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Reaction of 4-meth­oxy­aceto­phenone with diethyl oxalate under basic conditions produced 3,4-dihy­droxy-1,6-bis­(4-meth­oxy­phenyl)hexa-2,4-diene-1,6-dione, C20H18O6, (1). The mol­ecules lie across a crystallographic inversion centre and intra­molecular hydrogen bonding, similar to acetyl­acetone, is observed, confirming that the mol­ecule is in the di-enol-dione tautomeric form. Additional O—H...O hydrogen bonds link the mol­ecules into chains parallel to the b axis. The structure is compared with that of redetermined 4-methyl­phenyl com­pound 3,4-dihy­droxy-1,6-bis­(4-methyl­phenyl)hexa-2,4-diene-1,6-dione, C20H18O4, (2), which crystallizes in a similar fashion. The salt, catena-poly[[μ2-2-hy­droxy-4-(4-meth­oxy­phenyl)-4-oxo­but-2-enoato-κ3O1,O2:O4][μ2-2-hy­droxy-4-(4-meth­oxy­phenyl)-4-oxobut-2-enoic acid-κ2O1:O4]potassium], [K(C11H9O5)(C11H10O5)]n, (3), was isolated as a by-product of the synthesis of (1). The two organic species are linked by a strong hydrogen bond between the carb­oxy­lic acid and carboxyl­ate groups. They are further stabilized and linked into a double-chain structure via the seven-coordinate potassium ion.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270113025973/mx3105sup1.cif
Contains datablocks compound1, compound2, compound3, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113025973/mx3105compound1sup2.hkl
Contains datablock compound1

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113025973/mx3105compound2sup3.hkl
Contains datablock compound2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270113025973/mx3105compound3sup4.hkl
Contains datablock compound3

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S0108270113025973/mx3105compound1sup5.cml
Supplementary material

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S0108270113025973/mx3105compound2sup6.cml
Supplementary material

CCDC references: 962293; 962294; 962295

Computing details top

For all compounds, data collection: SHELXTL (Sheldrick, 2008); cell refinement: SHELXTL (Sheldrick, 2008); data reduction: SHELXTL (Sheldrick, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008) and Mercury (Macrae et al., 2008). Software used to prepare material for publication: SHELXL97 (Sheldrick, 2008), enCIFer (Allen et al., 2004) and publCIF (Westrip 2010) for compound1, compound3; SHELXL97 (Sheldrick, 2008), enCIFer (Allen et al., 2004) and publCIF (Westrip, 2010) for compound2.

(compound1) 3,4-Dihydroxy-1,6-bis(4-methoxyphenyl)hexa-2,4-diene-1,6-dione top
Crystal data top
C20H18O6F(000) = 372
Mr = 354.34Dx = 1.471 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 6419 reflections
a = 15.4385 (6) Åθ = 2.7–30.4°
b = 6.1475 (2) ŵ = 0.11 mm1
c = 8.7281 (3) ÅT = 116 K
β = 105.029 (2)°Plate, yellow
V = 800.03 (5) Å30.55 × 0.33 × 0.12 mm
Z = 2
Data collection top
Bruker APEXII CCD area-detector
diffractometer
2313 independent reflections
Radiation source: fine-focus sealed tube2155 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.029
φ and ω scansθmax = 30.0°, θmin = 2.7°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 2021
Tmin = 0.943, Tmax = 0.987k = 88
16170 measured reflectionsl = 1212
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043Hydrogen site location: difference Fourier map
wR(F2) = 0.113H atoms treated by a mixture of independent and constrained refinement
S = 1.12 w = 1/[σ2(Fo2) + (0.0523P)2 + 0.2726P]
where P = (Fo2 + 2Fc2)/3
2313 reflections(Δ/σ)max < 0.001
