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The an­hydrous form, (I), of the title compound, (−)-2-(1,2,3,4,4a,7-hexa­hydro-4a,8-di­methyl-1,7-dioxo-2-naphthyl)­propionic acid, C15H18O4, derived from a naturally occurring sesquiterpenoid, has two mol­ecules in the asymmetric unit, (I) and (I′), differing in the conformations of the saturated ring and the carboxyl group. The compound aggregates as carboxyl-to-ketone hydrogen-bonding catemers [O...O = 2.776 (3) and 2.775 (3) Å]. Two crystallographically independent sets of single-strand hydrogen-bonding helices with opposite end-to-end orientation pass through the cell in the b direction, one consisting exclusively of mol­ecules of (I) and the other entirely of (I′). Three C—H...O=C close contacts are found in (I). The monohydrate, C15H18O4·H2O, (II), with two mol­ecules of (I) plus two water mol­ecules in its asymmetric unit, forms a complex three-dimensional hydrogen-bonding network including acid-to-water, water-to-acid, water-to-ketone, water-to-water and acid-to-acid hydrogen bonds, plus three C—H...O=C close contacts. In both (I) and (II), only the ketone remote from the acid is involved in hydrogen bonding.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270101009441/fg1635sup1.cif
Contains datablocks I, II, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270101009441/fg1635Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270101009441/fg1635IIsup3.hkl
Contains datablock II

CCDC references: 173371; 173372

Comment top

Our continuing interest in the crystallography of keto carboxylic acids lies in exploring the molecular characteristics that control the various hydrogen-bonding patterns. Functionally unelaborated acids, with one hydrogen-bond donor and one receptor, usually aggregate in the solid as dimers, rarely as catemers (chains). Appending a ketone function provides an excess of receptors and creates opportunities for at least three additional hydrogen-bonding modes. The commonest of these, the acid-to-ketone catemer, forms a sizeable overall minority of keto acid hydrogen-bonding cases and, in the presence of certain molecular features, becomes the dominant hydrogen-bonding mode (Brunskill et al., 1997).

As we have previously suggested, carboxyl dimerization is discouraged by the presence of conformational restrictions (Brunskill et al., 1999) or of only one enantiomer (Lalancette et al., 1998). A factor that may favour carboxyl-to-ketone hydrogen-bonding patterns is the presence of multiple ketone receptors for the hydrogen bond (Brunskill et al., 1999). The title compound, (I), derived from a sesquiterpene isolate of Artemisia, is a bicyclic γ,ζ-diketo acid, present as a single enantiomer, and we report here that (I) adopts the carboxyl-to-ketone catemeric hydrogen-bonding mode in the solid state and also crystallizes as a monohydrate, (II), with a complex hydrogen-bonding pattern. \sch

Fig. 1 shows the asymmetric unit of the anhydrous material, consisting of two molecules, (I) and (I'), which differ slightly in the flexure of the saturated ring and in the rotation of the carboxyl about the C9—C10 bond. The major conformational options lie in the branched chain attached at C2. Here, the substituents at C9, which has the S configuration, are staggered with respect to those at C2, so that the methyl is anti to C1; the C11—C9—C2—C1 torsion angle is 178.5 (2)° in (I) and -173.7 (2)° in (I'), a difference of 7.8 (2)°. In both (I) and (I'), the carboxyl group is turned so that its C O is away from the molecular face bearing the angular methyl, but in (I) the O3—C10—C9—C2 torsion angle is 41.3 (4)°, while in (I') it is 26.6 (4)°, a difference of 14.7 (4)°. In both species, the dienone ring is essentially planar, providing strong conjugation for the O2 ketone, but the saturated-ring ketone is rotated significantly from the conjugation plane; the dihedral angle for C1—C2—C8a—O1 versus the dienone ring is 52.00 (12)° for (I) and 58.17 (9)° for (I').

The partial averaging of C—O bond lengths and C—C—O angles by disorder often seen in acids is unique to the carboxyl-pairing pattern of hydrogen bonding, whose geometry permits transposition of the two carboxyl O atoms. As in other catemers, no significant averaging is observed for (I), whose bond lengths are 1.196 (3) and 1.333 (4) Å, with angles of 124.8 (3) and 112.1 (3)°; for (I'), the bond lengths are 1.196 (3) and 1.328 (3) Å, with angles of 124.8 (3) and 112.7 (2)°. Our own survey of 56 keto acid structures which are not acid dimers gives average values of 1.20 (1) and 1.32 (2) Å, and 124.5 (14) and 112.7 (17)°, for these bond lengths and angles, in accord with the typical values of 1.21 and 1.31 Å, and 123 and 112°, cited for highly ordered dimeric carboxyls (Borthwick, 1980). The three methyl groups are fully ordered in both (I) and (I'), and staggered relative to the substituents at their points of attachment.

Fig. 2 illustrates the packing of (I) and (I') in the cell, with extracellular molecules included to show the two crystallographically independent single-strand hydrogen-bonding catemers; one chain consists entirely of molecules of (I), while the other is made up exclusively of (I'). Each chain proceeds from the carboxyl of one molecule to the remote ketone (O2) of a neighbour. Among hydrogen-bonding catemers, the observed prevalence of subtypes, describing the relation of adjacent molecules, is screw > translation > glide, with the chains often following a cell axis. Here, the components of each chain are related by a twofold screw axis along b; the axis for helices of type (I) lies in the ab face of the chosen cell, while the counterdirectionally aligned type (I') helices follow an axis lying in the bc face. The intermolecular O···O distance and O—H···O angle are 2.776 (3) Å and 165°, respectively, within the type (I) chains, and 2.775 (3) Å and 160°, respectively, within the type (I') chains.

Consistent with the 14.7 (4)° difference found between (I) & (I') for the rotation of the COOH group about C9—C10, the intramolecular ketone versus carboxyl dihedral angles for (I) and (I') differ by only 14.7 (4)°. However, the intermolecular ketone versus carboxyl dihedral angles for screw-related molecules involved in hydrogen bonding are markedly different for the two types of chains; these values are 26.4 (4)° for the type-(I) chains and 78.9 (2)° for type-(I') chains. This difference is not related to the helical `pitches' of the two helices (Coté et al., 1997), which are found to be nearly identical, at 36.9° for (I) and 36.6° for (I'). It is a product of the different orientations of (I) and (I') relative to the b axis, about which they are rotated in the symmetry operation that generates their hydrogen-bonding partners. The result is hydrogen-bonding helices with identical periods and pitches but significantly different footprints on the ac face for the two types of helices. Although the intermolecular dihedral angles cited above differ by more than 75°, the geometry of the hydrogen-bonding itself for (I) versus (I') is remarkably similar. We characterize the geometry of hydrogen bonding to carbonyls using a combination of the H···OC angle and the H···OC—C torsion angle. These describe the approach of the H atom to the O atom in terms of its deviation from, respectively, CO axiality (ideal 120°) and planarity with the carbonyl (ideal 0°). In (I), these angles are 143.7 and 9.2°, respectively, while in (I') the same angles are 141.3 and 5.6°.

Intermolecular C—H···O close contacts were found involving O3 (2.51 Å to H13C in a molecule in the a direction), O1 (2.55 Å to H6A in a molecule in the b direction), and O3' (2.54 Å to H3B in a molecule in the c direction). These distances lie within the 2.7-?.?Å range we usually employ for non-bonded H···O packing interactions (Steiner, 1997). Using compiled data for a large number of C—H···O contacts, Steiner & Desiraju (1998) find significant statistical directionality even as far out as 3.0 Å, and conclude that these are legitimately viewed as `weak hydrogen bonds', with a greater contribution to packing forces than simple van der Waals attractions.

Fig. 3 shows the asymmetric unit for the hydrate, which also contains two molecules, (II) and (II'), plus two molecules of water. The conformations of (II) and (II') differ only slightly from one another and from those of (I) and (I'). The torsion angles C11—C9—C2—C1 and O3—C10—C9—C2 were used to illustrate this in the above discussion for (I) versus (I'); here, C11—C9—C2—C1 is -178.8 (4)° in (II) and 176.8 (4)° in (II'), a difference of 4.4 (4)°. In (II) and (II'), the O3—C10—C9—C2 torsion angles do not differ beyond experimental error: 38.9 (6)° for (II) and 37.9 (6)° in (II'). The dihedral angle for C1—C2—C8a—O1 versus the dienone ring is 55.7 (2)° in (II) and 58.3 (3)° in (II').

