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A notable feature of the structure of the title compound, C5H6N4O5, is the presence of four crystallographically independent and essentially planar but otherwise unremarkable mol­ecules in the asymmetric unit. The mol­ecules are distributed as two pairs which differ in conformation from one pair to the other in the orientation of one of the carbo­methoxy substituents relative to the tetrazole ring.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803018282/bt6328sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803018282/bt6328Isup2.hkl
Contains datablock I

CCDC reference: 222890

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](N-C) = 0.013 Å
  • R factor = 0.085
  • wR factor = 0.247
  • Data-to-parameter ratio = 8.2

checkCIF/PLATON results

No syntax errors found



Alert level A PLAT029_ALERT_3_A _diffrn_measured_fraction_theta_full Low ....... 0.89
Author Response: ... The intensity data used in this analysis dates back to the early 1980's when, in this laboratory, it was acceptable practice, in the course of data reduction, to elliminate reflections with negative intensities from the data. Since the crystals are no longer available there is no easy possibility of obtaining a new and more complete set of intensity data.

Alert level B PLAT230_ALERT_2_B Hirshfeld Test Diff for N4D - C3D = 7.89 su PLAT432_ALERT_2_B Short Inter X...Y Contact O1C .. C1B = 2.82 Ang. PLAT432_ALERT_2_B Short Inter X...Y Contact O5B .. C1D = 2.80 Ang.
Alert level C DIFMX01_ALERT_2_C The maximum difference density is > 0.1*ZMAX*0.75 _refine_diff_density_max given = 0.603 Test value = 0.600 DIFMX02_ALERT_1_C The minimum difference density is > 0.1*ZMAX*0.75 The relevant atom site should be identified. PLAT063_ALERT_3_C Crystal Probably too Large for Beam Size ....... 0.64 mm PLAT094_ALERT_2_C Ratio of Maximum / Minimum Residual Density .... 2.12 PLAT125_ALERT_4_C No _symmetry_space_group_name_Hall Given ....... ? PLAT230_ALERT_2_C Hirshfeld Test Diff for N1C - C5C = 5.36 su PLAT230_ALERT_2_C Hirshfeld Test Diff for N3C - N4C = 6.01 su PLAT230_ALERT_2_C Hirshfeld Test Diff for O4D - C3D = 6.20 su PLAT241_ALERT_2_C Check High U(eq) as Compared to Neighbors .... N2C PLAT242_ALERT_2_C Check Low U(eq) as Compared to Neighbors .... C3A PLAT242_ALERT_2_C Check Low U(eq) as Compared to Neighbors .... C3B PLAT242_ALERT_2_C Check Low U(eq) as Compared to Neighbors .... N1C PLAT242_ALERT_2_C Check Low U(eq) as Compared to Neighbors .... C3C PLAT242_ALERT_2_C Check Low U(eq) as Compared to Neighbors .... O4D PLAT242_ALERT_2_C Check Low U(eq) as Compared to Neighbors .... C1D PLAT432_ALERT_2_C Short Inter X...Y Contact O1A .. C3D = 3.01 Ang. PLAT432_ALERT_2_C Short Inter X...Y Contact O3C .. C5A = 2.95 Ang. PLAT432_ALERT_2_C Short Inter X...Y Contact O5C .. C5B = 2.92 Ang. PLAT432_ALERT_2_C Short Inter X...Y Contact O5D .. C3C = 2.92 Ang. PLAT432_ALERT_2_C Short Inter X...Y Contact N3C .. C1A = 2.97 Ang.
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 30.04 From the CIF: _reflns_number_total 4147 Count of symmetry unique reflns 5266 Completeness (_total/calc) 78.75% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 0 Fraction of Friedel pairs measured 0.000 Are heavy atom types Z>Si present no
1 ALERT level A = In general: serious problem 3 ALERT level B = Potentially serious problem 20 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 20 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion

Comment top

The asymmetric unit of the title compound, (I), contains four crystallographically independent molecules. The constituent atoms of all four molecules have been labelled in an identical manner except that the individual molecules are identified by the suffix A, B, C or D. The molecules can be considered in pairs as A with B (Fig. 1) and C with D (Fig. 2), which clearly differ in the orientation of one carbomethoxy group relative to the tetrazole ring. As can be seen in Table 1, which compares the geometric parameters for all four molecules, the only values, aside from the torsion angles about the C3—N4 bond, which are sensitive to the change in conformation are the C3—N4—C5 and C3—N4—N3 angles. Aside from this the bond lengths and angles are fully consistent with the connectivity and bond types indicated in the Scheme.

Experimental top

Compound (I) was prepared by saturating a vigorously stirred ice-cold solution of tetrazol-5-one (Haines et al., 1982) (1.72 g, 0.02 mol) and dry pyridine (3.96 g, 0.05 mol) in anhydrous diethyl ether (100 ml) with gaseous phosgene (COCl2), allowing the solution come to room temperature (298 K) and continuing stirring for a further 10 min before the addition of methanol (10 ml) and further pyridine (3.96 g, 0.05 mol). After filtration removal of solvent from the filtrate furnished solid (I) which was recrystallized from diethyl ether to provide crystals suitable for analysis.

Refinement top

In the final stages of refinement, the H atoms of the methyl groups were introduced in calculated positions, with C—H = 0.96 Å, and allowed for as riding, with Uiso(H) = 1.5Ueq(C). The approximate orientation of the methyl groups was initially determined but not further refined by employing the SHELXL97 (Sheldrick, 1997) AFIX 133 instruction.