122 parametersΔρmax = 0.36 e Å3
0 restraintsΔρmin = 0.32 e Å3
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
O10.00663 (6)0.71487 (12)0.97532 (10)0.02027 (19)
H10.0476 (10)0.642 (2)0.8907 (18)0.024*
O20.12517 (5)0.63048 (12)0.72353 (9)0.01960 (18)
O30.41635 (6)1.05028 (14)0.16040 (10)0.0264 (2)
C10.02613 (7)0.92265 (16)0.94117 (12)0.0153 (2)
C20.08909 (7)0.98991 (17)0.80906 (12)0.0168 (2)
H20.10001.14070.78940.020*
C30.13895 (7)0.83071 (17)0.69928 (12)0.0162 (2)
C40.20934 (7)0.90088 (17)0.55747 (12)0.0166 (2)
C50.27195 (8)0.74536 (17)0.48004 (13)0.0195 (2)
H50.26770.60030.51880.023*
C60.33969 (8)0.80018 (18)0.34814 (13)0.0221 (2)
H60.38200.69360.29740.026*
C70.34583 (8)1.01304 (18)0.28942 (13)0.0196 (2)
C80.28320 (7)1.16862 (17)0.36206 (12)0.0192 (2)
H80.28631.31200.32050.023*
C90.21571 (7)1.11223 (17)0.49676 (12)0.0182 (2)
H90.17361.21910.54780.022*
C100.43629 (8)1.27080 (19)0.11246 (15)0.0256 (3)
H10A0.45051.35240.19930.031*
H10B0.48791.27470.01920.031*
H10C0.38421.33660.08590.031*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0253 (4)0.0111 (3)0.0207 (4)0.0012 (3)0.0008 (3)0.0001 (3)
O20.0235 (4)0.0139 (3)0.0202 (4)0.0000 (3)0.0037 (3)0.0001 (3)
O30.0272 (5)0.0211 (4)0.0235 (4)0.0017 (3)0.0069 (3)0.0026 (3)
C10.0176 (5)0.0125 (4)0.0156 (4)0.0001 (3)0.0038 (4)0.0000 (4)
C20.0197 (5)0.0137 (4)0.0158 (4)0.0002 (3)0.0022 (4)0.0003 (4)
C30.0175 (5)0.0160 (4)0.0155 (4)0.0001 (3)0.0047 (3)0.0004 (4)
C40.0174 (5)0.0168 (4)0.0149 (4)0.0005 (4)0.0029 (4)0.0016 (4)
C50.0223 (5)0.0149 (4)0.0198 (5)0.0011 (4)0.0026 (4)0.0011 (4)
C60.0231 (6)0.0178 (5)0.0218 (5)0.0025 (4)0.0003 (4)0.0048 (4)
C70.0200 (5)0.0202 (5)0.0165 (5)0.0013 (4)0.0011 (4)0.0030 (4)
C80.0211 (5)0.0171 (5)0.0181 (5)0.0008 (4)0.0025 (4)0.0004 (4)
C90.0186 (5)0.0172 (5)0.0177 (5)0.0024 (4)0.0024 (4)0.0007 (4)
C100.0250 (6)0.0243 (5)0.0240 (5)0.0025 (4)0.0002 (4)0.0032 (4)
Geometric parameters (Å, º) top
O1—C11.3284 (12)C5—C61.3813 (15)
O1—H10.951 (15)C5—H50.9500
O2—C31.2577 (12)C6—C71.3996 (15)
O3—C71.3675 (13)C6—H60.9500
O3—C101.4285 (14)C7—C81.3906 (15)
C1—C21.3653 (14)C8—C91.3974 (14)
C1—C1i1.476 (2)C8—H80.9500
C2—C31.4443 (14)C9—H90.9500
C2—H20.9500C10—H10A0.9800
C3—C41.4837 (14)C10—H10B0.9800
C4—C91.3970 (15)C10—H10C0.9800
C4—C51.4023 (14)
C1—O1—H1102.2 (9)C5—C6—H6120.1
C7—O3—C10117.72 (9)C7—C6—H6120.1
O1—C1—C2123.44 (9)O3—C7—C8124.84 (10)
O1—C1—C1i114.34 (11)O3—C7—C6114.96 (10)
C2—C1—C1i122.23 (11)C8—C7—C6120.20 (10)
C1—C2—C3119.69 (9)C7—C8—C9119.44 (10)
C1—C2—H2120.2C7—C8—H8120.3
C3—C2—H2120.2C9—C8—H8120.3
O2—C3—C2120.91 (9)C4—C9—C8120.91 (10)
O2—C3—C4118.70 (9)C4—C9—H9119.5
C2—C3—C4120.37 (9)C8—C9—H9119.5
C9—C4—C5118.65 (10)O3—C10—H10A109.5
C9—C4—C3123.44 (9)O3—C10—H10B109.5
C5—C4—C3117.91 (9)H10A—C10—H10B109.5
C6—C5—C4120.90 (10)O3—C10—H10C109.5
C6—C5—H5119.5H10A—C10—H10C109.5
C4—C5—H5119.5H10B—C10—H10C109.5
C5—C6—C7119.87 (10)
O1—C1—C2—C30.73 (16)C4—C5—C6—C70.61 (18)
C1i—C1—C2—C3179.17 (12)C10—O3—C7—C810.96 (17)
C1—C2—C3—O20.05 (16)C10—O3—C7—C6168.78 (10)
C1—C2—C3—C4178.32 (10)C5—C6—C7—O3178.81 (10)
O2—C3—C4—C9163.46 (10)C5—C6—C7—C80.94 (18)
C2—C3—C4—C918.13 (16)O3—C7—C8—C9177.88 (10)
O2—C3—C4—C515.87 (15)C6—C7—C8—C91.84 (17)
C2—C3—C4—C5162.54 (10)C5—C4—C9—C80.27 (16)
C9—C4—C5—C61.20 (17)C3—C4—C9—C8179.59 (10)
C3—C4—C5—C6179.44 (10)C7—C8—C9—C41.24 (16)
Symmetry code: (i) x, y+2, z+2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O20.951 (15)1.631 (15)2.5224 (11)154.4 (14)
O1—H1···O1ii0.951 (15)2.526 (15)2.6760 (15)88.5 (9)
Symmetry code: (ii) x, y+1, z+2.
