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The crystal structures of three polymorphs found for the addition complex of urea and barbituric acid are described and compared. Two polymorphs are monoclinic, space groups
P2
1/
c and
Cc, whereas the third is triclinic,
. The displacement of electron density towards the mesomeric forms, corresponding to the tautomeric forms of higher stability, of the barbituric acid molecule seem to influence the type of hydrogen bonds formed, which in turn determines the different packing topology in the polymorphs. While the polymorphic forms can be easily differentiated at the first-level graph-set analysis of their hydrogen-bonding patterns, a higher-level analysis enables important features of the mutual spatial arrangement of the structural components to be revealed.
Supporting information
CCDC references: 705613; 705614; 705615
For all compounds, data collection: KappaCCD Server Software (Nonius, 1997); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: HKL DENZO and SCALEPACK (Otwinowski & Minor, 1997); program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); ORTEP-3 for Windows (Farrugia, 1997); Mercury (Version 1.4; Macrae et al., 2006); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).
(I) 2,4,6(1
H,3H,5
H)-Pyrimidinetrione urea addition compound
top
Crystal data top
C5H8N4O4 | F(000) = 392 |
Mr = 188.15 | Dx = 1.593 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 1657 reflections |
a = 7.8857 (3) Å | θ = 1.0–27.5° |
b = 6.9620 (2) Å | µ = 0.14 mm−1 |
c = 14.4283 (6) Å | T = 293 K |
β = 98.027 (1)° | Plate, yellowish |
V = 784.36 (5) Å3 | 0.30 × 0.22 × 0.05 mm |
Z = 4 | |
Data collection top
KappaCCD diffractometer | 1775 independent reflections |
Radiation source: fine-focus sealed tube | 1334 reflections with I > 2σ(I) |
Horizontally mounted graphite crystal monochromator | Rint = 0.025 |
Detector resolution: 9 pixels mm-1 | θmax = 27.5°, θmin = 3.3° |
ω scans at χ = 55 ° | h = −10→10 |
Absorption correction: multi-scan HKL DENZO and SCALEPACK (Otwinowski & Minor, 1997) | k = −9→8 |
Tmin = 0.960, Tmax = 0.993 | l = −18→18 |
3177 measured reflections | |
Refinement top
Refinement on F2 | 0 restraints |
Least-squares matrix: full | H-atom parameters constrained |
R[F2 > 2σ(F2)] = 0.043 | w = 1/[σ2(Fo2) + (0.0535P)2 + 0.1825P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.113 | (Δ/σ)max < 0.001 |
S = 1.03 | Δρmax = 0.21 e Å−3 |
1775 reflections | Δρmin = −0.19 e Å−3 |
118 parameters | |
Crystal data top
C5H8N4O4 | V = 784.36 (5) Å3 |
Mr = 188.15 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 7.8857 (3) Å | µ = 0.14 mm−1 |
b = 6.9620 (2) Å | T = 293 K |
c = 14.4283 (6) Å | 0.30 × 0.22 × 0.05 mm |
β = 98.027 (1)° | |
Data collection top
KappaCCD diffractometer | 1775 independent reflections |
Absorption correction: multi-scan HKL DENZO and SCALEPACK (Otwinowski & Minor, 1997) | 1334 reflections with I > 2σ(I) |
Tmin = 0.960, Tmax = 0.993 | Rint = 0.025 |
3177 measured reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.043 | 0 restraints |
wR(F2) = 0.113 | H-atom parameters constrained |
S = 1.03 | Δρmax = 0.21 e Å−3 |
1775 reflections | Δρmin = −0.19 e Å−3 |