Computing details top

Data collection: Nicolet P3 Software (Nicolet, 1980); cell refinement: Nicolet P3 Software; data reduction: RDNIC (Howie, 1980); program(s) used to solve structure: SHELXS90 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: SHELXL97 and PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. Molecule A of (I) showing the labelling scheme and the conformation of the molecule both of which apply also to molecule B. Non-H atoms are shown as 30% probability displacement ellipsoids and H atoms as small circles.
[Figure 2] Fig. 2. The labelling scheme and molecular conformation of molecules C and D of (I). The example shown is molecule C and the representation is otherwise the same as in Fig. 1.
Dimethyl 5-oxo-4,5-dihydro-1,2,3,4-tetrazole-1,4-dicarboxylate top
Crystal data top
C5H6N4O5F(000) = 832
Mr = 202.14Dx = 1.540 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
a = 10.023 (17) ÅCell parameters from 14 reflections
b = 15.92 (3) Åθ = 8.0–11.5°
c = 12.123 (15) ŵ = 0.14 mm1
β = 115.67 (11)°T = 298 K
V = 1744 (5) Å3Block, colourless
Z = 80.64 × 0.50 × 0.34 mm
Data collection top
Nicolet P3
diffractometer
Rint = 0.000
Radiation source: normal-focus sealed tubeθmax = 30.0°, θmin = 1.9°
Graphite monochromatorh = 014
θ–2θ scansk = 022
4147 measured reflectionsl = 1715
4147 independent reflections2 standard reflections every 50 reflections
2144 reflections with I > 2σ(I) intensity decay: none
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)] = 0.085Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.247H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.1438P)2]
where P = (Fo2 + 2Fc2)/3
4147 reflections(Δ/σ)max < 0.001
505 parametersΔρmax = 0.60 e Å3
1 restraintΔρmin = 0.28 e Å3
Crystal data top
C5H6N4O5V = 1744 (5) Å3
Mr = 202.14Z = 8
Monoclinic, P21Mo Kα radiation
a = 10.023 (17) ŵ = 0.14 mm1
b = 15.92 (3) ÅT = 298 K
c = 12.123 (15) Å0.64 × 0.50 × 0.34 mm
β = 115.67 (11)°
Data collection top
Nicolet P3
diffractometer
Rint = 0.000
4147 measured reflections2 standard reflections every 50 reflections
4147 independent reflections intensity decay: none
2144 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.0851 restraint
wR(F2) = 0.247H-atom parameters constrained
S = 1.00Δρmax = 0.60 e Å3
4147 reflectionsΔρmin = 0.28 e Å3
505 parameters
Special details top

Experimental. Scan rates, dependent on prescan intensity (Ip), were in the range 58.6 (Ip>2500) to 5.33 (Ip<150) ° 2θ min−1. Scan widths, dependent on 2θ, were in the range 2.4 to 2.8 ° 2θ. Stationary crystal, stationary counter background counts were taken on either side of the peak each for 25% of the total (peak plus background) count time.

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.

Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane)

− 6.4440 (0.1151) x − 1.5602 (0.1522) y + 11.6765 (0.0611) z = 1.4619 (0.2909)

* 0.0000 (0.0001) O1A * 0.0000 (0.0001) C1A * 0.0000 (0.0000) O2A 0.0874 (0.0323) C2A

Rms deviation of fitted atoms = 0.0000

− 5.9882 (0.0332) x − 3.0427 (0.0656) y + 11.6472 (0.0259) z = 0.3469 (0.0665)

Angle to previous plane (with approximate e.s.d.) = 6.04 (1.17)

* −0.0078 (0.0048) N1A * 0.0016 (0.0051) N2A * 0.0058 (0.0052) N3A * −0.0104 (0.0050) N4A * 0.0107 (0.0046) C5A −0.0049 (0.0127) O5A 0.1748 (0.0150) O1A 0.0645 (0.0130) C1A −0.0623 (0.0148) O2A 0.0181 (0.0216) C2A −0.1502 (0.0163) O3A −0.0176 (0.0133) C3A 0.0278 (0.0138) O4A −0.0376 (0.0209) C4A

Rms deviation of fitted atoms = 0.0080

5.8090 (0.0762) x + 4.8613 (0.2204) y − 11.2994 (0.0835) z = 1.1935 (0.2396)

Angle to previous plane (with approximate e.s.d.) = 6.76 (1.12)

* 0.0000 (0.0001) O3A * 0.0000 (0.0001) C3A * 0.0000 (0.0000) O4A −0.0577 (0.0316) C4A

Rms deviation of fitted atoms = 0.0000

− 5.9186 (0.0871) x + 4.0506 (0.2165) y + 11.4696 (0.0776) z = 6.9000 (0.0530)

Angle to previous plane (with approximate e.s.d.) = 32.51 (1.05)

* 0.0000 (0.0000) O1B * 0.0000 (0.0000) C1B * 0.0000 (0.0000) O2B 0.0031 (0.0328) C2B

Rms deviation of fitted atoms = 0.0000

− 6.1750 (0.0309) x + 3.7824 (0.0594) y + 11.4413 (0.0263) z = 6.8745 (0.0191)

Angle to previous plane (with approximate e.s.d.) = 1.95 (1.18)

* −0.0078 (0.0044) N1B * 0.0074 (0.0045) N2B * −0.0038 (0.0043) N3B * −0.0011 (0.0042) N4B * 0.0052 (0.0043) C5B −0.0522 (0.0118) O5B −0.1097 (0.0141) O1B −0.0799 (0.0128) C1B −0.0357 (0.0130) O2B −0.0208 (0.0208) C2B −0.0034 (0.0140) O3B −0.0618 (0.0122) C3B −0.1327 (0.0137) O4B −0.2493 (0.0214) C4B