(compound2) 3,4-Dihydroxy-1,6-bis(4-methylphenyl)hexa-2,4-diene-1,6-dione top
Crystal data top
C20H18O4F(000) = 340
Mr = 322.34Dx = 1.365 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 5544 reflections
a = 14.7710 (6) Åθ = 2.8–30.7°
b = 6.1622 (2) ŵ = 0.10 mm1
c = 8.6184 (3) ÅT = 116 K
β = 91.896 (2)°Plate, yellow
V = 784.03 (5) Å30.62 × 0.46 × 0.06 mm
Z = 2
Data collection top
Bruker APEXII CCD area-detector
diffractometer
2288 independent reflections
Radiation source: fine-focus sealed tube2150 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.045
φ and ω scansθmax = 30.0°, θmin = 2.8°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 2020
Tmin = 0.944, Tmax = 0.994k = 88
19282 measured reflectionsl = 1212
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)] = 0.067Hydrogen site location: difference Fourier map
wR(F2) = 0.151H atoms treated by a mixture of independent and constrained refinement
S = 1.25 w = 1/[σ2(Fo2) + (0.0474P)2 + 0.5796P]
where P = (Fo2 + 2Fc2)/3
2288 reflections(Δ/σ)max < 0.001
116 parametersΔρmax = 0.41 e Å3
0 restraintsΔρmin = 0.32 e Å3
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
O10.00746 (9)0.28418 (18)0.52331 (14)0.0208 (3)
H10.0479 (15)0.356 (4)0.589 (3)0.025*
O20.12923 (8)0.36429 (19)0.72956 (13)0.0203 (3)
C10.02699 (11)0.0771 (2)0.54860 (17)0.0159 (3)
C20.09117 (11)0.0077 (2)0.65506 (18)0.0175 (3)
H20.0990 (14)0.144 (3)0.670 (2)0.021*
C30.14247 (11)0.1644 (3)0.74647 (17)0.0169 (3)
C40.21345 (11)0.0898 (3)0.86024 (17)0.0174 (3)
C50.27745 (12)0.2403 (3)0.91639 (19)0.0213 (3)
H50.27460.38610.88070.026*
C60.34485 (12)0.1800 (3)1.0230 (2)0.0240 (4)
H60.38800.28431.05890.029*
C70.34998 (11)0.0329 (3)1.07841 (19)0.0217 (3)
C80.28543 (12)0.1814 (3)1.02491 (19)0.0216 (3)
H80.28710.32571.06380.026*
C90.21839 (12)0.1234 (3)0.91558 (19)0.0199 (3)
H90.17590.22860.87850.024*
C100.42402 (13)0.1005 (3)1.1934 (2)0.0306 (4)
H10A0.48080.11911.13940.037*
H10B0.40740.23791.24220.037*
H10C0.43190.01171.27340.037*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0289 (6)0.0104 (5)0.0227 (6)0.0004 (4)0.0055 (5)0.0011 (4)
O20.0276 (6)0.0138 (5)0.0196 (5)0.0009 (4)0.0003 (5)0.0004 (4)
C10.0207 (7)0.0126 (6)0.0146 (6)0.0004 (5)0.0020 (5)0.0007 (5)
C20.0235 (8)0.0138 (7)0.0152 (7)0.0006 (6)0.0007 (6)0.0001 (5)
C30.0204 (7)0.0168 (7)0.0137 (6)0.0005 (6)0.0028 (5)0.0003 (5)
C40.0212 (7)0.0177 (7)0.0133 (6)0.0005 (6)0.0019 (5)0.0016 (5)
C50.0263 (8)0.0172 (7)0.0204 (7)0.0032 (6)0.0002 (6)0.0008 (6)
C60.0239 (8)0.0245 (8)0.0235 (8)0.0051 (6)0.0022 (6)0.0029 (6)
C70.0207 (8)0.0258 (8)0.0186 (7)0.0012 (6)0.0001 (6)0.0024 (6)
C80.0261 (8)0.0178 (7)0.0206 (7)0.0008 (6)0.0012 (6)0.0001 (6)
C90.0246 (8)0.0171 (7)0.0180 (7)0.0023 (6)0.0010 (6)0.0003 (6)
C100.0250 (9)0.0353 (10)0.0310 (9)0.0028 (7)0.0057 (7)0.0024 (8)
