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The title solvate of the steroid 17[beta]-estradiol (E2) with methanol and water, C18H24O2·0.67CH4O·0.33H2O, is the first E2 derivative to contain three crystallographically independent mol­ecules in the asymmetric unit. The three steroid mol­ecules, along with two methanol mol­ecules and a water mol­ecule, create a three-dimensional hydrogen-bonded system. Three-sided columns are formed, with the estradiol mol­ecules aligned lengthwise parallel to (101), and joined by solvent mol­ecules at both hydro­philic ends. The three estradiol mol­ecules differ slightly in their ring-bowing angles, i.e. the angle between the mean plane of the A ring and that of the BCD ring; this angle ranges from 7.1 to 12.2°.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270102021637/sq1003sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102021637/sq1003Isup2.hkl
Contains datablock I

CCDC reference: 205312

Comment top

17β-Estradiol, E2, is a member of the estrogen family of hormones. In recent years, interest in these molecules has primarily focused on understanding their biological role in initiating breast cancer. It is well known that their ability to form hydrogen bonds in the active site of the estrogen receptor (ER) influences biological activity. This ability to form hydrogen bonds has been clearly demonstrated in an array of crystal structures, especially of E2, containing different solvent molecules or other hydrogen-bond acceptors.

When comparing these structures, the flexibility of the hydrophobic region of the molecule, more specifically the B ring, becomes very apparent. Several papers have already discussed the ring bowing of this molecule (Cooper & Norton, 1969; Cody et al., 1971; Busetta et al., 1976; Duax et al., 1979). Weize & Brooks (1994) took it a step further, performing molecular-modeling calculations on observed and novel confirmations. Ivanov and coworkers carried out a related study which included a larger body of compounds and more detailed analysis (Ivanov et al., 1998). They concluded that there are two possible conformations very close in energy, which differ in the B-ring arrangement, although the chance of the strained-geometry binding is low, as one quarter of the binding energy (−11.9 kcal mol−1; 1 kcal mol−1 = 4.184 kJ mol−1) is predicted to be lost (Anstead et al., 1997). The point initially postulated by Weize & Brooks remains, that the flexibility to allow bending or other conformational changes of the ligand in the receptor appears energetically achievable, and this could be an important property in determining their activity.

Molecular-dynamics studies on the ligand binding domain (LBD) of the ER demonstrate that the motion of the LBD requires the A ring to remain fairly steady while the CD ring retains a higher degree of freedom. The range of motion found in that study (Reference?) agrees very well with the reported crystal structures. It is well known that the hydrogen bonding of the ligand in the LBD causes conformational changes in the receptor. This seemingly accommodating motion of the LBD and the ligand supports the idea postulated by Weize & Brooks that the flexibility of E2, or of any other ligand which enters the LBD, could also effect the activity of the ligand. A more rigid or flexible ligand could change the natural motion of the ER complex, resulting in a change in activation factor (AF-2) activity, and therefore possibly effecting coactivator recruitment. This process is not well understood; the flexibility of the ligand is certainly only one of many physical factors associated in the activity of E2. The structure of the solvate reported here continues the trend in observing the flexibility of this molecule from a structural and hydrogen-bonding view, while the molecule lies in the lowest energy conformation.

The crystal of the title compound, (I), contains three crystallographically unique E2 molecules (Fig. 1). The B rings of the E2 molecules adopt the typical conformation of a distorted 7α,8β half chair, and this is responsible for most of the structural flexibility. Calculation of the ring-bowing angle, as defined by Duax & Norton (1975), reveals a range of 5.1° for the three molecules. Table 1 compares the ring-bowing angles of the known E2 crystal structures. The spread of over 12°, with angles found distributed over the entire range, indicate the shallowness of the potential associated with the bowing deformation. In a system as dynamic as the human body, the molecule would certainly have a wide range of conformations easily available. \sch

The packing of (I) results in three-sided cylinders of estradiol molecules arranged parallel to (101), with the C18 methyl group pointing towards the center (Fig. 1). This, of course, aligns the large hydrophobic regions of the molecules, as well as the hydrophilic hydroxy groups. These cylinders then stack on top of each other, creating three-sided columns (Fig. 2) held together by hydrogen bonds involving the hydroxy groups and the three solvent molecules. A more detailed picture of the hydrogen bonding between the solvent and E2 molecules can be seen in Fig. 3 and from Table 2. There is also an intercolumnar hydrogen bond, which occurs between the water molecule and a 3-hydroxy group. This, along with the intercolumnar hydrogen-bonded solvent, creates a hydrophilic layer which is approximately 30° from perpendicular to the columns (Fig. 4). Structurally, all bond lengths and angles are in expected ranges.

Experimental top

Crystals were grown by slow evaporation from a methanol solution open to the air. It is presumed that the methanol was either wet prior to use in this experiment or absorbed atmospheric moisture. Crystals of (I) were grown over the course of 3 d and harvested when reaching the appropriate size.

Refinement top

The absolute configuration of the E2 molecules in (I) was known from the natural product starting material. The intensity data were corrected for decay and absorption using SADABS (Sheldrick, 1996). All H atoms on the solvent molecules and on the hydroxy groups of the E2 molecules were located in the difference map and refined with isotropic displacement parameters. The remaining H atoms were included with idealized geometries, with C—H distances in the range 0.96–0.98 Å Is this added text OK?, and their isotropic displacement parameters were refined.

