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The title compound, C14H22O4S, crystallizes as a non-merohedral twin with a twinning ratio close to 1:1. The six-membered ring exhibits a half-chair conformation, and the seven-membered ring displays an irregular chair-like conformation.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805041140/sj6181sup1.cif
Contains datablocks global, II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805041140/sj6181IIsup2.hkl
Contains datablock II

CCDC reference: 296666

Key indicators

  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.049
  • wR factor = 0.119
  • Data-to-parameter ratio = 67.3

checkCIF/PLATON results

No syntax errors found



Alert level A REFLT03_ALERT_3_A Reflection count > 15% excess reflns - sys abs data present? From the CIF: _diffrn_reflns_theta_max 28.28 From the CIF: _diffrn_reflns_theta_full 28.28 From the CIF: _reflns_number_total 11919 TEST2: Reflns within _diffrn_reflns_theta_max Count of symmetry unique reflns 3517 Completeness (_total/calc) 338.90%
Author Response: The crystal under investigation was pseudo-merohedrally twinned with a BASF value of 0.4675(6) and both components were used for the hklf 5 refinement, resulting in a larger than expected number of total reflections.
PLAT021_ALERT_1_A Ratio Unique / Expected Reflections too High ...       3.39

Alert level C PLAT125_ALERT_4_C No _symmetry_space_group_name_Hall Given ....... ? PLAT230_ALERT_2_C Hirshfeld Test Diff for S5 - O1 .. 6.07 su
2 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion

Comment top

The background to this study is described in the first paper of this series (Zeller et al., 2006).

Compound (II) crystallizes in the triclinic space group P1 with Z = 2 as a racemic mixture of both enantiomers (Fig. 1). The crystal under investigation was found to be non-merohedrally twinned with two components of similar distribution. The data were integrated and the structure was solved and refined using commercial software as described in the Experimental section. The final BASF factor was found to be 0.4675 (6). Similar to four related endo-cycloadducts described previously (Zeller et al., 2004a,b,c,d), the six-membered ring of (II) exhibits the half-chair conformation expected for cyclohexenes. The angles at the unsaturated C atoms are 124.3 (1)° for C4—C3—C2 and 123.5 (1)° for C3—C4—C4A (Fig. 1).

The seven-membered ring displays an irregular chair-like conformation. The sterically demanding tert-butyl group on C7 is located in a pseudo-equatorial position. All intermolecular contacts in (II) are weak, the most pronounced being 3.465 (1) Å for O2···C13(−x, 1 − y, 1 − z). All bond lengths and angles are within their expected ranges.

Experimental top

The title compound was synthesized as described by Chumachenko et al. (2005) as a mixture of the exo- and two endo-cycloadducts, viz. (I), (II) and (III), in a ratio of 12/100/4, as established by 1H NMR of the crude reaction product. The title compound, (II), was isolated from the mixture by selective crystallization from ethyl acetate/hexanes (1:3 v/v) to yield crystals suitable for X-ray structural analysis. [The single-crystal structure of (I) is described in the previous article of this series (Zeller et al., 2006).]

Refinement top

The crystal under investigation was found to be non-merohedrally twinned. Two components were identified using GEMINI (Bruker, 1999) and both components were simultaniously integrated using SAINT-Plus (Bruker, 2003). The twin relationship was found to be described by the matrix (1.00039, 0.00139, −0.00035; −0.68441, −1.00009, 0.00096; −0.02404, −0.00039, −1.00027). The data set under investigation had 5380 identified reflections associated with component 1 only, 5367 reflections with component 2 only and 296 are belonging to both components. I/σ for the first component was 13.4 and 12.4 for the second. I/σ for overlapping reflections was 18.7. The data set was corrected for absorption using TWINABS (Bruker, 2003), which was also used to create both an HKLF 4 as well as an HKLF 5 format file. The HKLF 4 format file (with the non-overlapping reflections of component 1 only) was used to establish the space group and solve the structure. The HKLF 5 format file was used for the refinement of the structure; the twin ratio (BASF factor) refined to 0.4675 (6). All H atoms were positioned geometrically (C—H = 0.95–1.00 Å). They were refined with isotropic displacement parameters of 1.5 (methyl) or 1.2 (all others) times that of the equivalent isotropic displacement parameter of the adjacent C atom. Methyl H atoms were allowed to rotate to best fit the experimental data. The s.u. values of the cell parameters are taken from the software, recognizing that the values are unreasonably small (Herbstein, 2000).

