supplementary materials


Acta Cryst. (2008). E64, o1893    [ doi:10.1107/S1600536808028146 ]

4-Amino-3,5-dimethyl-4H1-,2,4-triazole-water (2/3)

L. Cheng, Y.-W. Zhang, Y.-Y. Sun and G. Xu

Abstract top

The asymmetric unit of the title compound, 2C4H8N4·3H2O, contains two crystallographically independent 4-amino-3,5-dimethyl-1,2,4-triazole molecules and three water molecules. The structure exhibits N-H...O, O-H...N and O-H...O hydrogen bonds.

Comment top

The derivatives of 4-amino-1,2,4-triazoles have considerable importance in medicinal chemistry, agricultural and industrial chemistry (Bentiss et al. 1999; Collin et al. 2003; Curtis et al. 2004). They have also been used as multidentate ligands in coordination chemistry (Beckmann et al. 2003). Here, we report a hydrated 4-amino-1,2,4-triazole (mta)2.3H2O (mta = 4-amino-3,5-dimethyl-1,2,4-triazole).

The asymmetric unit of the title compound contains two crystallographically independent mta molecules and three water molecules. The CN—N—C fragments of the tetrazine rings have the CN distances of 1.299 (2), 1.300 (2) and 1.304 (2) Å, and the N—N distances of 1.392 (2) and 1.389 (2) Å. All other C—N distances are between 1.352 (2) and 1.362 (2) Å, which are considered to have part double-bond character. In the crystalline state, the mta and crystal water molecules are linked together by N—H···O, O—H···N and O—H···O hydrogen bonding.

Related literature top

For related structures, see: Wang et al. (2006); Zachara et al. 2004). For related literature, see: Beckmann & Brooker (2003); Bentiss et al. (1999); Collin et al. (2003); Curtis (2004).

Experimental top

To a solution of mta (mta = 4-amino-3,5-dimethyl-1,2,4-triazole) (0.0228 g, 0.2 mmol) in CH3OH (5 ml), an aqueous solution (5 ml) of MnSO4.H2O (0.0169 g, 0.1 mmol) was added. The mixture was stirred for half an hour and filtered. The filtrate was allowed to evaporate slowly at room temperature. After several days, colorless block crystals were obtained in 5% yield (0.0007 g) based on mta.

Refinement top

H atoms bonded to O and N atoms were located in a difference map and freely refined. Other H atoms were positioned geometrically and refined using a riding model with C—H = 0.96 Å and with Uiso(H) = 1.5Uiso(C).

