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Taxifolin, also known as di­hydro­quercetin, is the major flavonoid in larch wood. It is well known as an antioxidant and a bioactive substance. Taxifolin as an active pharmaceutical ingredient is produced industrially in crystalline form during the processing of larch wood. Some information is available on nano- and microstructured particles of taxifolin. This paper reports on the generation of a new form of taxifolin as microtubes. These self-assembled tubes were obtained from raw taxifolin by crystal engineering with urea at ambient temperature and pressure. The parameters of temperature, pH value, molar ratio of taxifolin and urea, and time duration were optimized for yield enhancement of the microtubes. The water solubility and melting point of the new form of taxifolin were established. The microtubes were characterized by X-ray diffraction, X-ray powder diffraction, microscopy, mass spectrometry, 1H NMR spectroscopy, UV spectroscopy and Fourier transform infrared spectroscopy methods. The experimental results demonstrate that the microtubes and raw taxifolin both exist in crystalline form with the same structure of the crystal unit. However, they are characterized by different morphological and physicochemical properties. Computer simulation was performed to explain the mechanism of the self-assembly process.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520619000969/um5023sup1.cif
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520619000969/um5023Isup2.hkl
Contains datablock I

txt

Text file https://doi.org/10.1107/S2052520619000969/um5023sup3.txt
mol2 file with the results of the computer modeling of the taxifolin nanoparticle (Fig 9a and Fig 9b).

tif

Tagged Image Format File (TIF) image https://doi.org/10.1107/S2052520619000969/um5023sup4.tif
1H NMR of raw taxifolin

tif

Tagged Image Format File (TIF) image https://doi.org/10.1107/S2052520619000969/um5023sup5.tif
1H NMR of taxifolin microtubes

CCDC references: 186751815; 1892198

Computing details top

Program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997).