Geometric parameters (Å, º) top
O1—C11.3248 (18)C5—H50.9500
O1—H10.92 (2)C6—C71.397 (2)
O2—C31.2552 (19)C6—H60.9500
C1—C21.366 (2)C7—C81.390 (2)
C1—C1i1.482 (3)C7—C101.510 (2)
C2—C31.445 (2)C8—C91.391 (2)
C2—H20.95 (2)C8—H80.9500
C3—C41.485 (2)C9—H90.9500
C4—C91.399 (2)C10—H10A0.9800
C4—C51.399 (2)C10—H10B0.9800
C5—C61.383 (2)C10—H10C0.9800
C1—O1—H1103.3 (14)C5—C6—H6119.7
O1—C1—C2123.67 (14)C7—C6—H6119.7
O1—C1—C1i114.48 (17)C8—C7—C6118.44 (16)
C2—C1—C1i121.85 (17)C8—C7—C10120.67 (16)
C1—C2—C3119.81 (14)C6—C7—C10120.88 (16)
C1—C2—H2118.6 (13)C7—C8—C9121.39 (16)
C3—C2—H2121.5 (13)C7—C8—H8119.3
O2—C3—C2121.04 (15)C9—C8—H8119.3
O2—C3—C4118.97 (14)C8—C9—C4120.02 (15)
C2—C3—C4119.98 (14)C8—C9—H9120.0
C9—C4—C5118.53 (15)C4—C9—H9120.0
C9—C4—C3122.93 (14)C7—C10—H10A109.5
C5—C4—C3118.53 (14)C7—C10—H10B109.5
C6—C5—C4121.01 (16)H10A—C10—H10B109.5
C6—C5—H5119.5C7—C10—H10C109.5
C4—C5—H5119.5H10A—C10—H10C109.5
C5—C6—C7120.59 (16)H10B—C10—H10C109.5
O1—C1—C2—C30.5 (2)C3—C4—C5—C6179.73 (15)
C1i—C1—C2—C3179.62 (17)C4—C5—C6—C70.7 (3)
C1—C2—C3—O20.2 (2)C5—C6—C7—C80.5 (3)
C1—C2—C3—C4178.88 (14)C5—C6—C7—C10179.30 (17)
O2—C3—C4—C9163.58 (15)C6—C7—C8—C91.7 (3)
C2—C3—C4—C917.7 (2)C10—C7—C8—C9178.10 (16)
O2—C3—C4—C515.4 (2)C7—C8—C9—C41.7 (3)
C2—C3—C4—C5163.33 (15)C5—C4—C9—C80.5 (2)
C9—C4—C5—C60.7 (2)C3—C4—C9—C8178.51 (15)
Symmetry code: (i) x, y, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O20.92 (2)1.68 (2)2.5351 (17)153 (2)
O1—H1···O1ii0.92 (2)2.54 (2)2.698 (2)89.7 (14)
Symmetry code: (ii) x, y+1, z+1.
(compound3) catena-poly[[µ2-2-hydroxy-4-(4-methoxyphenyl)-4-oxobut-2-enoato-κ2O1,O2][µ2-2-hydroxy-4-(4-methoxyphenyl)-4-oxobut-2-enoic acid-κO1]potassium] top
Crystal data top
[K(C11H9O5)(C11H10O5)]F(000) = 1000
Mr = 482.47Dx = 1.551 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 9844 reflections
a = 15.3832 (4) Åθ = 2.7–33.6°
b = 6.3481 (1) ŵ = 0.32 mm1
c = 21.1606 (5) ÅT = 116 K
β = 90.582 (1)°Block, orange
V = 2066.31 (8) Å30.57 × 0.55 × 0.39 mm
Z = 4
Data collection top
Bruker APEXII CCD area-detector
diffractometer
6026 independent reflections
Radiation source: fine-focus sealed tube5402 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.034
φ and ω scansθmax = 30.0°, θmin = 2.7°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 2121
Tmin = 0.840, Tmax = 0.886k = 88
52473 measured reflectionsl = 2929
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.032H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.090 w = 1/[σ2(Fo2) + (0.0465P)2 + 0.7703P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max = 0.001
6026 reflectionsΔρmax = 0.47 e Å3
316 parametersΔρmin = 0.42 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0018 (3)
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