Rms deviation of fitted atoms = 0.0056

− 6.4053 (0.1115) x + 2.9317 (0.1350) y + 11.5159 (0.0680) z = 6.6195 (0.0793)

Angle to previous plane (with approximate e.s.d.) = 3.34 (1.22)

* 0.0000 (0.0000) O3B * 0.0000 (0.0000) C3B * 0.0000 (0.0000) O4B −0.1085 (0.0321) C4B

Rms deviation of fitted atoms = 0.0000

− 9.0321 (0.0766) x − 6.0281 (0.1392) y + 7.0408 (0.1553) z = 2.8781 (0.0679)

Angle to previous plane (with approximate e.s.d.) = 48.40 (1.15)

* 0.0000 (0.0001) O1C * 0.0000 (0.0001) C1C * 0.0000 (0.0000) O2C 0.0032 (0.0369) C2C

Rms deviation of fitted atoms = 0.0000

− 9.0030 (0.0239) x − 6.4164 (0.0561) y + 6.6345 (0.0419) z = 2.4307 (0.0491)

Angle to previous plane (with approximate e.s.d.) = 2.49 (1.16)

* −0.0005 (0.0044) N1C * 0.0044 (0.0053) N2C * −0.0061 (0.0049) N3C * 0.0055 (0.0045) N4C * −0.0033 (0.0043) C5C −0.0082 (0.0118) O5C 0.0192 (0.0150) O1C −0.0344 (0.0131) C1C −0.0675 (0.0140) O2C −0.0322 (0.0212) C2C −0.1003 (0.0151) O3C −0.0165 (0.0128) C3C 0.0586 (0.0147) O4C 0.0079 (0.0246) C4C

Rms deviation of fitted atoms = 0.0044

− 8.9913 (0.0896) x − 5.8990 (0.2159) y + 7.3431 (0.1009) z = 3.3458 (0.0902)

Angle to previous plane (with approximate e.s.d.) = 4.19 (1.39)

* 0.0000 (0.0002) O3C * 0.0000 (0.0001) C3C * 0.0000 (0.0000) O4C −0.0222 (0.0375) C4C

Rms deviation of fitted atoms = 0.0000

− 2.4950(0.1313) x + 12.5808(0.1569) y − 4.8133(0.0532) z = 10.0608(0.2448)

Angle to previous plane (with approximate e.s.d.) = 78.21 (1.02)

* 0.0000 (0.0000) O1D * 0.0000 (0.0000) C1D * 0.0000 (0.0000) O2D −0.1472 (0.0319) C2D

Rms deviation of fitted atoms = 0.0000

− 2.7569 (0.0437) x + 11.2720 (0.0536) y − 5.6638 (0.0503) z = 8.5867 (0.0560)

Angle to previous plane (with approximate e.s.d.) = 7.16 (1.25)

* 0.0137 (0.0050) N1D * −0.0084 (0.0058) N2D * −0.0008 (0.0056) N3D * 0.0095 (0.0049) N4D * −0.0140 (0.0046) C5D 0.0056 (0.0141) O5D −0.1671 (0.0165) O1D −0.1837 (0.0137) C1D −0.3189 (0.0159) O2D −0.6215 (0.0234) C2D −0.1467 (0.0167) O3D −0.1003 (0.0140) C3D −0.1451 (0.0153) O4D −0.2414 (0.0268) C4D

Rms deviation of fitted atoms = 0.0104

− 3.1562 (0.1021) x + 10.1842 (0.2447) y − 6.0086 (0.0741) z = 7.5299 (0.2090)

Angle to previous plane (with approximate e.s.d.) = 5.38 (1.75)