The specific juxtaposition of (II) and (II') illustrated was chosen to show that the carboxyl hydrogen-bonding in both (II) and (II') precludes dimer pairing, so that disordering of the carboxyl groups is not expected. The C—O bond lengths for (II) are 1.212 (5) and 1.313 (6) Å, with C—C—O angles of 123.2 (5) and 113.3 (4)°; for (II'), the bond lengths are 1.216 (5) and 1.320 (6) Å, with angles of 123.3 (4) and 112.9 (4)°. The direct acid-to-acid hydrogen bonding shown in Fig. 3 is the only hydrogen-bonding contact between (II) and (II') not mediated by water molecules. The two water molecules present play different roles in the hydrogen-bonding scheme, as illustrated in Fig. 4. A l l three methyls are fully ordered and staggered in both (II) and (II').

Fig. 4 illustrates the packing of the cell and the three-dimensional hydrogen-bonding network. Besides the acid-to-acid hydrogen bond shown in Fig. 3, this includes acid-to-water, water-to-acid, water-to-ketone and water-to-water hydrogen bonds. In both (II) and (II'), only the ζ-ketone (O2) remote from the acid is involved in the hydrogen bonding, as was the case for the anhydrous material. Two screw-related asymmetric units are shown, plus an extra molecule and peripheral waters. Besides the direct (two-bond) acid-to-acid hydrogen bond that distinguishes the chosen asymmetric unit, both three-bond and four-bond intermolecular carboxyl-to-ketone connections are found, mediated by single waters, and five-bond carboxyl-to-carboxyl and six-bond ketone-to-ketone connections are mediated through paired waters.

In (II), the criteria described above for characterizing the geometry of hydrogen bonding to carbonyls are applicable to four of the five hydrogen bonds present. Approach angles for the acid-to-acid hydrogen bond are: H4'···O3C10 155 and H4'···O3C10—O4 - 21°. Angles for the water-to-acid hydrogen bond are: HW1···O3C10 159 and HW1···O3 C10—O4 30°. Angles for the (acid-to-) water-to-ketone hydrogen bond are: HW2'···O2C7 118 and HW2'···O2C7—C6 - 20°. Angles for the (water-to-) water-to-ketone hydrogen bond are: HW3'···O2C7 127 and HW3'···O2C7—C6 - 31°.

One intermolecular C—H···OC close contact was found for the O1' ketone (2.50 Å to H3B in a molecule in the c direction), plus two for the O1 ketone: contacts of 2.49 Å to H3'A and 2.66 Å to H12F in separate molecules, both in the c direction.

The KBr infrared spectrum of (I) displays absorptions at 1737 (acid), 1699 (free ketone), 1652 (hydrogen-bonded ketone) and 1616 cm-1 (CC), consistent with known shifts due to the removal of hydrogen bonding from acid CO and the addition of hydrogen bonding to a ketone. The monohydrate displays strong KBr absorptions at 1724 and 1652 cm-1, with much weaker ones at 1674 and 1601 cm-1. In CHCl3 solution, where dimers predominate, a broad peak at 1706 cm-1 is accompanied by peaks at 1660 and 1633 cm-1, and a typical carboxyl-dilution shoulder near 1750 cm-1.

Experimental top

Commercial (-)-α-santonin of known relative and absolute stereochemistry (Barton et al., 1962; Nakazaki & Arakawa, 1962; Asher & Sim, 1965; Coggin & Sim, 1969) was obtained from Aldrich Chemical Co., Milwaukee, Wisconsin, USA, and subjected to the basic hydrolysis and CrO3 oxidation procedure described by Nishikawa et al. (1955). The optical rotation of (I) (m.p. 409 K) has been assigned (Nishikawa et al., 1955; Yanagita & Ogura, 1957). Crystals of (I) (m.p. 401 K) were obtained by evaporation of an ether solution. Crystals of the monohydrate, (II) (m.p. 378 K), were obtained from acetonitrile-water.

Refinement top

All H atoms for both (I) and (II) were found in electron-density difference maps, but were placed in calculated positions and allowed to refine as riding models. In (I), the phenyl H atoms were fixed at 0.93, the methine H atoms at 0.98, the methylene H atoms at 0.97, the methyl H atoms at 0.96 and the hydroxyl H atoms at 0.82 Å from their respective C or O atoms. The isotropic displacement parameters of the two acid H atoms were allowed to refine but the other H atoms were refined as groups, with the phenyl H atoms refining to 0.060 (4), the methine H atoms 0.036 (3), the methylene H atoms 0.050 (3) and the methyl H atoms 0.078 (3) Å2. For (II), the phenyl H atoms were fixed at 0.94, the methine H atoms at 0.99, the methylene H atoms at 0.98 and the methyl H atoms at 0.97 Å from their respective C atoms, and the hydroxyl H positions were allowed to refine; the water H atoms were fixed to be 0.83 Å from their respective O atom. The isotropic displacement parameters of the two acid H atoms, as well as those of the water molecules, were held at 0.08 Å2, while the displacement parameters of the remaining H atoms were tied to their repsective C atoms.

Computing details top

For both compounds, data collection: XSCANS (Siemens, 1996); cell refinement: XSCANS; data reduction: XSCANS; program(s) used to solve structure: SHELXTL (Sheldrick, 1997); 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 view of one of the two molecules in the asymmetric unit of (I), with the atom-numbering scheme. Displacement ellipsoids are drawn at the 20% probability level and H atoms are shown as spheres of arbitrary radii.
[Figure 2] Fig. 2. A packing diagram for (I), with two extracellular molecules to illustrate the two kinds of single-strand helical catemer proceeding in the b direction. Those of type (I) follow an axis in the ab face, and those of type (I') an axis in the bc face. Methylene and methine H atoms have been omitted for clarity. Displacement ellipsoids are drawn at the 20% probability level.
[Figure 3] Fig. 3. The molecular view of the asymmetric unit of (II) with the two associated water molecules; the atom-numbering scheme is the same as for (I). The molecule on the right is the primed species, (II'). Displacement ellipsoids are drawn at the 20% probability level and H atoms are shown as spheres of arbitrary radii.
[Figure 4] Fig. 4. A packing diagram for (II), with two asymmetric units, an extra molecule and several peripheral waters. The asymmetric units are distinguishable by their direct acid-to-acid hydrogen bonds (Fig. 3); the two shown are screw-related along b. Methylene and methine H atoms have been omitted for clarity. Displacement ellipsoids are drawn at the 20% probability level.
(I) (-)-2-(1,2,3,4,6,8a-hexahydro-5,8a-dimethyl-4,6-dioxo-3-naphthyl)propionic acid top
Crystal data top
C15H18O4Dx = 1.251 Mg m3
Mr = 262.29Melting point: 401 K
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
a = 7.679 (1) ÅCell parameters from 30 reflections
b = 14.644 (2) Åθ = 5.5–14.7°
c = 12.461 (1) ŵ = 0.09 mm1
β = 96.43 (1)°T = 293 K
V = 1392.4 (3) Å3Hexagonal prism, colourless
Z = 40.56 × 0.44 × 0.24 mm
F(000) = 560
Data collection top
Siemens P4
diffractometer
2110 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.024
Graphite monochromatorθmax = 25.0°, θmin = 2.2°
2θ/θ scansh = 99
Absorption correction: numerical
(SHELXTL; Sheldrick, 1997)
k = 1717
Tmin = 0.95, Tmax = 0.97l = 014
5478 measured reflections3 standard reflections every 97 reflections
2553 independent reflections intensity decay: variation < 1.5%
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)] = 0.033Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.077H atoms treated by a mixture of independent and constrained refinement
S = 1.08 w = 1/[σ2(Fo2) + (0.0321P)2 + 0.0377P]
where P = (Fo2 + 2Fc2)/3
2553 reflections(Δ/σ)max < 0.001
355 parametersΔρmax = 0.13 e Å3
1 restraintΔρmin = 0.10 e Å3
Crystal data top
C15H18O4V = 1392.4 (3) Å3
Mr = 262.29Z = 4
Monoclinic, P21Mo Kα radiation
a = 7.679 (1) ŵ = 0.09 mm1
b = 14.644 (2) ÅT = 293 K
c = 12.461 (1) Å0.56 × 0.44 × 0.24 mm
β = 96.43 (1)°
Data collection top
Siemens P4
diffractometer
2110 reflections with I > 2σ(I)
Absorption correction: numerical
(SHELXTL; Sheldrick, 1997)
Rint = 0.024
Tmin = 0.95, Tmax = 0.973 standard reflections every 97 reflections
5478 measured reflections intensity decay: variation < 1.5%
2553 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0331 restraint
wR(F2) = 0.077H atoms treated by a mixture of independent and constrained refinement
S = 1.08Δρmax = 0.13 e Å3
2553 reflectionsΔρmin = 0.10 e Å3
355 parameters
Special details top