118 parameters | |
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 | x | y | z | Uiso*/Ueq | |
O1 | 0.29444 (13) | 0.08443 (15) | −0.04154 (8) | 0.0405 (3) | |
C1 | 0.33939 (19) | 0.2365 (2) | 0.00107 (11) | 0.0312 (4) | |
N2 | 0.49808 (17) | 0.2593 (2) | 0.04500 (11) | 0.0453 (4) | |
H2A | 0.5718 | 0.1684 | 0.0444 | 0.054* | |
H2B | 0.5269 | 0.3648 | 0.0740 | 0.054* | |
N4 | 0.22878 (18) | 0.3807 (2) | 0.00349 (12) | 0.0490 (4) | |
H4A | 0.1255 | 0.3695 | −0.0244 | 0.059* | |
H4B | 0.2607 | 0.4848 | 0.0329 | 0.059* | |
N1 | 0.02901 (15) | 0.02606 (18) | 0.12628 (9) | 0.0316 (3) | |
H1 | −0.0651 | 0.0085 | 0.0893 | 0.038* | |
C2 | 0.15042 (18) | −0.1145 (2) | 0.12890 (11) | 0.0320 (4) | |
O2 | 0.12314 (14) | −0.26446 (16) | 0.08623 (9) | 0.0477 (4) | |
N3 | 0.30640 (15) | −0.07976 (18) | 0.18238 (9) | 0.0333 (3) | |
H3 | 0.3870 | −0.1613 | 0.1785 | 0.040* | |
C4 | 0.34359 (18) | 0.0726 (2) | 0.24078 (11) | 0.0319 (4) | |
O4 | 0.47961 (14) | 0.08108 (17) | 0.29313 (9) | 0.0448 (3) | |
C5 | 0.2109 (2) | 0.2251 (2) | 0.23773 (12) | 0.0384 (4) | |
H5A | 0.1878 | 0.2463 | 0.3012 | 0.046* | |
H5B | 0.2598 | 0.3430 | 0.2172 | 0.046* | |
C6 | 0.04407 (19) | 0.1936 (2) | 0.17773 (11) | 0.0333 (4) | |
O6 | −0.07375 (16) | 0.30556 (19) | 0.17366 (9) | 0.0511 (4) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0322 (6) | 0.0330 (6) | 0.0530 (7) | 0.0027 (5) | −0.0054 (5) | −0.0115 (5) |
C1 | 0.0313 (8) | 0.0284 (8) | 0.0334 (8) | −0.0004 (6) | 0.0025 (6) | −0.0012 (7) |
N2 | 0.0358 (8) | 0.0341 (8) | 0.0614 (10) | 0.0005 (6) | −0.0098 (7) | −0.0123 (7) |
N4 | 0.0377 (8) | 0.0345 (8) | 0.0721 (11) | 0.0043 (6) | −0.0014 (7) | −0.0159 (7) |
N1 | 0.0251 (6) | 0.0319 (7) | 0.0355 (7) | 0.0023 (5) | −0.0040 (5) | −0.0031 (6) |
C2 | 0.0281 (8) | 0.0299 (8) | 0.0367 (8) | −0.0005 (6) | −0.0003 (6) | −0.0012 (7) |
O2 | 0.0371 (7) | 0.0351 (7) | 0.0668 (9) | 0.0030 (5) | −0.0073 (6) | −0.0177 (6) |
N3 | 0.0257 (6) | 0.0289 (7) | 0.0435 (7) | 0.0026 (5) | −0.0008 (5) | −0.0035 (6) |
C4 | 0.0299 (8) | 0.0309 (8) | 0.0338 (8) | −0.0030 (6) | 0.0003 (6) | 0.0028 (7) |
O4 | 0.0347 (6) | 0.0422 (7) | 0.0521 (7) | −0.0021 (5) | −0.0125 (5) | −0.0007 (6) |
C5 | 0.0386 (9) | 0.0364 (9) | 0.0383 (9) | 0.0025 (7) | −0.0013 (7) | −0.0097 (7) |
C6 | 0.0326 (8) | 0.0348 (8) | 0.0321 (8) | 0.0046 (6) | 0.0033 (6) | −0.0002 (7) |
O6 | 0.0445 (7) | 0.0503 (8) | 0.0561 (8) | 0.0184 (6) | −0.0014 (6) | −0.0131 (6) |
Geometric parameters (Å, º) top
O1—C1 | 1.251 (2) | C2—O2 | 1.216 (2) |
C1—N2 | 1.331 (2) | C2—N3 | 1.379 (2) |
C1—N4 | 1.333 (2) | N3—C4 | 1.361 (2) |
N2—H2A | 0.8600 | N3—H3 | 0.8600 |
N2—H2B | 0.8600 | C4—O4 | 1.224 (2) |
N4—H4A | 0.8600 | C4—C5 | 1.487 (2) |
N4—H4B | 0.8600 | C5—C6 | 1.487 (2) |
N1—C2 | 1.366 (2) | C5—H5A | 0.9700 |
N1—C6 | 1.378 (2) | C5—H5B | 0.9700 |
N1—H1 | 0.8600 | C6—O6 | 1.208 (2) |
| | | |
O1—C1—N2 | 121.2 (1) | C4—N3—C2 | 125.5 (1) |
O1—C1—N4 | 120.6 (1) | C4—N3—H3 | 117.2 |
N2—C1—N4 | 118.2 (1) | C2—N3—H3 | 117.2 |
C1—N2—H2A | 120.0 | O4—C4—N3 | 120.9 (1) |
C1—N2—H2B | 120.0 | O4—C4—C5 | 122.4 (1) |
H2A—N2—H2B | 120.0 | N3—C4—C5 | 116.6 (1) |
C1—N4—H4A | 120.0 | C6—C5—C4 | 118.3 (1) |
C1—N4—H4B | 120.0 | C6—C5—H5A | 107.7 |
