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The title compound, C14H10N6O2·H2O, has inherent hydrogen-bonding sites that allow for a very tight packing structure. There are two organic mol­ecules and two water mol­ecules in the asymmetric unit, which are connected by N—H...O hydrogen bonds. The O atoms come from both water and urea, giving rise to a complex three-dimensional mol­ecular cluster. Features associated with the hydrogen bonding and solid-state emission and excitation spectra are discussed in the supplementary material.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807034198/fl2142sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807034198/fl2142Isup2.hkl
Contains datablock I

CCDC reference: 657789

Key indicators

  • Single-crystal X-ray study
  • T = 150 K
  • Mean [sigma](C-C)= 0.002 Å
  • R factor = 0.036
  • wR factor = 0.092
  • Data-to-parameter ratio = 12.0

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Comment top

The title compound (Scheme 1) has been snythesized before and included in many different metal systems as a ligand. Crystal structures of some of the complexes have been reported. (Deshpande et al., 2006; Elemans et al., 1998; Elemans et al., 2002; Kurth et al., 2001). To date the structure of the unbound ligand has not been solved. According to the crystal structure (Figure 1), each molecule forms three hydrogen bonds; one with another molecule and two with two different water molecules. Each water molecule forms four hydrogen bonds; two to urea NH groups, one to a urea ketone and one to a bipyridine nitrogen atom. The bipyridine rings are twisted out of plane which causes the urea groups to also twist. The hydrogen bonds of interest occur between H12—O1, H3—O2s, and H10—O2s, Table 1; these three bonds form a ring that gives stability to the molecule in the packing arrangement.

Photophysical Processes: The emission spectra and excitation spectra were determined in the solid state. The excitation spectra shows one major transition at 375 nm and is assigned to a π π* transition within the bipyridine moiety. The emission spectra and excitation spectra have good overlap. The emission spectra reveals very nice vibrational structure. The three major peaks are located at 405, 426, and 453 nm. The vibrational band spacing was found to be 1300 cm-1.

Related literature top

Synthesis: Deshpande et al. (2006); Elemans et al. (1998); Elemans et al. (2002); Kurth et al. (2001).

For related literature, see: Farrugia (1997).

Experimental top

1,10-phenanthroline-5,6-dione was prepared as previously reported. Urea was purchased from Aldrich and used as received. Toluene and glacial acetic acid were purchased from Fisher Scientific Company and used as received. 200 proof ethanol was purchased from AAPER alcohol and used without further purification.

Physical Measurements: Fluorescence measurements were obtained with a Spex Fluorolog 2:1:2 spectrophotometer. The crystals were placed between two glass slides and then lined up within the excitation chamber using a mount. The slit widths were maintained at 1.4 mm and the light intensity collected with a Hamamatsu R928 photomultiplier tube with a 900 V bias. Data was gathered at intervals of 0.1 nanometers and integrated for 0.1 s. The data was processed using the Origin 6.1 suite of software and massaged to give smoother spectra without loss of spectral features.

The title molecule was prepared and purified as previously reported. Crystals were obtained by refluxing the title molecule in glacial acetic acid and then allowing the solution to cool. Crystals suitable for X-Ray analysis formed on the bottom of the flask. Elemental Anyalysis: Anal. for C14H10N6O2.2H2O: %C, 50.90; %H, 4.24; %N, 25.45; Found. %C, 50.90; %H, 3.60; %N, 24.77.

Refinement top

All non-H atoms were refined using anisotropic displacement parameters. Hydrogen atoms on the solvate water molecule and urea N atoms were refined using isotropic displacement parameters. All other H atoms were included at idealized positions and not refined.

Structure description top

The title compound (Scheme 1) has been snythesized before and included in many different metal systems as a ligand. Crystal structures of some of the complexes have been reported. (Deshpande et al., 2006; Elemans et al., 1998; Elemans et al., 2002; Kurth et al., 2001). To date the structure of the unbound ligand has not been solved. According to the crystal structure (Figure 1), each molecule forms three hydrogen bonds; one with another molecule and two with two different water molecules. Each water molecule forms four hydrogen bonds; two to urea NH groups, one to a urea ketone and one to a bipyridine nitrogen atom. The bipyridine rings are twisted out of plane which causes the urea groups to also twist. The hydrogen bonds of interest occur between H12—O1, H3—O2s, and H10—O2s, Table 1; these three bonds form a ring that gives stability to the molecule in the packing arrangement.

