supplementary materials
2-(2-Naphthyl)-1,3-dioxane
The title compound was synthesized using a modified strategy described by
(Gopinath et al., 2002). To a solution of 2-naphthaldehyde (0.64 mmol),
trimethylorthoformate (1.41 mmol) and 1,3-propanediol (5.12 mmol) in dry
nitromethane (2 ml) was added tetrabutylammonium tribromide (0.025 mmol). The
homogeneous reaction mixture was stirred at r.t. and the progress of the
reaction monitored by TLC and GC. After completion of the reaction the mixture
was poured into a solution of NaHCO3 (10 ml) and the products were extracted
with diethyl ether (3 × 10 ml). The organic layer was separated, dried
over anhydrous Na2SO4 and concentrated. The white solid obtained was
purified by recrystallization in MeOH, giving colourless thin plate-like
crystals of the title compound.
1H NMR 400 MHz (CDCl3) δ 7.97 (br s, 1H, H1'), 7.85 (m, 3H,
H4',5',8'),
7.60 (dd, 1H, 3J3'-4' = 8.5 Hz, 3J3'-1' = 1.7 Hz, H3'), 7.48 (m, 2H,
H6',7'), 5.68 (s, 1H, H1), 4.33 (dddd, 2H, 2J3e-3a;5e-5a = -11.7 Hz,
3J3e-4a;5e-4a = 5.0 Hz, 3J3e-4e;5e-4e = 1.5 Hz, 4J3e-5e = 3.0 Hz,
H3e,5e), 4.06 (ddd, 2H, 2J3a-3e;5a-5e = -11.7 Hz, 3J3a-4a;5a-4a =
12.4 Hz, 3J3a-4e;5a-4e = 2.7 Hz, H3a,5a), 2.29( dtt, 1H, 2J4a-4e =
-13.5 Hz, 3J4a-3a;4a-5a = 12.4 Hz, 3J4a-3e;4a-5e = 5.0 Hz, H4a),
1.50 (dtt, 1H, 2J4e-4a = -13.5 Hz, 3J4e-3a;4e-5a = 2.7 Hz,
3J4e-3e;4e-5e = 1.5 Hz, H4 e); 13C NMR 100 MHz (CDCl3) δ 136.1
(C2'), (133.6, 133.1) (C9',10'), (128.4, 128.1, 127.7) (C4',5',8'),
(126.2, 126.0) (C6',7'), 125.3 (C1'), 123.8 (C3'), 101.8 (C1), 67.5
(C3,5), 25.9 (C4); HRMS (ESI, +): [M + Na]+ = 237.09. Note: The
same numbering scheme has been used for the crystal structure (Fig. 1). The
torsional angles of the 1,3-dioxane ring were measured to estimate the
coupling constants according to the Karplus equation.
In the final cycles of refinement, in the absence of significant anomalous
scattering effects, 944 (93%) Friedel pairs were merged and Δf" set to zero.
The H-atoms could all be located in difference electron-density maps. In the
final cycles of refinement they were included in calculated positions and
treated as riding atoms: C—H = 0.95–1.0 Å, with Uiso(H) =
1.2Ueq(parent C-atom). Using the one-circle Stoe Image Plate
Diffraction System it is not always possible to measure 100% of the Ewald
sphere, and here only 93.7% of the data were accessible out to 50° in 2θ.
This has little effect on the bond distances and angles when comparing their
values with those of the related structure mentioned above (Borbas et
al., 2002).
Data collection: EXPOSE in IPDS-I (Stoe & Cie, 2000); cell refinement: CELL in IPDS-I (Stoe & Cie, 2000); data reduction: INTEGRATE in IPDS-I (Stoe & Cie, 2000); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009) and Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008) and PLATON (Spek, 2009).