Experimental. Crystal mounted on glass fiber using epoxy resin

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
O10.7898 (3)0.17650 (14)0.54831 (14)0.0556 (5)
O20.6499 (3)0.50663 (14)0.37863 (17)0.0595 (6)
O31.1114 (3)0.18792 (17)0.7325 (2)0.0743 (7)
O41.0418 (3)0.04132 (14)0.7111 (2)0.0744 (7)
C10.7264 (3)0.23389 (18)0.60235 (19)0.0364 (6)
C20.7395 (3)0.22810 (18)0.72488 (19)0.0365 (6)
C30.5580 (4)0.2419 (2)0.7632 (2)0.0496 (7)
C40.4635 (4)0.3252 (2)0.7133 (2)0.0488 (7)
C4A0.4478 (3)0.32526 (19)0.5891 (2)0.0416 (6)
C50.3600 (4)0.4109 (2)0.5475 (3)0.0569 (8)
C60.4248 (4)0.4692 (2)0.4817 (3)0.0571 (8)
C70.5944 (3)0.45290 (18)0.4428 (2)0.0434 (7)
C80.6949 (3)0.37145 (17)0.4821 (2)0.0357 (6)
C8A0.6284 (3)0.31523 (17)0.55296 (18)0.0347 (6)
C90.8256 (3)0.13868 (19)0.7675 (2)0.0404 (6)
C101.0060 (4)0.1279 (2)0.7333 (2)0.0483 (7)
C110.8439 (4)0.1329 (2)0.8909 (2)0.0611 (8)
C120.8687 (4)0.3588 (2)0.4404 (2)0.0530 (7)
C130.3371 (4)0.2434 (2)0.5421 (3)0.0591 (8)
O1'0.5317 (3)0.61527 (15)0.7730 (2)0.0705 (7)
O2'0.9029 (3)0.36362 (14)1.01065 (18)0.0609 (6)
O3'0.5089 (3)0.7646 (2)0.96756 (18)0.0878 (9)
O4'0.3300 (3)0.83035 (15)0.83896 (16)0.0555 (5)
C1'0.6819 (3)0.63031 (19)0.8086 (2)0.0428 (6)
C2'0.7574 (3)0.72503 (19)0.8259 (2)0.0386 (6)
C3'0.9197 (3)0.7333 (2)0.7649 (2)0.0434 (6)
C4'1.0505 (3)0.65698 (18)0.7949 (2)0.0433 (7)
C4A'0.9720 (3)0.56014 (19)0.7775 (2)0.0432 (6)
C5'1.1047 (4)0.4901 (2)0.8162 (2)0.0521 (7)
C6'1.0814 (4)0.4270 (2)0.8898 (3)0.0536 (7)
C7'0.9221 (4)0.42372 (19)0.9427 (2)0.0469 (7)
C8'0.7879 (3)0.49391 (19)0.9153 (2)0.0464 (7)
C8A'0.8109 (3)0.55516 (19)0.8370 (2)0.0418 (6)
C9'0.6167 (3)0.79821 (18)0.7985 (2)0.0414 (6)
C10'0.4820 (4)0.79310 (19)0.8773 (2)0.0461 (7)
C11'0.6913 (4)0.8960 (2)0.8029 (3)0.0616 (9)
C12'0.6320 (4)0.4947 (2)0.9785 (3)0.0706 (10)
C13'0.9183 (4)0.5435 (2)0.6550 (2)0.0639 (9)
H41.14090.03800.69280.095 (14)*
H2A0.81440.27840.75410.036 (3)*
H3A0.48700.18810.74500.050 (3)*
H3B0.57140.24820.84120.050 (3)*
H4A0.52610.37960.74000.050 (3)*
H4B0.34700.32770.73620.050 (3)*
H5A0.25110.42430.56950.060 (4)*
H6A0.36160.52140.45980.060 (4)*
H9A0.75300.08750.73820.036 (3)*
H11A0.72970.13340.91530.078 (3)*
H11B0.91010.18430.92090.078 (3)*
H11C0.90340.07740.91390.078 (3)*
H12A0.85120.34720.36410.078 (3)*
H12B0.92870.30800.47650.078 (3)*
H12C0.93780.41310.45390.078 (3)*
H13A0.39140.18740.56840.078 (3)*
H13B0.33000.24460.46470.078 (3)*
H13C0.22140.24730.56400.078 (3)*
H4'0.26070.82610.88430.13 (2)*
H2'A0.79770.73090.90310.036 (3)*
H3'A0.88350.73130.68780.050 (3)*
H3'B0.97590.79170.78150.050 (3)*
H4'A1.09650.66370.87020.050 (3)*
H4'B1.14770.66330.75200.050 (3)*
H5'A1.21090.49050.78700.060 (4)*
H6'A1.16890.38390.90780.060 (4)*
H9'A0.55880.78670.72560.036 (3)*
H11D0.76700.90350.74720.078 (3)*
H11E0.75670.90630.87210.078 (3)*
H11F0.59670.93910.79220.078 (3)*
H12D0.56710.43900.96540.078 (3)*
H12E0.55820.54570.95620.078 (3)*
H12F0.67140.49981.05410.078 (3)*
H13D0.87940.48160.64400.078 (3)*
H13E1.01720.55430.61600.078 (3)*
H13F0.82500.58440.62950.078 (3)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0756 (14)0.0496 (11)0.0441 (10)0.0175 (11)0.0170 (10)0.0033 (10)
O20.0611 (13)0.0504 (12)0.0687 (14)0.0048 (11)0.0140 (11)0.0161 (11)
O30.0521 (13)0.0654 (15)0.1093 (19)0.0083 (12)0.0258 (13)0.0004 (14)
O40.0680 (15)0.0514 (14)0.1101 (18)0.0126 (12)0.0373 (14)0.0023 (13)
C10.0350 (13)0.0381 (14)0.0371 (13)0.0021 (12)0.0085 (11)0.0038 (12)
C20.0404 (13)0.0338 (13)0.0359 (13)0.0017 (12)0.0071 (11)0.0023 (11)
C30.0509 (16)0.0618 (19)0.0381 (14)0.0046 (15)0.0138 (13)0.0023 (14)
C40.0441 (14)0.0569 (18)0.0480 (15)0.0115 (14)0.0161 (12)0.0001 (14)
C4A0.0345 (13)0.0445 (15)0.0467 (15)0.0003 (13)0.0083 (11)0.0040 (13)
C50.0426 (16)0.067 (2)0.063 (2)0.0158 (16)0.0154 (14)0.0088 (17)
C60.0551 (18)0.0481 (18)0.069 (2)0.0141 (15)0.0118 (16)0.0159 (16)
C70.0460 (15)0.0407 (16)0.0431 (15)0.0052 (13)0.0035 (13)0.0019 (13)
C80.0360 (13)0.0361 (14)0.0351 (14)0.0038 (12)0.0037 (11)0.0036 (11)
C8A0.0344 (12)0.0381 (14)0.0317 (12)0.0013 (12)0.0042 (11)0.0053 (11)
C90.0421 (14)0.0377 (14)0.0424 (14)0.0007 (13)0.0087 (11)0.0023 (12)
C100.0503 (17)0.0463 (18)0.0489 (16)0.0052 (16)0.0073 (13)0.0064 (14)
C110.073 (2)0.064 (2)0.0481 (16)0.0116 (18)0.0119 (15)0.0129 (15)
C120.0498 (16)0.0579 (18)0.0537 (17)0.0027 (15)0.0170 (14)0.0062 (15)
C130.0437 (16)0.073 (2)0.0599 (18)0.0155 (17)0.0012 (14)0.0043 (17)