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SMART (Bruker, 2000); data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The asymmetric unit of the title compound with 30% thermal ellipsoids.
[Figure 2] Fig. 2. The three-dimensional supramolecular network of the title compound. The H atoms bonded to C atoms are omitted for clarity.
4-Amino-3,5-dimethyl-4H-1,2,4-triazole–water (2/3) top
Crystal data top
2C4H8N4·3H2OZ = 2
Mr = 278.34F(000) = 300
Triclinic, P1Dx = 1.225 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 7.194 (4) ÅCell parameters from 785 reflections
b = 8.680 (4) Åθ = 2.4–28.0°
c = 13.592 (7) ŵ = 0.10 mm1
α = 72.332 (8)°T = 293 K
β = 84.993 (8)°Block, colourless
γ = 68.936 (7)°0.20 × 0.18 × 0.17 mm
V = 754.5 (6) Å3
Data collection top
Bruker APEX CCD
diffractometer
2904 independent reflections
Radiation source: fine-focus sealed tube2447 reflections with I > 2σ(I)
graphiteRint = 0.014
φ and ω scanθmax = 26.0°, θmin = 2.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2000)
h = 88
Tmin = 0.981, Tmax = 0.984k = 1010
5166 measured reflectionsl = 1612
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.049H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.137 w = 1/[σ2(Fo2) + (0.0782P)2 + 0.0952P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
2904 reflectionsΔρmax = 0.27 e Å3
213 parametersΔρmin = 0.22 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.151 (12)
Crystal data top
2C4H8N4·3H2Oγ = 68.936 (7)°
Mr = 278.34V = 754.5 (6) Å3
Triclinic, P1Z = 2
a = 7.194 (4) ÅMo Kα radiation
b = 8.680 (4) ŵ = 0.10 mm1
c = 13.592 (7) ÅT = 293 K
α = 72.332 (8)°0.20 × 0.18 × 0.17 mm
β = 84.993 (8)°
Data collection top
Bruker APEX CCD
diffractometer
2904 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2000)
2447 reflections with I > 2σ(I)
Tmin = 0.981, Tmax = 0.984Rint = 0.014
5166 measured reflectionsθmax = 26.0°
Refinement top
R[F2 > 2σ(F2)] = 0.049H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.137Δρmax = 0.27 e Å3
S = 1.03Δρmin = 0.22 e Å3
2904 reflectionsAbsolute structure: ?
213 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
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
C10.2307 (2)0.21698 (19)0.03818 (12)0.0464 (4)
C20.2155 (3)0.3435 (2)0.09351 (15)0.0675 (5)
H2A0.21950.44870.04480.101*
H2B0.32490.29730.14220.101*
H2C0.09220.36660.12950.101*
C30.2508 (2)0.02273 (19)0.01050 (12)0.0450 (4)
C40.2584 (3)0.2021 (2)0.02881 (14)0.0574 (4)
H4A0.27430.22870.03570.086*
H4B0.13690.21340.05960.086*
H4C0.36910.28050.07440.086*
C50.2491 (2)0.3310 (2)0.54342 (13)0.0518 (4)
C60.2507 (4)0.2018 (3)0.59340 (17)0.0790 (6)
H6A0.26330.09470.54160.119*
H6B0.36120.18430.63890.119*
H6C0.12860.24210.63240.119*
C70.2362 (2)0.5735 (2)0.52294 (12)0.0500 (4)
C80.2197 (3)0.7564 (2)0.54624 (15)0.0691 (5)
H8A0.22590.78210.48300.104*
H8B0.09510.83040.58170.104*
H8C0.32740.77520.58920.104*