2-(2-Naphthyl)-1,3-dioxane
top
Crystal data top
| C14H14O2 | F(000) = 228 |
| Mr = 214.25 | Dx = 1.279 Mg m−3 |
| Monoclinic, P21 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2yb | Cell parameters from 4553 reflections |
| a = 7.5351 (6) Å | θ = 2.1–26.0° |
| b = 7.8575 (8) Å | µ = 0.08 mm−1 |
| c = 9.4057 (9) Å | T = 173 K |
| β = 92.839 (11)° | Plate, colourless |
| V = 556.20 (9) Å3 | 0.38 × 0.30 × 0.08 mm |
| Z = 2 | |
Data collection top
Stoe IPDS diffractometer | 951 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.024 |
| graphite | θmax = 26.0°, θmin = 2.2° |
| φ rotation scans | h = −8→8 |
| 4461 measured reflections | k = −9→9 |
| 1098 independent reflections | l = −11→11 |
Refinement top
| Refinement on F2 | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Secondary atom site location: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.024 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.061 | H-atom parameters constrained |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0412P)2] where P = (Fo2 + 2Fc2)/3 |
| 1098 reflections | (Δ/σ)max < 0.001 |
| 145 parameters | Δρmax = 0.13 e Å−3 |
| 1 restraint | Δρmin = −0.11 e Å−3 |
Crystal data top
| C14H14O2 | V = 556.20 (9) Å3 |
| Mr = 214.25 | Z = 2 |
| Monoclinic, P21 | Mo Kα radiation |
| a = 7.5351 (6) Å | µ = 0.08 mm−1 |
| b = 7.8575 (8) Å | T = 173 K |
| c = 9.4057 (9) Å | 0.38 × 0.30 × 0.08 mm |
| β = 92.839 (11)° | |
Data collection top
Stoe IPDS diffractometer | 951 reflections with I > 2σ(I) |
| 4461 measured reflections | Rint = 0.024 |
| 1098 independent reflections | θmax = 26.0° |
Refinement top
| R[F2 > 2σ(F2)] = 0.024 | 1 restraint |
| wR(F2) = 0.061 | H-atom parameters constrained |
| S = 1.05 | Δρmax = 0.13 e Å−3 |
| 1098 reflections | Δρmin = −0.11 e Å−3 |
| 145 parameters | |
Special details top
Geometry. Bond distances, angles etc. have been calculated using the rounded
fractional coordinates. All su's are estimated from the variances of the
(full) variance-covariance matrix. The cell e.s.d.'s are taken into account in
the estimation of distances, angles and torsion angles |
Refinement. In the final cycles of refinement, in the absence of significant anomalous
scattering effects, 944 (93%) Friedel pairs were merged and Δf " set to zero.
The H-atoms could all be located in difference electron-density maps. In the
final cycles of refinement they were included in calculated positions and
treated as riding atoms: C—H = 0.95 - 1.0 Å, with Uiso(H) =
1.2Ueq(parent C-atoms). Using the one-circle Stoe Image Plate
Diffraction System it is not always possible to measure 100% of the Ewald
sphere, and here only 93.7% of the data were accessible out to 50° in 2θ. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top| | x | y | z | Uiso*/Ueq | |
| O2 | 1.16506 (19) | 0.57058 (16) | 0.43163 (12) | 0.0337 (4) | |
| O6 | 1.33418 (18) | 0.38156 (15) | 0.57014 (12) | 0.0295 (4) | |
| C1 | 1.1616 (2) | 0.4392 (2) | 0.53276 (17) | 0.0251 (5) | |
| C1' | 0.9100 (2) | 0.46504 (19) | 0.69218 (16) | 0.0239 (5) | |
| C2' | 1.0796 (2) | 0.5075 (2) | 0.66364 (16) | 0.0240 (5) | |