H4A—N4—H4B | 120.0 | C4—C5—H5A | 107.7 |
C2—N1—C6 | 125.7 (1) | C6—C5—H5B | 107.7 |
C2—N1—H1 | 117.1 | C4—C5—H5B | 107.7 |
C6—N1—H1 | 117.1 | H5A—C5—H5B | 107.1 |
O2—C2—N1 | 121.8 (1) | O6—C6—N1 | 120.8 (1) |
O2—C2—N3 | 121.0 (1) | O6—C6—C5 | 123.0 (2) |
N1—C2—N3 | 117.2 (1) | N1—C6—C5 | 116.2 (1) |
| | | |
C6—N1—C2—O2 | 174.8 (2) | O4—C4—C5—C6 | −174.8 (2) |
C6—N1—C2—N3 | −5.1 (2) | N3—C4—C5—C6 | 4.8 (2) |
O2—C2—N3—C4 | −172.2 (2) | C2—N1—C6—O6 | −176.7 (2) |
N1—C2—N3—C4 | 7.7 (2) | C2—N1—C6—C5 | 2.8 (2) |
C2—N3—C4—O4 | 172.0 (2) | C4—C5—C6—O6 | 176.9 (2) |
C2—N3—C4—C5 | −7.6 (2) | C4—C5—C6—N1 | −2.6 (2) |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···O1i | 0.86 | 2.06 | 2.903 (2) | 168 |
N2—H2B···O4ii | 0.86 | 2.44 | 3.223 (2) | 151 |
N4—H4A···O2iii | 0.86 | 2.17 | 3.005 (2) | 165 |
N4—H4B···O2iv | 0.86 | 2.25 | 2.916 (2) | 135 |
N1—H1···O1iii | 0.86 | 1.95 | 2.779 (2) | 160 |
N3—H3···O4v | 0.86 | 2.09 | 2.895 (2) | 156 |
Symmetry codes: (i) −x+1, −y, −z; (ii) −x+1, y+1/2, −z+1/2; (iii) −x, −y, −z; (iv) x, y+1, z; (v) −x+1, y−1/2, −z+1/2. |
(II) 2,4,6(1
H,3H,5
H)-Pyrimidinetrione urea addition compound
top
Crystal data top
C5H8N4O4 | F(000) = 392 |
Mr = 188.15 | Dx = 1.556 Mg m−3 |
Monoclinic, Cc | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: C -2yc | Cell parameters from 1182 reflections |
a = 15.9423 (7) Å | θ = 1.0–30.0° |
b = 5.0984 (3) Å | µ = 0.14 mm−1 |
c = 10.5534 (5) Å | T = 293 K |
β = 110.570 (2)° | Block, colourless |
V = 803.09 (7) Å3 | 0.32 × 0.22 × 0.12 mm |
Z = 4 | |
Data collection top
KappaCCD diffractometer | 1169 independent reflections |
Radiation source: fine-focus sealed tube | 1099 reflections with I > 2σ(I) |
Horizontally mounted graphite crystal monochromator | Rint = 0.016 |
Detector resolution: 9 pixels mm-1 | θmax = 30.0°, θmin = 4.1° |
ω scans at χ = 55 ° | h = −21→20 |
Absorption correction: multi-scan HKL DENZO and SCALEPACK (Otwinowski & Minor, 1997) | k = −4→7 |
Tmin = 0.958, Tmax = 0.984 | l = −14→14 |
3691 measured reflections | |
Refinement top
Refinement on F2 | H-atom parameters constrained |
Least-squares matrix: full | w = 1/[σ2(Fo2) + (0.0491P)2 + 0.0769P] where P = (Fo2 + 2Fc2)/3 |
R[F2 > 2σ(F2)] = 0.033 | (Δ/σ)max < 0.001 |
wR(F2) = 0.083 | Δρmax = 0.15 e Å−3 |
S = 1.06 | Δρmin = −0.17 e Å−3 |
1169 reflections | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
118 parameters | Absolute structure parameter: 0.00 (3) |
2 restraints | |
Crystal data top
C5H8N4O4 | V = 803.09 (7) Å3 |
Mr = 188.15 | Z = 4 |
Monoclinic, Cc | Mo Kα radiation |
a = 15.9423 (7) Å | µ = 0.14 mm−1 |
b = 5.0984 (3) Å | T = 293 K |
c = 10.5534 (5) Å | 0.32 × 0.22 × 0.12 mm |
β = 110.570 (2)° | |
Data collection top
KappaCCD diffractometer | 1169 independent reflections |
Absorption correction: multi-scan HKL DENZO and SCALEPACK (Otwinowski & Minor, 1997) | 1099 reflections with I > 2σ(I) |
Tmin = 0.958, Tmax = 0.984 | Rint = 0.016 |
3691 measured reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.033 | H-atom parameters constrained |
wR(F2) = 0.083 | Δρmax = 0.15 e Å−3 |
S = 1.06 | Δρmin = −0.17 e Å−3 |
1169 reflections | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