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Siemens, 1994); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. A view of molecule A of (I), with the atom-numbering scheme; the other two molecules are similarly labeled, with the corresponding suffix B or C. Displacement ellipsoids are plotted at the 50% probability level. The solvent molecules have been omitted for clarity; the water molecule was labeled O3, while the O atoms of the methanol molecules A and B were labeled O4, with their C atoms labeled C19.
[Figure 2] Fig. 2. The molecular arrangement of (I), looking down the three-sided column. Displacement ellipsoids are plotted at the 50% probability level [symmetry codes: (i) x, y, z; (ii) −2 − x, y − 1/2, −1 − z; (iii) x − 1, y, z].
[Figure 3] Fig. 3. The packing of E2 groups in (I), with the hydrogen-bonded solvent molecules, viewed perpendicular to the columns. Dotted lines indicate the region detailed in Fig. 4. Displacement ellipsoids are plotted at the 50% probability level [symmetry codes: (i) x, y, z; (ii) 1 + x, y, 1 + z; (iii) −2 − x, y − 1/2, −1 − z; (iv) −1 − x, y − 1/2, −z; (v) x, y, 1 + z; (vi) −x, y − 1/2, −z].
[Figure 4] Fig. 4. The hydrogen-bonded region of the column shown in Fig. 3, including the solvent molecules and only the A or D rings of E2. Displacement ellipsoids are plotted at the 50% probability level [symmetry codes: (i) x, y, z; (ii) −x, y − 1/2, −z; (iii) −1 − x, y − 1/2, −z; (iv) 1 + x, y, 1 + z; (v) −2 − x, y − 1/2, −1 − z; (vi) x, y, 1 + z].
[Figure 5] Fig. 5. A schematic diagram of the packed columns in (I) and their relation to the hydrophilic layer containing the hydroxy groups and solvent molecules.
estra-1,3,5(10)-triene-3,17β-diol-methanol-water (3/2/1) top
Crystal data top
C18H24O2·0.67CH4O·0.33H2OF(000) = 980
Mr = 299.74Dx = 1.212 Mg m3
Monoclinic, P21Ag Kα radiation, λ = 0.56085 Å
a = 11.7152 (4) ÅCell parameters from 7309 reflections
b = 19.6270 (6) Åθ = 2.3–27.9°
c = 12.1310 (4) ŵ = 0.05 mm1
β = 117.978 (1)°T = 298 K
V = 2463.34 (14) Å3Cuboid, colorless
Z = 60.4 × 0.3 × 0.3 mm
Data collection top
Siemens SMART Platform CCD area-detector
diffractometer
21122 independent reflections
Radiation source: fine-focus sealed tube15597 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.048
ω scansθmax = 27.9°, θmin = 1.5°
Absorption correction: empirical (using intensity measurements)
multipole expansion (Blessing, 1995) using SADABS (Sheldrick, 1996)
h = 1819
Tmin = 0.840, Tmax = 0.985k = 3229
44195 measured reflectionsl = 2020
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)] = 0.058Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.145H atoms treated by a mixture of independent and constrained refinement
S = 0.99 w = 1/[σ2(Fo2) + (0.0812P)2]
where P = (Fo2 + 2Fc2)/3
21122 reflections(Δ/σ)max = 0.001
698 parametersΔρmax = 0.41 e Å3
1 restraintΔρmin = 0.23 e Å3
Crystal data top
C18H24O2·0.67CH4O·0.33H2OV = 2463.34 (14) Å3
Mr = 299.74Z = 6
Monoclinic, P21Ag Kα radiation, λ = 0.56085 Å
a = 11.7152 (4) ŵ = 0.05 mm1
b = 19.6270 (6) ÅT = 298 K
c = 12.1310 (4) Å0.4 × 0.3 × 0.3 mm
β = 117.978 (1)°
Data collection top
Siemens SMART Platform CCD area-detector
diffractometer
21122 independent reflections
Absorption correction: empirical (using intensity measurements)
multipole expansion (Blessing, 1995) using SADABS (Sheldrick, 1996)
15597 reflections with I > 2σ(I)
Tmin = 0.840, Tmax = 0.985Rint = 0.048
44195 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0581 restraint
wR(F2) = 0.145H atoms treated by a mixture of independent and constrained refinement
S = 0.99Δρmax = 0.41 e Å3
21122 reflectionsΔρmin = 0.23 e Å3
698 parameters
Special details top

Experimental. Preliminary examination and data collection were performed at 298 (1) K on a Siemens SMART Platform diffractometer equipped with a 2 K CCD detector located 6.12 cm from the crystal. 0.3° ω scans were carried out at three different ϕ settings and a detector position of −25° in 2θ, corresponding to a nominal sphere of data, with the frame time set at 30 s. The unit cell was initially refined with the SMART Software Package (Bruker, 1998). The final unit cell was obtained from the refinement of 7309 reflections after integration (SAINT 6; Bruker, 1999). The decay correction was applied simultaneously with the absorption correction in SADABS. No formal measure of the extent of decay is printed out by this program. The final unit cell is obtained from the refinement of the XYZ weighted centroids of reflections above 20 σ(I).