| C3 | 1.2305 (3) | 0.5057 (3) | 0.30168 (18) | 0.0417 (7) | |
| C3' | 1.1796 (3) | 0.6163 (2) | 0.75664 (17) | 0.0277 (6) | |
| C4 | 1.4131 (3) | 0.4321 (3) | 0.32815 (19) | 0.0400 (7) | |
| C4' | 1.1073 (3) | 0.6764 (2) | 0.87667 (18) | 0.0297 (6) | |
| C5 | 1.4128 (3) | 0.3067 (3) | 0.44944 (18) | 0.0348 (6) | |
| C5' | 0.8555 (3) | 0.6908 (2) | 1.03543 (18) | 0.0309 (6) | |
| C6' | 0.6865 (3) | 0.6467 (2) | 1.06380 (18) | 0.0316 (6) | |
| C7' | 0.5852 (3) | 0.5438 (2) | 0.96939 (18) | 0.0328 (6) | |
| C8' | 0.6551 (2) | 0.4853 (2) | 0.84779 (18) | 0.0284 (5) | |
| C9' | 0.8310 (2) | 0.52609 (19) | 0.81562 (16) | 0.0236 (5) | |
| C10' | 0.9334 (2) | 0.63231 (19) | 0.91039 (17) | 0.0239 (5) | |
| H1 | 1.08840 | 0.34250 | 0.49320 | 0.0300* | |
| H1' | 0.84350 | 0.39320 | 0.62810 | 0.0290* | |
| H3' | 1.29720 | 0.64750 | 0.73540 | 0.0330* | |
| H3A | 1.14900 | 0.41670 | 0.26250 | 0.0500* | |
| H3E | 1.23480 | 0.59870 | 0.23090 | 0.0500* | |
| H4' | 1.17550 | 0.74940 | 0.93860 | 0.0360* | |
| H4A | 1.45060 | 0.37410 | 0.24110 | 0.0480* | |
| H4E | 1.49890 | 0.52450 | 0.35160 | 0.0480* | |
| H5' | 0.92210 | 0.76160 | 1.10020 | 0.0370* | |
| H5A | 1.53630 | 0.27170 | 0.47590 | 0.0420* | |
| H5E | 1.34500 | 0.20400 | 0.41910 | 0.0420* | |
| H6' | 0.63660 | 0.68620 | 1.14860 | 0.0380* | |
| H7' | 0.46700 | 0.51460 | 0.99020 | 0.0390* | |
| H8' | 0.58470 | 0.41640 | 0.78400 | 0.0340* | |
Atomic displacement parameters (Å2) top| | U11 | U22 | U33 | U12 | U13 | U23 |
| O2 | 0.0500 (9) | 0.0289 (6) | 0.0225 (6) | 0.0088 (6) | 0.0049 (5) | 0.0012 (5) |
| O6 | 0.0283 (8) | 0.0376 (7) | 0.0228 (5) | 0.0058 (6) | 0.0027 (5) | −0.0007 (5) |
| C1 | 0.0269 (11) | 0.0239 (8) | 0.0244 (8) | −0.0013 (6) | 0.0008 (7) | 0.0000 (6) |
| C1' | 0.0245 (11) | 0.0228 (8) | 0.0240 (8) | −0.0016 (6) | −0.0023 (7) | 0.0007 (6) |
| C2' | 0.0265 (11) | 0.0229 (8) | 0.0225 (8) | −0.0003 (7) | 0.0012 (7) | 0.0021 (7) |
| C3 | 0.0679 (17) | 0.0358 (9) | 0.0220 (8) | 0.0095 (10) | 0.0084 (9) | 0.0013 (8) |
| C3' | 0.0224 (11) | 0.0303 (9) | 0.0307 (9) | −0.0050 (7) | 0.0031 (7) | −0.0032 (7) |
| C4 | 0.0533 (16) | 0.0374 (10) | 0.0306 (9) | −0.0015 (9) | 0.0158 (9) | −0.0061 (8) |
| C4' | 0.0273 (12) | 0.0299 (9) | 0.0317 (9) | −0.0050 (7) | −0.0007 (7) | −0.0058 (7) |
| C5 | 0.0371 (13) | 0.0395 (10) | 0.0283 (9) | 0.0069 (8) | 0.0077 (8) | −0.0053 (8) |
| C5' | 0.0345 (14) | 0.0286 (9) | 0.0298 (9) | 0.0016 (7) | 0.0026 (8) | −0.0023 (7) |
| C6' | 0.0322 (12) | 0.0327 (9) | 0.0309 (8) | 0.0066 (8) | 0.0105 (7) | 0.0024 (7) |
| C7' | 0.0230 (12) | 0.0382 (11) | 0.0377 (9) | 0.0031 (7) | 0.0063 (8) | 0.0075 (8) |
| C8' | 0.0222 (11) | 0.0316 (9) | 0.0313 (8) | −0.0035 (8) | 0.0004 (7) | 0.0029 (7) |
| C9' | 0.0222 (11) | 0.0226 (8) | 0.0257 (8) | 0.0007 (6) | −0.0005 (7) | 0.0051 (6) |
| C10' | 0.0242 (11) | 0.0211 (7) | 0.0264 (8) | 0.0010 (7) | 0.0013 (7) | 0.0007 (6) |
Geometric parameters (Å, °) top
| O2—C1 | 1.405 (2) | C8'—C9' | 1.411 (2) |
| O2—C3 | 1.434 (2) | C9'—C10' | 1.421 (2) |
| O6—C1 | 1.405 (2) | C1—H1 | 1.0000 |
| O6—C5 | 1.433 (2) | C1'—H1' | 0.9500 |
| C1—C2' | 1.504 (2) | C3—H3A | 0.9900 |