118 parameters | Absolute structure parameter: 0.00 (3) |
2 restraints | |
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 | x | y | z | Uiso*/Ueq | |
O1 | 0.76305 (8) | 0.5526 (3) | 0.56200 (11) | 0.0355 (3) | |
C1 | 0.68332 (11) | 0.4865 (4) | 0.49837 (16) | 0.0311 (3) | |
N2 | 0.64621 (11) | 0.2830 (4) | 0.53835 (17) | 0.0497 (4) | |
H2A | 0.6769 | 0.1945 | 0.6088 | 0.060* | |
H2B | 0.5916 | 0.2403 | 0.4937 | 0.060* | |
N4 | 0.63236 (12) | 0.6185 (4) | 0.38989 (18) | 0.0508 (5) | |
H4A | 0.6538 | 0.7522 | 0.3619 | 0.061* | |
H4B | 0.5780 | 0.5701 | 0.3477 | 0.061* | |
N1 | 0.84095 (10) | −0.0066 (3) | 0.49126 (14) | 0.0326 (3) | |
H1 | 0.8125 | −0.1336 | 0.5117 | 0.039* | |
C2 | 0.80045 (10) | 0.1134 (3) | 0.36886 (16) | 0.0314 (3) | |
O2 | 0.72846 (10) | 0.0353 (3) | 0.28983 (13) | 0.0462 (4) | |
N3 | 0.84309 (9) | 0.3242 (3) | 0.33813 (13) | 0.0329 (3) | |
H3 | 0.8166 | 0.4013 | 0.2620 | 0.039* | |
C4 | 0.92426 (10) | 0.4221 (3) | 0.41845 (16) | 0.0320 (3) | |
O4 | 0.95950 (10) | 0.6007 (3) | 0.37923 (15) | 0.0470 (4) | |
C5 | 0.96514 (11) | 0.3047 (3) | 0.55714 (16) | 0.0354 (3) | |
H5A | 1.0277 | 0.2683 | 0.5729 | 0.042* | |
H5B | 0.9632 | 0.4353 | 0.6229 | 0.042* | |
C6 | 0.92271 (10) | 0.0581 (3) | 0.58379 (15) | 0.0306 (3) | |
O6 | 0.95728 (9) | −0.0776 (3) | 0.68302 (14) | 0.0446 (3) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0288 (6) | 0.0431 (7) | 0.0289 (6) | −0.0064 (5) | 0.0028 (5) | −0.0013 (5) |
C1 | 0.0285 (7) | 0.0362 (8) | 0.0260 (6) | −0.0022 (6) | 0.0063 (5) | −0.0055 (5) |
N2 | 0.0359 (8) | 0.0574 (10) | 0.0457 (9) | −0.0149 (7) | 0.0016 (7) | 0.0097 (8) |
N4 | 0.0362 (8) | 0.0540 (10) | 0.0451 (9) | −0.0113 (7) | −0.0072 (7) | 0.0129 (8) |
N1 | 0.0286 (6) | 0.0329 (6) | 0.0314 (6) | −0.0052 (5) | 0.0043 (5) | 0.0017 (5) |
C2 | 0.0277 (7) | 0.0365 (8) | 0.0273 (7) | −0.0035 (6) | 0.0065 (6) | −0.0024 (6) |
O2 | 0.0369 (7) | 0.0572 (8) | 0.0335 (6) | −0.0138 (6) | −0.0013 (5) | 0.0014 (6) |
N3 | 0.0323 (6) | 0.0401 (7) | 0.0233 (6) | −0.0030 (5) | 0.0061 (5) | 0.0019 (5) |
C4 | 0.0299 (8) | 0.0337 (8) | 0.0312 (7) | −0.0024 (6) | 0.0095 (6) | −0.0020 (6) |
O4 | 0.0440 (7) | 0.0506 (8) | 0.0424 (7) | −0.0146 (6) | 0.0101 (6) | 0.0082 (6) |
C5 | 0.0305 (7) | 0.0385 (8) | 0.0318 (8) | −0.0067 (6) | 0.0041 (6) | 0.0001 (6) |
C6 | 0.0264 (7) | 0.0321 (7) | 0.0289 (7) | 0.0005 (6) | 0.0045 (6) | −0.0012 (6) |
O6 | 0.0385 (7) | 0.0435 (7) | 0.0390 (7) | −0.0041 (6) | −0.0022 (5) | 0.0097 (5) |
Geometric parameters (Å, º) top
O1—C1 | 1.257 (2) | C2—O2 | 1.224 (2) |
C1—N4 | 1.330 (2) | C2—N3 | 1.370 (2) |
C1—N2 | 1.334 (2) | N3—C4 | 1.368 (2) |
N2—H2A | 0.8600 | N3—H3 | 0.8600 |
N2—H2B | 0.8600 | C4—O4 | 1.216 (2) |
N4—H4A | 0.8600 | C4—C5 | 1.502 (2) |
N4—H4B | 0.8600 | C5—C6 | 1.500 (2) |
N1—C6 | 1.366 (2) | C5—H5A | 0.9700 |
N1—C2 | 1.369 (2) | C5—H5B | 0.9700 |
N1—H1 | 0.8600 | C6—O6 | 1.214 (2) |
| | | |
O1—C1—N4 | 121.4 (2) | C4—N3—C2 | 125.4 (1) |
O1—C1—N2 | 121.1 (2) | C4—N3—H3 | 117.3 |
N4—C1—N2 | 117.5 (2) | C2—N3—H3 | 117.3 |
C1—N2—H2A | 120.0 | O4—C4—N3 | 120.8 (2) |
C1—N2—H2B | 120.0 | O4—C4—C5 | 122.4 (2) |
H2A—N2—H2B | 120.0 | N3—C4—C5 | 116.8 (1) |
C1—N4—H4A | 120.0 | C6—C5—C4 | 116.6 (1) |
