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ISSN: 2414-3146

2-Amino-5-chloro­pyridin-1-ium barbiturate dihydrate

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aDepartment of Chemistry, Periyar Maniammai Institute of Science & Technology, Thanjavur, Tamilnadu-613403, India, bDepartment of Chemistry, Government Arts and Science College, Karambakudi, Pudukottai, Tamilnadu-622302, India, and cFaculty of Chemistry and Chemical Technology, University of Ljubljana, Slovenia
*Correspondence e-mail: [email protected]

Edited by W. T. A. Harrison, University of Aberdeen, United Kingdom (Received 9 March 2026; accepted 6 April 2026; online 10 April 2026)

In the title hydrated salt, C5H6ClN2+·C4H3N2O3·2H2O, the asymmetric unit contains two cations, two anions and four water mol­ecules of crystallization. In the extended structure, the barbiturate (2,4,6-trioxo-1,3-diazinan-5-ide) anions form a wave-like supra­molecular [001] chain decorated by the cations, mediated by numerous N—H⋯O hydrogen bonds. Adjacent chains are cross-linked by [010] chains of water mol­ecules featuring four- and six-membered rings and five-membered carboxyl­ate aggregates via O—H⋯O hydrogen bonds.

3D view (loading...)
[Scheme 3D1]
Chemical scheme
[Scheme 1]

Structure description

The crystal structure of 2-amino-5-chloro­pyridine, C5H5ClN2 (Kvick & Backéus, 1974View full citation) and its diverse salts with di­carb­oxy­lic acids (Jayanalina et al., 2015View full citation), aromatic acids (Hanif et al., 2020View full citation) and other inorganic anions such as nitrate (Zaouali Zgolli et al., 2009View full citation), phosphate (Akriche & Rzaigui, 2005View full citation), sulfonate (Jagan & Boopathi, 2020View full citation) and tri­fluoro­acetate (Hemamalini & Fun, 2010View full citation) have been extensively studied, highlighting its diverse hydrogen-bonding inter­actions. Barbiturates derived from barbituric acid (C4H4N2O3) play a significant role in biological systems (Hueso Ureña et al., 2003View full citation). Research on barbiturate salts and co-crystals demonstrate that hydrogen bonding is a key driving force for structure and property modulation.

Hydrogen bonding not only increases the reactivity and electrophilicity of barbiturates (Bauer & Spange, 2010View full citation), but also governs their supra­molecular organization in host–guest systems and polymeric assemblies, particularly those involving Hamilton-type receptors (Chang & Hamilton, 1988View full citation). Thus hydrogen bonding acts as the primary driving force behind barbiturate self-assembly and functional behaviour and indicates its significance in supra­molecular chemistry, materials science and biomimetic design. As part of our studies in this area, we now report the synthesis and structure of the title hydrated salt, C5H6ClN2+·C4H3N2O3·2H2O (I).

The asymmetric unit of (I) consists of two crystallographically independent 2-amino-5-chloro­pyridinium cations, two barbiturate anions and four water mol­ecules of crystallization in space group P21/c. The proton acceptance from the barbituric acid occurs at the pyridine ring N atoms of the cations (Fig. 1[link]) which is evident from the widening of the C1—N1—C5 and C6—N3—C10 bond angles [122.67 (13) and 122.84 (14)°, respectively] compared to the unprotonated mol­ecule, in which the bond angle is around 118° (Anantheeswary et al., 2024View full citation). The deprotonation of the barbituric acid occurs from the active methyl­ene groups (atoms C13 and C17) driven by the electron withdrawing carbonyl group at both sides and this is supported by the sp2 hybridization at these atoms in (I) implied by the C—C—C bond angles [C12—C13—C14 = 121.55 (14); C16—C17—C18 = 121.61 (14)°]. Overall, both barbiturate anions display a nearly planar six-membered ring: the deviations of the atoms from the mean plane are small (±0.025 Å and ±0.013 Å for the O1 and O4 anions, respectively). These structural parameters align well with known data for barbiturate systems (Gelbrich et al., 2015View full citation) and indicate that the barbiturate anion in (I) adopts a stabilized, delocalized and nearly planar conformation.