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
O1A0.58213 (11)0.44581 (7)0.24230 (11)0.0243 (2)
H1OA0.564 (3)0.4213 (14)0.191 (2)0.035 (7)*
O1B0.36786 (12)0.07606 (7)0.02309 (10)0.0242 (2)
H1OB0.310 (3)0.0470 (16)0.011 (3)0.060 (9)*
O1C0.38139 (12)0.14101 (7)0.19736 (10)0.0252 (2)
H1OC0.426 (2)0.1207 (13)0.180 (2)0.031 (6)*
C1A0.87445 (15)0.46604 (8)0.53895 (14)0.0220 (3)
H1A0.91400.49970.59890.030 (6)*
C1B0.66131 (15)0.10511 (8)0.31570 (14)0.0215 (3)
H1B0.73820.12920.34290.016 (4)*
C1C0.10431 (16)0.11852 (8)0.11370 (14)0.0211 (3)
H1C0.08470.09780.18950.032 (6)*
O2A1.54143 (11)0.36438 (7)1.05600 (10)0.0258 (2)
H2OA1.588 (2)0.3607 (12)1.028 (2)0.031 (6)*
O2B1.16785 (11)0.00670 (7)0.96783 (11)0.0265 (2)
H2OB1.181 (2)0.0430 (13)0.965 (2)0.024 (6)*
O2C0.54233 (12)0.24553 (7)0.63644 (11)0.0262 (2)
H2OC0.558 (2)0.2163 (13)0.679 (2)0.028 (6)*
C2A0.75822 (16)0.48097 (8)0.43363 (14)0.0228 (3)
H2A0.72150.52400.42320.025 (5)*
C2B0.57070 (16)0.10814 (8)0.19012 (14)0.0227 (3)
H2B0.58710.13380.13470.039 (6)*
C2C0.22891 (15)0.11229 (8)0.01588 (14)0.0220 (3)
H2C0.29090.08730.02590.034 (6)*
O30.55538 (14)0.07846 (8)0.16279 (14)0.0310 (3)
H3OA0.562 (3)0.0433 (19)0.182 (3)0.064 (10)*
H3OB0.572 (3)0.0802 (15)0.109 (3)0.044 (7)*
C3A0.69777 (14)0.43054 (8)0.34417 (13)0.0194 (3)
C3B0.45539 (14)0.07245 (8)0.14829 (13)0.0193 (3)
C3C0.25995 (15)0.14399 (8)0.09777 (13)0.0201 (3)
C4A0.75440 (14)0.36653 (8)0.36054 (13)0.0180 (2)
H4A0.71340.33290.30080.018 (5)*
C4B0.43123 (14)0.03468 (8)0.23238 (13)0.0185 (2)
H4B0.35350.01130.20430.014 (4)*
C4C0.16536 (15)0.17949 (8)0.11182 (13)0.0201 (3)
H4C0.18600.20000.18800.023 (5)*
O4A0.68702 (12)0.35029 (7)0.77190 (11)0.0278 (2)
H4OA0.638 (3)0.3198 (15)0.726 (2)0.042 (7)*
O4B1.74589 (11)0.35945 (6)1.01033 (11)0.0253 (2)
H4OB1.732 (2)0.3502 (12)0.943 (2)0.032 (6)*
C5A0.87205 (13)0.35197 (7)0.46537 (12)0.0167 (2)
C5B0.52322 (14)0.03151 (7)0.35913 (13)0.0171 (2)
C5C0.03962 (14)0.18516 (8)0.01380 (13)0.0186 (2)
C6A0.93086 (15)0.28226 (8)0.47474 (13)0.0206 (3)
H6A0.86250.24850.44460.024 (5)*
H6B0.97120.28090.42090.027 (5)*
C6B0.49137 (14)0.01254 (8)0.44334 (13)0.0205 (3)
H6C0.40350.00310.42670.020 (5)*
H6D0.49550.06000.42350.038 (6)*
C6C0.05782 (15)0.22562 (9)0.03581 (13)0.0223 (3)
H6E0.04970.21340.11670.038 (6)*
H6F0.03790.27370.03800.021 (5)*
C7A1.03110 (15)0.26353 (8)0.60694 (14)0.0212 (3)
H7A0.98830.25360.65680.022 (5)*
H7B1.07750.22300.60500.035 (6)*
C7B0.58222 (14)0.00116 (9)0.58210 (13)0.0216 (3)
H7C0.56050.04130.60870.016 (4)*
H7D0.57200.03790.63030.020 (5)*
C7C0.19687 (15)0.21376 (9)0.06365 (13)0.0230 (3)
H7E0.22530.16910.05250.033 (6)*
H7F0.25280.24760.05550.029 (5)*
C8A1.12641 (13)0.32245 (7)0.66598 (12)0.0157 (2)
H8A1.16450.33400.61170.013 (4)*
C8B0.72234 (13)0.00134 (8)0.60554 (12)0.0174 (2)
H8B0.73960.03940.56890.011 (4)*
C8C0.20613 (14)0.21864 (7)0.19346 (12)0.0167 (2)
H8C0.16600.26150.19870.018 (5)*
C9A1.05536 (14)0.38532 (7)0.67877 (12)0.0180 (2)
H9A1.02600.37310.73970.026 (5)*
C9B0.74143 (14)0.06525 (8)0.54097 (13)0.0187 (2)
H9B0.72500.10500.58040.017 (4)*
C9C0.13013 (14)0.15915 (7)0.21100 (13)0.0182 (2)
H9C0.17440.11720.20890.026 (5)*
C10A0.93396 (14)0.40215 (7)0.55787 (13)0.0176 (2)
C10B0.64086 (14)0.06704 (7)0.40294 (13)0.0179 (2)
C10C0.00703 (14)0.15472 (7)0.10297 (13)0.0181 (2)
C11A1.14894 (17)0.44601 (8)0.73560 (16)0.0278 (3)
H11A1.10240.48420.74610.038 (6)*
H11B1.18120.45980.67850.037 (6)*
C11B0.88177 (14)0.07140 (9)0.56326 (14)0.0221 (3)
H11D0.89920.03480.51960.023 (5)*
H11C0.89170.11420.52860.024 (5)*
C11C0.13627 (15)0.16209 (8)0.34092 (13)0.0216 (3)
H11F0.09460.12190.35210.026 (5)*
H11E0.08880.20170.34490.020 (5)*
C12A1.26406 (16)0.42772 (9)0.86301 (15)0.0258 (3)
H12B1.23310.42000.92340.032 (6)*
H12A1.32430.46560.89220.024 (5)*
C12B0.98135 (15)0.06837 (9)0.70274 (14)0.0231 (3)
H12D0.97330.10890.74440.027 (5)*
H12C1.06790.06760.71120.039 (6)*
C12C0.27582 (15)0.16589 (8)0.44779 (14)0.0220 (3)