Photophysical Processes: The emission spectra and excitation spectra were determined in the solid state. The excitation spectra shows one major transition at 375 nm and is assigned to a π π* transition within the bipyridine moiety. The emission spectra and excitation spectra have good overlap. The emission spectra reveals very nice vibrational structure. The three major peaks are located at 405, 426, and 453 nm. The vibrational band spacing was found to be 1300 cm-1.

Synthesis: Deshpande et al. (2006); Elemans et al. (1998); Elemans et al. (2002); Kurth et al. (2001).

For related literature, see: Farrugia (1997).

Computing details top

Data collection: SMART (Bruker, 2006); cell refinement: SAINT (Bruker, 2006); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Bruker, 2006); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 2006); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. View of (1) (50% probability displacement ellipsoids) H atoms have been added for clarity of hydrogen bonding (Farrugia, 1997).
4 b,5,7,7a-Tetrahydro-4 b,7a-epiminomethanoimino-6H- imidazo[4,5-f][1,10]phenanthroline-6,13-dione monohydrate top
Crystal data top
C14H10N6O2·H2OF(000) = 1296
Mr = 312.30Dx = 1.502 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P2ybcCell parameters from 9312 reflections
a = 18.5164 (18) Åθ = 2.9–27.1°
b = 12.3920 (12) ŵ = 0.11 mm1
c = 12.6929 (13) ÅT = 150 K
β = 108.528 (5)°Block, lusterous grey
V = 2761.5 (5) Å30.49 × 0.30 × 0.25 mm
Z = 8
Data collection top
Bruker SMART CCD area-detector
diffractometer
5422 independent reflections
Radiation source: fine-focus sealed tube4600 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.032
φ and ω scansθmax = 26.0°, θmin = 3.4°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 2222
Tmin = 0.938, Tmax = 0.973k = 1515
68322 measured reflectionsl = 1515
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)] = 0.036Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.092H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0397P)2 + 1.7397P]
where P = (Fo2 + 2Fc2)/3
5422 reflections(Δ/σ)max = 0.001
451 parametersΔρmax = 0.51 e Å3
0 restraintsΔρmin = 0.27 e Å3
Crystal data top
C14H10N6O2·H2OV = 2761.5 (5) Å3
Mr = 312.30Z = 8
Monoclinic, P21/cMo Kα radiation
a = 18.5164 (18) ŵ = 0.11 mm1
b = 12.3920 (12) ÅT = 150 K
c = 12.6929 (13) Å0.49 × 0.30 × 0.25 mm
β = 108.528 (5)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
5422 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
4600 reflections with I > 2σ(I)
Tmin = 0.938, Tmax = 0.973Rint = 0.032
68322 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0360 restraints
wR(F2) = 0.092H atoms treated by a mixture of independent and constrained refinement
S = 1.03Δρmax = 0.51 e Å3
5422 reflectionsΔρmin = 0.27 e Å3