[Figure 1]
Figure 1
The mol­ecular structure of (I) with displacement ellipsoids drawn at the 50% probability level.

In the extended structure of (I), the anions are linked by pairwise N—H⋯O hydrogen bonds into wave-like [001] ribbons, with the O1 and O4 anions alternating in the chains. Atoms N5 and N7 (donors) and carbonyl oxygen atoms O3 and O6 (acceptors) form one pairwise linkage and atoms N6 and N8 (donors) and O1 and O4 (acceptors) the other, which leads to two distinct R22(8) ring motifs (Table 1[link]). The [001] chains are decorated by the cations: the C1 cation links to atoms O1, O5 and O6 in the anions and the C6 cation to O2, O3 and O4 via strong N—H⋯O hydrogen bonds to render R32(10) ring motifs. Taken together, these hydrogen bonds lead to propagate a wave-like supra­molecular ribbon as shown in Fig. 2[link]. Adjacent anion/cation supra­molecular sheets are connected by four- and six-membered [010] tape-like arrays of water mol­ecules which form various Ow—Hw⋯Ow and Ow—Hw⋯Oc (w = water, c = carbon­yl) hydrogen bonds. This arrangement has a close resemblance to the water tape T4(2) and T6(2) motifs in the systematic classification of hydrated organic crystal structures reported in the literature (Infantes & Motherwell, 2002View full citation). In addition, the inter­action between the water mol­ecules O7, O9 and O10 and the carbonyl O2 atom of the anion leads to an R54(10) ring motif. The existence of the four- and six-membered water loops and five-membered carbon­yl–water loops generates two different DDAA (D = donor, A = acceptor) hydrogen-bonded arrays with ring motifs of R54(10), R66(12) and R54(10) and R54(10), R42(8) and R54(10), along the a axis direction as shown in Fig. 3[link].

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1⋯O6 0.87 1.85 2.7207 (18) 176
N2—H2A⋯O1 0.89 2.02 2.7461 (18) 138
N2—H2B⋯O5i 0.89 1.87 2.7610 (17) 180
N3—H3A⋯O3 0.86 1.83 2.6863 (18) 177
N4—H4A⋯O4 0.87 2.00 2.7248 (18) 139
N4—H4B⋯O2ii 0.89 1.97 2.8606 (17) 173
N5—H5A⋯O6 0.87 2.02 2.8786 (17) 173
N6—H6⋯O4i 0.89 2.03 2.9005 (17) 170
N7—H7A⋯O3 0.87 2.06 2.8985 (17) 163
N8—H8A⋯O1ii 0.88 2.01 2.8762 (16) 172
O7—H7B⋯O5 0.86 1.92 2.7581 (16) 164
O7—H7C⋯O2iii 0.82 2.13 2.9155 (18) 160
O8—H8B⋯O10 0.86 1.89 2.739 (2) 167
O8—H8C⋯O2 0.89 1.91 2.7810 (16) 165
O9—H9A⋯O8 0.86 1.93 2.7864 (18) 168
O10—H10B⋯O7iii 0.87 1.96 2.8287 (18) 175
C10—H10⋯O7iii 0.95 2.44 3.321 (2) 153
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation.
[Figure 2]
Figure 2
A view of a wave-like supra­molecular chain built up from N—H⋯O hydrogen bonds [symmetry codes: (i) x, Mathematical equation − y, −Mathematical equation + z; (ii) x, Mathematical equation − y, Mathematical equation + z].
[Figure 3]
Figure 3
A water chain extending along the c-axis direction cross-linking the supra­molecular chains [symmetry code: (iii) 1 − x, Mathematical equation + y, 3/2 - −z].

A possible offset aromatic ππ stacking inter­action between barbiturate rings [Cg1⋯Cg2vi; symmetry code: (vi) 1 − x, −Mathematical equation + y, 3/2 − z; Cg1 = C11–C14/N5/N6 centroid; Cg2 = C15–C18/N7/N8 centroid] occurs with centroid-to-centroid and perpendicular distances of 3.7978 (9) and 3.4530 (6) Å, respectively. However, the large slippage angle of 30.5° suggests that this inter­action is weak.