(I) top
Crystal data top
C30H24O19F(000) = 1424
Mr = 688.49Dx = 1.517 Mg m3
Monoclinic, C2Mo Kα radiation, λ = 0.71073 Å
a = 23.2416 (14) ÅCell parameters from 1657 reflections
b = 5.2305 (3) Åθ = 3.3–28.7°
c = 25.4061 (14) ŵ = 0.13 mm1
β = 102.634 (5)°T = 150 K
V = 3013.7 (3) Å3Prism
Z = 40.40 × 0.37 × 0.32 mm
Data collection top
Xcalibur
diffractometer
Rint = 0.041
Radiation source: fine-focus sealed tubeθmax = 26.2°, θmin = 3.3°
Graphite monochromatorh = 2818
5773 measured reflectionsk = 66
4746 independent reflectionsl = 2331
2823 reflections with I > 2σ(I)
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.071H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.190 w = 1/[σ2(Fo2) + (0.0938P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.056
4746 reflectionsΔρmax = 0.35 e Å3
442 parametersΔρmin = 0.37 e Å3
1 restraintAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 2 (2)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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
O10.21443 (19)0.1170 (8)0.33401 (18)0.0231 (11)
O30.31724 (19)0.6288 (9)0.32036 (19)0.0286 (12)
H3B0.32720.68680.29370.043*
O40.2607 (2)0.5528 (9)0.21473 (19)0.0257 (11)
O50.1773 (2)0.3147 (9)0.14320 (18)0.0299 (12)
H50.19950.43420.15420.045*
O70.07525 (19)0.3522 (9)0.20816 (19)0.0268 (12)
H70.05900.35280.17610.040*
O3'0.3971 (2)0.0118 (9)0.4942 (2)0.0349 (13)
H3'A0.39870.09790.47150.052*
O4'0.3812 (2)0.3901 (10)0.55885 (19)0.0366 (13)
H4'A0.37270.51450.57530.055*
C20.2435 (3)0.3626 (12)0.3458 (2)0.0168 (14)
H2A0.21360.49790.34090.020*
C30.2835 (3)0.4049 (13)0.3059 (3)0.0198 (15)
H3A0.31090.26010.30930.024*
C40.2474 (3)0.4070 (12)0.2490 (3)0.0210 (16)
C50.1671 (3)0.1794 (13)0.1856 (3)0.0187 (15)
C60.1252 (3)0.0142 (13)0.1748 (3)0.0230 (16)
H6A0.10440.04590.13980.028*
C70.1153 (3)0.1596 (12)0.2180 (3)0.0156 (14)
C80.1439 (3)0.1140 (12)0.2703 (3)0.0202 (15)
H8A0.13500.20970.29840.024*
C90.1868 (3)0.0786 (13)0.2811 (3)0.0210 (16)
C100.1996 (3)0.2279 (12)0.2381 (3)0.0226 (17)
C1'0.2772 (3)0.3617 (12)0.4036 (3)0.0204 (15)
C2'0.3201 (3)0.1759 (13)0.4218 (3)0.0228 (16)
H2'A0.32600.04560.39870.027*
C3'0.3537 (3)0.1834 (12)0.4736 (3)0.0214 (16)
C4'0.3447 (3)0.3839 (13)0.5067 (3)0.0249 (17)
C5'0.3019 (3)0.5624 (12)0.4907 (3)0.0240 (16)
H5'A0.29550.68880.51460.029*
C6'0.2675 (3)0.5545 (13)0.4381 (3)0.0226 (16)
H6'A0.23850.67690.42650.027*
O1A0.42206 (19)1.4284 (9)0.15135 (18)0.0247 (11)
O3A0.3063 (2)0.9559 (9)0.1548 (2)0.0313 (13)
H3AB0.30160.86810.18020.047*
O4A0.36906 (19)0.9534 (9)0.25845 (18)0.0254 (11)
O5A0.4445 (2)1.1812 (9)0.33740 (19)0.0313 (13)
H5A0.42141.06980.32320.047*
O7A0.55295 (18)1.8702 (8)0.28973 (18)0.0250 (11)
H7A0.55771.94800.26300.038*
O3'A0.3819 (2)0.9274 (10)0.0350 (2)0.0397 (14)
H3"A0.36170.90880.06550.060*
O4'A0.3052 (2)1.2774 (9)0.09109 (19)0.0298 (12)
H4"A0.27821.37560.10370.045*
C2A0.3631 (3)1.3118 (12)0.1369 (3)0.0227 (16)
H2AA0.33511.42650.14880.027*
C3A0.3637 (3)1.0601 (12)0.1664 (3)0.0204 (15)
H3AA0.38980.94210.15290.024*
C4A0.3876 (3)1.0946 (13)0.2270 (3)0.0249 (17)
C5A0.4577 (3)1.3339 (13)0.2988 (3)0.0239 (16)