451 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
xyzUiso*/Ueq
C10.57536 (9)0.51053 (14)0.23035 (13)0.0250 (3)
H10.62460.51050.22610.030*
C20.52109 (9)0.44802 (14)0.15553 (14)0.0269 (4)
H20.53370.40600.10320.032*
C30.44753 (9)0.44943 (13)0.16025 (13)0.0235 (3)
H3A0.40950.40930.11000.028*
C40.43105 (8)0.51152 (11)0.24095 (12)0.0169 (3)
C50.48988 (8)0.57012 (12)0.31489 (12)0.0165 (3)
C60.47687 (8)0.63485 (11)0.40588 (11)0.0168 (3)
C70.40602 (8)0.63639 (11)0.42213 (11)0.0163 (3)
C80.39791 (9)0.69468 (13)0.51159 (13)0.0233 (3)
H80.35120.69750.52450.028*
C90.46028 (9)0.74809 (13)0.58058 (13)0.0262 (4)
H9A0.45680.78660.64160.031*
C100.52840 (9)0.74329 (13)0.55719 (13)0.0244 (3)
H10A0.57020.78000.60390.029*
C110.34995 (8)0.51796 (11)0.24373 (11)0.0153 (3)
C120.33911 (8)0.57274 (11)0.34914 (11)0.0156 (3)
C130.30689 (8)0.39172 (12)0.34652 (12)0.0178 (3)
C140.25196 (8)0.64364 (12)0.18811 (12)0.0183 (3)
C150.10575 (9)0.01787 (15)0.16880 (14)0.0300 (4)
H150.15620.01710.16790.036*
C160.06494 (9)0.11252 (14)0.19842 (14)0.0291 (4)
H160.08840.17520.21150.035*
C170.01127 (9)0.11196 (13)0.20813 (13)0.0241 (3)
H170.04100.17320.23230.029*
C180.04323 (8)0.01847 (12)0.18134 (12)0.0182 (3)
C190.00374 (8)0.07056 (12)0.14324 (12)0.0194 (3)
C200.02424 (8)0.16725 (12)0.09892 (12)0.0191 (3)
C210.10197 (8)0.18120 (12)0.11607 (12)0.0176 (3)
C220.12512 (9)0.27078 (12)0.06906 (13)0.0226 (3)
H220.17640.28210.07850.027*
C230.07080 (9)0.34281 (13)0.00801 (14)0.0276 (4)
H230.08490.40380.02350.033*
C240.00518 (9)0.32203 (13)0.00505 (14)0.0274 (4)
H240.04160.37040.04640.033*
C250.12815 (8)0.01245 (11)0.19996 (12)0.0168 (3)
C260.15898 (8)0.10310 (12)0.18926 (12)0.0169 (3)
C270.21494 (8)0.02458 (12)0.10467 (12)0.0197 (3)
C280.20351 (8)0.05141 (12)0.37338 (12)0.0208 (3)
H30.3210 (10)0.3610 (15)0.2068 (15)0.024 (5)*
H40.3084 (11)0.4909 (16)0.4657 (17)0.034 (5)*
H50.2869 (11)0.5538 (15)0.0913 (17)0.029 (5)*
H90.1498 (11)0.1433 (17)0.1173 (16)0.033 (5)*
H120.2169 (10)0.1955 (16)0.3208 (15)0.030 (5)*
H1S0.1442 (12)0.7076 (18)0.3928 (17)0.042 (6)*
H2S0.1900 (13)0.7700 (18)0.475 (2)0.052 (7)*
H3S0.3089 (13)0.2631 (19)0.538 (2)0.052 (7)*
H4S0.3637 (13)0.3118 (18)0.6218 (18)0.047 (6)*
N10.56110 (7)0.57086 (11)0.30836 (10)0.0212 (3)
N20.53740 (7)0.68914 (10)0.47175 (10)0.0219 (3)
N30.31824 (7)0.41111 (10)0.24826 (11)0.0188 (3)
N40.32376 (7)0.48165 (10)0.40966 (10)0.0196 (3)
N50.30309 (7)0.58453 (10)0.15337 (10)0.0185 (3)
N60.27320 (7)0.64070 (11)0.30005 (10)0.0204 (3)
H60.25000.67550.33840.024*
N70.07688 (7)0.07247 (11)0.14138 (11)0.0254 (3)
N80.02873 (7)0.23627 (11)0.03853 (11)0.0256 (3)
N90.15350 (7)0.07390 (11)0.12206 (11)0.0203 (3)
N100.22032 (7)0.07727 (10)0.14546 (11)0.0200 (3)
H100.25610.12150.14540.024*
N110.17069 (7)0.03684 (10)0.31552 (10)0.0206 (3)