H12F0.31990.12340.45210.025 (5)*
H12E0.27430.17210.52640.027 (5)*
C13A1.33352 (13)0.36405 (7)0.85340 (12)0.0172 (2)
C13B0.96102 (14)0.00486 (8)0.76528 (13)0.0184 (2)
C13C0.34993 (14)0.22482 (7)0.42817 (12)0.0177 (2)
C14A1.23506 (14)0.30552 (7)0.79588 (13)0.0177 (2)
H14A1.19390.30010.84950.024 (5)*
C14B0.82073 (14)0.00455 (8)0.74365 (12)0.0181 (2)
H14B0.80730.04840.77450.023 (5)*
C14C0.34407 (14)0.21704 (8)0.29916 (13)0.0184 (2)
H14C0.37770.17150.29780.024 (5)*
C15A1.31869 (16)0.24181 (8)0.81685 (15)0.0260 (3)
H15A1.27460.20130.82290.041 (7)*
H15B1.34070.23590.74970.039 (6)*
C15B0.81885 (16)0.04996 (9)0.83370 (14)0.0246 (3)
H15C0.75280.04010.85820.023 (5)*
H15D0.80320.09480.79590.021 (5)*
C15C0.44498 (16)0.26782 (9)0.30191 (14)0.0248 (3)
H15E0.48050.25290.24800.028 (5)*
H15F0.40760.31280.27580.031 (6)*
C16A1.44122 (16)0.25672 (9)0.94259 (15)0.0262 (3)
H16A1.51860.25340.93280.039 (6)*
H16B1.44800.22471.00630.046 (7)*
C16B0.95591 (16)0.04548 (9)0.94733 (14)0.0258 (3)
H16C0.99760.08980.96550.037 (6)*
H16D0.95110.02951.02070.038 (6)*
C16C0.55067 (16)0.26816 (10)0.44117 (15)0.0279 (3)
H16E0.56550.31410.47450.027 (5)*
H16F0.63140.25000.44960.027 (5)*
C17A1.42375 (14)0.32978 (8)0.97817 (13)0.0205 (3)
H17A1.37550.32631.02560.018 (5)*
C17B1.03165 (14)0.00568 (8)0.90947 (13)0.0223 (3)
H17B1.01900.05100.93590.034 (6)*
C17C0.49737 (15)0.22253 (8)0.51007 (13)0.0213 (3)
H17C0.52730.17570.51170.022 (5)*
C18A1.40797 (16)0.37955 (9)0.78083 (14)0.0248 (3)
H18C1.46750.41620.82070.037 (6)*
H18B1.45480.33970.77940.038 (6)*
H18A1.34820.39240.69690.026 (5)*
C18B0.99729 (15)0.05956 (8)0.71729 (14)0.0227 (3)
H18F0.95300.05970.62770.019 (5)*
H18E1.08890.06020.74640.043 (7)*
H18D0.97270.09910.74780.034 (6)*
C18C0.29872 (16)0.29384 (8)0.44580 (14)0.0231 (3)
H18I0.30470.29570.52740.042 (7)*
H18H0.34940.32990.43730.052 (8)*
H18G0.21010.29900.38370.037 (6)*
C19A0.78384 (17)0.36507 (10)0.73591 (17)0.0311 (4)
H19A0.83960.40030.78870.044 (7)*
H19B0.83370.32480.74410.063 (9)*
H19C0.74360.38010.65070.028 (5)*
C19B1.81899 (17)0.30435 (9)1.08827 (16)0.0282 (3)
H19G1.83790.31341.17290.031 (6)*
H19D1.76990.26301.06040.034 (6)*
H19E1.89830.29951.08390.045 (7)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O1A0.0197 (5)0.0271 (6)0.0183 (5)0.0061 (4)0.0025 (4)0.0009 (4)
O1B0.0230 (5)0.0288 (6)0.0156 (4)0.0007 (5)0.0047 (4)0.0011 (4)
O1C0.0203 (5)0.0309 (6)0.0194 (5)0.0071 (5)0.0051 (4)0.0025 (4)
C1A0.0218 (7)0.0205 (7)0.0199 (6)0.0032 (5)0.0066 (5)0.0038 (5)
C1B0.0194 (6)0.0212 (7)0.0204 (6)0.0024 (5)0.0065 (5)0.0018 (5)
C1C0.0237 (7)0.0204 (7)0.0187 (6)0.0029 (5)0.0094 (5)0.0028 (5)
O2A0.0168 (5)0.0391 (7)0.0173 (5)0.0037 (5)0.0045 (4)0.0053 (4)
O2B0.0174 (5)0.0276 (6)0.0242 (5)0.0015 (5)0.0012 (4)0.0005 (4)
O2C0.0285 (6)0.0276 (6)0.0157 (5)0.0019 (5)0.0046 (4)0.0017 (4)
C2A0.0238 (7)0.0210 (7)0.0197 (6)0.0064 (5)0.0068 (5)0.0014 (5)
C2B0.0224 (7)0.0223 (7)0.0211 (6)0.0017 (6)0.0084 (5)0.0054 (5)
C2C0.0224 (7)0.0216 (7)0.0214 (6)0.0045 (6)0.0098 (5)0.0013 (5)
O30.0372 (7)0.0294 (7)0.0327 (7)0.0120 (6)0.0217 (6)0.0083 (5)
C3A0.0180 (6)0.0226 (7)0.0163 (5)0.0032 (5)0.0069 (5)0.0013 (5)
C3B0.0205 (6)0.0181 (6)0.0166 (6)0.0030 (5)0.0065 (5)0.0002 (5)
C3C0.0205 (6)0.0201 (7)0.0185 (6)0.0035 (5)0.0080 (5)0.0004 (5)
C4A0.0152 (5)0.0208 (6)0.0163 (5)0.0006 (5)0.0059 (4)0.0006 (5)
C4B0.0171 (6)0.0197 (6)0.0162 (5)0.0002 (5)0.0056 (5)0.0011 (5)
C4C0.0218 (6)0.0215 (7)0.0173 (6)0.0023 (5)0.0095 (5)0.0009 (5)
O4A0.0244 (6)0.0361 (7)0.0255 (5)0.0071 (5)0.0139 (5)0.0048 (5)
O4B0.0226 (5)0.0290 (6)0.0220 (5)0.0017 (5)0.0084 (4)0.0023 (4)
C5A0.0156 (6)0.0183 (6)0.0163 (5)0.0010 (5)0.0076 (5)0.0013 (4)
C5B0.0170 (6)0.0157 (6)0.0171 (5)0.0013 (5)0.0068 (5)0.0003 (4)
C5C0.0209 (6)0.0191 (6)0.0167 (6)0.0021 (5)0.0095 (5)0.0004 (5)
C6A0.0186 (6)0.0171 (6)0.0190 (6)0.0013 (5)0.0029 (5)0.0033 (5)
C6B0.0156 (6)0.0254 (7)0.0182 (6)0.0023 (5)0.0061 (5)0.0010 (5)
