Literature DB >> 21587656

Butallyl-onal 1,4-dioxane hemisolvate.

Thomas Gelbrich1, Denise Rossi, Ulrich J Griesser.   

Abstract

THE ASYMMETRIC UNIT OF THE TITLE COMPOUND [SYSTEMATIC NAME: 5-(1-bromo-prop-2-en-1-yl)-5-sec-butyl-pyrimidine-2,4,6-trione 1,4-dioxane hemisolvate], C(11)H(15)BrN(2)O(3)·0.5C(4)H(8)O(2), contains one half-mol-ecule of 1,4-dioxane and one mol-ecule of butallyl-onal, with an almost planar barbiturate ring [largest deviation from the mean plane = 0.049 (5) Å]. The centrosymmetric dioxane mol-ecule adopts a nearly ideal chair conformation. The barbiturate mol-ecules are linked together by an N-H⋯O hydrogen bond, giving a single-stranded chain. Additionally, each dioxane mol-ecule acts as a bridge between two anti-parallel strands of hydrogen-bonded barbiturate mol-ecules via two hydrogen bonds, N-H⋯O(dioxane)O⋯H-N. Thus, a ladder structure is obtained, with the connected barbiturate mol-ecules forming the 'stiles' and the bridging dioxane mol-ecules the 'rungs'.

Entities:  

Year:  2010        PMID: 21587656      PMCID: PMC2983364          DOI: 10.1107/S1600536810038651

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For the preparation of butallyl­onal, see: J. D. Riedel Akt.-Ges. (1924 ▶); Boedecker (1929 ▶). For related structures, see: Al-Saqqar et al. (2004 ▶); Gelbrich et al. (2007 ▶, 2010 ▶); Craven et al. (1969 ▶); Gatehouse & Craven (1971 ▶); Lewis et al. (2004 ▶); Zencirci et al. (2009 ▶). For hydrogen-bond motifs, see: Bernstein et al. (1995 ▶).

Experimental

Crystal data

C11H15BrN2O3·0.5C4H8O2 M = 347.21 Monoclinic, a = 10.494 (2) Å b = 6.7679 (8) Å c = 21.864 (3) Å β = 97.294 (15)° V = 1540.3 (4) Å3 Z = 4 Mo Kα radiation μ = 2.68 mm−1 T = 293 K 0.25 × 0.08 × 0.07 mm

Data collection

Oxford Diffraction Xcalibur Ruby Gemini ultra diffractometer Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2007 ▶) T min = 0.990, T max = 1.000 9189 measured reflections 2714 independent reflections 1171 reflections with I > 2σ(I) R int = 0.100