| C1'—C2' | 1.360 (2) | C3—H3E | 0.9900 |
| C1'—C9' | 1.415 (2) | C3'—H3' | 0.9500 |
| C2'—C3' | 1.414 (2) | C4—H4A | 0.9900 |
| C3—C4 | 1.502 (3) | C4—H4E | 0.9900 |
| C3'—C4' | 1.362 (3) | C4'—H4' | 0.9500 |
| C4—C5 | 1.508 (3) | C5—H5A | 0.9900 |
| C4'—C10' | 1.407 (3) | C5—H5E | 0.9900 |
| C5'—C6' | 1.359 (3) | C5'—H5' | 0.9500 |
| C5'—C10' | 1.417 (2) | C6'—H6' | 0.9500 |
| C6'—C7' | 1.399 (3) | C7'—H7' | 0.9500 |
| C7'—C8' | 1.363 (2) | C8'—H8' | 0.9500 |
| | | |
| C1—O2—C3 | 109.55 (14) | C9'—C1'—H1' | 119.00 |
| C1—O6—C5 | 110.36 (13) | O2—C3—H3A | 110.00 |
| O2—C1—O6 | 110.99 (13) | O2—C3—H3E | 110.00 |
| O2—C1—C2' | 108.32 (13) | C4—C3—H3A | 110.00 |
| O6—C1—C2' | 108.84 (13) | C4—C3—H3E | 110.00 |
| C2'—C1'—C9' | 121.09 (14) | H3A—C3—H3E | 108.00 |
| C1—C2'—C1' | 120.15 (14) | C2'—C3'—H3' | 120.00 |
| C1—C2'—C3' | 119.63 (14) | C4'—C3'—H3' | 120.00 |
| C1'—C2'—C3' | 120.22 (15) | C3—C4—H4A | 110.00 |
| O2—C3—C4 | 110.27 (15) | C3—C4—H4E | 110.00 |
| C2'—C3'—C4' | 119.98 (19) | C5—C4—H4A | 110.00 |
| C3—C4—C5 | 109.96 (18) | C5—C4—H4E | 110.00 |
| C3'—C4'—C10' | 121.12 (17) | H4A—C4—H4E | 108.00 |
| O6—C5—C4 | 110.33 (18) | C3'—C4'—H4' | 119.00 |
| C6'—C5'—C10' | 120.74 (16) | C10'—C4'—H4' | 119.00 |
| C5'—C6'—C7' | 120.65 (17) | O6—C5—H5A | 110.00 |
| C6'—C7'—C8' | 120.42 (19) | O6—C5—H5E | 110.00 |
| C7'—C8'—C9' | 120.64 (16) | C4—C5—H5A | 110.00 |
| C1'—C9'—C8' | 122.48 (14) | C4—C5—H5E | 110.00 |
| C1'—C9'—C10' | 118.47 (14) | H5A—C5—H5E | 108.00 |
| C8'—C9'—C10' | 119.06 (14) | C6'—C5'—H5' | 120.00 |
| C4'—C10'—C5' | 122.42 (15) | C10'—C5'—H5' | 120.00 |
| C4'—C10'—C9' | 119.09 (14) | C5'—C6'—H6' | 120.00 |
| C5'—C10'—C9' | 118.49 (15) | C7'—C6'—H6' | 120.00 |
| O2—C1—H1 | 110.00 | C6'—C7'—H7' | 120.00 |
| O6—C1—H1 | 110.00 | C8'—C7'—H7' | 120.00 |
| C2'—C1—H1 | 110.00 | C7'—C8'—H8' | 120.00 |
| C2'—C1'—H1' | 119.00 | C9'—C8'—H8' | 120.00 |
| | | |
| C3—O2—C1—O6 | 64.83 (17) | O2—C3—C4—C5 | 51.9 (2) |
| C3—O2—C1—C2' | −175.74 (14) | C2'—C3'—C4'—C10' | −0.1 (3) |
| C1—O2—C3—C4 | −58.4 (2) | C3—C4—C5—O6 | −50.8 (2) |
| C5—O6—C1—O2 | −64.14 (17) | C3'—C4'—C10'—C5' | 179.07 (16) |
| C5—O6—C1—C2' | 176.74 (14) | C3'—C4'—C10'—C9' | −1.3 (2) |
| C1—O6—C5—C4 | 56.5 (2) | C10'—C5'—C6'—C7' | −0.6 (3) |
| O2—C1—C2'—C1' | 104.47 (17) | C6'—C5'—C10'—C4' | 179.42 (16) |
| O2—C1—C2'—C3' | −75.40 (18) | C6'—C5'—C10'—C9' | −0.2 (2) |
| O6—C1—C2'—C1' | −134.75 (15) | C5'—C6'—C7'—C8' | 0.4 (3) |
| O6—C1—C2'—C3' | 45.38 (19) | C6'—C7'—C8'—C9' | 0.6 (2) |
| C9'—C1'—C2'—C1 | 179.19 (14) | C7'—C8'—C9'—C1' | 178.60 (15) |
| C9'—C1'—C2'—C3' | −0.9 (2) | C7'—C8'—C9'—C10' | −1.4 (2) |
| C2'—C1'—C9'—C8' | 179.59 (15) | C1'—C9'—C10'—C4' | 1.6 (2) |
| C2'—C1'—C9'—C10' | −0.5 (2) | C1'—C9'—C10'—C5' | −178.80 (14) |
| C1—C2'—C3'—C4' | −178.90 (15) | C8'—C9'—C10'—C4' | −178.48 (15) |
| C1'—C2'—C3'—C4' | 1.2 (2) | C8'—C9'—C10'—C5' | 1.2 (2) |
Hydrogen-bond geometry (Å, °) top
| D—H···A | D—H | H···A | D···A | D—H···A |
| C1'—H1'···O2i | 0.95 | 2.60 | 3.349 (2) | 136 |
| C5'—H5'···Cg1ii | 0.95 | 2.70 | 3.555 (2) | 151 |
| C4'—H4'···Cg2ii | 0.95 | 2.92 | 3.776 (2) | 150 |