C6C0.0216 (7)0.0291 (8)0.0163 (6)0.0053 (6)0.0090 (5)0.0020 (5)
C7A0.0191 (6)0.0153 (6)0.0219 (6)0.0005 (5)0.0037 (5)0.0009 (5)
C7B0.0166 (6)0.0298 (7)0.0166 (6)0.0005 (6)0.0063 (5)0.0010 (5)
C7C0.0221 (7)0.0322 (8)0.0168 (6)0.0015 (6)0.0110 (5)0.0004 (5)
C8A0.0152 (5)0.0147 (6)0.0153 (5)0.0002 (4)0.0055 (4)0.0004 (4)
C8B0.0151 (5)0.0197 (6)0.0157 (5)0.0001 (5)0.0058 (4)0.0001 (5)
C8C0.0174 (6)0.0178 (6)0.0155 (5)0.0001 (5)0.0083 (5)0.0005 (4)
C9A0.0165 (6)0.0201 (6)0.0146 (5)0.0014 (5)0.0051 (5)0.0017 (4)
C9B0.0173 (6)0.0186 (6)0.0166 (5)0.0012 (5)0.0050 (5)0.0010 (5)
C9C0.0209 (6)0.0169 (6)0.0172 (5)0.0002 (5)0.0092 (5)0.0010 (5)
C10A0.0165 (6)0.0184 (6)0.0155 (5)0.0012 (5)0.0055 (5)0.0015 (4)
C10B0.0177 (6)0.0166 (6)0.0173 (5)0.0018 (5)0.0066 (5)0.0009 (5)
C10C0.0205 (6)0.0162 (6)0.0172 (5)0.0016 (5)0.0086 (5)0.0001 (5)
C11A0.0250 (7)0.0185 (7)0.0265 (7)0.0025 (6)0.0009 (6)0.0055 (6)
C11B0.0167 (6)0.0263 (7)0.0195 (6)0.0029 (5)0.0054 (5)0.0030 (5)
C11C0.0230 (7)0.0257 (7)0.0163 (6)0.0055 (6)0.0093 (5)0.0011 (5)
C12A0.0214 (7)0.0259 (7)0.0220 (7)0.0020 (6)0.0034 (5)0.0088 (6)
C12B0.0180 (6)0.0253 (7)0.0204 (6)0.0020 (6)0.0044 (5)0.0007 (5)
C12C0.0247 (7)0.0220 (7)0.0181 (6)0.0012 (6)0.0091 (5)0.0040 (5)
C13A0.0155 (5)0.0194 (6)0.0150 (5)0.0014 (5)0.0059 (4)0.0013 (5)
C13B0.0156 (5)0.0203 (6)0.0166 (5)0.0004 (5)0.0053 (5)0.0017 (5)
C13C0.0179 (6)0.0193 (6)0.0151 (5)0.0005 (5)0.0071 (5)0.0004 (5)
C14A0.0165 (6)0.0176 (6)0.0170 (5)0.0018 (5)0.0060 (5)0.0006 (5)
C14B0.0169 (6)0.0210 (6)0.0142 (5)0.0019 (5)0.0055 (4)0.0006 (5)
C14C0.0189 (6)0.0202 (6)0.0169 (6)0.0007 (5)0.0091 (5)0.0003 (5)
C15A0.0204 (7)0.0186 (7)0.0265 (7)0.0017 (6)0.0006 (6)0.0001 (5)
C15B0.0213 (7)0.0318 (8)0.0185 (6)0.0011 (6)0.0075 (5)0.0050 (6)
C15C0.0217 (7)0.0343 (8)0.0180 (6)0.0055 (6)0.0091 (5)0.0015 (6)
C16A0.0197 (7)0.0250 (8)0.0245 (7)0.0024 (6)0.0025 (5)0.0032 (6)
C16B0.0228 (7)0.0341 (8)0.0165 (6)0.0037 (6)0.0059 (5)0.0030 (6)
C16C0.0193 (7)0.0388 (9)0.0214 (7)0.0048 (6)0.0062 (5)0.0026 (6)
C17A0.0164 (6)0.0273 (7)0.0154 (5)0.0013 (5)0.0053 (5)0.0013 (5)
C17B0.0170 (6)0.0255 (7)0.0176 (6)0.0028 (5)0.0024 (5)0.0026 (5)
C17C0.0183 (6)0.0244 (7)0.0175 (6)0.0006 (5)0.0054 (5)0.0000 (5)
C18A0.0223 (7)0.0329 (8)0.0192 (6)0.0073 (6)0.0096 (5)0.0004 (6)
C18B0.0198 (6)0.0247 (7)0.0214 (6)0.0042 (6)0.0078 (5)0.0018 (5)
C18C0.0252 (7)0.0223 (7)0.0207 (6)0.0017 (6)0.0099 (6)0.0034 (5)
C19A0.0234 (7)0.0372 (10)0.0359 (8)0.0034 (7)0.0165 (7)0.0000 (7)
C19B0.0254 (8)0.0272 (8)0.0295 (8)0.0006 (6)0.0109 (6)0.0053 (6)
Geometric parameters (Å, º) top
O1A—C3A1.3716 (18)C9A—H9A0.9800
O1A—H1OA0.74 (3)C9B—C10B1.5305 (19)
O1B—C3B1.3792 (17)C9B—C11B1.541 (2)
O1B—H1OB0.85 (3)C9B—H9B0.9800
O1C—C3C1.3691 (18)C9C—C10C1.527 (2)
O1C—H1OC0.76 (3)C9C—C11C1.5447 (19)
C1A—C2A1.393 (2)C9C—H9C0.9800
C1A—C10A1.400 (2)C11A—C12A1.543 (2)
C1A—H1A0.9300C11A—H11A0.9700
C1B—C2B1.391 (2)C11A—H11B0.9700
C1B—C10B1.405 (2)C11B—C12B1.541 (2)
C1B—H1B0.9300C11B—H11D0.9700
C1C—C2C1.389 (2)C11B—H11C0.9700
C1C—C10C1.400 (2)C11C—C12C1.540 (2)
C1C—H1C0.9300C11C—H11F0.9700
O2A—C17A1.4254 (19)C11C—H11E0.9700
O2A—H2OA0.76 (3)C12A—C13A1.525 (2)
O2B—C17B1.4305 (19)C12A—H12B0.9700
O2B—H2OB0.73 (2)C12A—H12A0.9700
O2C—C17C1.4400 (19)C12B—C13B1.535 (2)
O2C—H2OC0.73 (2)C12B—H12D0.9700
C2A—C3A1.392 (2)C12B—H12C0.9700
C2A—H2A0.9300C12C—C13C1.530 (2)
C2B—C3B1.389 (2)C12C—H12F0.9700
C2B—H2B0.9300C12C—H12E0.9700
C2C—C3C1.396 (2)C13A—C18A1.533 (2)
C2C—H2C0.9300C13A—C17A1.536 (2)
O3—H3OA0.72 (4)C13A—C14A1.543 (2)
O3—H3OB0.76 (3)C13B—C18B1.533 (2)
C3A—C4A1.391 (2)C13B—C14B1.538 (2)
C3B—C4B1.393 (2)C13B—C17B1.545 (2)
C3C—C4C1.386 (2)C13C—C18C1.537 (2)
C4A—C5A1.3979 (19)C13C—C17C1.537 (2)
C4A—H4A0.9300C13C—C14C1.5416 (19)
C4B—C5B1.4053 (19)C14A—C15A1.534 (2)
C4B—H4B0.9300C14A—H14A0.9800
C4C—C5C1.397 (2)C14B—C15B1.537 (2)
C4C—H4C0.9300C14B—H14B0.9800
O4A—C19A1.423 (2)C14C—C15C1.535 (2)
O4A—H4OA0.83 (3)C14C—H14C0.9800
O4B—C19B1.427 (2)C15A—C16A1.555 (2)