C1—N4—H4B | 120.0 | C6—C5—H5A | 108.2 |
H4A—N4—H4B | 120.0 | C4—C5—H5A | 108.2 |
C6—N1—C2 | 125.6 (2) | C6—C5—H5B | 108.2 |
C6—N1—H1 | 117.2 | C4—C5—H5B | 108.2 |
C2—N1—H1 | 117.2 | H5A—C5—H5B | 107.3 |
O2—C2—N1 | 121.1 (2) | O6—C6—N1 | 120.6 (2) |
O2—C2—N3 | 121.2 (2) | O6—C6—C5 | 122.8 (1) |
N1—C2—N3 | 117.7 (1) | N1—C6—C5 | 116.6 (1) |
| | | |
C6—N1—C2—O2 | 177.1 (2) | O4—C4—C5—C6 | −170.2 (2) |
C6—N1—C2—N3 | −3.1 (2) | N3—C4—C5—C6 | 11.9 (2) |
O2—C2—N3—C4 | −178.6 (2) | C2—N1—C6—O6 | −172.1 (2) |
N1—C2—N3—C4 | 1.6 (2) | C2—N1—C6—C5 | 9.2 (2) |
C2—N3—C4—O4 | 175.6 (2) | C4—C5—C6—O6 | 168.2 (2) |
C2—N3—C4—C5 | −6.4 (2) | C4—C5—C6—N1 | −13.1 (2) |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···O2i | 0.86 | 2.14 | 2.992 (2) | 169 |
N2—H2B···O4ii | 0.86 | 2.15 | 3.005 (2) | 175 |
N4—H4A···O2iii | 0.86 | 2.17 | 3.019 (2) | 169 |
N4—H4B···O6iv | 0.86 | 2.09 | 2.884 (2) | 153 |
N1—H1···O1v | 0.86 | 1.94 | 2.793 (2) | 172 |
N3—H3···O1vi | 0.86 | 1.99 | 2.811 (2) | 158 |
Symmetry codes: (i) x, −y, z+1/2; (ii) x−1/2, y−1/2, z; (iii) x, y+1, z; (iv) x−1/2, −y+1/2, z−1/2; (v) x, y−1, z; (vi) x, −y+1, z−1/2. |
(III) 2,4,6(1
H,3H,5
H)-Pyrimidinetrione urea addition compound
top
Crystal data top
C5H8N4O4 | Z = 4 |
Mr = 188.15 | F(000) = 392 |
Triclinic, P1 | Dx = 1.586 Mg m−3 |
a = 8.1588 (4) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 9.1117 (4) Å | Cell parameters from 2050 reflections |
c = 10.9268 (5) Å | θ = 2.9–29.1° |
α = 100.248 (2)° | µ = 0.14 mm−1 |
β = 91.515 (2)° | T = 293 K |
γ = 99.192 (2)° | Block, colourless |
V = 787.82 (6) Å3 | 0.35 × 0.13 × 0.13 mm |
Data collection top
KappaCCD diffractometer | 3584 independent reflections |
Radiation source: fine-focus sealed tube | 2380 reflections with I > 2σ(I) |
Horizontally mounted graphite crystal monochromator | Rint = 0.017 |
Detector resolution: 9 pixels mm-1 | θmax = 27.5°, θmin = 3.1° |
ω scans at χ = 55 ° | h = −9→10 |
Absorption correction: multi-scan HKL DENZO and SCALEPACK (Otwinowski & Minor, 1997) | k = −9→11 |
Tmin = 0.953, Tmax = 0.982 | l = −14→14 |
4828 measured reflections | |
Refinement top
Refinement on F2 | 0 restraints |
Least-squares matrix: full | H-atom parameters constrained |
R[F2 > 2σ(F2)] = 0.053 | w = 1/[σ2(Fo2) + (0.0476P)2 + 0.2967P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.137 | (Δ/σ)max < 0.001 |
S = 1.03 | Δρmax = 0.22 e Å−3 |
3584 reflections | Δρmin = −0.19 e Å−3 |
235 parameters | |
Crystal data top
C5H8N4O4 | γ = 99.192 (2)° |
Mr = 188.15 | V = 787.82 (6) Å3 |
Triclinic, P1 | Z = 4 |
a = 8.1588 (4) Å | Mo Kα radiation |
b = 9.1117 (4) Å | µ = 0.14 mm−1 |
c = 10.9268 (5) Å | T = 293 K |
α = 100.248 (2)° | 0.35 × 0.13 × 0.13 mm |
β = 91.515 (2)° | |
Data collection top
KappaCCD diffractometer | 3584 independent reflections |
Absorption correction: multi-scan HKL DENZO and SCALEPACK (Otwinowski & Minor, 1997) | 2380 reflections with I > 2σ(I) |
Tmin = 0.953, Tmax = 0.982 | Rint = 0.017 |
4828 measured reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.053 | 0 restraints |
wR(F2) = 0.137 | H-atom parameters constrained |
S = 1.03 | Δρmax = 0.22 e Å−3 |
3584 reflections | Δρmin = −0.19 e Å−3 |
235 parameters | |