H110.17440.10050.34370.025*
N120.18480 (7)0.13935 (10)0.30379 (10)0.0202 (3)
O10.28503 (6)0.30545 (9)0.37483 (9)0.0255 (3)
O20.19669 (6)0.69224 (9)0.12627 (9)0.0242 (2)
O30.25792 (6)0.06517 (9)0.05968 (9)0.0267 (3)
O40.24213 (7)0.05573 (9)0.47204 (9)0.0297 (3)
O1S0.17949 (6)0.75357 (9)0.40465 (10)0.0208 (2)
O2S0.32338 (6)0.27096 (9)0.60645 (10)0.0197 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0189 (8)0.0316 (9)0.0270 (8)0.0013 (7)0.0110 (6)0.0040 (7)
C20.0283 (8)0.0293 (9)0.0277 (8)0.0016 (7)0.0154 (7)0.0090 (7)
C30.0241 (8)0.0244 (8)0.0235 (8)0.0058 (6)0.0095 (6)0.0075 (6)
C40.0193 (7)0.0151 (7)0.0170 (7)0.0002 (6)0.0070 (6)0.0016 (6)
C50.0168 (7)0.0162 (7)0.0163 (7)0.0010 (6)0.0048 (6)0.0028 (6)
C60.0182 (7)0.0147 (7)0.0161 (7)0.0008 (6)0.0033 (6)0.0018 (6)
C70.0181 (7)0.0150 (7)0.0149 (7)0.0002 (6)0.0040 (6)0.0011 (6)
C80.0232 (8)0.0251 (8)0.0243 (8)0.0026 (6)0.0113 (6)0.0050 (6)
C90.0293 (9)0.0277 (9)0.0216 (8)0.0017 (7)0.0081 (7)0.0100 (7)
C100.0215 (8)0.0238 (8)0.0239 (8)0.0027 (6)0.0016 (6)0.0076 (6)
C110.0169 (7)0.0148 (7)0.0137 (7)0.0023 (5)0.0041 (5)0.0017 (5)
C120.0150 (7)0.0170 (7)0.0156 (7)0.0002 (6)0.0059 (6)0.0004 (6)
C130.0131 (7)0.0207 (8)0.0176 (7)0.0014 (6)0.0020 (6)0.0020 (6)
C140.0180 (7)0.0163 (7)0.0199 (7)0.0014 (6)0.0049 (6)0.0004 (6)
C150.0176 (8)0.0381 (10)0.0353 (9)0.0022 (7)0.0098 (7)0.0106 (8)
C160.0235 (8)0.0294 (9)0.0346 (9)0.0058 (7)0.0094 (7)0.0100 (7)
C170.0226 (8)0.0224 (8)0.0264 (8)0.0003 (6)0.0065 (6)0.0060 (7)
C180.0175 (7)0.0208 (7)0.0162 (7)0.0016 (6)0.0053 (6)0.0000 (6)
C190.0170 (7)0.0233 (8)0.0174 (7)0.0013 (6)0.0050 (6)0.0014 (6)
C200.0185 (7)0.0196 (7)0.0188 (7)0.0008 (6)0.0053 (6)0.0001 (6)
C210.0193 (7)0.0169 (7)0.0168 (7)0.0000 (6)0.0059 (6)0.0011 (6)
C220.0195 (7)0.0219 (8)0.0270 (8)0.0012 (6)0.0082 (6)0.0025 (6)
C230.0282 (8)0.0228 (8)0.0330 (9)0.0016 (7)0.0116 (7)0.0088 (7)
C240.0235 (8)0.0232 (8)0.0334 (9)0.0048 (7)0.0062 (7)0.0105 (7)
C250.0181 (7)0.0147 (7)0.0168 (7)0.0002 (6)0.0044 (6)0.0009 (6)
C260.0149 (7)0.0166 (7)0.0189 (7)0.0014 (6)0.0052 (6)0.0009 (6)
C270.0191 (7)0.0208 (8)0.0188 (7)0.0006 (6)0.0055 (6)0.0011 (6)
C280.0204 (7)0.0212 (8)0.0200 (8)0.0008 (6)0.0051 (6)0.0003 (6)
N10.0167 (6)0.0243 (7)0.0227 (7)0.0004 (5)0.0063 (5)0.0017 (5)
N20.0185 (6)0.0227 (7)0.0223 (7)0.0014 (5)0.0036 (5)0.0042 (5)
N30.0219 (7)0.0158 (6)0.0195 (6)0.0040 (5)0.0078 (5)0.0043 (5)
N40.0241 (7)0.0210 (7)0.0160 (6)0.0051 (5)0.0095 (5)0.0003 (5)
N50.0199 (6)0.0215 (7)0.0129 (6)0.0017 (5)0.0037 (5)0.0004 (5)
N60.0179 (6)0.0258 (7)0.0173 (6)0.0067 (5)0.0052 (5)0.0024 (5)
N70.0172 (6)0.0297 (7)0.0294 (7)0.0008 (5)0.0077 (6)0.0072 (6)
N80.0198 (7)0.0236 (7)0.0317 (7)0.0033 (5)0.0059 (6)0.0074 (6)
N90.0220 (7)0.0166 (7)0.0250 (7)0.0026 (5)0.0113 (5)0.0040 (5)
