C0.9800C23—H23C0.9800
C12—C4i1.509 (3)C24—C16i1.510 (3)
C12—H12A0.9900C24—H24A0.9900
C12—H12B0.9900C24—H24B0.9900
O1—C1—C2124.9 (2)O3—C13—C14125.3 (2)
O1—C1—H1117.5O3—C13—H13117.4
C2—C1—H1117.5C14—C13—H13117.4
C7—C2—C3119.6 (2)C19—C14—C15119.7 (2)
C7—C2—C1119.6 (2)C19—C14—C13119.5 (2)
C3—C2—C1120.7 (2)C15—C14—C13120.7 (2)
O2—C3—C4119.0 (2)O4—C15—C16118.93 (19)
O2—C3—C2121.0 (2)O4—C15—C14121.2 (2)
C4—C3—C2120.0 (2)C16—C15—C14119.9 (2)
C5—C4—C3118.1 (2)C17—C16—C15118.1 (2)
C5—C4—C12121.46 (18)C17—C16—C24121.28 (18)
C3—C4—C12120.42 (18)C15—C16—C24120.63 (18)
C4—C5—C6123.8 (2)C16—C17—C18124.1 (2)
C4—C5—H5118.1C16—C17—H17118.0
C6—C5—H5118.1C18—C17—H17118.0
C7—C6—C5116.6 (2)C19—C18—C17116.4 (2)
C7—C6—C8123.9 (2)C19—C18—C20123.5 (2)
C5—C6—C8119.5 (2)C17—C18—C20120.1 (2)
C6—C7—C2121.8 (2)C18—C19—C14121.8 (2)
C6—C7—H7119.1C18—C19—H19119.1
C2—C7—H7119.1C14—C19—H19119.1
C3—O2—H2110.1 (15)C15—O4—H4108.5 (16)
C10—C8—C6109.8 (2)C22—C20—C18109.5 (2)
C10—C8—C11110.0 (2)C22—C20—C23108.6 (2)
C6—C8—C11108.98 (19)C18—C20—C23112.0 (2)
C10—C8—C9108.4 (2)C22—C20—C21109.6 (2)
C6—C8—C9111.98 (19)C18—C20—C21108.81 (19)
C11—C8—C9107.7 (2)C23—C20—C21108.3 (2)
C8—C9—H9A109.5C20—C21—H21A109.5
C8—C9—H9B109.5C20—C21—H21B109.5
H9A—C9—H9B109.5H21A—C21—H21B109.5
C8—C9—H9C109.5C20—C21—H21C109.5
H9A—C9—H9C109.5H21A—C21—H21C109.5
H9B—C9—H9C109.5H21B—C21—H21C109.5
C8—C10—H10A109.5C20—C22—H22A109.5
C8—C10—H10B109.5C20—C22—H22B109.5
H10A—C10—H10B109.5H22A—C22—H22B109.5
C8—C10—H10C109.5C20—C22—H22C109.5
H10A—C10—H10C109.5H22A—C22—H22C109.5
H10B—C10—H10C109.5H22B—C22—H22C109.5
C8—C11—H11A109.5C20—C23—H23A109.5
C8—C11—H11B109.5C20—C23—H23B109.5
H11A—C11—H11B109.5H23A—C23—H23B109.5
C8—C11—H11C109.5C20—C23—H23C109.5
H11A—C11—H11C109.5H23A—C23—H23C109.5
H11B—C11—H11C109.5H23B—C23—H23C109.5
C4i—C12—C4112.3 (3)C16i—C24—C16112.4 (2)
C4i—C12—H12A109.2C16i—C24—H24A109.1
C4—C12—H12A109.2C16—C24—H24A109.1
C4i—C12—H12B109.2C16i—C24—H24B109.1
C4—C12—H12B109.2C16—C24—H24B109.1
H12A—C12—H12B107.9H24A—C24—H24B107.9
O1—C1—C2—C7179.5 (2)O3—C13—C14—C19179.5 (2)
O1—C1—C2—C30.8 (4)O3—C13—C14—C152.0 (4)
C7—C2—C3—O2177.7 (2)C19—C14—C15—O4177.66 (19)
C1—C2—C3—O22.0 (3)C13—C14—C15—O40.8 (3)
C7—C2—C3—C41.4 (3)C19—C14—C15—C161.4 (3)
C1—C2—C3—C4178.9 (2)C13—C14—C15—C16179.9 (2)
O2—C3—C4—C5178.70 (19)O4—C15—C16—C17178.75 (19)
C2—C3—C4—C50.4 (3)C14—C15—C16—C170.4 (3)
O2—C3—C4—C120.1 (3)O4—C15—C16—C240.7 (3)
C2—C3—C4—C12179.0 (2)C14—C15—C16—C24178.5 (2)
C3—C4—C5—C61.4 (3)C15—C16—C17—C181.0 (3)
C12—C4—C5—C6177.2 (2)C24—C16—C17—C18177.0 (2)
C4—C5—C6—C72.1 (3)C16—C17—C18—C191.3 (3)
C4—C5—C6—C8176.2 (2)C16—C17—C18—C20177.5 (2)
C5—C6—C7—C21.1 (3)C17—C18—C19—C140.1 (3)
C8—C6—C7—C2177.2 (2)C20—C18—C19—C14178.6 (2)
C3—C2—C7—C60.6 (3)C15—C14—C19—C181.2 (3)
C1—C2—C7—C6179.7 (2)C13—C14—C19—C18179.7 (2)
C7—C6—C8—C10122.3 (2)C19—C18—C20—C22125.2 (3)
C5—C6—C8—C1059.5 (3)C17—C18—C20—C2256.1 (3)
C7—C6—C8—C11117.2 (2)C19—C18—C20—C234.6 (3)
C5—C6—C8—C1161.0 (3)C17—C18—C20—C23176.7 (2)
C7—C6—C8—C91.8 (3)C19—C18—C20—C21115.0 (3)
C5—C6—C8—C9180.0 (2)C17—C18—C20—C2163.7 (3)
C5—C4—C12—C4i100.4 (2)C17—C16—C24—C16i101.4 (2)
C3—C4—C12—C4i78.14 (18)C15—C16—C24—C16i76.67 (18)
Symmetry code: (i) x, y, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H2···O10.94 (2)1.81 (2)2.625 (3)144 (2)
O4—H4···O30.88 (2)1.85 (2)2.631 (2)147 (2)
C13—H13···O3ii0.952.573.454 (3)156
Symmetry code: (ii) x, y+2, z+1.