O1'0.0409 (12)0.0545 (14)0.1141 (19)0.0060 (10)0.0007 (12)0.0067 (13)
O2'0.0563 (12)0.0522 (13)0.0760 (15)0.0043 (10)0.0163 (11)0.0176 (11)
O3'0.0897 (16)0.121 (2)0.0585 (15)0.0478 (16)0.0336 (13)0.0365 (14)
O4'0.0457 (11)0.0603 (13)0.0607 (12)0.0025 (10)0.0076 (10)0.0045 (11)
C1'0.0349 (15)0.0454 (16)0.0497 (15)0.0049 (13)0.0118 (12)0.0017 (13)
C2'0.0427 (14)0.0415 (14)0.0324 (13)0.0025 (12)0.0071 (11)0.0010 (11)
C3'0.0428 (14)0.0480 (16)0.0398 (14)0.0081 (14)0.0063 (12)0.0034 (13)
C4'0.0358 (14)0.0545 (19)0.0408 (14)0.0068 (13)0.0101 (11)0.0002 (13)
C4A'0.0424 (14)0.0461 (16)0.0423 (15)0.0012 (13)0.0097 (12)0.0062 (13)
C5'0.0480 (16)0.0552 (19)0.0556 (18)0.0034 (15)0.0170 (14)0.0057 (15)
C6'0.0477 (16)0.0473 (17)0.0668 (19)0.0122 (14)0.0114 (14)0.0011 (16)
C7'0.0510 (16)0.0422 (16)0.0481 (16)0.0002 (14)0.0075 (13)0.0026 (14)
C8'0.0406 (14)0.0396 (15)0.0606 (18)0.0053 (13)0.0128 (13)0.0011 (14)
C8A'0.0343 (13)0.0392 (15)0.0519 (15)0.0057 (12)0.0049 (12)0.0063 (13)
C9'0.0478 (15)0.0398 (15)0.0368 (13)0.0013 (13)0.0055 (12)0.0053 (12)
C10'0.0482 (16)0.0404 (15)0.0506 (17)0.0036 (13)0.0095 (13)0.0009 (13)
C11'0.0593 (19)0.0450 (17)0.081 (2)0.0018 (16)0.0091 (17)0.0130 (16)
C12'0.0597 (19)0.060 (2)0.097 (3)0.0141 (18)0.0331 (18)0.0298 (19)
C13'0.078 (2)0.066 (2)0.0475 (17)0.0016 (18)0.0066 (16)0.0157 (16)
Geometric parameters (Å, º) top
O1—C11.212 (3)C9'—C10'1.506 (4)
O2—C71.232 (3)C9'—C11'1.541 (4)
O3—C101.196 (3)O4—H40.8200
O4—C101.333 (4)C2—H2A0.9800
C1—C8A1.503 (4)C3—H3A0.9700
C1—C21.521 (3)C3—H3B0.9700
C2—C91.535 (4)C4—H4A0.9700
C2—C31.536 (3)C4—H4B0.9700
C3—C41.517 (4)C5—H5A0.9300
C4—C4A1.539 (4)C6—H6A0.9300
C4A—C51.489 (4)C9—H9A0.9800
C4A—C8A1.513 (3)C11—H11A0.9600
C4A—C131.546 (4)C11—H11B0.9600
C5—C61.319 (4)C11—H11C0.9600
C6—C71.459 (4)C12—H12A0.9600
C7—C81.474 (4)C12—H12B0.9600
C8—C8A1.349 (3)C12—H12C0.9600
C8—C121.497 (4)C13—H13A0.9600
C9—C101.503 (4)C13—H13B0.9600
C9—C111.530 (4)C13—H13C0.9600
O1'—C1'1.208 (3)O4'—H4'0.8200
O2'—C7'1.241 (3)C2'—H2'A0.9800
O3'—C10'1.196 (3)C3'—H3'A0.9700
O4'—C10'1.328 (3)C3'—H3'B0.9700
C1'—C8A'1.496 (4)C4'—H4'A0.9700
C1'—C2'1.510 (4)C4'—H4'B0.9700
C2'—C9'1.533 (4)C5'—H5'A0.9300
C2'—C3'1.535 (3)C6'—H6'A0.9300
C3'—C4'1.520 (4)C9'—H9'A0.9800
C4'—C4A'1.547 (4)C11'—H11D0.9600
C4A'—C5'1.488 (4)C11'—H11E0.9600
C4A'—C8A'1.514 (4)C11'—H11F0.9600
C4A'—C13'1.555 (4)C12'—H12D0.9600
C5'—C6'1.327 (4)C12'—H12E0.9600
C6'—C7'1.454 (4)C12'—H12F0.9600
C7'—C8'1.468 (4)C13'—H13D0.9600
C8'—C8A'1.351 (4)C13'—H13E0.9600
C8'—C12'1.505 (4)C13'—H13F0.9600
O1—C1—C8A122.4 (2)H3A—C3—H3B107.8
O1—C1—C2122.2 (2)C3—C4—H4A109.0
C8A—C1—C2115.4 (2)C4A—C4—H4A109.0
C1—C2—C9111.9 (2)C3—C4—H4B109.0
C1—C2—C3110.17 (19)C4A—C4—H4B109.0
C9—C2—C3112.0 (2)H4A—C4—H4B107.8
C4—C3—C2112.8 (2)C6—C5—H5A117.5
C3—C4—C4A113.1 (2)C4A—C5—H5A117.5
C5—C4A—C8A111.9 (2)C5—C6—H6A119.5
C5—C4A—C4109.4 (2)C7—C6—H6A119.5
C8A—C4A—C4109.13 (19)C10—C9—H9A108.5
C5—C4A—C13108.2 (2)C11—C9—H9A108.5
C8A—C4A—C13107.2 (2)C2—C9—H9A108.5
C4—C4A—C13111.0 (2)C9—C11—H11A109.5
C6—C5—C4A125.0 (3)C9—C11—H11B109.5
C5—C6—C7120.9 (3)H11A—C11—H11B109.5
O2—C7—C6119.9 (3)C9—C11—H11C109.5
O2—C7—C8121.7 (2)H11A—C11—H11C109.5
C6—C7—C8118.4 (2)H11B—C11—H11C109.5
C8A—C8—C7119.2 (2)C8—C12—H12A109.5
C8A—C8—C12124.7 (2)C8—C12—H12B109.5
C7—C8—C12116.1 (2)H12A—C12—H12B109.5
C8—C8A—C1122.9 (2)C8—C12—H12C109.5
C8—C8A—C4A124.2 (2)H12A—C12—H12C109.5
C1—C8A—C4A112.9 (2)H12B—C12—H12C109.5
C10—C9—C11107.2 (2)C4A—C13—H13A109.5
C10—C9—C2111.5 (2)C4A—C13—H13B109.5
C11—C9—C2112.5 (2)H13A—C13—H13B109.5
O3—C10—O4122.8 (3)C4A—C13—H13C109.5
O3—C10—C9124.8 (3)H13A—C13—H13C109.5
O4—C10—C9112.1 (3)H13B—C13—H13C109.5
O1'—C1'—C8A'122.1 (3)C10'—O4'—H4'109.5
O1'—C1'—C2'123.7 (3)C1'—C2'—H2'A107.1
C8A'—C1'—C2'114.1 (2)C9'—C2'—H2'A107.1
C1'—C2'—C9'111.1 (2)C3'—C2'—H2'A107.1
C1'—C2'—C3'108.7 (2)C4'—C3'—H3'A109.3
C9'—C2'—C3'115.2 (2)C2'—C3'—H3'A109.3
C4'—C3'—C2'111.8 (2)C4'—C3'—H3'B109.3
C3'—C4'—C4A'113.8 (2)C2'—C3'—H3'B109.3
C5'—C4A'—C8A'112.0 (2)H3'A—C3'—H3'B107.9
C5'—C4A'—C4'110.2 (2)C3'—C4'—H4'A108.8
C8A'—C4A'—C4'107.6 (2)C4A'—C4'—H4'A108.8
C5'—C4A'—C13'107.9 (2)C3'—C4'—H4'B108.8
C8A'—C4A'—C13'109.4 (2)C4A'—C4'—H4'B108.8
C4'—C4A'—C13'109.7 (2)H4'A—C4'—H4'B107.7
C6'—C5'—C4A'124.3 (3)C6'—C5'—H5'A117.8
C5'—C6'—C7'121.4 (3)C4A'—C5'—H5'A117.8
O2'—C7'—C6'120.2 (3)C5'—C6'—H6'A119.3
O2'—C7'—C8'121.4 (3)C7'—C6'—H6'A119.3
C6'—C7'—C8'118.4 (3)C10'—C9'—H9'A108.8
C8A'—C8'—C7'119.2 (2)C2'—C9'—H9'A108.8