* 0.0000 (0.0000) O3D * 0.0000 (0.0000) C3D * 0.0000 (0.0000) O4D 0.0456 (0.0378) C4D

Rms deviation of fitted atoms = 0.0000

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
N1A0.7832 (7)0.9408 (5)0.6776 (6)0.0612 (18)
N2A0.6546 (9)0.9887 (6)0.6248 (8)0.078 (2)
N3A0.5497 (8)0.9415 (6)0.5589 (7)0.074 (2)
N4A0.6056 (7)0.8618 (5)0.5654 (6)0.0603 (18)
C5A0.7574 (9)0.8570 (6)0.6440 (8)0.061 (2)
O5A0.8408 (6)0.7995 (4)0.6705 (6)0.0744 (17)
C1A0.9190 (10)0.9760 (7)0.7628 (8)0.068 (2)
O1A1.0264 (7)0.9336 (5)0.8164 (6)0.088 (2)
O2A0.9074 (8)1.0579 (5)0.7673 (6)0.086 (2)
C2A1.0365 (13)1.1007 (9)0.8518 (12)0.113 (5)
H1A1.03651.10190.93090.170*
H2A1.03671.15710.82400.170*
H3A1.12331.07180.85730.170*
C3A0.5176 (10)0.7925 (6)0.5014 (8)0.063 (2)
O3A0.5691 (8)0.7251 (5)0.4989 (7)0.099 (2)
O4A0.3804 (7)0.8155 (5)0.4408 (7)0.083 (2)
C4A0.2790 (10)0.7521 (7)0.3664 (9)0.080 (3)
H4A0.33000.71380.33680.119*
H5A0.19920.77820.29830.119*
H6A0.24000.72190.41460.119*
N1B0.0776 (7)0.2916 (4)0.5457 (6)0.0555 (16)
N2B0.0287 (8)0.2117 (6)0.5470 (7)0.066 (2)
N3B0.1341 (8)0.1651 (5)0.6183 (7)0.0616 (17)
N4B0.2579 (7)0.2169 (4)0.6682 (6)0.0497 (15)
C5B0.2250 (9)0.2980 (6)0.6242 (7)0.057 (2)
O5B0.3049 (7)0.3571 (4)0.6428 (6)0.0796 (18)
C1B0.0130 (10)0.3554 (6)0.4693 (7)0.063 (2)
O1B0.0323 (8)0.4233 (5)0.4687 (6)0.0846 (19)
O2B0.1487 (7)0.3266 (5)0.4095 (6)0.0798 (19)
C2B0.2541 (11)0.3915 (9)0.3325 (10)0.100 (4)
H1B0.21620.44620.36330.151*
H2B0.34800.38370.33450.151*
H3B0.26640.38640.24970.151*
C3B0.3968 (9)0.1853 (5)0.7484 (7)0.0551 (19)
O3B0.5033 (7)0.2293 (5)0.7964 (6)0.087 (2)
O4B0.3894 (7)0.1054 (4)0.7646 (6)0.0811 (19)
C4B0.5287 (13)0.0650 (9)0.8429 (11)0.103 (4)
H4B0.60090.07690.81290.154*
H5B0.51410.00540.84270.154*
H6B0.56300.08600.92490.154*
N1C0.0401 (6)0.4396 (4)0.8459 (6)0.0488 (14)
N2C0.0876 (10)0.4835 (6)0.9535 (8)0.083 (2)
N3C0.1773 (9)0.4487 (7)1.0399 (7)0.081 (2)
N4C0.1993 (7)0.3660 (5)0.9916 (7)0.0633 (18)
C5C0.1171 (9)0.3594 (6)0.8724 (9)0.060 (2)
O5C0.1068 (8)0.3059 (4)0.8059 (6)0.0764 (17)
C1C0.0599 (11)0.4690 (7)0.7335 (10)0.078 (3)
O1C0.1010 (8)0.4236 (5)0.6419 (6)0.095 (2)
O2C0.0997 (7)0.5406 (5)0.7437 (9)0.105 (3)
C2C0.2199 (14)0.5770 (8)0.6213 (11)0.106 (4)
H1C0.21470.54860.55340.159*
H2C0.20250.63600.61670.159*
H3C0.31620.56900.61850.159*
C3C0.3038 (10)0.3144 (6)1.0802 (10)0.069 (2)
O3C0.3747 (8)0.3341 (6)1.1829 (7)0.102 (3)
O4C0.3064 (7)0.2431 (5)1.0261 (7)0.093 (2)
C4C0.4150 (16)0.1835 (9)1.1081 (14)0.145 (6)
H4C0.51300.20431.12970.217*
H5C0.40280.13021.06770.217*
H6C0.40050.17671.18090.217*
N1D0.4752 (7)0.9605 (5)0.1618 (6)0.0606 (18)
N2D0.3769 (10)0.9618 (6)0.2161 (9)0.091 (3)
N3D0.2763 (9)0.9109 (7)0.1625 (8)0.090 (3)
N4D0.3025 (7)0.8716 (5)0.0696 (7)0.0665 (19)
C5D0.4309 (9)0.9005 (6)0.0688 (7)0.065 (2)
O5D0.4863 (9)0.8831 (6)0.0038 (7)0.099 (2)
C1D0.6122 (9)1.0038 (5)0.2161 (8)0.059 (2)
O1D0.6957 (7)1.0033 (5)0.1716 (6)0.089 (2)
O2D0.6190 (7)1.0424 (4)0.3135 (7)0.0860 (19)
C2D0.7561 (14)1.0860 (8)0.3869 (12)0.130 (6)
H1D0.83511.04590.42120.195*
H2D0.74621.11590.45170.195*
H3D0.77771.12490.33630.195*
C3D0.1946 (13)0.8050 (7)0.0091 (9)0.079 (3)
O3D0.0990 (9)0.7898 (6)0.0335 (9)0.110 (3)
O4D0.2383 (7)0.7726 (4)0.0689 (6)0.0849 (19)