Computing details top

Data collection: SMART (Bruker, 2002); cell refinement: SAINT-Plus (Bruker, 2003); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXTL (Bruker, 2000); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing 50% probability displacement ellipsoids.
(4aSR,7SR,9aSR)-7-tert-Butyl-9a-methyl-5,5-dioxo-1,2,4a,9a-tetrahydro-8-oxa- 5λ6-thiabenzocycloheptan-9-one top
Crystal data top
C14H22O4SZ = 2
Mr = 286.38F(000) = 308
Triclinic, P1Dx = 1.345 Mg m3
a = 5.6949 (5) ÅMo Kα radiation, λ = 0.71073 Å
b = 11.1309 (10) ÅCell parameters from 6500 reflections
c = 12.3085 (11) Åθ = 3.2–30.6°
α = 112.539 (2)°µ = 0.24 mm1
β = 90.278 (2)°T = 100 K
γ = 100.160 (2)°Block, colourless
V = 707.07 (11) Å30.29 × 0.20 × 0.18 mm
Data collection top
Bruker SMART APEX CCD
diffractometer
11919 independent reflections
Radiation source: fine-focus sealed tube11372 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.000
ω scansθmax = 28.3°, θmin = 1.8°
Absorption correction: multi-scan
(TWINABS in SAINT-Plus; Bruker, 2003)
h = 77
Tmin = 0.870, Tmax = 0.96k = 1414
11949 measured reflectionsl = 1616
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)] = 0.049Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.119H-atom parameters constrained
S = 1.16 w = 1/[σ2(Fo2) + (0.0415P)2 + 0.3942P]
where P = (Fo2 + 2Fc2)/3
11919 reflections(Δ/σ)max < 0.001
177 parametersΔρmax = 0.57 e Å3
0 restraintsΔρmin = 0.39 e Å3
Crystal data top
C14H22O4Sγ = 100.160 (2)°
Mr = 286.38V = 707.07 (11) Å3
Triclinic, P1Z = 2
a = 5.6949 (5) ÅMo Kα radiation
b = 11.1309 (10) ŵ = 0.24 mm1
c = 12.3085 (11) ÅT = 100 K
α = 112.539 (2)°0.29 × 0.20 × 0.18 mm
β = 90.278 (2)°
Data collection top
Bruker SMART APEX CCD
diffractometer
11919 independent reflections
Absorption correction: multi-scan
(TWINABS in SAINT-Plus; Bruker, 2003)
11372 reflections with I > 2σ(I)
Tmin = 0.870, Tmax = 0.96Rint = 0.000
11949 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0490 restraints
wR(F2) = 0.119H-atom parameters constrained
S = 1.16Δρmax = 0.57 e Å3
11919 reflectionsΔρmin = 0.39 e Å3
177 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.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.5899 (2)0.79692 (11)0.24787 (10)0.0175 (2)
H1A0.69280.79040.30970.021*