C6A0.4982 (3)1.5253 (12)0.3130 (3)0.0202 (16)
H6AA0.51571.55150.34910.024*
C7A0.5132 (3)1.6792 (12)0.2744 (3)0.0237 (17)
C8A0.4877 (3)1.6451 (12)0.2197 (3)0.0178 (15)
H8AA0.49871.74820.19370.021*
C9A0.4459 (3)1.4559 (12)0.2049 (3)0.0210 (16)
C1OA0.4297 (3)1.2959 (12)0.2435 (3)0.0154 (14)
C1'A0.3475 (3)1.2991 (12)0.0766 (3)0.0252 (17)
C2'A0.3704 (3)1.1134 (13)0.0478 (3)0.0264 (17)
H2'B0.39530.98830.06640.032*
C3'A0.3568 (3)1.1118 (13)0.0082 (3)0.0250 (17)
C4'A0.3187 (3)1.2979 (13)0.0358 (3)0.0254 (17)
C5'A0.2965 (3)1.4846 (13)0.0076 (3)0.0300 (19)
H5'B0.27171.61010.02610.036*
C6'A0.3111 (3)1.4859 (12)0.0487 (3)0.0221 (16)
H6'B0.29631.61330.06760.027*
OW10.4182 (2)0.2752 (9)0.4121 (2)0.0331 (13)
OW20.6149 (2)1.8651 (12)0.3912 (2)0.0542 (17)
OW30.4988 (2)1.3164 (11)0.4451 (2)0.0487 (16)
OW40.0212 (3)0.455 (2)0.1040 (3)0.114 (3)
OW50.0123 (4)0.046 (2)0.0485 (4)0.139 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.024 (2)0.024 (3)0.021 (3)0.005 (2)0.003 (2)0.002 (2)
O30.032 (3)0.030 (3)0.026 (3)0.015 (2)0.011 (2)0.001 (2)
O40.029 (2)0.027 (3)0.022 (3)0.010 (2)0.009 (2)0.000 (2)
O50.042 (3)0.040 (3)0.008 (3)0.014 (3)0.006 (2)0.002 (2)
O70.030 (3)0.026 (3)0.023 (3)0.013 (2)0.003 (2)0.006 (2)
O3'0.038 (3)0.030 (3)0.033 (4)0.005 (2)0.000 (2)0.001 (2)
O4'0.039 (3)0.057 (4)0.012 (3)0.003 (3)0.001 (2)0.002 (3)
C20.018 (3)0.022 (4)0.008 (4)0.003 (3)0.002 (3)0.003 (3)
C30.018 (3)0.025 (4)0.017 (4)0.006 (3)0.003 (3)0.002 (3)
C40.020 (3)0.018 (4)0.026 (5)0.002 (3)0.008 (3)0.004 (3)
C50.024 (3)0.030 (4)0.002 (4)0.006 (3)0.003 (3)0.001 (3)
C60.028 (4)0.026 (4)0.015 (4)0.002 (3)0.005 (3)0.009 (3)
C70.016 (3)0.019 (3)0.012 (4)0.001 (3)0.004 (3)0.002 (3)
C80.025 (3)0.018 (3)0.020 (4)0.000 (3)0.010 (3)0.003 (3)
C90.020 (3)0.027 (4)0.017 (4)0.005 (3)0.007 (3)0.000 (3)
C100.020 (3)0.017 (4)0.032 (5)0.000 (3)0.010 (3)0.001 (3)
C1'0.022 (3)0.020 (4)0.020 (4)0.004 (3)0.008 (3)0.000 (3)
C2'0.027 (4)0.021 (4)0.019 (4)0.004 (3)0.002 (3)0.003 (3)
C3'0.019 (3)0.018 (3)0.025 (5)0.002 (3)0.000 (3)0.004 (3)
C4'0.025 (4)0.031 (4)0.019 (5)0.008 (3)0.005 (3)0.001 (3)
C5'0.028 (4)0.023 (4)0.021 (5)0.004 (3)0.007 (3)0.002 (3)
C6'0.023 (3)0.027 (4)0.018 (4)0.000 (3)0.005 (3)0.000 (3)
O1A0.026 (2)0.034 (3)0.012 (3)0.010 (2)0.001 (2)0.001 (2)
O3A0.029 (3)0.032 (3)0.030 (3)0.014 (2)0.001 (2)0.002 (2)
O4A0.026 (2)0.031 (3)0.018 (3)0.012 (2)0.000 (2)0.001 (2)
O5A0.038 (3)0.033 (3)0.020 (3)0.017 (2)0.000 (2)0.002 (2)
O7A0.030 (3)0.024 (3)0.020 (3)0.009 (2)0.004 (2)0.004 (2)
O3'A0.043 (3)0.039 (3)0.034 (4)0.013 (3)0.003 (3)0.005 (3)
O4'A0.040 (3)0.036 (3)0.013 (3)0.011 (2)0.005 (2)0.009 (2)
C2A0.023 (3)0.019 (4)0.025 (5)0.004 (3)0.003 (3)0.005 (3)
C3A0.018 (3)0.023 (4)0.018 (4)0.006 (3)0.002 (3)0.004 (3)
C4A0.019 (3)0.016 (4)0.041 (5)0.001 (3)0.011 (3)0.003 (3)
C5A0.019 (3)0.025 (4)0.028 (5)0.001 (3)0.008 (3)0.004 (3)
C6A0.019 (3)0.025 (4)0.015 (4)0.002 (3)0.001 (3)0.002 (3)
C7A0.015 (3)0.018 (4)0.038 (5)0.004 (3)0.006 (3)0.003 (3)
C8A0.023 (3)0.018 (3)0.012 (4)0.002 (3)0.003 (3)0.000 (3)
C9A0.021 (3)0.020 (4)0.022 (5)0.001 (3)0.005 (3)0.002 (3)