N10.2638 (2)0.08533 (18)0.07827 (10)0.0528 (4)
N20.2508 (2)0.23853 (17)0.06052 (10)0.0533 (4)
N30.22893 (18)0.05496 (15)0.08561 (9)0.0433 (3)
N40.2136 (3)0.02566 (19)0.19138 (10)0.0543 (4)
H4D0.100 (3)0.047 (3)0.2139 (15)0.071 (6)*
H4E0.320 (3)0.030 (3)0.2220 (15)0.071 (6)*
N50.2546 (2)0.46293 (18)0.43183 (10)0.0568 (4)
N60.2637 (2)0.30785 (18)0.44498 (11)0.0579 (4)
N70.2326 (2)0.49581 (17)0.59485 (9)0.0511 (4)
N80.2096 (4)0.5651 (3)0.70320 (12)0.0790 (6)
H8D0.105 (4)0.659 (4)0.710 (2)0.109 (10)*
H8E0.325 (5)0.589 (4)0.726 (2)0.119 (10)*
O1W0.1595 (3)0.1723 (3)0.26863 (18)0.1022 (7)
H1WA0.219 (5)0.280 (4)0.254 (2)0.132 (12)*
H1WB0.248 (5)0.128 (4)0.254 (2)0.131 (11)*
O2W0.3524 (2)0.47375 (18)0.23848 (12)0.0706 (4)
H2WA0.308 (4)0.412 (3)0.186 (2)0.090 (7)*
H2WB0.308 (4)0.466 (3)0.296 (2)0.101 (8)*
O3W0.3962 (2)0.02300 (16)0.26616 (11)0.0610 (4)
H3WA0.341 (3)0.055 (3)0.2121 (18)0.079 (6)*
H3WB0.349 (4)0.114 (3)0.321 (2)0.093 (8)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0471 (8)0.0429 (8)0.0438 (8)0.0139 (6)0.0002 (6)0.0069 (6)
C20.0849 (13)0.0529 (10)0.0645 (11)0.0241 (9)0.0015 (10)0.0161 (9)
C30.0393 (7)0.0485 (8)0.0455 (8)0.0143 (6)0.0017 (6)0.0128 (7)
C40.0574 (10)0.0543 (10)0.0636 (11)0.0213 (8)0.0020 (8)0.0198 (8)
C50.0514 (9)0.0550 (9)0.0478 (9)0.0184 (7)0.0075 (7)0.0152 (7)
C60.0942 (15)0.0765 (13)0.0778 (14)0.0334 (11)0.0145 (11)0.0378 (11)
C70.0513 (9)0.0539 (9)0.0444 (9)0.0212 (7)0.0050 (7)0.0115 (7)
C80.0833 (13)0.0610 (11)0.0660 (12)0.0345 (10)0.0060 (10)0.0129 (9)
N10.0571 (8)0.0584 (8)0.0431 (7)0.0227 (6)0.0055 (6)0.0134 (6)
N20.0589 (8)0.0512 (8)0.0455 (8)0.0221 (6)0.0029 (6)0.0053 (6)
N30.0445 (7)0.0430 (7)0.0374 (7)0.0144 (5)0.0013 (5)0.0060 (5)
N40.0632 (9)0.0543 (8)0.0378 (7)0.0206 (7)0.0038 (7)0.0034 (6)
N50.0697 (9)0.0578 (8)0.0427 (8)0.0249 (7)0.0031 (6)0.0119 (6)
N60.0709 (9)0.0516 (8)0.0467 (8)0.0213 (7)0.0030 (6)0.0086 (6)
N70.0565 (8)0.0584 (8)0.0368 (7)0.0242 (6)0.0045 (6)0.0080 (6)
N80.1082 (16)0.0910 (14)0.0374 (8)0.0448 (13)0.0018 (9)0.0062 (8)
O1W0.0737 (10)0.0831 (12)0.170 (2)0.0312 (9)0.0195 (10)0.0655 (13)
O2W0.1040 (11)0.0668 (9)0.0514 (8)0.0482 (8)0.0005 (7)0.0090 (6)
O3W0.0781 (9)0.0496 (7)0.0488 (7)0.0161 (6)0.0067 (6)0.0143 (6)
Geometric parameters (Å, °) top
C1—N21.300 (2)C7—N71.352 (2)
C1—N31.362 (2)C7—C81.483 (2)
C1—C21.478 (2)C8—H8A0.9600
C2—H2A0.9600C8—H8B0.9600
C2—H2B0.9600C8—H8C0.9600
C2—H2C0.9600N1—N21.391 (2)
C3—N11.304 (2)N3—N41.4091 (18)
C3—N31.355 (2)N4—H4D0.93 (2)
C3—C41.482 (2)N4—H4E0.88 (2)
C4—H4A0.9600N5—N61.389 (2)
C4—H4B0.9600N7—N81.411 (2)
C4—H4C0.9600N8—H8D0.88 (3)
C5—N61.299 (2)N8—H8E0.93 (3)
C5—N71.354 (2)O1W—H1WA0.84 (3)
C5—C61.474 (3)O1W—H1WB0.92 (3)
C6—H6A0.9600O2W—H2WA0.87 (3)
C6—H6B0.9600O2W—H2WB0.90 (3)
C6—H6C0.9600O3W—H3WA0.88 (2)
C7—N51.299 (2)O3W—H3WB0.89 (3)
N2—C1—N3109.30 (14)N5—C7—C8126.38 (16)