Refinement

R[F 2 > 2σ(F 2)] = 0.064 wR(F 2) = 0.145 S = 0.95 2714 reflections 189 parameters 2 restraints H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.56 e Å−3 Δρmin = −0.33 e Å−3 Data collection: CrysAlis PRO (Oxford Diffraction, 2007 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: XP in SHELXTL (Sheldrick, 2008 ▶) and Mercury (Bruno et al., 2002 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810038651/fj2340sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810038651/fj2340Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C11H15BrN2O3·0.5C4H8O2F(000) = 712
Mr = 347.21Dx = 1.497 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 837 reflections
a = 10.494 (2) Åθ = 2.5–28.5°
b = 6.7679 (8) ŵ = 2.68 mm1
c = 21.864 (3) ÅT = 293 K
β = 97.294 (15)°Prism, colourless
V = 1540.3 (4) Å30.25 × 0.08 × 0.07 mm
Z = 4
Oxford Diffraction Xcalibur Ruby Gemini ultra diffractometer2714 independent reflections
Radiation source: Enhance Ultra (Cu) X-ray Source1171 reflections with I > 2σ(I)
mirrorRint = 0.100
Detector resolution: 10.3575 pixels mm-1θmax = 25.1°, θmin = 3.2°
ω scansh = −10→12
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2007)k = −8→8
Tmin = 0.990, Tmax = 1.000l = −25→26
9189 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.064Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.145H atoms treated by a mixture of independent and constrained refinement
S = 0.95w = 1/[σ2(Fo2) + (0.0409P)2] where P = (Fo2 + 2Fc2)/3
2714 reflections(Δ/σ)max < 0.001
189 parametersΔρmax = 0.56 e Å3
2 restraintsΔρmin = −0.33 e Å3
Experimental. CrysAlisPro, Oxford Diffraction Ltd., Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
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.
xyzUiso*/Ueq
Br10.64263 (9)0.24500 (13)0.04609 (4)0.0951 (4)
N10.4336 (5)0.4954 (6)0.1405 (2)0.0504 (15)
H10.435 (6)0.6246 (17)0.138 (2)0.061*
N30.3225 (5)0.2096 (6)0.1096 (2)0.0468 (14)
H30.253 (3)0.163 (7)0.087 (2)0.056*
O20.2482 (5)0.5076 (6)0.0762 (2)0.0786 (16)
O60.6264 (5)0.4897 (5)0.1981 (2)0.0752 (16)
O40.3920 (4)−0.0903 (5)0.13692 (18)0.0579 (13)
C20.3306 (7)0.4133 (8)0.1065 (3)0.0519 (18)
C40.4088 (6)0.0884 (8)0.1410 (3)0.0450 (16)
C50.5229 (6)0.1748 (6)0.1812 (3)0.0386 (15)
C60.5334 (7)0.4010 (8)0.1731 (3)0.0505 (18)
C70.6478 (6)0.0760 (8)0.1667 (3)0.0501 (17)
H7A0.71910.16160.18170.060*
H7B0.6588−0.04630.18990.060*
C80.6567 (6)0.0305 (9)0.1013 (3)0.0606 (19)
C90.6782 (7)−0.1521 (11)0.0779 (3)0.084 (2)
H9A0.6886−0.26090.10400.101*
H9B0.6823−0.16750.03600.101*
C100.5050 (7)0.1407 (8)0.2512 (3)0.0605 (19)
H100.58150.19590.27560.073*
C120.4966 (9)−0.0656 (10)0.2707 (4)0.097 (3)
H12A0.5544−0.14610.24990.117*
H12B0.4099−0.11400.25930.117*
C130.5331 (10)−0.0833 (13)0.3418 (3)0.129 (4)
H13D0.6067−0.00200.35460.193*
H13E0.5530−0.21840.35250.193*
H13F0.4622−0.04040.36220.193*
C140.3888 (8)0.2595 (10)0.2694 (3)0.103 (3)
H14A0.40320.39820.26400.154*
H14B0.37930.23380.31170.154*
H14C0.31200.22010.24360.154*
O1S0.1014 (4)0.0764 (5)0.04030 (19)0.0650 (14)
C1S0.0085 (7)0.2010 (7)0.0056 (3)0.072 (2)
H1S10.04910.3243−0.00360.086*
H1S2−0.05950.23130.03030.086*
C2S0.0465 (7)−0.1081 (8)0.0515 (3)0.066 (2)
H2S1−0.0200−0.08990.07810.080*
H2S20.1119−0.19380.07270.080*
U11U22U33U12U13U23
Br10.1010 (8)0.1162 (6)0.0699 (6)0.0078 (6)0.0173 (5)0.0284 (5)