C4D0.1302 (17)0.7034 (12)0.1370 (13)0.144 (6)
H4D0.12700.66290.07940.215*
H5D0.16160.67630.19250.215*
H6D0.03340.72700.18210.215*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.052 (4)0.067 (5)0.068 (4)0.009 (4)0.029 (3)0.008 (4)
N2A0.070 (5)0.073 (5)0.092 (6)0.026 (4)0.036 (5)0.020 (5)
N3A0.057 (4)0.074 (5)0.074 (5)0.021 (4)0.014 (4)0.001 (4)
N4A0.056 (4)0.068 (5)0.052 (4)0.015 (4)0.019 (3)0.011 (3)
C5A0.062 (5)0.066 (6)0.062 (5)0.005 (5)0.034 (4)0.009 (4)
O5A0.064 (3)0.057 (3)0.097 (4)0.027 (3)0.031 (3)0.015 (3)
C1A0.063 (5)0.087 (8)0.059 (5)0.003 (5)0.032 (4)0.010 (5)
O1A0.066 (4)0.096 (6)0.091 (5)0.022 (4)0.024 (4)0.011 (4)
O2A0.083 (5)0.066 (5)0.093 (5)0.005 (3)0.023 (4)0.012 (4)
C2A0.097 (8)0.105 (9)0.125 (9)0.042 (8)0.035 (7)0.023 (8)
C3A0.067 (5)0.067 (6)0.049 (4)0.015 (5)0.020 (4)0.025 (4)
O3A0.082 (5)0.067 (5)0.119 (6)0.023 (4)0.016 (4)0.016 (4)
O4A0.061 (4)0.087 (5)0.103 (5)0.014 (4)0.037 (4)0.005 (4)
C4A0.069 (6)0.085 (7)0.087 (6)0.008 (5)0.035 (5)0.003 (6)
N1B0.055 (4)0.053 (4)0.060 (4)0.009 (3)0.027 (3)0.004 (3)
N2B0.060 (4)0.079 (5)0.065 (4)0.018 (4)0.032 (4)0.009 (4)
N3B0.055 (4)0.055 (4)0.077 (4)0.004 (3)0.030 (4)0.000 (4)
N4B0.050 (4)0.043 (4)0.060 (4)0.010 (3)0.028 (3)0.010 (3)
C5B0.062 (5)0.063 (5)0.051 (4)0.025 (4)0.027 (4)0.013 (4)
O5B0.070 (4)0.068 (4)0.093 (5)0.018 (4)0.028 (3)0.012 (4)
C1B0.071 (5)0.067 (6)0.053 (5)0.016 (5)0.029 (4)0.001 (4)
O1B0.096 (5)0.079 (5)0.087 (4)0.004 (4)0.047 (4)0.002 (4)
O2B0.067 (4)0.093 (5)0.073 (4)0.002 (4)0.024 (3)0.006 (4)
C2B0.064 (6)0.133 (11)0.091 (7)0.029 (7)0.021 (5)0.025 (7)
C3B0.055 (5)0.052 (5)0.061 (5)0.005 (4)0.028 (4)0.016 (4)
O3B0.062 (4)0.089 (5)0.090 (4)0.015 (4)0.014 (3)0.020 (4)
O4B0.070 (4)0.066 (5)0.095 (4)0.007 (3)0.025 (4)0.008 (4)
C4B0.086 (7)0.102 (9)0.097 (8)0.012 (6)0.017 (6)0.010 (7)
N1C0.047 (3)0.042 (3)0.056 (4)0.003 (3)0.020 (3)0.006 (3)
N2C0.089 (6)0.090 (6)0.078 (6)0.005 (5)0.046 (5)0.003 (5)
N3C0.075 (5)0.114 (7)0.051 (4)0.022 (5)0.024 (4)0.009 (5)
N4C0.057 (4)0.058 (4)0.076 (5)0.004 (4)0.029 (4)0.003 (4)
C5C0.053 (4)0.062 (6)0.070 (6)0.017 (4)0.030 (4)0.000 (5)
O5C0.094 (4)0.061 (4)0.079 (4)0.005 (3)0.041 (3)0.007 (4)
C1C0.076 (6)0.078 (7)0.091 (7)0.012 (6)0.046 (6)0.006 (6)
O1C0.107 (5)0.098 (5)0.068 (4)0.014 (4)0.027 (4)0.001 (4)
O2C0.067 (4)0.069 (5)0.176 (8)0.005 (4)0.049 (5)0.015 (5)
C2C0.119 (9)0.082 (8)0.115 (8)0.034 (7)0.049 (7)0.055 (7)
C3C0.059 (5)0.063 (6)0.086 (7)0.002 (5)0.032 (5)0.012 (6)
O3C0.081 (4)0.145 (8)0.076 (5)0.010 (5)0.029 (4)0.001 (5)
O4C0.074 (4)0.070 (5)0.106 (5)0.006 (4)0.011 (4)0.023 (4)
C4C0.128 (12)0.094 (10)0.168 (14)0.060 (9)0.022 (10)0.041 (10)
N1D0.058 (4)0.062 (4)0.066 (4)0.016 (3)0.031 (3)0.000 (3)
N2D0.070 (5)0.097 (7)0.118 (7)0.011 (5)0.052 (5)0.022 (6)
N3D0.075 (5)0.109 (7)0.099 (6)0.015 (5)0.049 (5)0.001 (6)
N4D0.052 (4)0.056 (4)0.077 (5)0.010 (4)0.015 (4)0.011 (4)
C5D0.062 (5)0.078 (6)0.056 (5)0.023 (5)0.028 (4)0.009 (4)
O5D0.105 (5)0.129 (7)0.086 (4)0.017 (5)0.062 (4)0.010 (5)
C1D0.049 (4)0.045 (4)0.075 (5)0.000 (4)0.021 (4)0.003 (4)
O1D0.069 (4)0.109 (6)0.096 (5)0.005 (4)0.041 (4)0.019 (4)
O2D0.087 (4)0.058 (4)0.103 (5)0.004 (3)0.032 (4)0.015 (4)