Experimental details

(II)(III)(IVa)(IVb)
Crystal data
Chemical formulaC29H40O4C29H36O4C23H28O4C23H28O4
Mr452.61448.58368.45368.45
Crystal system, space groupTriclinic, P1Monoclinic, P21/cTetragonal, I41/aMonoclinic, C2/c
Temperature (K)150150150153
a, b, c (Å)10.6025 (11), 11.9199 (12), 12.4180 (13)16.2931 (10), 10.1951 (6), 16.4318 (10)12.7930 (7), 12.7930 (7), 24.158 (2)26.809 (2), 8.4543 (7), 21.3720 (18)
α, β, γ (°)64.611 (2), 82.672 (2), 66.330 (2)90, 108.367 (1), 9090, 90, 9090, 120.618 (1), 90
V3)1296.7 (2)2590.4 (3)3953.7 (4)4168.7 (6)
Z2488
Radiation typeMo KαMo KαMo KαMo Kα
µ (mm1)0.080.080.080.08
Crystal size (mm)0.29 × 0.17 × 0.120.26 × 0.16 × 0.140.28 × 0.20 × 0.050.48 × 0.38 × 0.16
Data collection
DiffractometerBruker SMART 1000 CCD area-detector
diffractometer
Bruker SMART 1000 CCD area-detector
diffractometer
Bruker SMART 1000 CCD area-detector
diffractometer
Bruker SMART 1000 CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 2001)
Multi-scan
(SADABS; Sheldrick, 2001)
Multi-scan
(SADABS; Sheldrick, 2001)
Multi-scan
(SADABS; Sheldrick, 2001)
Tmin, Tmax0.938, 1.0000.900, 1.0000.931, 1.0000.919, 1.000
No. of measured, independent and
observed [I > 2σ(I)] reflections
9408, 4565, 3085 17928, 4559, 3620 19093, 1736, 1203 14739, 3668, 2235
Rint0.0250.0200.0560.049
(sin θ/λ)max1)0.5950.5950.5940.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.057, 0.173, 1.04 0.043, 0.123, 1.02 0.043, 0.120, 1.04 0.047, 0.132, 1.01
No. of reflections4565455917363668
No. of parameters310317125251
H-atom treatmentH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrainedH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.69, 0.220.29, 0.180.19, 0.210.20, 0.18

Computer programs: SMART (Bruker, 1998), SMART, SAINT (Bruker, 1998), SHELXTL (Sheldrick, 2001), SHELXTL.

Hydrogen-bond geometry (Å, º) for (II) top
D—H···AD—HH···AD···AD—H···A
O1—H1OB···O4i0.821.992.749 (2)155
O1—H1OA···O4ii0.831.932.744 (3)166
O4—H4OA···O1i0.911.852.749 (2)167
O4—H4OB···O1iii0.841.902.744 (3)177
Symmetry codes: (i) x, y+1, z; (ii) x+1, y, z; (iii) x1, y, z.
Hydrogen-bond geometry (Å, º) for (III) top
D—H···AD—HH···AD···AD—H···A
C5—H5···O1i0.952.463.406 (2)171
C14—H14···O4ii0.952.623.560 (2)170
Symmetry codes: (i) x, y+1/2, z1/2; (ii) x, y+1/2, z+1/2.
Hydrogen-bond geometry (Å, º) for (IVa) top
D—H···AD—HH···AD···AD—H···A
O2—H2···O10.92 (2)1.80 (2)2.645 (2)151 (2)
Hydrogen-bond geometry (Å, º) for (IVb) top
D—H···AD—HH···AD···AD—H···A
O2—H2···O10.94 (2)1.81 (2)2.625 (3)144 (2)
O4—H4···O30.88 (2)1.85 (2)2.631 (2)147 (2)
C13—H13···O3i0.952.573.454 (3)156
Symmetry code: (i) x, y+2, z+1.
 

Acknowledgements

The authors thank Professor M. A. McKervey and Dr H. Q. N. Gunaratne, CSS Limited, for helpful discussions.

References

First citationBarreira Fontecha, J., Goetz, S. & McKee, V. (2002). Angew. Chem. Int. Ed. 41, 4554–4556.  CrossRef Google Scholar
First citationBoss, R. & Scheffold, R. (1976). Angew. Chem. 88, 578–579.  CrossRef CAS Google Scholar
First citationBruker (1998). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationDhawan, B. & Gutsche, C. D. (1983). J. Org. Chem. 48, 1536–1539.  CrossRef CAS Web of Science Google Scholar
First citationMasci, B., Levi Mortera, S., Seralessandri, L. & Thuery, P. (2004) Acta Cryst. C60, o107–o109.  Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
First citationSheldrick, G. M. (2001). SHELXTL (Version 6.12) and SADABS (Version 6.12). Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationTaniguchi, S. (1984). Bull. Chem. Soc. Jpn, 57, 2683–2684.  CrossRef CAS Web of Science Google Scholar

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