N10.050 (4)0.025 (2)0.070 (3)−0.006 (3)−0.019 (3)0.003 (3)
N30.048 (4)0.025 (2)0.062 (3)−0.006 (2)−0.014 (3)0.002 (2)
O20.068 (4)0.046 (2)0.112 (4)0.003 (2)−0.028 (3)0.021 (2)
O60.072 (4)0.051 (2)0.092 (4)−0.017 (2)−0.032 (3)−0.008 (2)
O40.063 (3)0.027 (2)0.078 (3)−0.0022 (19)−0.011 (2)0.0016 (19)
C20.056 (5)0.037 (3)0.061 (4)0.004 (3)0.000 (4)0.009 (3)
C40.057 (5)0.036 (3)0.042 (4)−0.002 (3)0.006 (3)0.006 (3)
C50.043 (4)0.027 (3)0.044 (4)0.001 (3)−0.003 (3)0.005 (2)
C60.059 (5)0.042 (3)0.046 (4)0.009 (4)−0.011 (4)0.002 (3)
C70.044 (5)0.047 (3)0.059 (4)0.000 (3)0.003 (3)−0.001 (3)
C80.049 (5)0.066 (4)0.068 (5)−0.003 (4)0.009 (4)−0.002 (4)
C90.091 (7)0.098 (5)0.068 (5)0.003 (5)0.031 (5)0.005 (4)
C100.082 (6)0.050 (3)0.052 (4)0.020 (4)0.017 (4)0.006 (3)
C120.107 (8)0.084 (5)0.103 (7)−0.001 (5)0.023 (6)0.008 (5)
C130.144 (9)0.186 (8)0.060 (6)0.060 (8)0.029 (6)0.072 (6)
C140.132 (8)0.114 (6)0.067 (5)0.072 (6)0.032 (5)0.019 (5)
O1S0.058 (3)0.046 (2)0.080 (3)−0.003 (2)−0.031 (3)0.001 (2)
C1S0.071 (5)0.041 (3)0.097 (6)0.006 (3)−0.016 (4)−0.002 (4)
C2S0.073 (6)0.056 (4)0.063 (5)0.004 (4)−0.014 (4)0.012 (3)
Br1—C81.881 (6)C10—C121.466 (8)
N1—C61.351 (7)C10—C141.553 (9)
N1—C21.351 (7)C10—H100.9800
N1—H10.876 (10)C12—C131.558 (9)
N3—C41.344 (6)C12—H12A0.9700
N3—C21.384 (7)C12—H12B0.9700
N3—H30.89 (4)C13—H13D0.9600
O2—C21.203 (6)C13—H13E0.9600
O6—C61.215 (6)C13—H13F0.9600
O4—C41.224 (5)C14—H14A0.9600
C4—C51.510 (7)C14—H14B0.9600
C5—C71.540 (8)C14—H14C0.9600
C5—C61.547 (7)O1S—C2S1.410 (7)
C5—C101.583 (8)O1S—C1S1.431 (7)
C7—C81.479 (8)C1S—C2Si1.452 (8)
C7—H7A0.9700C1S—H1S10.9700
C7—H7B0.9700C1S—H1S20.9700
C8—C91.366 (8)C2S—C1Si1.452 (8)
C9—H9A0.9300C2S—H2S10.9700
C9—H9B0.9300C2S—H2S20.9700
C6—N1—C2127.5 (5)C14—C10—C5111.4 (5)
C6—N1—H1119 (4)C12—C10—H10106.3
C2—N1—H1113 (4)C14—C10—H10106.3
C4—N3—C2126.3 (5)C5—C10—H10106.3
C4—N3—H3121 (3)C10—C12—C13110.3 (6)
C2—N3—H3112 (3)C10—C12—H12A109.6
O2—C2—N1123.6 (5)C13—C12—H12A109.6
O2—C2—N3120.8 (6)C10—C12—H12B109.6
N1—C2—N3115.6 (5)C13—C12—H12B109.6
O4—C4—N3118.9 (5)H12A—C12—H12B108.1
O4—C4—C5121.4 (5)C12—C13—H13D109.5
N3—C4—C5119.6 (4)C12—C13—H13E109.5
C4—C5—C7110.2 (4)H13D—C13—H13E109.5
C4—C5—C6112.3 (5)C12—C13—H13F109.5
C7—C5—C6109.4 (5)H13D—C13—H13F109.5
C4—C5—C10108.8 (5)H13E—C13—H13F109.5
C7—C5—C10110.2 (5)C10—C14—H14A109.5
C6—C5—C10105.9 (4)C10—C14—H14B109.5
O6—C6—N1121.9 (5)H14A—C14—H14B109.5
O6—C6—C5120.2 (5)C10—C14—H14C109.5
N1—C6—C5117.8 (5)H14A—C14—H14C109.5
C8—C7—C5116.7 (5)H14B—C14—H14C109.5
C8—C7—H7A108.1C2S—O1S—C1S110.4 (4)
C5—C7—H7A108.1O1S—C1S—C2Si111.7 (5)
C8—C7—H7B108.1O1S—C1S—H1S1109.3
C5—C7—H7B108.1C2Si—C1S—H1S1109.3
H7A—C7—H7B107.3O1S—C1S—H1S2109.3
C9—C8—C7125.7 (6)C2Si—C1S—H1S2109.3
C9—C8—Br1117.5 (6)H1S1—C1S—H1S2107.9
C7—C8—Br1116.8 (4)O1S—C2S—C1Si111.1 (5)
C8—C9—H9A120.0O1S—C2S—H2S1109.4
C8—C9—H9B120.0C1Si—C2S—H2S1109.4
H9A—C9—H9B120.0O1S—C2S—H2S2109.4
C12—C10—C14110.0 (7)C1Si—C2S—H2S2109.4
C12—C10—C5116.0 (5)H2S1—C2S—H2S2108.0
D—H···AD—HH···AD···AD—H···A
N1—H1···O4ii0.88 (1)1.98 (2)2.837 (5)166 (6)
N3—H3···O1S0.89 (4)1.87 (4)2.757 (6)177 (5)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H1⋯O4i0.88 (1)1.98 (2)2.837 (5)166 (6)
N3—H3⋯O1S0.89 (4)1.87 (4)2.757 (6)177 (5)

Symmetry code: (i) .

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