C8A'—C8'—C12'123.3 (3)C11'—C9'—H9'A108.8
C7'—C8'—C12'117.5 (3)C9'—C11'—H11D109.5
C8'—C8A'—C1'121.5 (2)C9'—C11'—H11E109.5
C8'—C8A'—C4A'124.5 (2)H11D—C11'—H11E109.5
C1'—C8A'—C4A'113.8 (2)C9'—C11'—H11F109.5
C10'—C9'—C2'109.8 (2)H11D—C11'—H11F109.5
C10'—C9'—C11'107.6 (2)H11E—C11'—H11F109.5
C2'—C9'—C11'113.1 (2)C8'—C12'—H12D109.5
O3'—C10'—O4'122.3 (3)C8'—C12'—H12E109.5
O3'—C10'—C9'124.8 (3)H12D—C12'—H12E109.5
O4'—C10'—C9'112.7 (2)C8'—C12'—H12F109.5
C10—O4—H4109.5H12D—C12'—H12F109.5
C1—C2—H2A107.5H12E—C12'—H12F109.5
C9—C2—H2A107.5C4A'—C13'—H13D109.5
C3—C2—H2A107.5C4A'—C13'—H13E109.5
C4—C3—H3A109.0H13D—C13'—H13E109.5
C2—C3—H3A109.0C4A'—C13'—H13F109.5
C4—C3—H3B109.0H13D—C13'—H13F109.5
C2—C3—H3B109.0H13E—C13'—H13F109.5
O1—C1—C2—C95.1 (3)O1'—C1'—C2'—C9'3.1 (4)
C8A—C1—C2—C9174.5 (2)C8A'—C1'—C2'—C9'178.3 (2)
O1—C1—C2—C3130.4 (3)O1'—C1'—C2'—C3'124.7 (3)
C8A—C1—C2—C349.2 (3)C8A'—C1'—C2'—C3'53.9 (3)
C1—C2—C3—C449.3 (3)C1'—C2'—C3'—C4'53.2 (3)
C9—C2—C3—C4174.5 (2)C9'—C2'—C3'—C4'178.7 (2)
C2—C3—C4—C4A54.5 (3)C2'—C3'—C4'—C4A'55.8 (3)
C3—C4—C4A—C5177.8 (2)C3'—C4'—C4A'—C5'175.8 (2)
C3—C4—C4A—C8A55.1 (3)C3'—C4'—C4A'—C8A'53.4 (3)
C3—C4—C4A—C1362.8 (3)C3'—C4'—C4A'—C13'65.5 (3)
C8A—C4A—C5—C63.8 (4)C8A'—C4A'—C5'—C6'3.7 (4)
C4—C4A—C5—C6124.9 (4)C4'—C4A'—C5'—C6'123.5 (3)
C13—C4A—C5—C6114.0 (4)C13'—C4A'—C5'—C6'116.8 (3)
C4A—C5—C6—C70.4 (5)C4A'—C5'—C6'—C7'2.5 (5)
C5—C6—C7—O2177.6 (3)C5'—C6'—C7'—O2'179.4 (3)
C5—C6—C7—C82.3 (5)C5'—C6'—C7'—C8'1.7 (4)
O2—C7—C8—C8A179.5 (3)O2'—C7'—C8'—C8A'176.8 (3)
C6—C7—C8—C8A0.6 (4)C6'—C7'—C8'—C8A'4.4 (4)
O2—C7—C8—C120.8 (4)O2'—C7'—C8'—C12'4.5 (4)
C6—C7—C8—C12179.4 (2)C6'—C7'—C8'—C12'174.3 (3)
C7—C8—C8A—C1176.2 (2)C7'—C8'—C8A'—C1'177.6 (2)
C12—C8—C8A—C12.4 (4)C12'—C8'—C8A'—C1'1.0 (4)
C7—C8—C8A—C4A5.4 (4)C7'—C8'—C8A'—C4A'3.1 (4)
C12—C8—C8A—C4A175.9 (2)C12'—C8'—C8A'—C4A'175.6 (3)
O1—C1—C8A—C852.0 (4)O1'—C1'—C8A'—C8'62.7 (4)
C2—C1—C8A—C8128.4 (2)C2'—C1'—C8A'—C8'118.6 (3)
O1—C1—C8A—C4A126.5 (3)O1'—C1'—C8A'—C4A'122.2 (3)
C2—C1—C8A—C4A53.1 (3)C2'—C1'—C8A'—C4A'56.5 (3)
C5—C4A—C8A—C86.9 (3)C5'—C4A'—C8A'—C8'0.8 (4)
C4—C4A—C8A—C8128.1 (3)C4'—C4A'—C8A'—C8'122.1 (3)
C13—C4A—C8A—C8111.6 (3)C13'—C4A'—C8A'—C8'118.8 (3)
C5—C4A—C8A—C1174.6 (2)C5'—C4A'—C8A'—C1'174.1 (2)
C4—C4A—C8A—C153.4 (3)C4'—C4A'—C8A'—C1'52.9 (3)
C13—C4A—C8A—C166.9 (3)C13'—C4A'—C8A'—C1'66.3 (3)
C1—C2—C9—C1058.1 (3)C1'—C2'—C9'—C10'66.1 (3)
C3—C2—C9—C10177.6 (2)C3'—C2'—C9'—C10'169.7 (2)
C1—C2—C9—C11178.5 (2)C1'—C2'—C9'—C11'173.7 (2)
C3—C2—C9—C1157.2 (3)C3'—C2'—C9'—C11'49.5 (3)
C11—C9—C10—O382.2 (4)C2'—C9'—C10'—O3'26.6 (4)
C2—C9—C10—O341.3 (4)C11'—C9'—C10'—O3'96.9 (4)
C11—C9—C10—O493.0 (3)C2'—C9'—C10'—O4'158.2 (2)
C2—C9—C10—O4143.5 (2)C11'—C9'—C10'—O4'78.3 (3)
(II) (-)-2-(1,2,3,4,6,8a-hexahydro-5,8a-dimethyl-4,6-dioxo-3-naphthyl)propionic acid monohydrate top
Crystal data top
C15H18O4·H2ODx = 1.245 Mg m3
Mr = 280.31Melting point: 378 K
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
a = 8.720 (1) ÅCell parameters from 20 reflections
b = 18.170 (3) Åθ = 2.2–14.3°
c = 9.589 (2) ŵ = 0.09 mm1
β = 100.13 (2)°T = 248 K
V = 1495.6 (4) Å3Plate, colourless
Z = 40.4 × 0.3 × 0.2 mm
F(000) = 600
Data collection top
Siemens P4
diffractometer
Rint = 0.055
Radiation source: fine-focus sealed tubeθmax = 25.0°, θmin = 2.2°
Graphite monochromatorh = 1010
2θ/θ scansk = 2121
5800 measured reflectionsl = 1111
2725 independent reflections3 standard reflections every 97 reflections
1932 reflections with I > 2σ(I) intensity decay: variation < 1.5%
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)] = 0.052Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.103H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0291P)2 + 0.2925P]
where P = (Fo2 + 2Fc2)/3
2725 reflections(Δ/σ)max = 0.02
372 parametersΔρmax = 0.29 e Å3
5 restraintsΔρmin = 0.27 e Å3
Crystal data top
C15H18O4·H2OV = 1495.6 (4) Å3
Mr = 280.31Z = 4
Monoclinic, P21Mo Kα radiation
a = 8.720 (1) ŵ = 0.09 mm1
b = 18.170 (3) ÅT = 248 K
c = 9.589 (2) Å0.4 × 0.3 × 0.2 mm
β = 100.13 (2)°
Data collection top
Siemens P4
diffractometer
Rint = 0.055
5800 measured reflections3 standard reflections every 97 reflections
2725 independent reflections intensity decay: variation < 1.5%
1932 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.0525 restraints
wR(F2) = 0.103H atoms treated by a mixture of independent and constrained refinement
S = 1.05Δρmax = 0.29 e Å3
2725 reflectionsΔρmin = 0.27 e Å3
372 parameters
Special details top