Synthesis and crystallization

The title compound was synthesized by mixing 20 ml ethanol:water (1:1 v/v) solutions of 2-amino-5-chloro­pyridine (0.25 mmol) and barbituric acid (0.25 mmol) and the resulting clear solution was then warmed over a water bath for 20 min at 353 K. The solution was then allowed to cool to room temperature and after a few days, colourless crystals of (I) were separated out from the mother liquor.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link].

Table 2
Experimental details

Crystal data
Chemical formula C5H6ClN2+·C4H3N2O3·2H2O
Mr 292.68
Crystal system, space group Monoclinic, P21/c
Temperature (K) 150
a, b, c (Å) 18.8228 (10), 6.9495 (4), 19.3563 (10)
β (°) 99.817 (5)
V3) 2494.9 (2)
Z 8
Radiation type Mo Kα
μ (mm−1) 0.33
Crystal size (mm) 0.30 × 0.20 × 0.20
 
Data collection
Diffractometer SuperNova, Dual, Cu at home/near, Atlas
Absorption correction Multi-scan (CrysAlis PRO; Rigaku OD, 2019View full citation)
Tmin, Tmax 0.812, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 13946, 6542, 5147
Rint 0.023
(sin θ/λ)max−1) 0.712
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.040, 0.108, 1.04
No. of reflections 6542
No. of parameters 343
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.33, −0.30
Computer programs: CrysAlis PRO (Rigaku OD, 2019View full citation), SHELXT2018/2 (Sheldrick, 2015aView full citation), SHELXL2018/3 (Sheldrick, 2015bView full citation), PLATON (Spek, 2020View full citation), Mercury (Macrae et al., 2020View full citation), POVRay (Cason, 2004View full citation), PLATON (Spek, 2020View full citation) and publCIF (Westrip, 2010View full citation).

Structural data


Computing details top

2-Amino-5-chloropyridin-1-ium 2,4,6-trioxo-1,3-diazinan-5-ide dihydrate top
Crystal data top
C5H6ClN2+·C4H3N2O3·2H2OF(000) = 1216
Mr = 292.68Dx = 1.558 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 4971 reflections
a = 18.8228 (10) Åθ = 3.6–30.0°
b = 6.9495 (4) ŵ = 0.33 mm1
c = 19.3563 (10) ÅT = 150 K
β = 99.817 (5)°Prism, yellow
V = 2494.9 (2) Å30.30 × 0.20 × 0.20 mm
Z = 8
Data collection top
SuperNova, Dual, Cu at home/near, Atlas
diffractometer
6542 independent reflections
Radiation source: micro-focus sealed X-ray tube5147 reflections with I > 2σ(I)
SuperNova (Mo) X-ray Source monochromatorRint = 0.023
Detector resolution: 10.4933 pixels mm-1θmax = 30.4°, θmin = 2.6°
ωw scansh = 2424
Absorption correction: multi-scan
(CrysAlis PRO; Rigaku OD, 2019)
k = 96
Tmin = 0.812, Tmax = 1.000l = 1825
13946 measured reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.040H-atom parameters constrained
wR(F2) = 0.108 W = 1/[Σ2(FO2) + (0.0476P)2 + 0.6984P] WHERE P = (FO2 + 2FC2)/3
S = 1.04(Δ/σ)max = 0.001
6542 reflectionsΔρmax = 0.33 e Å3
343 parametersΔρmin = 0.30 e Å3
Special details top

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell esds are taken into account in the estimation of distances, angles and torsion angles

Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > 2sigma(F2) is used only for calculating -R-factor-obs 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.