H1B0.68150.78350.17740.021*
O10.58397 (14)0.64822 (8)0.42340 (7)0.02023 (18)
C20.5279 (2)0.93488 (11)0.29225 (10)0.0206 (2)
H2A0.67381.00200.33090.025*
H2B0.47110.95180.22420.025*
O20.23163 (15)0.69741 (8)0.53791 (7)0.02208 (19)
C30.3392 (2)0.94932 (11)0.37784 (10)0.0197 (2)
H30.31371.03620.42300.024*
O30.62698 (15)0.52763 (8)0.14649 (7)0.02197 (18)
C40.2049 (2)0.84889 (11)0.39487 (10)0.0177 (2)
H40.09460.86810.45400.021*
C4A0.21794 (19)0.70603 (11)0.32544 (9)0.0144 (2)
H4A0.05070.65700.29540.017*
S50.32699 (5)0.63747 (3)0.42553 (2)0.01507 (7)
C60.1931 (2)0.46497 (10)0.36741 (9)0.0171 (2)
H6A0.23060.42640.42420.020*
H6B0.01710.45560.35900.020*
C70.27879 (19)0.38690 (10)0.24789 (9)0.0148 (2)
H70.45340.38740.25780.018*
O80.24300 (14)0.45871 (7)0.17398 (6)0.01538 (16)
C90.4354 (2)0.55294 (11)0.17472 (9)0.0156 (2)
C9A0.36523 (19)0.68776 (10)0.21616 (9)0.0143 (2)
C100.1434 (2)0.24316 (11)0.18638 (10)0.0157 (2)
C110.1893 (2)0.16651 (11)0.26202 (11)0.0204 (2)
H11A0.11900.07240.21980.031*
H11B0.11610.20140.33690.031*
H11C0.36210.17670.27770.031*
C120.2411 (2)0.18335 (11)0.06519 (10)0.0204 (2)
H12A0.41450.19060.07540.031*
H12B0.20680.23150.01680.031*
H12C0.16450.08980.02590.031*
C130.1261 (2)0.23669 (11)0.16971 (10)0.0183 (2)
H13A0.15320.29800.13340.027*
H13B0.19360.26170.24660.027*
H13C0.20370.14620.11850.027*
C140.2036 (2)0.68826 (11)0.11570 (10)0.0187 (2)
H14A0.29330.67510.04560.028*
H14B0.15130.77350.14060.028*
H14C0.06340.61650.09700.028*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0165 (5)0.0182 (5)0.0192 (5)0.0021 (4)0.0023 (4)0.0096 (4)
O10.0200 (4)0.0217 (4)0.0199 (4)0.0017 (3)0.0029 (3)0.0101 (3)
C20.0240 (6)0.0170 (5)0.0208 (6)0.0019 (5)0.0014 (5)0.0084 (5)
O20.0301 (5)0.0205 (4)0.0131 (4)0.0015 (4)0.0031 (3)0.0053 (3)
C30.0242 (6)0.0166 (5)0.0172 (5)0.0067 (5)0.0017 (5)0.0043 (4)
O30.0202 (4)0.0213 (4)0.0268 (4)0.0070 (3)0.0084 (4)0.0106 (4)
C40.0188 (5)0.0194 (5)0.0145 (5)0.0075 (5)0.0009 (4)0.0045 (4)
C4A0.0148 (5)0.0174 (5)0.0122 (5)0.0037 (4)0.0010 (4)0.0068 (4)
S50.01788 (13)0.01539 (13)0.01137 (12)0.00068 (10)0.00038 (10)0.00569 (10)
C60.0209 (6)0.0135 (5)0.0155 (5)0.0014 (4)0.0002 (4)0.0064 (4)
C70.0151 (5)0.0164 (5)0.0153 (5)0.0035 (4)0.0000 (4)0.0085 (4)