Experimental. Crystal mounted on glass fiber with epoxy resin

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
O10.7849 (4)0.37401 (19)0.1651 (3)0.0456 (9)
O20.5164 (5)0.2379 (2)0.5464 (4)0.0647 (11)
O30.8529 (5)0.5388 (2)0.2780 (4)0.0647 (12)
O40.9098 (4)0.5363 (2)0.0610 (4)0.0566 (11)
O50.5996 (6)0.5984 (2)0.3871 (5)0.113 (2)
C10.8648 (5)0.3599 (3)0.2800 (5)0.0321 (11)
C21.0110 (5)0.4011 (2)0.3375 (5)0.0308 (11)
C31.1424 (5)0.3474 (3)0.3928 (5)0.0369 (12)
C41.0929 (6)0.2859 (3)0.4863 (5)0.0421 (13)
C4A0.9461 (6)0.2435 (3)0.4132 (5)0.0369 (12)
C50.9020 (7)0.1873 (3)0.5128 (5)0.0560 (15)
C60.7659 (8)0.1864 (3)0.5542 (6)0.0595 (16)
C70.6458 (7)0.2404 (3)0.5093 (5)0.0515 (15)
C80.6828 (5)0.3007 (3)0.4170 (5)0.0398 (12)
C8A0.8203 (5)0.3002 (3)0.3717 (4)0.0317 (11)
C91.0537 (5)0.4571 (2)0.2307 (5)0.0318 (11)
C100.9257 (6)0.5134 (3)0.1926 (5)0.0398 (12)
C111.2033 (6)0.4978 (3)0.2868 (6)0.0522 (15)
C120.5621 (6)0.3602 (3)0.3823 (6)0.0544 (15)
C130.9829 (7)0.2028 (3)0.2810 (5)0.0563 (16)
O1'0.2954 (4)0.30355 (19)1.0949 (3)0.0461 (9)
O2'0.1393 (4)0.4348 (2)0.7202 (4)0.0657 (11)
O3'0.3080 (4)0.14375 (19)0.9993 (4)0.0540 (10)
O4'0.4751 (4)0.1499 (2)1.2045 (4)0.0510 (10)
O5'0.6715 (5)0.5586 (2)0.6627 (3)0.0875 (15)
C1'0.3207 (5)0.3170 (2)0.9773 (5)0.0328 (11)
C2'0.4411 (5)0.2762 (2)0.9114 (5)0.0317 (11)
C3'0.5461 (5)0.3317 (3)0.8511 (5)0.0362 (12)
C4'0.4540 (5)0.3915 (3)0.7612 (5)0.0405 (12)
C4A'0.3414 (6)0.4329 (3)0.8417 (5)0.0394 (12)
C5'0.2531 (6)0.4898 (3)0.7465 (5)0.0478 (13)
C6'0.1002 (7)0.4909 (3)0.7093 (6)0.0538 (15)
C7'0.0030 (6)0.4341 (3)0.7567 (5)0.0424 (13)
C8'0.0815 (5)0.3749 (3)0.8480 (5)0.0348 (11)
C8A'0.2358 (5)0.3767 (2)0.8881 (4)0.0309 (11)
C9'0.5320 (5)0.2220 (3)1.0160 (5)0.0359 (12)
C10'0.4244 (6)0.1692 (3)1.0717 (5)0.0372 (12)
C11'0.6498 (6)0.1761 (3)0.9502 (6)0.0503 (14)
C12'0.0232 (6)0.3155 (3)0.8852 (5)0.0498 (14)
C13'0.4354 (6)0.4731 (3)0.9717 (5)0.0502 (15)
H40.842 (7)0.577 (3)0.048 (6)0.080*
HW10.67610.58600.35170.080*
HW20.55640.63960.38380.080*
H20.98990.42950.42010.037*
H3A1.22930.37490.44780.044*
H3B1.17970.32500.31200.044*
H4A1.07180.30760.57460.051*
H4B1.17920.25110.51090.051*
H50.97520.15080.54770.067*
H60.74580.14880.61580.071*
H91.06700.43050.14350.020 (10)*
H11A1.29040.46400.29540.078*
H11B1.19750.51840.37910.078*
H11C1.21770.53720.22200.078*
H12A0.54030.38160.46940.082*
H12B0.46730.33930.32890.082*
H12C0.60090.39810.32630.082*
H13A1.01000.23840.21410.085*
H13B0.89200.17510.23700.085*
H13C1.06950.16940.30930.085*
H4'0.429 (7)0.117 (4)1.239 (6)0.080*
HW30.73190.52310.68060.080*
HW40.66360.56980.57760.080*
H2'0.38470.24730.83080.038*
H3'A0.61650.35490.92980.043*
H3'B0.61010.30520.79320.043*
H4'A0.39410.36910.67580.049*
H4'B0.52690.42680.73150.049*
H5'0.31040.52700.71110.057*
H6'0.05290.52900.65090.065*
H9A0.58980.25021.09690.043*
H11D0.70420.14261.02080.075*
H11E0.72440.20870.91790.075*
H11F0.59500.14810.87060.075*
H12D0.03830.27930.94510.075*
H12E0.07590.29190.79930.075*
H12F0.09980.33670.93550.075*
H13D0.36430.49911.02170.075*
H13E0.50630.50800.94030.075*
H13F0.49440.43741.03470.075*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0360 (18)0.059 (2)0.0395 (19)0.0042 (19)0.0008 (16)0.0098 (19)
O20.073 (3)0.067 (3)0.064 (3)0.022 (2)0.038 (2)0.008 (2)
O30.078 (3)0.063 (3)0.060 (2)0.033 (2)0.033 (2)0.011 (2)
O40.067 (3)0.056 (3)0.050 (2)0.026 (2)0.019 (2)0.015 (2)
O50.146 (5)0.115 (4)0.093 (3)0.082 (4)0.066 (3)0.024 (3)
C10.028 (2)0.038 (3)0.031 (3)0.009 (2)0.006 (2)0.001 (2)
C20.030 (3)0.030 (3)0.034 (3)0.002 (2)0.008 (2)0.001 (2)
C30.028 (3)0.045 (3)0.036 (3)0.007 (2)0.000 (2)0.001 (2)
C40.043 (3)0.043 (3)0.038 (3)0.011 (3)0.000 (2)0.008 (2)
C4A0.044 (3)0.035 (3)0.031 (2)0.004 (3)0.006 (2)0.003 (2)
C50.073 (4)0.041 (3)0.054 (4)0.003 (3)0.013 (3)0.005 (3)
C60.090 (5)0.041 (3)0.050 (3)0.003 (4)0.019 (3)0.010 (3)
C70.057 (4)0.058 (4)0.043 (3)0.023 (3)0.018 (3)0.010 (3)
C80.042 (3)0.047 (3)0.033 (3)0.017 (3)0.015 (2)0.002 (2)
C8A0.035 (3)0.029 (3)0.029 (2)0.009 (2)0.001 (2)0.003 (2)
C90.030 (2)0.032 (3)0.036 (3)0.001 (2)0.013 (2)0.005 (2)
C100.048 (3)0.035 (3)0.039 (3)0.001 (2)0.014 (3)0.001 (2)
C110.043 (3)0.041 (3)0.074 (4)0.007 (3)0.013 (3)0.004 (3)
C120.031 (3)0.079 (4)0.055 (3)0.009 (3)0.011 (2)0.006 (3)
C130.074 (4)0.043 (3)0.054 (3)0.010 (3)0.014 (3)0.006 (3)
O1'0.055 (2)0.051 (2)0.0364 (19)0.0061 (19)0.0198 (17)0.0072 (17)
O2'0.045 (2)0.066 (3)0.081 (3)0.017 (2)0.003 (2)0.000 (2)
O3'0.057 (2)0.041 (2)0.061 (2)0.0157 (19)0.002 (2)0.0012 (18)
O4'0.056 (2)0.050 (2)0.045 (2)0.0085 (19)0.0049 (18)0.0088 (18)
O5'0.131 (4)0.072 (3)0.068 (3)0.054 (3)0.038 (3)0.008 (2)
C1'0.030 (3)0.028 (3)0.040 (3)0.011 (2)0.005 (2)0.004 (2)
C2'0.033 (3)0.033 (3)0.029 (2)0.002 (2)0.006 (2)0.005 (2)
C3'0.029 (3)0.051 (3)0.031 (3)0.005 (2)0.010 (2)0.002 (2)
C4'0.043 (3)0.047 (3)0.032 (3)0.007 (3)0.010 (2)0.010 (2)
C4A'0.047 (3)0.034 (3)0.036 (3)0.003 (3)0.003 (2)0.001 (2)
C5'0.062 (4)0.030 (3)0.052 (3)0.002 (3)0.013 (3)0.009 (3)
C6'0.063 (4)0.037 (3)0.059 (4)0.015 (3)0.005 (3)0.012 (3)
C7'0.049 (3)0.039 (3)0.040 (3)0.010 (3)0.010 (3)0.008 (3)
C8'0.038 (3)0.032 (3)0.035 (2)0.005 (2)0.008 (2)0.004 (2)
C8A'0.038 (3)0.024 (3)0.032 (2)0.003 (2)0.008 (2)0.004 (2)
C9'0.034 (3)0.034 (3)0.039 (3)0.006 (2)0.005 (2)0.002 (2)
C10'0.042 (3)0.030 (3)0.037 (3)0.004 (2)0.000 (2)0.006 (2)
C11'0.042 (3)0.043 (3)0.067 (3)0.006 (3)0.014 (3)0.002 (3)
C12'0.035 (3)0.068 (4)0.048 (3)0.004 (3)0.012 (2)0.001 (3)
C13'0.061 (4)0.034 (3)0.055 (4)0.011 (3)0.009 (3)0.005 (3)
Geometric parameters (Å, º) top
O1—C11.222 (5)O4—H40.94 (6)
O2—C71.242 (6)O5—HW10.8307
O3—C101.212 (5)O5—HW20.8373
O4—C101.313 (6)C2—H20.9900
C1—C8A1.490 (6)C3—H3A0.9800