C2D0.120 (9)0.059 (7)0.129 (10)0.004 (7)0.023 (8)0.027 (7)
C3D0.094 (7)0.070 (7)0.065 (6)0.055 (6)0.027 (5)0.017 (5)
O3D0.095 (5)0.095 (5)0.152 (7)0.012 (5)0.065 (5)0.022 (5)
O4D0.081 (4)0.063 (4)0.091 (5)0.003 (4)0.019 (4)0.003 (4)
C4D0.135 (12)0.133 (13)0.122 (11)0.014 (10)0.017 (9)0.032 (10)
Geometric parameters (Å, º) top
N1A—C5A1.387 (12)N1C—N2C1.370 (11)
N1A—N2A1.392 (10)N1C—C1C1.377 (12)
N1A—C1A1.419 (12)N1C—C5C1.455 (12)
N2A—N3A1.257 (12)N2C—N3C1.182 (11)
N3A—N4A1.376 (11)N3C—N4C1.496 (13)
N4A—C5A1.404 (11)N4C—C5C1.322 (12)
N4A—C3A1.416 (13)N4C—C3C1.397 (12)
C5A—O5A1.187 (10)C5C—O5C1.146 (11)
C1A—O1A1.197 (11)C1C—O2C1.232 (13)
C1A—O2A1.313 (12)C1C—O1C1.237 (13)
O2A—C2A1.428 (13)O2C—C2C1.563 (13)
C2A—H1A0.9600C2C—H1C0.9600
C2A—H2A0.9600C2C—H2C0.9600
C2A—H3A0.9600C2C—H3C0.9600
C3A—O3A1.197 (12)C3C—O3C1.177 (12)
C3A—O4A1.300 (11)C3C—O4C1.317 (12)
O4A—C4A1.439 (12)O4C—C4C1.462 (13)
C4A—H4A0.9600C4C—H4C0.9600
C4A—H5A0.9600C4C—H5C0.9600
C4A—H6A0.9600C4C—H6C0.9600
N1B—N2B1.366 (11)N1D—C5D1.395 (11)
N1B—C5B1.372 (10)N1D—N2D1.403 (11)
N1B—C1B1.409 (12)N1D—C1D1.418 (11)
N2B—N3B1.273 (11)N2D—N3D1.235 (12)
N3B—N4B1.391 (9)N3D—N4D1.410 (11)
N4B—C5B1.382 (12)N4D—C5D1.370 (12)
N4B—C3B1.402 (11)N4D—C3D1.463 (14)
C5B—O5B1.191 (10)C5D—O5D1.177 (10)
C1B—O1B1.174 (12)C1D—O1D1.176 (10)
C1B—O2B1.315 (11)C1D—O2D1.307 (11)
O2B—C2B1.484 (13)O2D—C2D1.449 (13)
C2B—H1B0.9600C2D—H1D0.9600
C2B—H2B0.9600C2D—H2D0.9600
C2B—H3B0.9600C2D—H3D0.9600
C3B—O3B1.196 (10)C3D—O3D1.145 (12)
C3B—O4B1.295 (11)C3D—O4D1.309 (11)
O4B—C4B1.455 (12)O4D—C4D1.515 (18)
C4B—H4B0.9600C4D—H4D0.9600
C4B—H5B0.9600C4D—H5D0.9600
C4B—H6B0.9600C4D—H6D0.9600
C5A—N1A—N2A112.0 (8)N2C—N1C—C1C124.9 (8)
C5A—N1A—C1A126.3 (8)N2C—N1C—C5C107.7 (7)
N2A—N1A—C1A121.6 (8)C1C—N1C—C5C127.3 (8)
N3A—N2A—N1A108.6 (8)N3C—N2C—N1C115.0 (9)
N2A—N3A—N4A107.9 (7)N2C—N3C—N4C104.5 (7)
N3A—N4A—C5A112.6 (8)C5C—N4C—C3C134.3 (9)
N3A—N4A—C3A123.1 (7)C5C—N4C—N3C111.7 (8)
C5A—N4A—C3A124.3 (7)C3C—N4C—N3C113.9 (8)
O5A—C5A—N1A130.0 (8)O5C—C5C—N4C130.7 (9)
O5A—C5A—N4A130.9 (9)O5C—C5C—N1C128.3 (8)
N1A—C5A—N4A99.0 (7)N4C—C5C—N1C101.1 (8)
O1A—C1A—O2A127.8 (10)O2C—C1C—O1C129.4 (11)
O1A—C1A—N1A121.8 (10)O2C—C1C—N1C110.1 (10)
O2A—C1A—N1A110.4 (8)O1C—C1C—N1C120.4 (10)
C1A—O2A—C2A115.8 (9)C1C—O2C—C2C113.5 (10)
O2A—C2A—H1A109.5O2C—C2C—H1C109.5
O2A—C2A—H2A109.5O2C—C2C—H2C109.5
H1A—C2A—H2A109.5H1C—C2C—H2C109.5
O2A—C2A—H3A109.5O2C—C2C—H3C109.5
H1A—C2A—H3A109.5H1C—C2C—H3C109.5
H2A—C2A—H3A109.5H2C—C2C—H3C109.5
O3A—C3A—O4A126.9 (10)O3C—C3C—O4C128.5 (10)
O3A—C3A—N4A122.7 (8)O3C—C3C—N4C124.4 (10)
O4A—C3A—N4A110.2 (8)O4C—C3C—N4C107.1 (9)
C3A—O4A—C4A116.3 (8)C3C—O4C—C4C113.0 (9)
O4A—C4A—H4A109.5O4C—C4C—H4C109.5
O4A—C4A—H5A109.5O4C—C4C—H5C109.5
H4A—C4A—H5A109.5H4C—C4C—H5C109.5
O4A—C4A—H6A109.5O4C—C4C—H6C109.5
H4A—C4A—H6A109.5H4C—C4C—H6C109.5
H5A—C4A—H6A109.5H5C—C4C—H6C109.5
N2B—N1B—C5B110.2 (7)C5D—N1D—N2D110.2 (8)
N2B—N1B—C1B123.2 (7)C5D—N1D—C1D127.9 (7)
C5B—N1B—C1B126.6 (7)N2D—N1D—C1D120.7 (7)
N3B—N2B—N1B110.7 (7)N3D—N2D—N1D108.9 (8)
N2B—N3B—N4B105.8 (7)N2D—N3D—N4D108.6 (8)
C5B—N4B—N3B111.6 (6)C5D—N4D—N3D110.9 (8)
C5B—N4B—C3B127.0 (7)C5D—N4D—C3D137.1 (9)
N3B—N4B—C3B121.3 (7)N3D—N4D—C3D111.7 (8)
O5B—C5B—N1B128.6 (9)O5D—C5D—N4D130.0 (10)
O5B—C5B—N4B129.5 (8)O5D—C5D—N1D128.6 (9)