C1OA0.016 (3)0.022 (3)0.005 (4)0.000 (3)0.005 (3)0.000 (3)
C1'A0.024 (3)0.017 (4)0.036 (5)0.004 (3)0.008 (3)0.003 (3)
C2'A0.022 (3)0.022 (4)0.030 (5)0.004 (3)0.005 (3)0.003 (3)
C3'A0.024 (3)0.029 (4)0.021 (5)0.003 (3)0.005 (3)0.000 (3)
C4'A0.024 (4)0.024 (4)0.025 (5)0.002 (3)0.004 (3)0.000 (3)
C5'A0.026 (4)0.023 (4)0.041 (6)0.004 (3)0.009 (4)0.007 (3)
C6'A0.028 (4)0.024 (4)0.013 (4)0.003 (3)0.002 (3)0.005 (3)
OW10.036 (3)0.043 (3)0.020 (3)0.001 (2)0.007 (2)0.001 (2)
OW20.050 (3)0.065 (4)0.049 (4)0.020 (3)0.014 (3)0.029 (3)
OW30.042 (3)0.066 (4)0.031 (4)0.013 (3)0.004 (3)0.009 (3)
OW40.073 (5)0.170 (9)0.093 (7)0.013 (6)0.007 (5)0.008 (6)
OW50.112 (7)0.174 (11)0.139 (9)0.039 (7)0.041 (7)0.031 (8)
Geometric parameters (Å, º) top
O1—C91.372 (8)O1A—C9A1.359 (8)
O1—C21.452 (7)O1A—C2A1.471 (7)
O3—C31.412 (7)O3A—C3A1.410 (7)
O4—C41.247 (8)O4A—C4A1.233 (8)
O5—C51.353 (8)O5A—C5A1.351 (8)
O7—C71.357 (7)O7A—C7A1.359 (7)
O3'—C3'1.366 (7)O3'A—C3'A1.382 (8)
O4'—C4'1.408 (8)O4'A—C4'A1.374 (8)
C2—C1'1.505 (9)C2A—C1'A1.498 (10)
C2—C31.534 (8)C2A—C3A1.514 (9)
C3—C41.504 (9)C3A—C4A1.528 (10)
C4—C101.434 (9)C4A—C1OA1.437 (9)
C5—C61.390 (9)C5A—C6A1.367 (9)
C5—C101.403 (9)C5A—C1OA1.427 (9)
C6—C71.396 (9)C6A—C7A1.372 (9)
C7—C81.371 (9)C7A—C8A1.398 (10)
C8—C91.401 (9)C8A—C9A1.379 (9)
C9—C101.427 (9)C9A—C1OA1.403 (9)
C1'—C6'1.388 (9)C1'A—C6'A1.380 (9)
C1'—C2'1.397 (9)C1'A—C2'A1.390 (10)
C2'—C3'1.376 (9)C2'A—C3'A1.389 (10)
C3'—C4'1.389 (10)C3'A—C4'A1.397 (9)
C4'—C5'1.360 (9)C4'A—C5'A1.377 (10)
C5'—C6'1.400 (9)C5'A—C6'A1.397 (10)
C9—O1—C2115.4 (5)C9A—O1A—C2A116.6 (5)
O1—C2—C1'108.5 (5)O1A—C2A—C1'A106.1 (5)
O1—C2—C3108.2 (5)O1A—C2A—C3A109.3 (5)
C1'—C2—C3112.4 (5)C1'A—C2A—C3A116.3 (6)
O3—C3—C4113.9 (6)O3A—C3A—C2A109.1 (5)
O3—C3—C2109.3 (5)O3A—C3A—C4A112.1 (6)
C4—C3—C2110.1 (5)C2A—C3A—C4A111.0 (5)
O4—C4—C10124.3 (7)O4A—C4A—C1OA124.2 (7)
O4—C4—C3120.3 (6)O4A—C4A—C3A118.7 (6)
C10—C4—C3115.3 (6)C1OA—C4A—C3A117.1 (6)
O5—C5—C6117.4 (6)O5A—C5A—C6A119.7 (6)
O5—C5—C10120.7 (6)O5A—C5A—C1OA120.3 (6)
C6—C5—C10121.8 (6)C6A—C5A—C1OA120.0 (6)
C5—C6—C7118.1 (6)C5A—C6A—C7A120.6 (7)
O7—C7—C8118.4 (6)O7A—C7A—C6A119.3 (6)
O7—C7—C6119.0 (6)O7A—C7A—C8A119.5 (6)
C8—C7—C6122.6 (6)C6A—C7A—C8A121.2 (6)
C7—C8—C9119.2 (6)C9A—C8A—C7A118.8 (6)
O1—C9—C8117.2 (6)O1A—C9A—C8A117.2 (6)
O1—C9—C10122.6 (6)O1A—C9A—C1OA121.6 (6)
C8—C9—C10120.2 (6)C8A—C9A—C1OA121.2 (6)
C5—C10—C9118.0 (6)C9A—C1OA—C5A118.2 (6)
C5—C10—C4122.4 (6)C9A—C1OA—C4A120.2 (6)
C9—C10—C4119.4 (7)C5A—C1OA—C4A121.6 (6)
C6'—C1'—C2'119.9 (6)C6'A—C1'A—C2'A119.2 (7)
C6'—C1'—C2119.5 (6)C6'A—C1'A—C2A118.5 (6)
C2'—C1'—C2120.5 (6)C2'A—C1'A—C2A122.2 (6)
C3'—C2'—C1'120.8 (7)C3'A—C2'A—C1'A121.0 (7)
O3'—C3'—C2'124.4 (6)O3'A—C3'A—C4'A121.9 (6)
O3'—C3'—C4'117.4 (6)O3'A—C3'A—C2'A118.8 (6)
C2'—C3'—C4'118.1 (6)C4'A—C3'A—C2'A119.3 (6)
C5'—C4'—C3'122.3 (7)O4'A—C4'A—C5'A124.0 (6)
C5'—C4'—O4'121.1 (6)O4'A—C4'A—C3'A115.9 (6)
C3'—C4'—O4'116.6 (6)C5'A—C4'A—C3'A120.0 (7)
C4'—C5'—C6'119.5 (7)C4'A—C5'A—C6'A120.1 (7)
C1'—C6'—C5'119.2 (7)C1'A—C6'A—C5'A120.4 (6)
 

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