Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Jul 25;68(Pt 8):o2555. doi: 10.1107/S1600536812033387

Bis(melaminium) succinate succinic acid monosolvate dihydrate

Barbara Froschauer a, Matthias Weil b,*
PMCID: PMC3414998  PMID: 22904985

Abstract

The asymmetric unit of the solvated title salt, 2C3H7N6 +·C4H4O4 2−·C4H6O4·2H2O, contains one essentially planar melaminium (2,4,6-triamino-1,3,5-triazin-1-ium) cation (r.m.s. deviation of the non-H atoms = 0.0097 Å), one-half of a succinate anion, one-half of a succinic acid solvent mol­ecule and one water molecule of crystallization; full mol­ecules are generated by inversion symmetry. Supra­molecular layers parallel to (12-1) are formed through extensive inter­molecular hydrogen bonding of the types O—H⋯O, N—H⋯N and N—H⋯O between the components.

Related literature  

For the use of melaminium salts in polymer science, see: Weinstabl et al. (2001). For a list of structurally determined melaminium salts of purely organic carb­oxy­lic acids, see: Froschauer & Weil (2012).graphic file with name e-68-o2555-scheme1.jpg

Experimental  

Crystal data  

  • 2C3H7N6 +·C4H4O4 2−·C4H6O4·2H2O

  • M r = 524.48

  • Triclinic, Inline graphic

  • a = 7.1193 (7) Å

  • b = 8.1650 (8) Å

  • c = 9.5595 (9) Å

  • α = 88.013 (2)°

  • β = 84.647 (2)°

  • γ = 88.093 (2)°

  • V = 552.68 (9) Å3

  • Z = 1

  • Mo Kα radiation

  • μ = 0.13 mm−1

  • T = 293 K

  • 0.23 × 0.18 × 0.12 mm

Data collection  

  • Siemens SMART CCD diffractometer

  • 5533 measured reflections

  • 2719 independent reflections

  • 1545 reflections with I > 2σ(I)

  • R int = 0.028

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.047

  • wR(F 2) = 0.142

  • S = 0.97

  • 2719 reflections

  • 173 parameters

  • 3 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.30 e Å−3

  • Δρmin = −0.26 e Å−3

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2006) and ATOMS (Dowty, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812033387/cv5324sup1.cif

e-68-o2555-sup1.cif (21KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812033387/cv5324Isup2.hkl

e-68-o2555-Isup2.hkl (133.5KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812033387/cv5324Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N4—H3⋯N2i 0.86 2.10 2.959 (2) 176
N1—H1⋯O1 0.86 2.01 2.844 (2) 164
N5—H4⋯O3ii 0.86 2.13 2.976 (2) 170
N6—H6⋯N3iii 0.86 2.16 3.015 (2) 173
N1—H1⋯O2 0.86 2.50 3.199 (2) 138
N4—H2⋯O3iv 0.86 2.14 2.799 (2) 134
N4—H2⋯O1 0.86 2.56 3.268 (2) 141
N6—H7⋯O2 0.86 1.94 2.782 (2) 166
N5—H5⋯O1W v 0.86 2.11 2.912 (2) 154
O1W—H1W⋯O4 0.88 (2) 2.35 (2) 3.195 (2) 162 (3)
O1W—H2W⋯O2vi 0.86 (2) 1.89 (2) 2.726 (2) 167 (3)
O4—H12⋯O1iv 1.02 (2) 1.55 (2) 2.5673 (19) 177 (3)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic; (v) Inline graphic; (vi) Inline graphic.

Acknowledgments

The X-ray centre of the Vienna University of Technology is acknowledged for financial support and for providing access to the single-crystal diffractometer.

supplementary crystallographic information

Comment

The potential substitution of melamine through organic melaminium salts for production of melamine urea formaldehyde (MUF) resins (Weinstabl et al., 2001) render the structural investigation of these compounds interesting. A list of already determined structures of purely organic melaminium salts has been compiled recently by Froschauer & Weil (2012).