N1B—C5B—N4B101.7 (7)N4D—C5D—N1D101.4 (7)
O1B—C1B—O2B128.9 (10)O1D—C1D—O2D130.5 (9)
O1B—C1B—N1B121.8 (8)O1D—C1D—N1D121.5 (8)
O2B—C1B—N1B109.2 (8)O2D—C1D—N1D108.0 (8)
C1B—O2B—C2B112.9 (8)C1D—O2D—C2D116.4 (9)
O2B—C2B—H1B109.5O2D—C2D—H1D109.5
O2B—C2B—H2B109.5O2D—C2D—H2D109.5
H1B—C2B—H2B109.5H1D—C2D—H2D109.5
O2B—C2B—H3B109.5O2D—C2D—H3D109.5
H1B—C2B—H3B109.5H1D—C2D—H3D109.5
H2B—C2B—H3B109.5H2D—C2D—H3D109.5
O3B—C3B—O4B126.9 (9)O3D—C3D—O4D133.0 (12)
O3B—C3B—N4B122.4 (8)O3D—C3D—N4D122.9 (10)
O4B—C3B—N4B110.7 (7)O4D—C3D—N4D104.0 (10)
C3B—O4B—C4B115.6 (8)C3D—O4D—C4D107.2 (10)
O4B—C4B—H4B109.5O4D—C4D—H4D109.5
O4B—C4B—H5B109.5O4D—C4D—H5D109.5
H4B—C4B—H5B109.5H4D—C4D—H5D109.5
O4B—C4B—H6B109.5O4D—C4D—H6D109.5
H4B—C4B—H6B109.5H4D—C4D—H6D109.5
H5B—C4B—H6B109.5H5D—C4D—H6D109.5
C5A—N1A—N2A—N3A0.9 (10)C1C—N1C—N2C—N3C177.8 (8)
C1A—N1A—N2A—N3A176.3 (7)C5C—N1C—N2C—N3C0.6 (10)
N1A—N2A—N3A—N4A0.4 (10)N1C—N2C—N3C—N4C1.1 (10)
N2A—N3A—N4A—C5A1.6 (10)N2C—N3C—N4C—C5C1.2 (9)
N2A—N3A—N4A—C3A179.7 (7)N2C—N3C—N4C—C3C179.5 (7)
N2A—N1A—C5A—O5A179.1 (9)C3C—N4C—C5C—O5C1.6 (16)
C1A—N1A—C5A—O5A5.8 (14)N3C—N4C—C5C—O5C179.4 (9)
N2A—N1A—C5A—N4A1.7 (8)C3C—N4C—C5C—N1C178.6 (8)
C1A—N1A—C5A—N4A176.8 (7)N3C—N4C—C5C—N1C0.8 (8)
N3A—N4A—C5A—O5A179.3 (9)N2C—N1C—C5C—O5C180.0 (9)
C3A—N4A—C5A—O5A2.0 (14)C1C—N1C—C5C—O5C1.6 (13)
N3A—N4A—C5A—N1A2.0 (9)N2C—N1C—C5C—N4C0.2 (8)
C3A—N4A—C5A—N1A179.3 (7)C1C—N1C—C5C—N4C178.5 (7)
C5A—N1A—C1A—O1A1.3 (13)N2C—N1C—C1C—O2C0.4 (12)
N2A—N1A—C1A—O1A173.3 (8)C5C—N1C—C1C—O2C177.7 (7)
C5A—N1A—C1A—O2A176.1 (8)N2C—N1C—C1C—O1C177.0 (8)
N2A—N1A—C1A—O2A9.3 (11)C5C—N1C—C1C—O1C4.9 (13)
O1A—C1A—O2A—C2A3.9 (14)O1C—C1C—O2C—C2C0.1 (15)
N1A—C1A—O2A—C2A178.9 (8)N1C—C1C—O2C—C2C177.0 (7)
N3A—N4A—C3A—O3A173.2 (9)C5C—N4C—C3C—O3C174.3 (9)
C5A—N4A—C3A—O3A8.2 (13)N3C—N4C—C3C—O3C3.4 (13)
N3A—N4A—C3A—O4A1.6 (11)C5C—N4C—C3C—O4C5.1 (13)
C5A—N4A—C3A—O4A176.9 (7)N3C—N4C—C3C—O4C177.2 (7)
O3A—C3A—O4A—C4A2.6 (14)O3C—C3C—O4C—C4C0.9 (16)
N4A—C3A—O4A—C4A177.2 (7)N4C—C3C—O4C—C4C178.4 (9)
C5B—N1B—N2B—N3B1.6 (9)C5D—N1D—N2D—N3D2.2 (11)
C1B—N1B—N2B—N3B176.1 (7)C1D—N1D—N2D—N3D170.8 (8)
N1B—N2B—N3B—N4B1.1 (8)N1D—N2D—N3D—N4D0.7 (11)
N2B—N3B—N4B—C5B0.3 (8)N2D—N3D—N4D—C5D1.0 (11)
N2B—N3B—N4B—C3B177.6 (7)N2D—N3D—N4D—C3D175.0 (8)
N2B—N1B—C5B—O5B176.9 (8)N3D—N4D—C5D—O5D178.8 (10)
C1B—N1B—C5B—O5B0.7 (13)C3D—N4D—C5D—O5D9.5 (16)
N2B—N1B—C5B—N4B1.3 (8)N3D—N4D—C5D—N1D2.2 (8)
C1B—N1B—C5B—N4B176.4 (7)C3D—N4D—C5D—N1D174.0 (8)
N3B—N4B—C5B—O5B176.2 (8)N2D—N1D—C5D—O5D179.2 (10)
C3B—N4B—C5B—O5B0.9 (13)C1D—N1D—C5D—O5D13.2 (15)
N3B—N4B—C5B—N1B0.6 (8)N2D—N1D—C5D—N4D2.6 (9)
C3B—N4B—C5B—N1B176.5 (7)C1D—N1D—C5D—N4D170.2 (7)
N2B—N1B—C1B—O1B178.9 (8)C5D—N1D—C1D—O1D13.6 (13)
C5B—N1B—C1B—O1B1.6 (13)N2D—N1D—C1D—O1D180.0 (8)
N2B—N1B—C1B—O2B4.2 (11)C5D—N1D—C1D—O2D168.6 (8)
C5B—N1B—C1B—O2B178.4 (7)N2D—N1D—C1D—O2D2.2 (10)
O1B—C1B—O2B—C2B0.1 (14)O1D—C1D—O2D—C2D6.5 (14)
N1B—C1B—O2B—C2B176.4 (7)N1D—C1D—O2D—C2D176.0 (8)
C5B—N4B—C3B—O3B6.4 (12)C5D—N4D—C3D—O3D173.9 (10)
N3B—N4B—C3B—O3B176.7 (8)N3D—N4D—C3D—O3D2.2 (12)
C5B—N4B—C3B—O4B176.0 (7)C5D—N4D—C3D—O4D5.1 (12)
N3B—N4B—C3B—O4B0.8 (10)N3D—N4D—C3D—O4D176.9 (7)
O3B—C3B—O4B—C4B4.7 (14)O3D—C3D—O4D—C4D1.8 (15)
N4B—C3B—O4B—C4B177.9 (8)N4D—C3D—O4D—C4D179.3 (8)