N100.0155 (6)0.0175 (6)0.0289 (7)0.0023 (5)0.0099 (5)0.0000 (5)
N110.0224 (7)0.0166 (6)0.0194 (6)0.0005 (5)0.0019 (5)0.0039 (5)
N120.0230 (7)0.0162 (6)0.0182 (6)0.0031 (5)0.0020 (5)0.0011 (5)
O10.0283 (6)0.0230 (6)0.0234 (6)0.0104 (5)0.0056 (5)0.0023 (5)
O20.0227 (6)0.0239 (6)0.0224 (6)0.0061 (5)0.0020 (5)0.0036 (5)
O30.0278 (6)0.0256 (6)0.0324 (6)0.0000 (5)0.0178 (5)0.0029 (5)
O40.0353 (7)0.0282 (6)0.0179 (6)0.0016 (5)0.0022 (5)0.0011 (5)
O1S0.0223 (6)0.0195 (6)0.0216 (6)0.0005 (5)0.0086 (5)0.0013 (5)
O2S0.0185 (6)0.0214 (6)0.0200 (6)0.0015 (4)0.0072 (4)0.0011 (4)
Geometric parameters (Å, º) top
C1—N11.332 (2)C17—H170.9300
C1—C21.380 (2)C18—C191.393 (2)
C1—H10.9300C18—C251.516 (2)
C2—C31.382 (2)C19—N71.3471 (19)
C2—H20.9300C19—C201.485 (2)
C3—C41.390 (2)C20—N81.3428 (19)
C3—H3A0.9300C20—C211.396 (2)
C4—C51.395 (2)C21—C221.391 (2)
C4—C111.515 (2)C21—C261.513 (2)
C5—N11.3474 (19)C22—C231.383 (2)
C5—C61.487 (2)C22—H220.9300
C6—N21.3462 (19)C23—C241.387 (2)
C6—C71.391 (2)C23—H230.9300
C7—C81.394 (2)C24—N81.334 (2)
C7—C121.5120 (19)C24—H240.9300
C8—C91.377 (2)C25—N91.4397 (19)
C8—H80.9300C25—N111.4591 (18)
C9—C101.386 (2)C25—C261.563 (2)
C9—H9A0.9300C26—N121.4498 (19)
C10—N21.330 (2)C26—N101.4500 (19)
C10—H10A0.9300C27—O31.2253 (18)
C11—N51.4548 (18)C27—N101.356 (2)
C11—N31.4569 (19)C27—N91.370 (2)
C11—C121.5691 (19)C28—O41.2302 (18)
C12—N41.4435 (19)C28—N111.349 (2)
C12—N61.4502 (18)C28—N121.376 (2)
C13—O11.2362 (18)N3—H30.826 (19)
C13—N41.350 (2)N4—H40.85 (2)
C13—N31.3506 (19)N5—H50.84 (2)
C14—O21.2312 (18)N6—H60.8600
C14—N61.3490 (19)N9—H90.86 (2)
C14—N51.3756 (19)N10—H100.8600
C15—N71.334 (2)N11—H110.8600
C15—C161.381 (2)N12—H120.90 (2)
C15—H150.9300O1S—H1S0.84 (2)
C16—C171.377 (2)O1S—H2S0.87 (2)
C16—H160.9300O2S—H3S0.83 (3)
C17—C181.391 (2)O2S—H4S0.87 (2)
N1—C1—C2123.60 (14)N8—C20—C21122.67 (14)
N1—C1—H1118.2N8—C20—C19116.78 (13)
C2—C1—H1118.2C21—C20—C19120.48 (13)
C1—C2—C3118.36 (14)C22—C21—C20118.35 (13)
C1—C2—H2120.8C22—C21—C26121.59 (13)
C3—C2—H2120.8C20—C21—C26119.99 (13)
C2—C3—C4119.27 (14)C23—C22—C21119.15 (14)
C2—C3—H3A120.4C23—C22—H22120.4
C4—C3—H3A120.4C21—C22—H22120.4
C3—C4—C5118.46 (13)C22—C23—C24118.45 (15)
C3—C4—C11119.83 (13)C22—C23—H23120.8
C5—C4—C11121.66 (13)C24—C23—H23120.8
N1—C5—C4122.18 (13)N8—C24—C23123.45 (15)
N1—C5—C6116.57 (12)N8—C24—H24118.3
C4—C5—C6121.25 (13)C23—C24—H24118.3
N2—C6—C7122.63 (13)N9—C25—N11113.03 (12)
N2—C6—C5116.33 (13)N9—C25—C18114.54 (12)
C7—C6—C5121.03 (13)N11—C25—C18110.39 (12)
C6—C7—C8118.60 (13)N9—C25—C26102.53 (11)
C6—C7—C12121.99 (13)N11—C25—C26100.47 (11)
C8—C7—C12119.35 (13)C18—C25—C26114.90 (12)
C9—C8—C7118.79 (14)N12—C26—N10113.83 (12)
C9—C8—H8120.6N12—C26—C21111.15 (12)
C7—C8—H8120.6N10—C26—C21112.60 (12)
C8—C9—C10118.66 (14)N12—C26—C25102.11 (11)