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 | x | y | z | Uiso*/Ueq | |
N1A | 0.7813 (2) | 0.04121 (19) | 0.52443 (15) | 0.0420 (4) | |
H1A | 0.7609 | 0.0212 | 0.5971 | 0.050* | |
C2A | 0.6814 (3) | −0.0434 (2) | 0.42570 (18) | 0.0401 (5) | |
O2A | 0.5749 (2) | −0.14712 (17) | 0.44075 (13) | 0.0544 (4) | |
N3A | 0.7088 (2) | −0.0068 (2) | 0.31096 (16) | 0.0463 (5) | |
H3A | 0.6472 | −0.0608 | 0.2489 | 0.056* | |
C4A | 0.8263 (3) | 0.1087 (2) | 0.28616 (19) | 0.0426 (5) | |
O4A | 0.8402 (2) | 0.1331 (2) | 0.18121 (14) | 0.0632 (5) | |
C5A | 0.9343 (3) | 0.1979 (2) | 0.39424 (18) | 0.0411 (5) | |
H5A1 | 1.0490 | 0.1935 | 0.3748 | 0.049* | |
H5A2 | 0.9197 | 0.3026 | 0.4020 | 0.049* | |
C6A | 0.9096 (2) | 0.1537 (2) | 0.51749 (19) | 0.0389 (5) | |
O6A | 0.99946 (19) | 0.21308 (18) | 0.60997 (14) | 0.0548 (4) | |
N1B | 0.6821 (2) | 0.42592 (19) | 0.96006 (15) | 0.0403 (4) | |
H1B | 0.6549 | 0.4113 | 1.0330 | 0.048* | |
C2B | 0.5979 (2) | 0.3292 (2) | 0.86060 (18) | 0.0388 (5) | |
O2B | 0.4860 (2) | 0.22890 (18) | 0.87468 (14) | 0.0566 (5) | |
N3B | 0.6444 (2) | 0.34856 (19) | 0.74367 (15) | 0.0417 (4) | |
H3B | 0.5977 | 0.2821 | 0.6815 | 0.050* | |
C4B | 0.7586 (3) | 0.4646 (2) | 0.71804 (19) | 0.0397 (5) | |
O4B | 0.7809 (2) | 0.47970 (19) | 0.61115 (13) | 0.0569 (4) | |
C5B | 0.8523 (3) | 0.5679 (3) | 0.82745 (19) | 0.0456 (5) | |
H5B1 | 0.8406 | 0.6707 | 0.8212 | 0.055* | |
H5B2 | 0.9692 | 0.5608 | 0.8208 | 0.055* | |
C6B | 0.8053 (3) | 0.5434 (2) | 0.95412 (19) | 0.0401 (5) | |
O6B | 0.8734 (2) | 0.62294 (18) | 1.04861 (14) | 0.0573 (5) | |
O1A | 0.45510 (19) | 0.62811 (17) | 0.82492 (13) | 0.0490 (4) | |
C1A | 0.3897 (3) | 0.5897 (2) | 0.71742 (19) | 0.0396 (5) | |
N2A | 0.4423 (2) | 0.6616 (2) | 0.62667 (17) | 0.0569 (5) | |
H2A1 | 0.5232 | 0.7366 | 0.6416 | 0.068* | |
H2A2 | 0.3955 | 0.6333 | 0.5530 | 0.068* | |
N4A | 0.2615 (3) | 0.4753 (2) | 0.6897 (2) | 0.0637 (6) | |
H4A1 | 0.2231 | 0.4272 | 0.7466 | 0.076* | |
H4A2 | 0.2175 | 0.4499 | 0.6149 | 0.076* | |
O1B | 0.7245 (2) | −0.07543 (18) | 0.73102 (13) | 0.0587 (5) | |
C1B | 0.7595 (3) | −0.0159 (2) | 0.84199 (19) | 0.0427 (5) | |
N2B | 0.8721 (3) | 0.1093 (2) | 0.8735 (2) | 0.0619 (6) | |
H2B1 | 0.9221 | 0.1503 | 0.8166 | 0.074* | |
H2B2 | 0.8950 | 0.1491 | 0.9507 | 0.074* | |
N4B | 0.6877 (3) | −0.0768 (2) | 0.93195 (17) | 0.0666 (6) | |
H4B1 | 0.6158 | −0.1585 | 0.9141 | 0.080* | |
H4B2 | 0.7127 | −0.0348 | 1.0085 | 0.080* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
N1A | 0.0447 (10) | 0.0466 (10) | 0.0274 (9) | −0.0121 (8) | 0.0000 (7) | 0.0052 (8) |
C2A | 0.0411 (12) | 0.0408 (11) | 0.0320 (11) | −0.0066 (9) | 0.0003 (9) | 0.0019 (9) |
O2A | 0.0618 (10) | 0.0527 (9) | 0.0364 (8) | −0.0254 (8) | −0.0002 (7) | 0.0068 (7) |
N3A | 0.0505 (11) | 0.0467 (10) | 0.0332 (9) | −0.0136 (8) | −0.0043 (8) | 0.0051 (8) |
C4A | 0.0447 (12) | 0.0456 (12) | 0.0349 (11) | 0.0007 (9) | 0.0044 (9) | 0.0064 (10) |
O4A | 0.0781 (12) | 0.0715 (12) | 0.0355 (9) | −0.0075 (9) | 0.0052 (8) | 0.0154 (8) |
C5A | 0.0381 (11) | 0.0419 (11) | 0.0395 (12) | −0.0064 (9) | 0.0017 (9) | 0.0096 (9) |
C6A | 0.0347 (11) | 0.0393 (11) | 0.0377 (11) | −0.0011 (9) | 0.0021 (8) | −0.0001 (9) |