C1—C21.498 (6)C3—H3B0.9800
C2—C31.527 (6)C4—H4A0.9800
C2—C91.535 (6)C4—H4B0.9800
C3—C41.542 (7)C5—H50.9400
C4—C4A1.552 (6)C6—H60.9400
C4A—C51.494 (7)C9—H90.9900
C4A—C8A1.507 (6)C11—H11A0.9700
C4A—C131.548 (6)C11—H11B0.9700
C5—C61.316 (8)C11—H11C0.9700
C6—C71.444 (8)C12—H12A0.9700
C7—C81.479 (7)C12—H12B0.9700
C8—C8A1.345 (6)C12—H12C0.9700
C8—C121.505 (7)C13—H13A0.9700
C9—C101.511 (6)C13—H13B0.9700
C9—C111.513 (6)C13—H13C0.9700
O1'—C1'1.212 (5)O4'—H4'0.82 (6)
O2'—C7'1.228 (6)O5'—HW30.8314
O3'—C10'1.216 (5)O5'—HW40.8318
O4'—C10'1.320 (6)C2'—H2'0.9900
C1'—C8A'1.494 (6)C3'—H3'A0.9800
C1'—C2'1.511 (6)C3'—H3'B0.9800
C2'—C9'1.525 (6)C4'—H4'A0.9800
C2'—C3'1.541 (6)C4'—H4'B0.9800
C3'—C4'1.524 (6)C5'—H5'0.9400
C4'—C4A'1.546 (6)C6'—H6'0.9400
C4A'—C8A'1.494 (6)C9'—H9A0.9900
C4A'—C5'1.499 (6)C11'—H11D0.9700
C4A'—C13'1.550 (6)C11'—H11E0.9700
C5'—C6'1.318 (7)C11'—H11F0.9700
C6'—C7'1.458 (7)C12'—H12D0.9700
C7'—C8'1.476 (7)C12'—H12E0.9700
C8'—C8A'1.333 (6)C12'—H12F0.9700
C8'—C12'1.498 (7)C13'—H13D0.9700
C9'—C10'1.504 (7)C13'—H13E0.9700
C9'—C11'1.542 (7)C13'—H13F0.9700
O1—C1—C8A121.2 (4)H3A—C3—H3B107.7
O1—C1—C2122.7 (4)C3—C4—H4A109.0
C8A—C1—C2116.1 (4)C4A—C4—H4A109.0
C1—C2—C3110.3 (4)C3—C4—H4B109.0
C1—C2—C9112.1 (4)C4A—C4—H4B109.0
C3—C2—C9113.5 (4)H4A—C4—H4B107.8
C2—C3—C4113.2 (4)C6—C5—H5118.4
C3—C4—C4A113.0 (4)C4A—C5—H5118.4
C5—C4A—C8A112.3 (4)C5—C6—H6118.4
C5—C4A—C13108.1 (4)C7—C6—H6118.4
C8A—C4A—C13110.9 (4)C10—C9—H9108.5
C5—C4A—C4109.6 (4)C11—C9—H9108.5
C8A—C4A—C4106.5 (4)C2—C9—H9108.5
C13—C4A—C4109.5 (4)C9—C11—H11A109.5
C6—C5—C4A123.3 (6)C9—C11—H11B109.5
C5—C6—C7123.1 (5)H11A—C11—H11B109.5
O2—C7—C6122.5 (5)C9—C11—H11C109.5
O2—C7—C8120.2 (5)H11A—C11—H11C109.5
C6—C7—C8117.3 (5)H11B—C11—H11C109.5
C8A—C8—C7119.3 (5)C8—C12—H12A109.5
C8A—C8—C12124.2 (5)C8—C12—H12B109.5
C7—C8—C12116.5 (4)H12A—C12—H12B109.5
C8—C8A—C1121.7 (4)C8—C12—H12C109.5
C8—C8A—C4A124.6 (4)H12A—C12—H12C109.5
C1—C8A—C4A113.6 (4)H12B—C12—H12C109.5
C10—C9—C11108.0 (4)C4A—C13—H13A109.5
C10—C9—C2110.8 (4)C4A—C13—H13B109.5
C11—C9—C2112.5 (4)H13A—C13—H13B109.5
O3—C10—O4123.3 (5)C4A—C13—H13C109.5
O3—C10—C9123.2 (5)H13A—C13—H13C109.5
O4—C10—C9113.3 (4)H13B—C13—H13C109.5
O1'—C1'—C8A'121.8 (4)C10'—O4'—H4'119 (4)
O1'—C1'—C2'122.9 (4)HW3—O5'—HW4109.4
C8A'—C1'—C2'115.3 (4)C1'—C2'—H2'107.5
C1'—C2'—C9'111.1 (4)C9'—C2'—H2'107.5
C1'—C2'—C3'109.8 (4)C3'—C2'—H2'107.5
C9'—C2'—C3'113.3 (4)C4'—C3'—H3'A109.0
C4'—C3'—C2'112.9 (4)C2'—C3'—H3'A109.0
C3'—C4'—C4A'112.5 (4)C4'—C3'—H3'B109.0
C8A'—C4A'—C5'112.0 (4)C2'—C3'—H3'B109.0
C8A'—C4A'—C4'107.2 (4)H3'A—C3'—H3'B107.8
C5'—C4A'—C4'109.6 (4)C3'—C4'—H4'A109.1
C8A'—C4A'—C13'110.4 (4)C4A'—C4'—H4'A109.1
C5'—C4A'—C13'107.9 (4)C3'—C4'—H4'B109.1
C4'—C4A'—C13'109.8 (4)C4A'—C4'—H4'B109.1
C6'—C5'—C4A'124.2 (5)H4'A—C4'—H4'B107.8
C5'—C6'—C7'121.4 (5)C6'—C5'—H5'117.9
O2'—C7'—C6'121.1 (5)C4A'—C5'—H5'117.9
O2'—C7'—C8'121.1 (5)C5'—C6'—H6'119.3
C6'—C7'—C8'117.8 (4)C7'—C6'—H6'119.3
C8A'—C8'—C7'119.5 (5)C10'—C9'—H9A108.4
C8A'—C8'—C12'125.2 (5)C2'—C9'—H9A108.4
C7'—C8'—C12'115.3 (4)C11'—C9'—H9A108.4
C8'—C8A'—C4A'125.1 (4)C9'—C11'—H11D109.5
C8'—C8A'—C1'121.3 (4)C9'—C11'—H11E109.5
C4A'—C8A'—C1'113.4 (4)H11D—C11'—H11E109.5
C10'—C9'—C2'111.2 (4)C9'—C11'—H11F109.5
C10'—C9'—C11'107.6 (4)H11D—C11'—H11F109.5
C2'—C9'—C11'112.8 (4)H11E—C11'—H11F109.5
O3'—C10'—O4'123.7 (5)C8'—C12'—H12D109.5
O3'—C10'—C9'123.3 (4)C8'—C12'—H12E109.5
O4'—C10'—C9'112.9 (4)H12D—C12'—H12E109.5
C10—O4—H4109 (4)C8'—C12'—H12F109.5
HW1—O5—HW2127.9H12D—C12'—H12F109.5
C1—C2—H2106.8H12E—C12'—H12F109.5
C3—C2—H2106.8C4A'—C13'—H13D109.5
C9—C2—H2106.8C4A'—C13'—H13E109.5
C2—C3—H3A108.9H13D—C13'—H13E109.5
C4—C3—H3A108.9C4A'—C13'—H13F109.5
C2—C3—H3B108.9H13D—C13'—H13F109.5
C4—C3—H3B108.9H13E—C13'—H13F109.5
O1—C1—C2—C3132.5 (4)O1'—C1'—C2'—C9'4.6 (6)
C8A—C1—C2—C347.9 (5)C8A'—C1'—C2'—C9'174.3 (4)
O1—C1—C2—C94.9 (6)O1'—C1'—C2'—C3'130.7 (4)
C8A—C1—C2—C9175.5 (4)C8A'—C1'—C2'—C3'48.2 (5)
C1—C2—C3—C446.5 (5)C1'—C2'—C3'—C4'48.0 (5)
C9—C2—C3—C4173.4 (4)C9'—C2'—C3'—C4'172.8 (4)
C2—C3—C4—C4A53.6 (5)C2'—C3'—C4'—C4A'54.9 (5)
C3—C4—C4A—C5177.6 (4)C3'—C4'—C4A'—C8A'57.3 (5)
C3—C4—C4A—C8A55.9 (5)C3'—C4'—C4A'—C5'179.1 (4)
C3—C4—C4A—C1364.0 (5)C3'—C4'—C4A'—C13'62.6 (5)
C8A—C4A—C5—C62.6 (7)C8A'—C4A'—C5'—C6'0.8 (7)
C13—C4A—C5—C6120.0 (6)C4'—C4A'—C5'—C6'119.6 (6)
C4—C4A—C5—C6120.7 (6)C13'—C4A'—C5'—C6'120.9 (6)
C4A—C5—C6—C71.1 (9)C4A'—C5'—C6'—C7'1.5 (8)
C5—C6—C7—O2178.2 (6)C5'—C6'—C7'—O2'179.0 (5)
C5—C6—C7—C82.4 (8)C5'—C6'—C7'—C8'0.1 (8)
O2—C7—C8—C8A176.4 (5)O2'—C7'—C8'—C8A'178.5 (5)
C6—C7—C8—C8A4.2 (7)C6'—C7'—C8'—C8A'2.6 (6)
O2—C7—C8—C124.9 (7)O2'—C7'—C8'—C12'2.9 (7)
C6—C7—C8—C12174.5 (5)C6'—C7'—C8'—C12'176.0 (4)
C7—C8—C8A—C1179.2 (4)C7'—C8'—C8A'—C4A'3.5 (7)
C12—C8—C8A—C10.5 (7)C12'—C8'—C8A'—C4A'175.0 (4)
C7—C8—C8A—C4A2.7 (7)C7'—C8'—C8A'—C1'178.4 (4)
C12—C8—C8A—C4A175.9 (4)C12'—C8'—C8A'—C1'0.1 (7)
O1—C1—C8A—C858.4 (6)C5'—C4A'—C8A'—C8'1.8 (6)
C2—C1—C8A—C8121.2 (5)C4'—C4A'—C8A'—C8'118.4 (5)
O1—C1—C8A—C4A124.8 (4)C13'—C4A'—C8A'—C8'122.1 (5)
C2—C1—C8A—C4A55.6 (5)C5'—C4A'—C8A'—C1'177.1 (4)
C5—C4A—C8A—C80.6 (6)C4'—C4A'—C8A'—C1'56.9 (5)
C13—C4A—C8A—C8120.4 (5)C13'—C4A'—C8A'—C1'62.7 (5)
C4—C4A—C8A—C8120.5 (5)O1'—C1'—C8A'—C8'61.2 (6)
C5—C4A—C8A—C1176.1 (4)C2'—C1'—C8A'—C8'119.9 (5)
C13—C4A—C8A—C162.8 (5)O1'—C1'—C8A'—C4A'123.3 (5)
C4—C4A—C8A—C156.2 (5)C2'—C1'—C8A'—C4A'55.5 (5)
C1—C2—C9—C1060.3 (5)C1'—C2'—C9'—C10'55.8 (5)
C3—C2—C9—C10173.8 (4)C3'—C2'—C9'—C10'180.0 (4)
C1—C2—C9—C11178.8 (4)C1'—C2'—C9'—C11'176.8 (4)
C3—C2—C9—C1152.9 (5)C3'—C2'—C9'—C11'59.1 (5)
C11—C9—C10—O384.7 (6)C2'—C9'—C10'—O3'37.9 (6)
C2—C9—C10—O338.9 (6)C11'—C9'—C10'—O3'86.0 (6)
C11—C9—C10—O490.2 (5)C2'—C9'—C10'—O4'146.1 (4)
C2—C9—C10—O4146.2 (4)C11'—C9'—C10'—O4'90.0 (5)