O80.0166 (4)0.0162 (4)0.0147 (4)0.0023 (3)0.0012 (3)0.0080 (3)
C90.0181 (5)0.0179 (5)0.0116 (5)0.0029 (4)0.0014 (4)0.0066 (4)
C9A0.0156 (5)0.0156 (5)0.0129 (5)0.0036 (4)0.0022 (4)0.0067 (4)
C100.0159 (5)0.0139 (5)0.0169 (5)0.0024 (4)0.0003 (4)0.0058 (4)
C110.0200 (6)0.0172 (5)0.0260 (6)0.0040 (4)0.0005 (5)0.0105 (5)
C120.0171 (5)0.0181 (5)0.0211 (6)0.0020 (4)0.0024 (4)0.0029 (5)
C130.0157 (5)0.0192 (5)0.0188 (5)0.0027 (4)0.0014 (4)0.0064 (4)
C140.0217 (6)0.0208 (6)0.0147 (5)0.0048 (5)0.0005 (4)0.0079 (4)
Geometric parameters (Å, º) top
C1—C21.5270 (16)C7—O81.4565 (12)
C1—C9A1.5327 (15)C7—C101.5356 (15)
C1—H1A0.9900C7—H71.0000
C1—H1B0.9900O8—C91.3738 (13)
O1—S51.4484 (8)C9—C9A1.5160 (15)
C2—C31.4943 (16)C9A—C141.5401 (15)
C2—H2A0.9900C10—C111.5324 (15)
C2—H2B0.9900C10—C131.5327 (15)
O2—S51.4426 (8)C10—C121.5347 (15)
C3—C41.3260 (16)C11—H11A0.9800
C3—H30.9500C11—H11B0.9800
O3—C91.1950 (14)C11—H11C0.9800
C4—C4A1.5049 (15)C12—H12A0.9800
C4—H40.9500C12—H12B0.9800
C4A—C9A1.5542 (14)C12—H12C0.9800
C4A—S51.8347 (11)C13—H13A0.9800
C4A—H4A1.0000C13—H13B0.9800
S5—C61.7902 (11)C13—H13C0.9800
C6—C71.5276 (15)C14—H14A0.9800
C6—H6A0.9900C14—H14B0.9800
C6—H6B0.9900C14—H14C0.9800
C2—C1—C9A111.80 (9)C10—C7—H7109.2
C2—C1—H1A109.3C9—O8—C7115.39 (8)
C9A—C1—H1A109.3O3—C9—O8122.90 (10)
C2—C1—H1B109.3O3—C9—C9A127.11 (10)
C9A—C1—H1B109.3O8—C9—C9A109.99 (9)
H1A—C1—H1B107.9C9—C9A—C1109.98 (9)
C3—C2—C1111.98 (9)C9—C9A—C14107.43 (9)
C3—C2—H2A109.2C1—C9A—C14111.71 (9)
C1—C2—H2A109.2C9—C9A—C4A108.66 (8)
C3—C2—H2B109.2C1—C9A—C4A110.41 (9)
C1—C2—H2B109.2C14—C9A—C4A108.56 (9)
H2A—C2—H2B107.9C11—C10—C13109.72 (9)
C4—C3—C2124.29 (11)C11—C10—C12110.20 (9)
C4—C3—H3117.9C13—C10—C12109.29 (9)
C2—C3—H3117.9C11—C10—C7108.44 (9)
C3—C4—C4A123.45 (10)C13—C10—C7111.37 (9)
C3—C4—H4118.3C12—C10—C7107.80 (9)
C4A—C4—H4118.3C10—C11—H11A109.5
C4—C4A—C9A112.39 (9)C10—C11—H11B109.5
C4—C4A—S5108.89 (7)H11A—C11—H11B109.5
C9A—C4A—S5113.65 (7)C10—C11—H11C109.5
C4—C4A—H4A107.2H11A—C11—H11C109.5
C9A—C4A—H4A107.2H11B—C11—H11C109.5
S5—C4A—H4A107.2C10—C12—H12A109.5
O2—S5—O1117.93 (5)C10—C12—H12B109.5
O2—S5—C6106.80 (5)H12A—C12—H12B109.5
O1—S5—C6107.89 (5)C10—C12—H12C109.5
O2—S5—C4A107.59 (5)H12A—C12—H12C109.5
O1—S5—C4A109.71 (5)H12B—C12—H12C109.5
C6—S5—C4A106.31 (5)C10—C13—H13A109.5