O4B—H4OB0.78 (2)C15A—H15A0.9700
C5A—C10A1.4112 (19)C15A—H15B0.9700
C5A—C6A1.512 (2)C15B—C16B1.552 (2)
C5B—C10B1.407 (2)C15B—H15C0.9700
C5B—C6B1.513 (2)C15B—H15D0.9700
C5C—C10C1.4149 (19)C15C—C16C1.557 (2)
C5C—C6C1.514 (2)C15C—H15E0.9700
C6A—C7A1.523 (2)C15C—H15F0.9700
C6A—H6A0.9700C16A—C17A1.539 (2)
C6A—H6B0.9700C16A—H16A0.9700
C6B—C7B1.528 (2)C16A—H16B0.9700
C6B—H6C0.9700C16B—C17B1.546 (2)
C6B—H6D0.9700C16B—H16C0.9700
C6C—C7C1.523 (2)C16B—H16D0.9700
C6C—H6E0.9700C16C—C17C1.543 (2)
C6C—H6F0.9700C16C—H16E0.9700
C7A—C8A1.532 (2)C16C—H16F0.9700
C7A—H7A0.9700C17A—H17A0.9800
C7A—H7B0.9700C17B—H17B0.9800
C7B—C8B1.530 (2)C17C—H17C0.9800
C7B—H7C0.9700C18A—H18C0.9600
C7B—H7D0.9700C18A—H18B0.9600
C7C—C8C1.5299 (19)C18A—H18A0.9600
C7C—H7E0.9700C18B—H18F0.9600
C7C—H7F0.9700C18B—H18E0.9600
C8A—C14A1.5270 (19)C18B—H18D0.9600
C8A—C9A1.536 (2)C18C—H18I0.9600
C8A—H8A0.9800C18C—H18H0.9600
C8B—C14B1.5257 (18)C18C—H18G0.9600
C8B—C9B1.550 (2)C19A—H19A0.9600
C8B—H8B0.9800C19A—H19B0.9600
C8C—C14C1.521 (2)C19A—H19C0.9600
C8C—C9C1.542 (2)C19B—H19G0.9600
C8C—H8C0.9800C19B—H19D0.9600
C9A—C10A1.5251 (19)C19B—H19E0.9600
C9A—C11A1.545 (2)
C3A—O1A—H1OA113 (2)H11D—C11B—H11C107.8
C3B—O1B—H1OB106 (2)C12C—C11C—C9C112.56 (12)
C3C—O1C—H1OC110.3 (18)C12C—C11C—H11F109.1
C2A—C1A—C10A122.41 (14)C9C—C11C—H11F109.1
C2A—C1A—H1A118.8C12C—C11C—H11E109.1
C10A—C1A—H1A118.8C9C—C11C—H11E109.1
C2B—C1B—C10B122.39 (14)H11F—C11C—H11E107.8
C2B—C1B—H1B118.8C13A—C12A—C11A111.17 (12)
C10B—C1B—H1B118.8C13A—C12A—H12B109.4
C2C—C1C—C10C122.72 (13)C11A—C12A—H12B109.4
C2C—C1C—H1C118.6C13A—C12A—H12A109.4
C10C—C1C—H1C118.6C11A—C12A—H12A109.4
C17A—O2A—H2OA109.3 (18)H12B—C12A—H12A108.0
C17B—O2B—H2OB110.2 (19)C13B—C12B—C11B111.16 (12)
C17C—O2C—H2OC110.2 (19)C13B—C12B—H12D109.4
C3A—C2A—C1A119.11 (14)C11B—C12B—H12D109.4
C3A—C2A—H2A120.4C13B—C12B—H12C109.4
C1A—C2A—H2A120.4C11B—C12B—H12C109.4
C3B—C2B—C1B119.36 (14)H12D—C12B—H12C108.0
C3B—C2B—H2B120.3C13C—C12C—C11C111.18 (12)
C1B—C2B—H2B120.3C13C—C12C—H12F109.4
C1C—C2C—C3C119.14 (14)C11C—C12C—H12F109.4
C1C—C2C—H2C120.4C13C—C12C—H12E109.4
C3C—C2C—H2C120.4C11C—C12C—H12E109.4
H3OA—O3—H3OB107 (3)H12F—C12C—H12E108.0
O1A—C3A—C4A121.96 (14)C12A—C13A—C18A110.43 (14)
O1A—C3A—C2A118.25 (13)C12A—C13A—C17A115.38 (12)
C4A—C3A—C2A119.79 (13)C18A—C13A—C17A109.81 (12)
O1B—C3B—C2B118.01 (13)C12A—C13A—C14A109.39 (12)
O1B—C3B—C4B122.15 (14)C18A—C13A—C14A113.21 (12)
C2B—C3B—C4B119.84 (13)C17A—C13A—C14A98.19 (11)
O1C—C3C—C4C118.22 (13)C18B—C13B—C12B110.32 (12)
O1C—C3C—C2C122.26 (14)C18B—C13B—C14B113.36 (12)
C4C—C3C—C2C119.52 (14)C12B—C13B—C14B108.67 (12)
C3A—C4A—C5A121.01 (13)C18B—C13B—C17B109.99 (12)
C3A—C4A—H4A119.5C12B—C13B—C17B115.23 (12)
C5A—C4A—H4A119.5C14B—C13B—C17B98.92 (11)
C3B—C4B—C5B120.65 (14)C12C—C13C—C18C110.95 (13)
C3B—C4B—H4B119.7C12C—C13C—C17C115.14 (12)
C5B—C4B—H4B119.7C18C—C13C—C17C109.24 (12)
C3C—C4C—C5C121.33 (13)C12C—C13C—C14C108.95 (12)
C3C—C4C—H4C119.3C18C—C13C—C14C113.22 (12)
C5C—C4C—H4C119.3C17C—C13C—C14C98.90 (11)
C19A—O4A—H4OA109.7 (19)C8A—C14A—C15A120.45 (12)
C19B—O4B—H4OB106.5 (18)C8A—C14A—C13A112.89 (11)
C4A—C5A—C10A120.02 (13)C15A—C14A—C13A104.35 (12)
C4A—C5A—C6A118.25 (12)C8A—C14A—H14A106.1
C10A—C5A—C6A121.71 (12)C15A—C14A—H14A106.1
C4B—C5B—C10B120.24 (13)C13A—C14A—H14A106.1
C4B—C5B—C6B117.31 (13)C8B—C14B—C15B119.77 (13)
C10B—C5B—C6B122.43 (12)C8B—C14B—C13B112.57 (11)
C4C—C5C—C10C120.00 (13)C15B—C14B—C13B104.60 (12)
C4C—C5C—C6C118.22 (12)C8B—C14B—H14B106.4
C10C—C5C—C6C121.77 (13)C15B—C14B—H14B106.4
C5A—C6A—C7A113.37 (12)C13B—C14B—H14B106.4
C5A—C6A—H6A108.9C8C—C14C—C15C120.53 (12)
C7A—C6A—H6A108.9C8C—C14C—C13C112.18 (11)
C5A—C6A—H6B108.9C15C—C14C—C13C104.28 (11)
C7A—C6A—H6B108.9C8C—C14C—H14C106.3
H6A—C6A—H6B107.7C15C—C14C—H14C106.3
C5B—C6B—C7B113.29 (12)C13C—C14C—H14C106.3
C5B—C6B—H6C108.9C14A—C15A—C16A103.48 (13)
C7B—C6B—H6C108.9C14A—C15A—H15A111.1
C5B—C6B—H6D108.9C16A—C15A—H15A111.1
C7B—C6B—H6D108.9C14A—C15A—H15B111.1