Experimental details

(I)(II)
Crystal data
Chemical formulaC15H18O4C15H18O4·H2O
Mr262.29280.31
Crystal system, space groupMonoclinic, P21Monoclinic, P21
Temperature (K)293248
a, b, c (Å)7.679 (1), 14.644 (2), 12.461 (1)8.720 (1), 18.170 (3), 9.589 (2)
α, β, γ (°)90, 96.43 (1), 9090, 100.13 (2), 90
V3)1392.4 (3)1495.6 (4)
Z44
Radiation typeMo KαMo Kα
µ (mm1)0.090.09
Crystal size (mm)0.56 × 0.44 × 0.240.4 × 0.3 × 0.2
Data collection
DiffractometerSiemens P4
diffractometer
Siemens P4
diffractometer
Absorption correctionNumerical
(SHELXTL; Sheldrick, 1997)
Tmin, Tmax0.95, 0.97
No. of measured, independent and
observed [I > 2σ(I)] reflections
5478, 2553, 2110 5800, 2725, 1932
Rint0.0240.055
(sin θ/λ)max1)0.5940.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.033, 0.077, 1.08 0.052, 0.103, 1.05
No. of reflections25532725
No. of parameters355372
No. of restraints15
H-atom treatmentH atoms treated by a mixture of independent and constrained refinementH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.13, 0.100.29, 0.27

Computer programs: XSCANS (Siemens, 1996), XSCANS, SHELXTL (Sheldrick, 1997), SHELXTL.

Selected geometric parameters (Å, º) for (I) top
O3—C101.196 (3)O3'—C10'1.196 (3)
O4—C101.333 (4)O4'—C10'1.328 (3)
O3—C10—C9124.8 (3)O3'—C10'—C9'124.8 (3)
O4—C10—C9112.1 (3)O4'—C10'—C9'112.7 (2)
Selected geometric parameters (Å, º) for (II) top
O3—C101.212 (5)O3'—C10'1.216 (5)
O4—C101.313 (6)O4'—C10'1.320 (6)
O3—C10—C9123.2 (5)O3'—C10'—C9'123.3 (4)
O4—C10—C9113.3 (4)O4'—C10'—C9'112.9 (4)
 

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