The H atoms of the –NH2 groups were located from a difference Fourier map and refined freely. The other H atoms were placed geometrically and refined using a riding model.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cl10.87257 (2)0.58875 (6)0.79957 (2)0.0262 (1)
Cl20.01456 (2)0.65022 (7)0.64189 (2)0.0331 (1)
O10.48161 (6)0.29532 (19)0.55832 (5)0.0241 (3)
O20.24377 (6)0.15226 (18)0.50080 (5)0.0232 (3)
O30.33892 (6)0.45699 (17)0.71542 (5)0.0209 (3)
N50.40902 (7)0.3677 (2)0.63664 (6)0.0172 (3)
N60.36206 (6)0.2313 (2)0.52973 (6)0.0180 (3)
O40.39978 (6)0.39067 (19)0.89731 (6)0.0272 (4)
O50.63610 (6)0.23191 (18)0.95562 (5)0.0229 (3)
O60.53956 (6)0.46773 (18)0.73026 (5)0.0216 (3)
C110.42087 (8)0.2982 (2)0.57385 (7)0.0178 (4)
C120.29255 (8)0.2292 (2)0.54502 (7)0.0178 (4)
C130.28334 (8)0.3118 (2)0.60855 (7)0.0190 (4)
C140.34145 (8)0.3827 (2)0.65576 (7)0.0173 (4)
N70.47177 (7)0.4344 (2)0.81589 (6)0.0189 (4)
N80.51837 (7)0.3158 (2)0.92568 (6)0.0199 (4)
C150.46008 (8)0.3809 (2)0.88069 (8)0.0192 (4)
C160.58734 (8)0.2981 (2)0.90937 (8)0.0178 (4)
C170.59555 (8)0.3545 (2)0.84172 (7)0.0190 (4)
C180.53785 (8)0.4195 (2)0.79346 (7)0.0177 (4)
N10.67547 (7)0.4856 (2)0.70029 (6)0.0192 (4)
N20.62458 (7)0.3966 (2)0.58823 (7)0.0261 (4)
C10.68229 (8)0.4424 (2)0.63372 (8)0.0196 (4)
C20.75242 (8)0.4493 (2)0.61612 (8)0.0217 (5)
C30.81029 (8)0.4945 (2)0.66553 (8)0.0220 (4)
C40.79994 (8)0.5347 (2)0.73472 (8)0.0199 (4)
C50.73289 (8)0.5300 (2)0.75058 (8)0.0199 (4)
N30.20843 (7)0.53881 (19)0.74635 (6)0.0188 (4)
N40.25572 (7)0.4593 (2)0.86099 (7)0.0244 (4)
C60.19906 (8)0.5027 (2)0.81288 (8)0.0193 (4)
O70.77655 (6)0.2806 (2)0.93547 (6)0.0325 (4)
C70.12861 (9)0.5152 (3)0.82787 (8)0.0253 (5)
C80.07259 (9)0.5605 (3)0.77660 (8)0.0265 (5)
C90.08531 (9)0.5963 (2)0.70812 (8)0.0224 (5)
C100.15318 (9)0.5862 (2)0.69438 (8)0.0217 (4)
O80.09636 (6)0.2133 (2)0.49087 (6)0.0346 (4)
O90.00582 (7)0.1255 (2)0.57464 (7)0.0385 (4)
O100.11145 (7)0.6003 (2)0.47080 (7)0.0395 (4)
H5A0.446010.403940.666800.0210*
H60.369700.182000.489470.0220*
H130.236250.319830.619840.0230*
H7A0.433320.467000.786720.0230*
H8A0.510610.273940.966390.0240*
H170.641910.347970.828680.0230*
H10.632570.478950.711810.0230*
H20.758920.422050.569510.0260*
H2A0.581180.388030.600770.0310*
H2B0.628280.355030.545270.0310*
H30.857220.499130.653720.0260*
H50.725730.557820.796960.0240*