K10.094861 (16)0.35025 (4)0.081718 (11)0.02174 (7)
O10.10832 (5)0.25622 (12)0.12862 (4)0.02025 (16)
H10.0616 (10)0.146 (2)0.1106 (7)0.024*
O20.19157 (5)0.02958 (12)0.14601 (4)0.01979 (16)
O30.23039 (5)0.51295 (12)0.16089 (4)0.02209 (17)
H20.2761 (10)0.580 (3)0.1754 (7)0.027*
O40.37824 (5)0.58187 (12)0.21043 (4)0.02280 (17)
O80.71085 (5)0.13407 (13)0.32273 (5)0.02622 (18)
C10.17878 (7)0.15990 (15)0.14749 (5)0.01563 (18)
C20.24789 (7)0.31033 (16)0.17157 (5)0.01602 (18)
C30.32152 (7)0.23950 (16)0.20031 (5)0.01704 (19)
H30.3295 (9)0.094 (2)0.2060 (7)0.020*
C40.38838 (7)0.38792 (16)0.21960 (5)0.01727 (19)
C50.47061 (7)0.31106 (16)0.24838 (5)0.01718 (19)
C60.54056 (7)0.45201 (17)0.25357 (6)0.0221 (2)
H60.53350.59350.23990.027*
C70.61938 (7)0.38761 (18)0.27830 (6)0.0244 (2)
H70.66660.48390.28060.029*
C80.63018 (7)0.18150 (17)0.29998 (5)0.0195 (2)
C90.56060 (7)0.04037 (17)0.29702 (5)0.0196 (2)
H90.56690.09870.31300.024*
C100.48194 (7)0.10559 (17)0.27046 (5)0.0186 (2)
H100.43510.00850.26730.022*
C110.72737 (8)0.07866 (19)0.34241 (6)0.0270 (2)
H11A0.71980.17360.30630.032*
H11B0.78700.08990.35870.032*
H11C0.68650.11770.37570.032*
O210.00426 (5)0.00255 (12)0.08664 (4)0.02243 (17)
O220.08478 (5)0.24898 (12)0.04660 (4)0.02125 (16)
O230.09110 (5)0.30340 (12)0.04625 (4)0.01976 (16)
H220.1306 (10)0.386 (2)0.0348 (7)0.024*
O240.23541 (5)0.43226 (12)0.00102 (4)0.02236 (17)
O280.59212 (5)0.11734 (14)0.11483 (5)0.02695 (19)
C210.06453 (6)0.06570 (15)0.05847 (5)0.01456 (18)
C220.12488 (7)0.11186 (15)0.03830 (5)0.01493 (18)
C230.20529 (7)0.07281 (16)0.01429 (5)0.01698 (19)
H230.2255 (9)0.066 (2)0.0116 (7)0.020*
C240.26057 (7)0.24507 (16)0.00662 (5)0.01689 (19)
C250.34704 (6)0.20051 (16)0.03497 (5)0.01650 (19)
C260.40475 (7)0.36872 (16)0.04486 (5)0.0202 (2)
H260.38790.50720.03300.024*
C270.48552 (7)0.33529 (18)0.07160 (6)0.0228 (2)
H270.52420.45030.07760.027*
C280.51075 (7)0.13258 (17)0.09002 (5)0.0196 (2)
C290.45353 (7)0.03595 (17)0.08203 (6)0.0212 (2)
H290.46970.17340.09540.025*
C300.37267 (7)0.00053 (17)0.05422 (5)0.0201 (2)
H300.33400.11560.04820.024*
C310.62155 (8)0.0852 (2)0.13503 (6)0.0278 (2)
H31A0.58380.13730.16860.033*
H31B0.68130.07410.15110.033*
H31C0.61970.18310.09920.033*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
K10.02692 (13)0.01534 (11)0.02285 (12)0.00585 (8)0.00509 (9)0.00186 (8)
O10.0181 (4)0.0139 (3)0.0286 (4)0.0009 (3)0.0086 (3)0.0010 (3)
O20.0204 (4)0.0137 (3)0.0252 (4)0.0008 (3)0.0055 (3)0.0001 (3)
O30.0232 (4)0.0131 (3)0.0298 (4)0.0011 (3)0.0099 (3)0.0011 (3)
O40.0246 (4)0.0166 (3)0.0271 (4)0.0022 (3)0.0061 (3)0.0004 (3)
O80.0151 (4)0.0239 (4)0.0396 (5)0.0013 (3)0.0071 (3)0.0008 (3)
C10.0165 (4)0.0151 (4)0.0153 (4)0.0005 (3)0.0020 (3)0.0002 (3)
C20.0185 (5)0.0139 (4)0.0157 (4)0.0004 (3)0.0020 (4)0.0010 (3)