| C3—H3A···Cg1i | 0.99 | 2.99 | 3.927 (2) | 159 |
| Symmetry codes: (i) −x+2, y−1/2, −z+1; (ii) −x+2, y+1/2, −z+2. |
Table 1
Hydrogen-bond geometry (Å, °) top
| D—H···A | D—H | H···A | D···A | D—H···A |
| C1'—H1'···O2i | 0.95 | 2.60 | 3.349 (2) | 136 |
| C5'—H5'···Cg1ii | 0.95 | 2.70 | 3.555 (2) | 151 |
| C4'—H4'···Cg2ii | 0.95 | 2.92 | 3.776 (2) | 150 |
| C3—H3A···Cg1i | 0.99 | 2.99 | 3.927 (2) | 159 |
| Symmetry codes: (i) −x+2, y−1/2, −z+1; (ii) −x+2, y+1/2, −z+2. |
HSE is grateful to the XRD Application Laboratory, Microsystems Technology
Division, Swiss Center for Electronics and Microtechnology, Neuchâtel, for
access to the X-ray diffraction equipment.
Allen, F. H. (2002). Acta Cryst. B58, 380–388.
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Borbas, A., Szoba, Z. B., Szilagyi, L., Benyei, A. & Liptak, A. (2002). Tetrahedron, 58, 5723–5732.
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Carmichael, I. & Hug, G. L. (1986). J. Phys. Chem. Ref. Data, 15, 1–250.
Cordes, E. H. & Bull, H. G. (1974). Chem. Rev. 74, 581–603.
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Kocienski, P. J. (1994). Carbonyl Protecting Groups, in Protecting Groups, ch. 5. New York: Thieme Medical Publishers.
Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453–457.
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Stoe & Cie (2000). IPDS-I. Stoe & Cie GmbH, Darmstadt, Germany.
Thevenet, D. & Neier, R. (2010). Org. Lett. In preparation.
Acetals are the most commonly used protecting groups for carbonyl compounds in organic synthesis (Kocienski, 1994; Showler & Darley, 1967), and many methods have been developed for their deprotection (Cordes & Bull, 1974; Fujioka et al., 2004; Ates et al., 2003). The title 2-naphthaldehyde acetal (Newman & Dickson, 1970; Carmichael & Hug, 1986) was synthesized to investigate the scope of a new photochemical reaction capable of hydrolysing the acetal into an aldehyde (Thevenet & Neier, 2010). The NMR spectra of the unsubstituted 1,3-dioxane ring displays a complicated AA'BB'MN system (Buys & Eliel, 1970), and the X-ray crystal structure was helpful for the interpretation of the NMR spectra (Thevenet & Neier, 2010).
The structure of the title compound is illustrated in Fig. 1, and the geometrical parameters are given in the Supplementary information and the archived CIF. The bond lengths and angles are close to those in three similar compounds located in the Cambridge Crystal Structure Database (CSD, V 5.30, last update Sept. 2009; Allen, 2002). For example, methyl 2,3-di-O-acteyl-4,6-O-(2-naphthyl)methylene-α-D-galactopyranoside (Borbas et al., 2002), which also crystallized in the monoclinic space group P21, and where the naphthalene ring is planar and the two six-membered rings in the galactopyranoside unit have chair conformations.
In the crystal of the title compound symmetry related molecules are connected via a C—H···O interaction (Table 1) giving rise to the formation of helical chains propagating in [010]. These chains are further linked via weak C—H···π interactions to form a two-dimensional network in (011) - see Fig. 2 and Table 1 for details.