N2—C1—C2126.85 (15)N7—C7—C8124.62 (15)
N3—C1—C2123.85 (15)C7—C8—H8A109.5
C1—C2—H2A109.5C7—C8—H8B109.5
C1—C2—H2B109.5H8A—C8—H8B109.5
H2A—C2—H2B109.5C7—C8—H8C109.5
C1—C2—H2C109.5H8A—C8—H8C109.5
H2A—C2—H2C109.5H8B—C8—H8C109.5
H2B—C2—H2C109.5C3—N1—N2107.78 (13)
N1—C3—N3109.02 (14)C1—N2—N1107.36 (12)
N1—C3—C4126.61 (15)C3—N3—C1106.55 (13)
N3—C3—C4124.37 (14)C3—N3—N4124.23 (13)
C3—C4—H4A109.5C1—N3—N4129.20 (13)
C3—C4—H4B109.5N3—N4—H4D106.6 (12)
H4A—C4—H4B109.5N3—N4—H4E105.8 (13)
C3—C4—H4C109.5H4D—N4—H4E109.1 (17)
H4A—C4—H4C109.5C7—N5—N6107.56 (14)
H4B—C4—H4C109.5C5—N6—N5107.64 (13)
N6—C5—N7108.89 (15)C7—N7—C5106.91 (14)
N6—C5—C6126.70 (17)C7—N7—N8129.47 (15)
N7—C5—C6124.41 (16)C5—N7—N8123.59 (15)
C5—C6—H6A109.5N7—N8—H8D102.0 (18)
C5—C6—H6B109.5N7—N8—H8E105.6 (17)
H6A—C6—H6B109.5H8D—N8—H8E112 (3)
C5—C6—H6C109.5H1WA—O1W—H1WB106 (3)
H6A—C6—H6C109.5H2WA—O2W—H2WB107 (2)
H6B—C6—H6C109.5H3WA—O3W—H3WB107 (2)
N5—C7—N7109.00 (15)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N4—H4D···O1W0.93 (2)2.00 (2)2.924 (3)170.9 (18)
N4—H4E···O3Wi0.88 (2)2.21 (2)3.078 (3)168.3 (18)
N8—H8E···O2Wii0.93 (3)2.23 (3)3.104 (3)156 (2)
O1W—H1WA···O2Wiii0.84 (3)1.95 (3)2.793 (3)173 (3)
O1W—H1WB···O3Wiv0.92 (3)1.93 (3)2.810 (2)160 (3)
O2W—H2WA···N20.87 (3)2.02 (3)2.885 (2)171 (2)
O2W—H2WB···N50.90 (3)1.93 (3)2.816 (2)168 (2)
O3W—H3WA···N10.88 (2)1.92 (2)2.787 (2)168 (2)
O3W—H3WB···N60.89 (3)1.93 (3)2.827 (2)176 (2)
Symmetry codes: (i) −x+1, −y, −z; (ii) −x+1, −y+1, −z−1; (iii) −x, −y+1, −z; (iv) −x, −y, −z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N4—H4D···O1W0.93 (2)2.00 (2)2.924 (3)170.9 (18)
N4—H4E···O3Wi0.88 (2)2.21 (2)3.078 (3)168.3 (18)
N8—H8E···O2Wii0.93 (3)2.23 (3)3.104 (3)156 (2)
O1W—H1WA···O2Wiii0.84 (3)1.95 (3)2.793 (3)173 (3)
O1W—H1WB···O3Wiv0.92 (3)1.93 (3)2.810 (2)160 (3)
O2W—H2WA···N20.87 (3)2.02 (3)2.885 (2)171 (2)
O2W—H2WB···N50.90 (3)1.93 (3)2.816 (2)168 (2)
O3W—H3WA···N10.88 (2)1.92 (2)2.787 (2)168 (2)
O3W—H3WB···N60.89 (3)1.93 (3)2.827 (2)176 (2)
Symmetry codes: (i) −x+1, −y, −z; (ii) −x+1, −y+1, −z−1; (iii) −x, −y+1, −z; (iv) −x, −y, −z.
Acknowledgements top

The authors thank the Program for Young Excellent Talents in Southeast University for financial support.

references
References top

Beckmann, U. & Brooker, S. (2003). Coord. Chem. Rev. 245, 17–29.

Bentiss, F., Lagrenee, M., Traisnel, M. & Hornez, J. C. (1999). Corros. Sci. 41, 789–803.

Bruker (2000). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.

Collin, X., Sauleau, A. & Coulon, J. (2003). Bioorg. Med. Chem. Lett. 13, 2601–2605.

Curtis, A. D. M. (2004). Sci. Synth., 13, 603–605.

Sheldrick, G. M. (2000). SADABS., University of Göttingen, Germany.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Wang, P., Ma, J. P., Huang, R.-Q. & Dong, Y.-B. (2006). Acta Cryst. E62, o2791–o2792.

Zachara, J., Madura, I. & Włostowski, M. (2004). Acta Cryst. C60, o57–o59.