C30.0180 (5)0.0155 (4)0.0175 (5)0.0013 (3)0.0029 (4)0.0002 (3)
C40.0182 (5)0.0186 (4)0.0150 (4)0.0012 (4)0.0014 (4)0.0002 (3)
C50.0163 (4)0.0184 (4)0.0169 (5)0.0026 (4)0.0015 (4)0.0008 (3)
C60.0208 (5)0.0172 (5)0.0284 (6)0.0042 (4)0.0036 (4)0.0002 (4)
C70.0183 (5)0.0208 (5)0.0339 (6)0.0063 (4)0.0035 (4)0.0017 (4)
C80.0144 (4)0.0220 (5)0.0220 (5)0.0020 (4)0.0019 (4)0.0037 (4)
C90.0172 (5)0.0187 (5)0.0229 (5)0.0025 (4)0.0031 (4)0.0012 (4)
C100.0164 (5)0.0193 (5)0.0202 (5)0.0048 (4)0.0022 (4)0.0012 (4)
C110.0197 (5)0.0265 (6)0.0348 (6)0.0025 (4)0.0026 (5)0.0007 (5)
O210.0185 (4)0.0140 (3)0.0346 (4)0.0009 (3)0.0112 (3)0.0001 (3)
O220.0229 (4)0.0131 (3)0.0277 (4)0.0023 (3)0.0056 (3)0.0009 (3)
O230.0196 (4)0.0115 (3)0.0280 (4)0.0002 (3)0.0056 (3)0.0003 (3)
O240.0213 (4)0.0159 (3)0.0297 (4)0.0002 (3)0.0068 (3)0.0005 (3)
O280.0174 (4)0.0265 (4)0.0368 (5)0.0006 (3)0.0097 (3)0.0003 (3)
C210.0144 (4)0.0134 (4)0.0159 (4)0.0001 (3)0.0008 (3)0.0008 (3)
C220.0163 (4)0.0131 (4)0.0153 (4)0.0000 (3)0.0002 (3)0.0000 (3)
C230.0160 (4)0.0144 (4)0.0204 (5)0.0003 (3)0.0024 (4)0.0012 (3)
C240.0162 (4)0.0176 (4)0.0168 (4)0.0006 (3)0.0015 (3)0.0004 (3)
C250.0149 (4)0.0177 (4)0.0169 (5)0.0008 (3)0.0016 (3)0.0007 (3)
C260.0194 (5)0.0162 (4)0.0249 (5)0.0017 (4)0.0033 (4)0.0016 (4)
C270.0185 (5)0.0197 (5)0.0300 (6)0.0043 (4)0.0051 (4)0.0008 (4)
C280.0156 (5)0.0227 (5)0.0206 (5)0.0005 (4)0.0023 (4)0.0014 (4)
C290.0189 (5)0.0178 (5)0.0268 (5)0.0014 (4)0.0037 (4)0.0001 (4)
C300.0173 (5)0.0173 (5)0.0256 (5)0.0011 (4)0.0032 (4)0.0012 (4)
C310.0230 (5)0.0320 (6)0.0284 (6)0.0072 (5)0.0056 (4)0.0017 (5)
Geometric parameters (Å, º) top
K1—O212.6404 (8)C10—K1vi3.3665 (11)
K1—O1i2.6953 (8)C10—H100.9500
K1—O22ii2.7931 (9)C11—H11A0.9800
K1—O3i2.7994 (8)C11—H11B0.9800
K1—O22.8578 (8)C11—H11C0.9800
K1—O232.9651 (8)O21—C211.2740 (12)
K1—O24iii3.0939 (9)O21—H11.361 (15)
K1—C10iv3.3665 (11)O22—C211.2297 (12)
K1—C21ii3.5003 (10)O22—K1ii2.7931 (9)
K1—K1iii4.8876 (5)O23—C221.3323 (12)
O1—C11.3037 (12)O23—H220.836 (16)
O1—K1v2.6953 (8)O24—C241.2549 (13)
O1—H11.071 (15)O24—K1iii3.0939 (9)
O2—C11.2193 (12)O28—C281.3559 (13)
O3—C21.3329 (12)O28—C311.4270 (15)
O3—K1v2.7994 (8)C21—C221.5188 (14)
O3—H20.875 (16)C21—K1ii3.5003 (10)
O4—C41.2559 (13)C22—C231.3554 (14)
O8—C81.3603 (13)C23—C241.4516 (14)
O8—C111.4351 (15)C23—H230.938 (15)
C1—C21.5135 (14)C24—C251.4810 (14)
C2—C31.3569 (14)C25—C301.3952 (14)
C3—C41.4503 (14)C25—C261.4029 (14)
C3—H30.939 (15)C26—C271.3765 (15)
C4—C51.4810 (14)C26—H260.9500
C5—C101.3959 (14)C27—C281.3984 (15)
C5—C61.4030 (14)C27—H270.9500
C6—C71.3778 (16)C28—C291.3946 (15)
C6—H60.9500C29—C301.3890 (14)
C7—C81.3959 (16)C29—H290.9500
C7—H70.9500C30—H300.9500
C8—C91.3967 (14)C31—H31A0.9800
C9—C101.3919 (14)C31—H31B0.9800