O6A | 0.0488 (9) | 0.0623 (10) | 0.0417 (9) | −0.0160 (8) | −0.0071 (7) | 0.0023 (8) |
N1B | 0.0447 (10) | 0.0444 (10) | 0.0265 (8) | −0.0073 (8) | −0.0003 (7) | 0.0055 (7) |
C2B | 0.0415 (12) | 0.0403 (11) | 0.0298 (10) | −0.0047 (9) | −0.0012 (8) | 0.0043 (9) |
O2B | 0.0601 (10) | 0.0607 (10) | 0.0361 (8) | −0.0262 (8) | 0.0018 (7) | 0.0072 (7) |
N3B | 0.0474 (10) | 0.0423 (10) | 0.0274 (9) | −0.0091 (8) | −0.0004 (7) | 0.0007 (7) |
C4B | 0.0383 (11) | 0.0450 (12) | 0.0348 (11) | 0.0034 (9) | 0.0020 (8) | 0.0083 (9) |
O4B | 0.0663 (11) | 0.0689 (11) | 0.0325 (8) | −0.0049 (8) | 0.0046 (7) | 0.0153 (8) |
C5B | 0.0418 (12) | 0.0503 (13) | 0.0397 (12) | −0.0094 (10) | 0.0000 (9) | 0.0107 (10) |
C6B | 0.0386 (11) | 0.0401 (11) | 0.0371 (11) | −0.0029 (9) | −0.0030 (8) | 0.0045 (9) |
O6B | 0.0634 (11) | 0.0571 (10) | 0.0382 (9) | −0.0184 (8) | −0.0084 (7) | 0.0004 (8) |
O1A | 0.0538 (9) | 0.0550 (9) | 0.0318 (8) | −0.0109 (7) | −0.0038 (6) | 0.0094 (7) |
C1A | 0.0391 (11) | 0.0394 (11) | 0.0372 (11) | 0.0004 (9) | −0.0005 (9) | 0.0043 (9) |
N2A | 0.0634 (13) | 0.0694 (13) | 0.0329 (10) | −0.0085 (10) | −0.0018 (9) | 0.0139 (9) |
N4A | 0.0601 (13) | 0.0554 (12) | 0.0632 (14) | −0.0172 (10) | −0.0134 (10) | 0.0041 (11) |
O1B | 0.0738 (11) | 0.0588 (10) | 0.0310 (8) | −0.0221 (8) | 0.0024 (7) | 0.0042 (7) |
C1B | 0.0490 (13) | 0.0416 (12) | 0.0336 (11) | −0.0022 (9) | −0.0001 (9) | 0.0054 (9) |
N2B | 0.0639 (13) | 0.0503 (12) | 0.0592 (13) | −0.0143 (10) | −0.0100 (10) | 0.0005 (10) |
N4B | 0.0990 (18) | 0.0606 (13) | 0.0318 (11) | −0.0134 (12) | 0.0078 (10) | 0.0092 (10) |
Geometric parameters (Å, º) top
N1A—C6A | 1.357 (2) | C4B—O4B | 1.215 (2) |
N1A—C2A | 1.371 (2) | C4B—C5B | 1.491 (3) |
N1A—H1A | 0.8600 | C5B—C6B | 1.491 (3) |
C2A—O2A | 1.215 (2) | C5B—H5B1 | 0.9700 |
C2A—N3A | 1.368 (3) | C5B—H5B2 | 0.9700 |
N3A—C4A | 1.376 (3) | C6B—O6B | 1.214 (2) |
N3A—H3A | 0.8600 | O1A—C1A | 1.244 (2) |
C4A—O4A | 1.211 (2) | C1A—N2A | 1.327 (3) |
C4A—C5A | 1.485 (3) | C1A—N4A | 1.340 (3) |
C5A—C6A | 1.482 (3) | N2A—H2A1 | 0.8600 |
C5A—H5A1 | 0.9700 | N2A—H2A2 | 0.8600 |
C5A—H5A2 | 0.9700 | N4A—H4A1 | 0.8600 |
C6A—O6A | 1.221 (2) | N4A—H4A2 | 0.8600 |
N1B—C6B | 1.359 (2) | O1B—C1B | 1.243 (2) |
N1B—C2B | 1.362 (2) | C1B—N4B | 1.319 (3) |
N1B—H1B | 0.8600 | C1B—N2B | 1.331 (3) |
C2B—O2B | 1.218 (2) | N2B—H2B1 | 0.8600 |
C2B—N3B | 1.375 (2) | N2B—H2B2 | 0.8600 |
N3B—C4B | 1.367 (3) | N4B—H4B1 | 0.8600 |
N3B—H3B | 0.8600 | N4B—H4B2 | 0.8600 |
| | | |
C6A—N1A—C2A | 125.7 (2) | O4B—C4B—N3B | 120.7 (2) |
C6A—N1A—H1A | 117.2 | O4B—C4B—C5B | 123.0 (2) |
C2A—N1A—H1A | 117.2 | N3B—C4B—C5B | 116.3 (2) |
O2A—C2A—N3A | 122.2 (2) | C4B—C5B—C6B | 117.8 (2) |
O2A—C2A—N1A | 120.7 (2) | C4B—C5B—H5B1 | 107.9 |
N3A—C2A—N1A | 117.2 (2) | C6B—C5B—H5B1 | 107.9 |
C2A—N3A—C4A | 125.8 (2) | C4B—C5B—H5B2 | 107.9 |
C2A—N3A—H3A | 117.1 | C6B—C5B—H5B2 | 107.9 |
C4A—N3A—H3A | 117.1 | H5B1—C5B—H5B2 | 107.2 |
O4A—C4A—N3A | 120.9 (2) | O6B—C6B—N1B | 120.6 (2) |
O4A—C4A—C5A | 122.9 (2) | O6B—C6B—C5B | 122.5 (2) |
N3A—C4A—C5A | 116.2 (2) | N1B—C6B—C5B | 116.9 (2) |
C6A—C5A—C4A | 118.0 (2) | O1A—C1A—N2A | 121.4 (2) |
C6A—C5A—H5A1 | 107.8 | O1A—C1A—N4A | 121.0 (2) |