Experimental details

Crystal data
Chemical formulaC5H6N4O5
Mr202.14
Crystal system, space groupMonoclinic, P21
Temperature (K)298
a, b, c (Å)10.023 (17), 15.92 (3), 12.123 (15)
β (°) 115.67 (11)
V3)1744 (5)
Z8
Radiation typeMo Kα
µ (mm1)0.14
Crystal size (mm)0.64 × 0.50 × 0.34
Data collection
DiffractometerNicolet P3
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
4147, 4147, 2144
Rint0.000
(sin θ/λ)max1)0.704
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.085, 0.247, 1.00
No. of reflections4147
No. of parameters505
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.60, 0.28

Computer programs: Nicolet P3 Software (Nicolet, 1980), Nicolet P3 Software, RDNIC (Howie, 1980), SHELXS90 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), ORTEP-3 for Windows (Farrugia, 1997), SHELXL97 and PLATON (Spek, 2003).

Comparison Table of bond lengths and angles (Å, °) for molecules A, B, C and D of (I) top
C1—N1—N2121.6 (8)123.2 (7)124.9 (8)120.7 (7)
O1—C1—N1121.8 (10)121.8 (8)120.4 (10)121.5 (8)
O2—C1—N1110.4 (8)109.2 (8)110.1 (10)108.0 (8)
O1—C1—O2127.8 (10)128.9 (10)129.4 (11)130.5 (9)
C2—O2—C1115.8 (9)112.9 (8)113.5 (10)116.4 (9)
C3—N4—C5124.3 (7)127.0 (7)134.3 (9)137.1 (9)
C3—N4—N3123.1 (7)121.3 (7)113.9 (8)111.7 (8)
O3—C3—N4122.7 (8)122.4 (8)124.4 (10)122.9 (10)
O4—C3—N4110.2 (8)110.7 (7)107.1 (9)104.0 (10)
O3—C3—O4126.9 (10)126.9 (9)128.5 (10)133.0 (12)
C4—O4—C3116.3 (8)115.6 (8)113.0 (9)107.2 (10)
O1—C1—N1—C5-1.3 (13)-1.6 (13)4.9 (13)13.6 (13)
O1—C1—N1—N2173.3 (8)-178.9 (8)-177.0 (8)-180.0 (8)
O2—C1—N1—C5176.1 (8)-178.4 (7)-177.7 (7)-168.6 (8)
O2—C1—N1—N2-9.3 (11)4.2 (11)0.4 (12)-2.2 (10)
O3—C3—N4—C5-8.2 (13)6.4 (12)174.3 (9)173.9 (10)
O3—C3—N4—N3173.2 (9)-176.7 (8)-3.4 (13)2.2 (12)
O4—C3—N4—C5176.9 (7)-176.0 (7)-5.1 (13)-5.1 (12)
O4—C3—N4—N3-1.6 (11)0.8 (10)177.2 (7)-176.9 (7)
 

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