C9—H90.9500C31—H31C0.9800
O21—K1—O1i144.12 (3)C5—C6—H6119.6
O21—K1—O22ii79.57 (3)C6—C7—C8120.28 (10)
O1i—K1—O22ii125.07 (2)C6—C7—H7119.9
O21—K1—O3i129.03 (3)C8—C7—H7119.9
O1i—K1—O3i55.82 (2)O8—C8—C7115.39 (9)
O22ii—K1—O3i133.38 (3)O8—C8—C9124.74 (10)
O21—K1—O269.48 (2)C7—C8—C9119.86 (10)
O1i—K1—O2116.57 (2)C10—C9—C8119.34 (10)
O22ii—K1—O2108.81 (2)C10—C9—H9120.3
O3i—K1—O263.58 (2)C8—C9—H9120.3
O21—K1—O2354.31 (2)C9—C10—C5121.21 (9)
O1i—K1—O23104.86 (2)C9—C10—K1vi87.79 (7)
O22ii—K1—O2371.76 (2)C5—C10—K1vi100.92 (7)
O3i—K1—O23153.30 (3)C9—C10—H10119.4
O2—K1—O23123.05 (2)C5—C10—H10119.4
O21—K1—O24iii140.57 (3)K1vi—C10—H1081.2
O1i—K1—O24iii74.82 (2)O8—C11—H11A109.5
O22ii—K1—O24iii66.32 (2)O8—C11—H11B109.5
O3i—K1—O24iii70.82 (2)H11A—C11—H11B109.5
O2—K1—O24iii102.55 (2)O8—C11—H11C109.5
O23—K1—O24iii125.66 (2)H11A—C11—H11C109.5
O21—K1—C10iv81.00 (3)H11B—C11—H11C109.5
O1i—K1—C10iv66.86 (3)C21—O21—K1133.21 (7)
O22ii—K1—C10iv154.94 (3)C21—O21—H1119.7 (6)
O3i—K1—C10iv71.60 (3)K1—O21—H1104.0 (6)
O2—K1—C10iv78.63 (3)C21—O22—K1ii115.33 (7)
O23—K1—C10iv84.07 (2)C22—O23—K1119.84 (6)
O24iii—K1—C10iv136.84 (2)C22—O23—H22104.7 (10)
O21—K1—C21ii61.96 (3)K1—O23—H22135.0 (10)
O1i—K1—C21ii143.08 (2)C24—O24—K1iii125.95 (7)
O22ii—K1—C21ii18.52 (2)C28—O28—C31117.98 (9)
O3i—K1—C21ii139.40 (3)O22—C21—O21126.93 (9)
O2—K1—C21ii95.75 (2)O22—C21—C22119.46 (9)
O23—K1—C21ii67.28 (2)O21—C21—C22113.60 (8)
O24iii—K1—C21ii81.40 (2)O22—C21—K1ii46.16 (5)
C10iv—K1—C21ii141.75 (2)O21—C21—K1ii131.45 (7)
O21—K1—K1iii92.650 (18)C22—C21—K1ii93.95 (6)
O1i—K1—K1iii86.737 (17)O23—C22—C23124.58 (9)
O22ii—K1—K1iii51.303 (17)O23—C22—C21113.91 (9)
O3i—K1—K1iii137.606 (18)C23—C22—C21121.50 (9)
O2—K1—K1iii156.663 (18)C22—C23—C24120.40 (9)
O23—K1—K1iii44.949 (16)C22—C23—H23119.7 (9)
O24iii—K1—K1iii81.459 (16)C24—C23—H23119.9 (9)
C10iv—K1—K1iii114.35 (2)O24—C24—C23120.36 (9)
C21ii—K1—K1iii61.807 (17)O24—C24—C25119.60 (9)
C1—O1—K1v127.44 (6)C23—C24—C25120.04 (9)
C1—O1—H1110.8 (8)C30—C25—C26118.44 (9)
K1v—O1—H1115.2 (8)C30—C25—C24122.89 (9)
C1—O2—K1129.17 (7)C26—C25—C24118.64 (9)
C2—O3—K1v123.28 (6)C27—C26—C25120.74 (10)
C2—O3—H2104.5 (10)C27—C26—H26119.6
K1v—O3—H2130.5 (10)C25—C26—H26119.6
C8—O8—C11117.98 (9)C26—C27—C28120.22 (10)
O2—C1—O1126.06 (10)C26—C27—H27119.9
O2—C1—C2121.21 (9)C28—C27—H27119.9
O1—C1—C2112.72 (8)O28—C28—C29124.84 (10)
O3—C2—C3124.19 (9)O28—C28—C27115.22 (10)
O3—C2—C1114.32 (9)C29—C28—C27119.94 (10)
C3—C2—C1121.47 (9)C30—C29—C28119.25 (10)
C2—C3—C4119.81 (9)C30—C29—H29120.4
C2—C3—H3119.4 (9)C28—C29—H29120.4
C4—C3—H3120.7 (9)C29—C30—C25121.39 (10)
O4—C4—C3120.45 (10)C29—C30—H30119.3
O4—C4—C5119.39 (9)C25—C30—H30119.3
C3—C4—C5120.13 (9)O28—C31—H31A109.5
C10—C5—C6118.46 (10)O28—C31—H31B109.5
C10—C5—C4123.28 (9)H31A—C31—H31B109.5
C6—C5—C4118.25 (10)O28—C31—H31C109.5