H3A0.250320.516910.736310.0230*
H4A0.298750.449010.850250.0290*
H4B0.249850.433010.904650.0290*
H70.120250.491710.874170.0300*
H80.025060.567960.786800.0320*
H100.162260.612160.648500.0260*
H7B0.733320.244060.938110.0490*
H7C0.779820.393060.949110.0490*
H8B0.095890.337080.488690.0520*
H8C0.143190.185080.501490.0520*
H9A0.030300.146030.553420.0580*
H9B0.022900.019030.556420.0580*
H10A0.077200.681960.458890.0590*
H10B0.144900.652960.501890.0590*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0180 (2)0.0300 (2)0.0287 (2)0.0023 (2)0.0017 (1)0.0038 (2)
Cl20.0236 (2)0.0411 (3)0.0310 (2)0.0059 (2)0.0059 (2)0.0034 (2)
O10.0148 (5)0.0390 (7)0.0196 (5)0.0032 (5)0.0062 (4)0.0073 (5)
O20.0161 (5)0.0331 (7)0.0197 (5)0.0034 (5)0.0015 (4)0.0030 (5)
O30.0169 (5)0.0315 (7)0.0152 (5)0.0011 (5)0.0052 (4)0.0026 (5)
N50.0130 (6)0.0243 (7)0.0144 (5)0.0011 (5)0.0026 (4)0.0022 (5)
N60.0146 (6)0.0263 (7)0.0136 (5)0.0008 (5)0.0040 (4)0.0027 (5)
O40.0157 (5)0.0467 (8)0.0205 (5)0.0053 (5)0.0072 (4)0.0080 (5)
O50.0160 (5)0.0336 (7)0.0186 (5)0.0033 (5)0.0018 (4)0.0047 (5)
O60.0168 (5)0.0346 (7)0.0138 (5)0.0001 (5)0.0042 (4)0.0025 (5)
C110.0160 (7)0.0216 (8)0.0163 (7)0.0001 (6)0.0038 (5)0.0005 (6)
C120.0151 (7)0.0221 (8)0.0166 (7)0.0003 (6)0.0035 (5)0.0039 (6)
C130.0139 (7)0.0253 (9)0.0184 (7)0.0010 (6)0.0048 (5)0.0017 (6)
C140.0173 (7)0.0211 (8)0.0145 (6)0.0016 (6)0.0057 (5)0.0030 (6)
N70.0149 (6)0.0278 (8)0.0141 (6)0.0025 (5)0.0028 (4)0.0031 (5)
N80.0165 (6)0.0299 (8)0.0139 (6)0.0022 (6)0.0047 (5)0.0056 (6)
C150.0156 (7)0.0250 (8)0.0177 (7)0.0004 (6)0.0050 (5)0.0013 (6)
C160.0149 (7)0.0200 (8)0.0190 (7)0.0005 (6)0.0044 (5)0.0002 (6)
C170.0140 (7)0.0250 (8)0.0187 (7)0.0000 (6)0.0052 (5)0.0007 (6)
C180.0162 (7)0.0207 (8)0.0170 (7)0.0028 (6)0.0055 (5)0.0030 (6)
N10.0150 (6)0.0256 (7)0.0180 (6)0.0013 (5)0.0059 (5)0.0010 (6)
N20.0182 (7)0.0417 (9)0.0190 (6)0.0050 (6)0.0047 (5)0.0073 (6)
C10.0186 (7)0.0216 (8)0.0190 (7)0.0008 (6)0.0045 (6)0.0000 (6)
C20.0211 (8)0.0256 (9)0.0202 (7)0.0011 (6)0.0091 (6)0.0025 (7)
C30.0165 (7)0.0230 (8)0.0283 (8)0.0016 (6)0.0090 (6)0.0021 (7)
C40.0172 (7)0.0187 (8)0.0228 (7)0.0017 (6)0.0010 (6)0.0005 (6)
C50.0204 (8)0.0221 (8)0.0172 (7)0.0002 (6)0.0030 (5)0.0018 (6)
N30.0155 (6)0.0226 (7)0.0193 (6)0.0012 (5)0.0061 (5)0.0011 (5)
N40.0171 (7)0.0359 (9)0.0206 (6)0.0036 (6)0.0040 (5)0.0044 (6)