C8—C9—H9A120.7N10—C26—C25100.56 (11)
C10—C9—H9A120.7C21—C26—C25115.86 (11)
N2—C10—C9123.69 (14)O3—C27—N10125.48 (14)
N2—C10—H10A118.2O3—C27—N9125.99 (14)
C9—C10—H10A118.2N10—C27—N9108.53 (13)
N5—C11—N3113.56 (11)O4—C28—N11127.22 (14)
N5—C11—C4111.02 (11)O4—C28—N12124.43 (14)
N3—C11—C4111.58 (12)N11—C28—N12108.33 (12)
N5—C11—C12102.77 (11)C1—N1—C5118.09 (13)
N3—C11—C12101.37 (11)C10—N2—C6117.59 (13)
C4—C11—C12116.03 (11)C13—N3—C11112.40 (12)
N4—C12—N6113.68 (12)C13—N3—H3121.0 (12)
N4—C12—C7110.09 (11)C11—N3—H3123.4 (12)
N6—C12—C7111.97 (12)C13—N4—C12112.16 (12)
N4—C12—C11102.45 (11)C13—N4—H4122.0 (13)
N6—C12—C11101.72 (11)C12—N4—H4120.8 (13)
C7—C12—C11116.50 (11)C14—N5—C11110.37 (12)
O1—C13—N4125.22 (14)C14—N5—H5117.7 (13)
O1—C13—N3125.71 (14)C11—N5—H5115.4 (13)
N4—C13—N3109.07 (13)C14—N6—C12113.08 (12)
O2—C14—N6126.14 (14)C14—N6—H6123.5
O2—C14—N5124.99 (14)C12—N6—H6123.5
N6—C14—N5108.86 (12)C15—N7—C19117.70 (14)
N7—C15—C16123.63 (15)C24—N8—C20117.93 (13)
N7—C15—H15118.2C27—N9—C25110.09 (12)
C16—C15—H15118.2C27—N9—H9119.0 (13)
C17—C16—C15118.47 (15)C25—N9—H9122.6 (13)
C17—C16—H16120.8C27—N10—C26112.37 (12)
C15—C16—H16120.8C27—N10—H10123.8
C16—C17—C18119.06 (15)C26—N10—H10123.8
C16—C17—H17120.5C28—N11—C25112.65 (12)
C18—C17—H17120.5C28—N11—H11123.7
C17—C18—C19118.50 (13)C25—N11—H11123.7
C17—C18—C25120.24 (13)C28—N12—C26109.51 (12)
C19—C18—C25121.16 (13)C28—N12—H12116.7 (12)
N7—C19—C18122.23 (14)C26—N12—H12117.7 (12)
N7—C19—C20116.68 (13)H1S—O1S—H2S104 (2)
C18—C19—C20121.06 (13)H3S—O2S—H4S106 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N12—H12···O10.90 (2)1.835 (2)2.726 (2)172.5 (1)
N3—H3···O2S0.826 (19)2.082 (2)2.907 (2)176.3 (1)
N10—H10···O2S0.861.992.833 (2)166

Experimental details

Crystal data
Chemical formulaC14H10N6O2·H2O
Mr312.30
Crystal system, space groupMonoclinic, P21/c
Temperature (K)150
a, b, c (Å)18.5164 (18), 12.3920 (12), 12.6929 (13)
β (°) 108.528 (5)
V3)2761.5 (5)
Z8
Radiation typeMo Kα
µ (mm1)0.11
Crystal size (mm)0.49 × 0.30 × 0.25
Data collection
DiffractometerBruker SMART CCD area-detector
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.938, 0.973
No. of measured, independent and
observed [I > 2σ(I)] reflections
68322, 5422, 4600
Rint0.032
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.036, 0.092, 1.03
No. of reflections5422
No. of parameters451
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.51, 0.27

Computer programs: SMART (Bruker, 2006), SAINT (Bruker, 2006), SAINT, SHELXTL (Bruker, 2006), SHELXL97 (Sheldrick, 1997), SHELXTL.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N12—H12···O10.90 (2)1.835 (2)2.726 (2)172.5 (1)
N3—H3···O2S0.826 (19)2.082 (2)2.907 (2)176.3 (1)
N10—H10···O2S0.861.992.833 (2)166
 

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