C7—C6—C5120.79 (10)H31A—C31—H31C109.5
C7—C6—H6119.6H31B—C31—H31C109.5
O21—K1—O2—C114.89 (9)C10iv—K1—O21—C21112.06 (10)
O1i—K1—O2—C1156.16 (9)C21ii—K1—O21—C2158.09 (10)
O22ii—K1—O2—C155.74 (10)K1iii—K1—O21—C212.18 (10)
O3i—K1—O2—C1174.39 (10)O21—K1—O23—C2213.80 (7)
O23—K1—O2—C124.30 (10)O1i—K1—O23—C22161.10 (7)
O24iii—K1—O2—C1124.71 (9)O22ii—K1—O23—C2276.32 (7)
C10iv—K1—O2—C199.44 (9)O3i—K1—O23—C22121.11 (8)
C21ii—K1—O2—C142.27 (9)O2—K1—O23—C2224.66 (8)
K1iii—K1—O2—C127.13 (12)O24iii—K1—O23—C22117.13 (7)
K1—O2—C1—O112.97 (16)C10iv—K1—O23—C2296.97 (7)
K1—O2—C1—C2165.83 (7)C21ii—K1—O23—C2257.12 (7)
K1v—O1—C1—O2150.54 (9)K1iii—K1—O23—C22129.34 (8)
K1v—O1—C1—C228.34 (12)K1ii—O22—C21—O21115.23 (10)
K1v—O3—C2—C3167.82 (8)K1ii—O22—C21—C2264.36 (11)
K1v—O3—C2—C110.92 (12)K1—O21—C21—O22152.29 (8)
O2—C1—C2—O3169.60 (10)K1—O21—C21—C2227.32 (14)
O1—C1—C2—O39.35 (13)K1—O21—C21—K1ii91.77 (10)
O2—C1—C2—C39.18 (16)K1—O23—C22—C23170.99 (8)
O1—C1—C2—C3171.88 (10)K1—O23—C22—C218.72 (11)
O3—C2—C3—C42.06 (16)O22—C21—C22—O23171.70 (9)
C1—C2—C3—C4176.58 (9)O21—C21—C22—O237.94 (13)
C2—C3—C4—O40.69 (16)K1ii—C21—C22—O23131.02 (8)
C2—C3—C4—C5177.25 (10)O22—C21—C22—C238.02 (15)
O4—C4—C5—C10168.35 (10)O21—C21—C22—C23172.34 (10)
C3—C4—C5—C1013.69 (16)K1ii—C21—C22—C2348.70 (10)
O4—C4—C5—C611.75 (15)O23—C22—C23—C241.78 (16)
C3—C4—C5—C6166.21 (10)C21—C22—C23—C24177.91 (9)
C10—C5—C6—C71.75 (17)K1iii—O24—C24—C2373.12 (12)
C4—C5—C6—C7178.16 (11)K1iii—O24—C24—C25106.63 (10)
C5—C6—C7—C81.48 (19)C22—C23—C24—O242.02 (16)
C11—O8—C8—C7176.55 (11)C22—C23—C24—C25177.73 (10)
C11—O8—C8—C93.15 (17)O24—C24—C25—C30166.98 (10)
C6—C7—C8—O8179.24 (11)C23—C24—C25—C3012.77 (16)
C6—C7—C8—C90.48 (18)O24—C24—C25—C2610.87 (15)
O8—C8—C9—C10177.59 (10)C23—C24—C25—C26169.37 (10)
C7—C8—C9—C102.10 (17)C30—C25—C26—C271.46 (17)
C8—C9—C10—C51.82 (17)C24—C25—C26—C27179.41 (10)
C8—C9—C10—K1vi103.26 (10)C25—C26—C27—C280.77 (18)
C6—C5—C10—C90.09 (16)C31—O28—C28—C290.75 (17)
C4—C5—C10—C9179.81 (10)C31—O28—C28—C27179.51 (10)
C6—C5—C10—K1vi93.99 (10)C26—C27—C28—O28178.95 (11)
C4—C5—C10—K1vi86.11 (10)C26—C27—C28—C290.81 (18)
O1i—K1—O21—C2185.91 (11)O28—C28—C29—C30178.08 (11)
O22ii—K1—O21—C2152.02 (10)C27—C28—C29—C301.65 (17)
O3i—K1—O21—C21169.40 (9)C28—C29—C30—C250.94 (17)
O2—K1—O21—C21166.79 (10)C26—C25—C30—C290.60 (17)
O23—K1—O21—C2122.92 (9)C24—C25—C30—C29178.45 (10)
O24iii—K1—O21—C2181.94 (10)
Symmetry codes: (i) x, y+1, z; (ii) x, y, z; (iii) x, y+1, z; (iv) x+1/2, y+1/2, z+1/2; (v) x, y1, z; (vi) x+1/2, y1/2, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O211.071 (15)1.361 (15)2.4322 (10)178.2 (15)
O3—H2···O40.875 (16)1.731 (16)2.5326 (11)151.1 (15)
O23—H22···O240.836 (16)1.800 (16)2.5599 (11)150.4 (15)
 

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