C60.0181 (7)0.0214 (8)0.0189 (7)0.0005 (6)0.0046 (5)0.0012 (6)
O70.0206 (6)0.0332 (7)0.0451 (7)0.0004 (5)0.0095 (5)0.0077 (6)
C70.0195 (8)0.0368 (10)0.0211 (7)0.0022 (7)0.0080 (6)0.0024 (7)
C80.0168 (8)0.0342 (10)0.0295 (8)0.0017 (7)0.0070 (6)0.0007 (8)
C90.0189 (8)0.0225 (8)0.0245 (8)0.0024 (6)0.0000 (6)0.0009 (7)
C100.0240 (8)0.0225 (8)0.0187 (7)0.0006 (6)0.0040 (6)0.0021 (6)
O80.0204 (6)0.0406 (8)0.0424 (7)0.0008 (6)0.0046 (5)0.0027 (6)
O90.0387 (8)0.0413 (8)0.0380 (7)0.0019 (6)0.0135 (6)0.0028 (6)
O100.0297 (7)0.0445 (9)0.0434 (7)0.0032 (6)0.0039 (6)0.0042 (7)
Geometric parameters (Å, º) top
Cl1—C41.7322 (16)C1—C21.419 (2)
Cl2—C91.7249 (17)N2—H2A0.8900
O1—C111.2309 (19)C2—C31.358 (2)
O2—C121.2624 (18)N2—H2B0.8900
O3—C141.2732 (17)C3—C41.414 (2)
N5—C111.3611 (18)C4—C51.349 (2)
N5—C141.388 (2)C2—H20.9500
N6—C111.3596 (19)C3—H30.9500
N6—C121.3899 (19)N3—C101.358 (2)
O4—C151.2332 (19)N3—C61.3527 (19)
N5—H5A0.8700N4—C61.326 (2)
O5—C161.2551 (19)C5—H50.9500
O6—C181.2741 (17)N3—H3A0.8600
N6—H60.8900N4—H4B0.8900
C12—C131.3944 (19)N4—H4A0.8700
C13—C141.391 (2)C6—C71.408 (2)
N7—C151.3616 (19)C7—C81.356 (2)
N7—C181.389 (2)C8—C91.409 (2)
N8—C151.357 (2)C9—C101.350 (2)
N8—C161.393 (2)C7—H70.9500
C13—H130.9500O7—H7C0.8200
N7—H7A0.8700O7—H7B0.8600
N8—H8A0.8800C8—H80.9500
C16—C171.400 (2)C10—H100.9500
C17—C181.382 (2)O8—H8B0.8600
N1—C11.3503 (19)O8—H8C0.8900
N1—C51.361 (2)O9—H9A0.8600
N2—C11.316 (2)O9—H9B0.8600
C17—H170.9500O10—H10A0.8600
N1—H10.8700O10—H10B0.8700
C11—N5—C14124.19 (13)C1—N1—H1118.00
C11—N6—C12124.41 (12)C1—N2—H2A122.00
C11—N5—H5A118.00C1—N2—H2B121.00
C14—N5—H5A118.00C1—C2—C3120.39 (14)
C11—N6—H6117.00H2A—N2—H2B117.00
C12—N6—H6119.00C2—C3—C4119.29 (14)
O1—C11—N6122.12 (13)C3—C4—C5119.74 (14)
N5—C11—N6116.26 (13)Cl1—C4—C3120.67 (12)
O1—C11—N5121.62 (13)Cl1—C4—C5119.58 (12)
O2—C12—N6117.54 (12)N1—C5—C4120.16 (14)
O2—C12—C13125.94 (14)C1—C2—H2120.00
N6—C12—C13116.52 (13)C3—C2—H2120.00
C12—C13—C14121.55 (14)C2—C3—H3120.00
O3—C14—C13126.36 (14)C4—C3—H3120.00
N5—C14—C13116.88 (12)C6—N3—C10122.84 (14)
O3—C14—N5116.75 (13)N1—C5—H5120.00
C15—N7—C18124.15 (13)C4—C5—H5120.00
C15—N8—C16124.54 (12)C10—N3—H3A120.00
C14—C13—H13119.00C6—N3—H3A117.00
C12—C13—H13119.00C6—N4—H4A121.00
C15—N7—H7A115.00H4A—N4—H4B119.00
C18—N7—H7A120.00C6—N4—H4B120.00
C15—N8—H8A117.00N3—C6—C7117.72 (14)
C16—N8—H8A119.00N3—C6—N4119.42 (14)