C4A—C5A—H5A1 | 107.8 | N2A—C1A—N4A | 117.6 (2) |
C6A—C5A—H5A2 | 107.8 | C1A—N2A—H2A1 | 120.0 |
C4A—C5A—H5A2 | 107.8 | C1A—N2A—H2A2 | 120.0 |
H5A1—C5A—H5A2 | 107.1 | H2A1—N2A—H2A2 | 120.0 |
O6A—C6A—N1A | 120.1 (2) | C1A—N4A—H4A1 | 120.0 |
O6A—C6A—C5A | 122.9 (2) | C1A—N4A—H4A2 | 120.0 |
N1A—C6A—C5A | 117.0 (2) | H4A1—N4A—H4A2 | 120.0 |
C6B—N1B—C2B | 125.7 (2) | O1B—C1B—N4B | 120.7 (2) |
C6B—N1B—H1B | 117.2 | O1B—C1B—N2B | 121.2 (2) |
C2B—N1B—H1B | 117.2 | N4B—C1B—N2B | 118.2 (2) |
O2B—C2B—N1B | 121.2 (2) | C1B—N2B—H2B1 | 120.0 |
O2B—C2B—N3B | 121.2 (2) | C1B—N2B—H2B2 | 120.0 |
N1B—C2B—N3B | 117.6 (2) | H2B1—N2B—H2B2 | 120.0 |
C4B—N3B—C2B | 125.5 (2) | C1B—N4B—H4B1 | 120.0 |
C4B—N3B—H3B | 117.3 | C1B—N4B—H4B2 | 120.0 |
C2B—N3B—H3B | 117.3 | H4B1—N4B—H4B2 | 120.0 |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N1A—H1A···O1B | 0.86 | 1.85 | 2.682 (2) | 164 |
N3A—H3A···O2Bi | 0.86 | 2.00 | 2.842 (2) | 166 |
N1B—H1B···O1Aii | 0.86 | 1.87 | 2.718 (2) | 167 |
N3B—H3B···O2Ai | 0.86 | 2.01 | 2.842 (2) | 162 |
N2A—H2A1···O1Biii | 0.86 | 2.24 | 3.077 (2) | 165 |
N2A—H2A2···O4Biv | 0.86 | 2.25 | 3.088 (2) | 164 |
N4B—H4B1···O1Av | 0.86 | 2.21 | 3.055 (3) | 167 |
N4B—H4B2···O4Avi | 0.86 | 2.31 | 3.135 (3) | 160 |
Symmetry codes: (i) −x+1, −y, −z+1; (ii) −x+1, −y+1, −z+2; (iii) x, y+1, z; (iv) −x+1, −y+1, −z+1; (v) x, y−1, z; (vi) x, y, z+1. |
Experimental details
| (I) | (II) | (III) |
Crystal data |
Chemical formula | C5H8N4O4 | C5H8N4O4 | C5H8N4O4 |
Mr | 188.15 | 188.15 | 188.15 |
Crystal system, space group | Monoclinic, P21/c | Monoclinic, Cc | Triclinic, P1 |
Temperature (K) | 293 | 293 | 293 |
a, b, c (Å) | 7.8857 (3), 6.9620 (2), 14.4283 (6) | 15.9423 (7), 5.0984 (3), 10.5534 (5) | 8.1588 (4), 9.1117 (4), 10.9268 (5) |
α, β, γ (°) | 90, 98.027 (1), 90 | 90, 110.570 (2), 90 | 100.248 (2), 91.515 (2), 99.192 (2) |
V (Å3) | 784.36 (5) | 803.09 (7) | 787.82 (6) |
Z | 4 | 4 | 4 |
Radiation type | Mo Kα | Mo Kα | Mo Kα |
µ (mm−1) | 0.14 | 0.14 | 0.14 |
Crystal size (mm) | 0.30 × 0.22 × 0.05 | 0.32 × 0.22 × 0.12 | 0.35 × 0.13 × 0.13 |
|
Data collection |
Diffractometer | KappaCCD diffractometer | KappaCCD diffractometer | KappaCCD diffractometer |
Absorption correction | Multi-scan HKL DENZO and SCALEPACK (Otwinowski & Minor, 1997) | Multi-scan HKL DENZO and SCALEPACK (Otwinowski & Minor, 1997) | Multi-scan HKL DENZO and SCALEPACK (Otwinowski & Minor, 1997) |
Tmin, Tmax | 0.960, 0.993 | 0.958, 0.984 | 0.953, 0.982 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3177, 1775, 1334 | 3691, 1169, 1099 | 4828, 3584, 2380 |
Rint | 0.025 | 0.016 | 0.017 |
(sin θ/λ)max (Å−1) | 0.649 | 0.704 | 0.650 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.043, 0.113, 1.03 | 0.033, 0.083, 1.06 | 0.053, 0.137, 1.03 |
No. of reflections | 1775 | 1169 | 3584 |
No. of parameters | 118 | 118 | 235 |
No. of restraints | 0 | 2 | 0 |
H-atom treatment | H-atom parameters constrained | H-atom parameters constrained | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.21, −0.19 | 0.15, −0.17 | 0.22, −0.19 |
Absolute structure | ? | Flack H D (1983), Acta Cryst. A39, 876-881 | ? |
Absolute structure parameter | ? | 0.00 (3) | ? |
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