H6C—C6B—H6D107.7C16A—C15A—H15B111.1
C5C—C6C—C7C113.26 (12)H15A—C15A—H15B109.0
C5C—C6C—H6E108.9C14B—C15B—C16B103.77 (13)
C7C—C6C—H6E108.9C14B—C15B—H15C111.0
C5C—C6C—H6F108.9C16B—C15B—H15C111.0
C7C—C6C—H6F108.9C14B—C15B—H15D111.0
H6E—C6C—H6F107.7C16B—C15B—H15D111.0
C6A—C7A—C8A110.06 (12)H15C—C15B—H15D109.0
C6A—C7A—H7A109.6C14C—C15C—C16C103.81 (12)
C8A—C7A—H7A109.6C14C—C15C—H15E111.0
C6A—C7A—H7B109.6C16C—C15C—H15E111.0
C8A—C7A—H7B109.6C14C—C15C—H15F111.0
H7A—C7A—H7B108.2C16C—C15C—H15F111.0
C6B—C7B—C8B109.97 (12)H15E—C15C—H15F109.0
C6B—C7B—H7C109.7C17A—C16A—C15A105.51 (12)
C8B—C7B—H7C109.7C17A—C16A—H16A110.6
C6B—C7B—H7D109.7C15A—C16A—H16A110.6
C8B—C7B—H7D109.7C17A—C16A—H16B110.6
H7C—C7B—H7D108.2C15A—C16A—H16B110.6
C6C—C7C—C8C109.81 (12)H16A—C16A—H16B108.8
C6C—C7C—H7E109.7C17B—C16B—C15B105.77 (12)
C8C—C7C—H7E109.7C17B—C16B—H16C110.6
C6C—C7C—H7F109.7C15B—C16B—H16C110.6
C8C—C7C—H7F109.7C17B—C16B—H16D110.6
H7E—C7C—H7F108.2C15B—C16B—H16D110.6
C14A—C8A—C7A112.96 (11)H16C—C16B—H16D108.7
C14A—C8A—C9A107.42 (11)C17C—C16C—C15C105.51 (13)
C7A—C8A—C9A110.06 (12)C17C—C16C—H16E110.6
C14A—C8A—H8A108.8C15C—C16C—H16E110.6
C7A—C8A—H8A108.8C17C—C16C—H16F110.6
C9A—C8A—H8A108.8C15C—C16C—H16F110.6
C14B—C8B—C7B113.42 (11)H16E—C16C—H16F108.8
C14B—C8B—C9B107.93 (11)O2A—C17A—C13A116.67 (13)
C7B—C8B—C9B109.19 (12)O2A—C17A—C16A114.53 (13)
C14B—C8B—H8B108.7C13A—C17A—C16A104.62 (12)
C7B—C8B—H8B108.7O2A—C17A—H17A106.8
C9B—C8B—H8B108.7C13A—C17A—H17A106.8
C14C—C8C—C7C113.63 (12)C16A—C17A—H17A106.8
C14C—C8C—C9C108.78 (11)O2B—C17B—C13B116.05 (13)
C7C—C8C—C9C109.14 (12)O2B—C17B—C16B113.90 (13)
C14C—C8C—H8C108.4C13B—C17B—C16B104.62 (12)
C7C—C8C—H8C108.4O2B—C17B—H17B107.3
C9C—C8C—H8C108.4C13B—C17B—H17B107.3
C10A—C9A—C8A112.45 (11)C16B—C17B—H17B107.3
C10A—C9A—C11A114.11 (12)O2C—C17C—C13C114.70 (13)
C8A—C9A—C11A111.08 (12)O2C—C17C—C16C110.85 (13)
C10A—C9A—H9A106.2C13C—C17C—C16C104.51 (12)
C8A—C9A—H9A106.2O2C—C17C—H17C108.9
C11A—C9A—H9A106.2C13C—C17C—H17C108.9
C10B—C9B—C11B113.62 (12)C16C—C17C—H17C108.9
C10B—C9B—C8B110.61 (11)C13A—C18A—H18C109.5
C11B—C9B—C8B111.71 (12)C13A—C18A—H18B109.5
C10B—C9B—H9B106.8H18C—C18A—H18B109.5
C11B—C9B—H9B106.8C13A—C18A—H18A109.5
C8B—C9B—H9B106.8H18C—C18A—H18A109.5
C10C—C9C—C8C111.59 (11)H18B—C18A—H18A109.5
C10C—C9C—C11C113.85 (12)C13B—C18B—H18F109.5
C8C—C9C—C11C111.03 (11)C13B—C18B—H18E109.5
C10C—C9C—H9C106.6H18F—C18B—H18E109.5
C8C—C9C—H9C106.6C13B—C18B—H18D109.5
C11C—C9C—H9C106.6H18F—C18B—H18D109.5
C1A—C10A—C5A117.64 (13)H18E—C18B—H18D109.5
C1A—C10A—C9A121.31 (12)C13C—C18C—H18I109.5
C5A—C10A—C9A120.87 (13)C13C—C18C—H18H109.5
C1B—C10B—C5B117.52 (13)H18I—C18C—H18H109.5
C1B—C10B—C9B121.37 (13)C13C—C18C—H18G109.5
C5B—C10B—C9B121.11 (13)H18I—C18C—H18G109.5
C1C—C10C—C5C117.28 (13)H18H—C18C—H18G109.5
C1C—C10C—C9C121.60 (12)O4A—C19A—H19A109.5
C5C—C10C—C9C121.08 (12)O4A—C19A—H19B109.5
C12A—C11A—C9A111.80 (14)H19A—C19A—H19B109.5
C12A—C11A—H11A109.3O4A—C19A—H19C109.5
C9A—C11A—H11A109.3H19A—C19A—H19C109.5
C12A—C11A—H11B109.3H19B—C19A—H19C109.5
C9A—C11A—H11B109.3O4B—C19B—H19G109.5
H11A—C11A—H11B107.9O4B—C19B—H19D109.5
C9B—C11B—C12B112.68 (12)H19G—C19B—H19D109.5
C9B—C11B—H11D109.1O4B—C19B—H19E109.5
C12B—C11B—H11D109.1H19G—C19B—H19E109.5
C9B—C11B—H11C109.1H19D—C19B—H19E109.5
C12B—C11B—H11C109.1
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1A—H1OA···O2Ai0.74 (3)1.89 (3)2.6226 (17)171 (3)
O1B—H1OB···O2Bi0.85 (3)1.83 (3)2.6654 (18)171 (3)
O1C—H1OC···O30.76 (3)1.82 (3)2.5767 (18)170 (3)
O2A—H2OA···O4B0.76 (3)1.97 (3)2.7017 (18)162 (2)
O2B—H2OB···O4Bii0.73 (2)2.06 (2)2.7823 (19)168 (2)
O2C—H2OC···O1Ciii0.73 (2)1.99 (3)2.7169 (17)175 (3)
O3—H3OA···O1Aiv0.72 (4)2.02 (4)2.743 (2)178 (4)
O3—H3OB···O1Bv0.76 (3)2.04 (3)2.7926 (19)173 (3)
O4A—H4OA···O2C0.83 (3)1.85 (3)2.6809 (18)174 (3)
O4B—H4OB···O4Avi0.78 (2)1.88 (2)2.6462 (17)166 (2)
Symmetry codes: (i) x+1, y, z+1; (ii) x3, y+1/2, z2; (iii) x1, y, z1; (iv) x, y+1/2, z; (v) x+1, y, z; (vi) x1, y, z.