O4—C15—N8122.03 (14)N4—C6—C7122.86 (14)
N7—C15—N8116.25 (13)C6—C7—C8120.38 (15)
O4—C15—N7121.72 (14)C7—C8—C9119.60 (16)
O5—C16—N8117.85 (13)C8—C9—C10119.63 (15)
O5—C16—C17125.85 (14)Cl2—C9—C8120.28 (13)
N8—C16—C17116.29 (13)Cl2—C9—C10120.09 (12)
C16—C17—C18121.61 (14)N3—C10—C9119.82 (14)
O6—C18—C17126.11 (14)C6—C7—H7120.00
N7—C18—C17117.09 (12)C8—C7—H7120.00
O6—C18—N7116.80 (13)H7B—O7—H7C106.00
C1—N1—C5122.67 (13)C7—C8—H8120.00
C16—C17—H17119.00C9—C8—H8120.00
C18—C17—H17119.00N3—C10—H10120.00
N1—C1—N2119.38 (14)C9—C10—H10120.00
N1—C1—C2117.72 (14)H8B—O8—H8C103.00
N2—C1—C2122.90 (14)H9A—O9—H9B103.00
C5—N1—H1119.00H10A—O10—H10B109.00
C14—N5—C11—O1176.94 (14)C16—C17—C18—O6177.54 (14)
C14—N5—C11—N63.5 (2)C16—C17—C18—N72.7 (2)
C11—N5—C14—O3177.60 (13)C5—N1—C1—N2178.47 (14)
C11—N5—C14—C133.6 (2)C5—N1—C1—C21.7 (2)
C12—N6—C11—O1179.22 (14)C1—N1—C5—C40.9 (2)
C12—N6—C11—N50.4 (2)N1—C1—C2—C31.2 (2)
C11—N6—C12—O2175.86 (14)N2—C1—C2—C3178.93 (14)
C11—N6—C12—C133.7 (2)C1—C2—C3—C40.0 (2)
O2—C12—C13—C14176.03 (14)C2—C3—C4—Cl1178.85 (11)
N6—C12—C13—C143.5 (2)C2—C3—C4—C50.8 (2)
C12—C13—C14—O3178.55 (14)Cl1—C4—C5—N1179.26 (11)
C12—C13—C14—N50.1 (2)C3—C4—C5—N10.4 (2)
C18—N7—C15—O4177.42 (14)C10—N3—C6—N4179.28 (14)
C18—N7—C15—N82.4 (2)C10—N3—C6—C70.1 (2)
C15—N7—C18—O6177.04 (14)C6—N3—C10—C90.9 (2)
C15—N7—C18—C173.2 (2)N3—C6—C7—C80.5 (3)
C16—N8—C15—O4178.69 (14)N4—C6—C7—C8179.89 (17)
C16—N8—C15—N71.1 (2)C6—C7—C8—C90.4 (3)
C15—N8—C16—O5178.53 (14)C7—C8—C9—Cl2178.93 (15)
C15—N8—C16—C170.7 (2)C7—C8—C9—C100.4 (3)
O5—C16—C17—C18177.64 (14)Cl2—C9—C10—N3178.31 (11)
N8—C16—C17—C181.6 (2)C8—C9—C10—N31.0 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O60.871.852.7207 (18)176
N2—H2A···O10.892.022.7461 (18)138
N2—H2B···O5i0.891.872.7610 (17)180
N3—H3A···O30.861.832.6863 (18)177
N4—H4A···O40.872.002.7248 (18)139
N4—H4B···O2ii0.891.972.8606 (17)173
N5—H5A···O60.872.022.8786 (17)173
N6—H6···O4i0.892.032.9005 (17)170
N7—H7A···O30.872.062.8985 (17)163
N8—H8A···O1ii0.882.012.8762 (16)172
O7—H7B···O50.861.922.7581 (16)164
O7—H7C···O2iii0.822.132.9155 (18)160
O8—H8B···O100.861.892.739 (2)167
O8—H8C···O20.891.912.7810 (16)165
O9—H9A···O80.861.932.7864 (18)168
O10—H10B···O7iii0.871.962.8287 (18)175
C10—H10···O7iii0.952.443.321 (2)153
Symmetry codes: (i) x, y+1/2, z1/2; (ii) x, y+1/2, z+1/2; (iii) x+1, y+1/2, z+3/2.
 