C7—C6—S5113.09 (7)C10—C13—H13B109.5
C7—C6—H6A109.0H13A—C13—H13B109.5
S5—C6—H6A109.0C10—C13—H13C109.5
C7—C6—H6B109.0H13A—C13—H13C109.5
S5—C6—H6B109.0H13B—C13—H13C109.5
H6A—C6—H6B107.8C9A—C14—H14A109.5
O8—C7—C6105.45 (8)C9A—C14—H14B109.5
O8—C7—C10108.56 (8)H14A—C14—H14B109.5
C6—C7—C10114.95 (9)C9A—C14—H14C109.5
O8—C7—H7109.2H14A—C14—H14C109.5
C6—C7—H7109.2H14B—C14—H14C109.5
C9A—C1—C2—C344.27 (13)O8—C9—C9A—C1165.31 (8)
C1—C2—C3—C413.48 (16)O3—C9—C9A—C14107.37 (13)
C2—C3—C4—C4A2.99 (18)O8—C9—C9A—C1472.91 (10)
C3—C4—C4A—C9A11.74 (15)O3—C9—C9A—C4A135.36 (11)
C3—C4—C4A—S5115.10 (11)O8—C9—C9A—C4A44.35 (11)
C4—C4A—S5—O235.29 (9)C2—C1—C9A—C9178.99 (9)
C9A—C4A—S5—O2161.40 (7)C2—C1—C9A—C1461.82 (12)
C4—C4A—S5—O194.17 (8)C2—C1—C9A—C4A59.09 (12)
C9A—C4A—S5—O131.94 (9)C4—C4A—C9A—C9162.38 (9)
C4—C4A—S5—C6149.42 (8)S5—C4A—C9A—C938.13 (11)
C9A—C4A—S5—C684.47 (8)C4—C4A—C9A—C141.69 (12)
O2—S5—C6—C7179.48 (8)S5—C4A—C9A—C182.56 (10)
O1—S5—C6—C751.78 (9)C4—C4A—C9A—C1481.08 (11)
C4A—S5—C6—C765.85 (9)S5—C4A—C9A—C14154.67 (7)
S5—C6—C7—O852.20 (10)O8—C7—C10—C11177.85 (8)
S5—C6—C7—C10171.72 (8)C6—C7—C10—C1164.37 (12)
C6—C7—O8—C991.56 (10)O8—C7—C10—C1361.33 (11)
C10—C7—O8—C9144.77 (9)C6—C7—C10—C1356.45 (12)
C7—O8—C9—O358.59 (14)O8—C7—C10—C1258.55 (11)
C7—O8—C9—C9A121.14 (9)C6—C7—C10—C12176.33 (9)
O3—C9—C9A—C114.41 (15)

Experimental details

Crystal data
Chemical formulaC14H22O4S
Mr286.38
Crystal system, space groupTriclinic, P1
Temperature (K)100
a, b, c (Å)5.6949 (5), 11.1309 (10), 12.3085 (11)
α, β, γ (°)112.539 (2), 90.278 (2), 100.160 (2)
V3)707.07 (11)
Z2
Radiation typeMo Kα
µ (mm1)0.24
Crystal size (mm)0.29 × 0.20 × 0.18
Data collection
DiffractometerBruker SMART APEX CCD
diffractometer
Absorption correctionMulti-scan
(TWINABS in SAINT-Plus; Bruker, 2003)
Tmin, Tmax0.870, 0.96
No. of measured, independent and
observed [I > 2σ(I)] reflections
11949, 11919, 11372
Rint0.000
(sin θ/λ)max1)0.667
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.049, 0.119, 1.16
No. of reflections11919
No. of parameters177
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.57, 0.39

Computer programs: SMART (Bruker, 2002), SAINT-Plus (Bruker, 2003), SAINT-Plus, SHELXTL (Bruker, 2000), SHELXTL.

 

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