Experimental details

Crystal data
Chemical formulaC18H24O2·0.67CH4O·0.33H2O
Mr299.74
Crystal system, space groupMonoclinic, P21
Temperature (K)298
a, b, c (Å)11.7152 (4), 19.6270 (6), 12.1310 (4)
β (°) 117.978 (1)
V3)2463.34 (14)
Z6
Radiation typeAg Kα, λ = 0.56085 Å
µ (mm1)0.05
Crystal size (mm)0.4 × 0.3 × 0.3
Data collection
DiffractometerSiemens SMART Platform CCD area-detector
diffractometer
Absorption correctionEmpirical (using intensity measurements)
multipole expansion (Blessing, 1995) using SADABS (Sheldrick, 1996)
Tmin, Tmax0.840, 0.985
No. of measured, independent and
observed [I > 2σ(I)] reflections
44195, 21122, 15597
Rint0.048
(sin θ/λ)max1)0.833
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.058, 0.145, 0.99
No. of reflections21122
No. of parameters698
No. of restraints1
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.41, 0.23

Computer programs: SMART (Bruker, 1998), SAINT (Bruker, 1999), SAINT, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), SHELXTL (Siemens, 1994), SHELXTL.

Selected bond lengths (Å) top
O1A—C3A1.3716 (18)C1A—C2A1.393 (2)
O1B—C3B1.3792 (17)C1A—C10A1.400 (2)
O1C—C3C1.3691 (18)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1A—H1OA···O2Ai0.74 (3)1.89 (3)2.6226 (17)171 (3)
O1B—H1OB···O2Bi0.85 (3)1.83 (3)2.6654 (18)171 (3)
O1C—H1OC···O30.76 (3)1.82 (3)2.5767 (18)170 (3)
O2A—H2OA···O4B0.76 (3)1.97 (3)2.7017 (18)162 (2)
O2B—H2OB···O4Bii0.73 (2)2.06 (2)2.7823 (19)168 (2)
O2C—H2OC···O1Ciii0.73 (2)1.99 (3)2.7169 (17)175 (3)
O3—H3OA···O1Aiv0.72 (4)2.02 (4)2.743 (2)178 (4)
O3—H3OB···O1Bv0.76 (3)2.04 (3)2.7926 (19)173 (3)
O4A—H4OA···O2C0.83 (3)1.85 (3)2.6809 (18)174 (3)
O4B—H4OB···O4Avi0.78 (2)1.88 (2)2.6462 (17)166 (2)
Symmetry codes: (i) x+1, y, z+1; (ii) x3, y+1/2, z2; (iii) x1, y, z1; (iv) x, y+1/2, z; (v) x+1, y, z; (vi) x1, y, z.
Comparison of ring bowing angles in reported E2 crystal structres (°) top
CompoundMolecule 1Molecule 2Molecule 3
angleangleangle
17β-estradiol-0.5H2Oa15.6--
17β-estradiol-propanol*12.9--
17β-estradiol-urea*5.6--
17β-estradiol-0.5MeOHb10.43.4-
(I)12.211.97.1
Notes: (a) Weize & Brooks (1994); (b) Parrish & Pinkerton (1999); * Query.
 

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