References

Return to citationAkriche, S. & Rzaigui, M. (2005). Acta Cryst. E61, o2607–o2609.  Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
Return to citationAnantheeswary, T. R., Gomathi, S., Shyamaladevi, R., Jegan Jennifer, S. & Abdul Razak, I. (2024). IUCrData 9, x241120.  Google Scholar
Return to citationBauer, M. & Spange, S. (2010). Eur. J. Org. Chem. pp. 259–264.  Web of Science CrossRef Google Scholar
Return to citationCason, C. J. (2004). POV-RAY for Windows. Persistence of Vision, Raytracer Pvt. Ltd, Victoria, Australia. http://www.povray.org.  Google Scholar
Return to citationChang, S. K. & Hamilton, A. D. (1988). J. Am. Chem. Soc. 110, 1318–1319.  CrossRef CAS Web of Science Google Scholar
Return to citationGelbrich, T., Meischberger, I. & Griesser, U. J. (2015). Acta Cryst. C71, 204–210.  Web of Science CSD CrossRef IUCr Journals Google Scholar
Return to citationHanif, M., Khan, E., Khalid, M., Tahir, M. N., Morais, S. F. A. & Braga, A. A. C. (2020). J. Mol. Struct. 1222, 128914–128914.  Web of Science CSD CrossRef CAS Google Scholar
Return to citationHemamalini, M. & Fun, H.-K. (2010). Acta Cryst. E66, o783–o784.  Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
Return to citationHueso Ureña, F., Illán-Cabeza, N. A., Moreno-Carretero, M. N., Martínez-Martos, J. M. & Ramírez-Expósito, M. J. (2003). J. Inorg. Biochem. 94, 326–334.  Web of Science PubMed Google Scholar
Return to citationInfantes, L. & Motherwell, S. (2002). CrystEngComm 4, 454–461.  Web of Science CrossRef CAS Google Scholar
Return to citationJagan, R. & Boopathi, K. (2020). Zh. Strukt. Khim. 61, 147–156.  Google Scholar
Return to citationJayanalina, T., Rajarajan, G., Boopathi, K. & Sreevani, K. (2015). J. Cryst. Growth 426, 9–14.  Web of Science CSD CrossRef CAS Google Scholar
Return to citationKvick, Å. & Backéus, M. (1974). Acta Cryst. B30, 474–480.  CSD CrossRef CAS IUCr Journals Web of Science Google Scholar
Return to citationMacrae, C. F., Sovago, I., Cottrell, S. J., Galek, P. T. A., McCabe, P., Pidcock, E., Platings, M., Shields, G. P., Stevens, J. S., Towler, M. & Wood, P. A. (2020). J. Appl. Cryst. 53, 226–235.  Web of Science CrossRef CAS IUCr Journals Google Scholar
Return to citationRigaku OD (2019). CrysAlis PRO. Rigaku Oxford Diffraction, Yarnton, England.  Google Scholar
Return to citationSheldrick, G. M. (2015a). Acta Cryst. A71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSheldrick, G. M. (2015b). Acta Cryst. C71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSpek, A. L. (2020). Acta Cryst. E76, 1–11.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationWestrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.  Web of Science CrossRef CAS IUCr Journals Google Scholar
Return to citationZaouali Zgolli, D., Boughzala, H. & Driss, A. (2009). Acta Cryst. E65, o2755.  Web of Science CSD CrossRef IUCr Journals Google Scholar

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