The pKa values of 4.21 and 5.72 for the first and second deprotonation step of succinic acid (the pKa of the first deprotonation step of melamine is 5.10) led to a doubly deprotonated anion in the title compound, bis-melaminium succinate succinic acid solvate dihydrate, 2(C3H7N6)+.C4H4O4-.C4H6O4.2(H2O). However, besides lattice water, there is also one succinic acid solvent molecule present in the unit cell. The succinic acid molecule and the succinate anion are located with their central C—C bond on inversion centres. As observed for all single protonated melaminium cations, the protonation of melamine takes place at one of the triazine N ring atoms (Fig. 1).

The melaminium cation is essentially planar with a r.m.s. deviation of 0.0097 Å. Likewise, the anion (r.m.s. deviation 0.039 Å) and the succinic acid molecule (r.m.s. deviation 0.060 Å) can be considered as planar. The angles between the least-squares planes of 6.59 (9) ° and 5.76 (12) ° between the anion and the cation and the succinic acid molecule, respectively, lead to the formation of supramolecular layers where cations are arranged in rows alternating with rows of anions, succinic acid solvent and lattice water molecules (Fig. 2). Extensive intermolecular hydrogen bonding of the types O—H···O, N—H···N and N—H···O between the molecular components is present. Details are reported in Table 1. The motif for the hydrogen-bonded assembly of two melaminium cations in such a layer is the same as in the hydrogenmalonate salt and other melaminium salts (Froschauer & Weil, 2012). In the crystal, the supramolecular layers are arranged parallel to (121) (Fig. 3) with an interplanar distance of approximately 3.15 Å.

Experimental

79.3 mmol melamine was dissolved under refluxing conditions in 200 ml distilled water. The stoichiometric quantity (1:1) of succinic acid was added within five minutes. The mixture was then refluxed for 30 minutes and then cooled to room temperature. The precipitate formed on cooling was separeted by filtration and washed with cold methanol. The crystalline product was then dried in vacuo at 303–313 K. Single crystal growth was accomplished by dissolution of 1 g of the crystalline product under refluxing conditions in an aqueous methanol solution (2:1 v/v) to get a saturated solution. Then the solution was slowly cooled down to room temperature. Suitable crystals were obtained by slow evaporation of the solvents during five days. The crystals were washed with methanol and dried in vacuo at room temperature giving analytical pure samples. CHN analysis (found/calc.): C (32.13/32.10), H (5.50/5.38), N (31.93/32.05). NMR: (solution, DMSO) chemical shift [p.p.m.]: 1H 10.37 (s, 2H), 6.22 (s, 6H), 2.39 (s, 4H); 13C 174.32, 166.43, 29.29.

Refinement

The proton at the triazine ring of the melaminium cation was clearly discernible from a difference Fourier map (like all other H atoms). For refinement, the H atoms attached to C or N atoms were set in calculated positions and treated as riding on their parent atoms with C—H = 0.97 Å and N—H = 0.86 Å and with Uiso(H) = 1.2Ueq(C,N). The proton of the carboxy group of the succinic acid solvent molecule was refined with a distance restraint O—H = 1.00 (2) Å; H atoms of the water molecule were likewise refined with a distance restraint of O—H = 0.88 (2) Å.

Figures

Fig. 1.

Fig. 1.

The molecular components of the title compound drawn with atomic displacement factors at the 90% probability level. H atoms are displayed as spheres with an arbirtary radius. For the centrosymmetric succinate anion and the succinic acid solvent molecule the symmetry-equivalent atoms are not labelled.

Fig. 2.

Fig. 2.

Supramolecular layer built up through hydrogen bonding interactions (dashed lines) between the molecular components.

Fig. 3.

Fig. 3.

The assembly of supramolecular layers in the crystal parallel to (121).

Crystal data

2C3H7N6+·C4H4O42·C4H6O4·2H2O Z = 1
Mr = 524.48 F(000) = 276
Triclinic, P1 Dx = 1.576 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 7.1193 (7) Å Cell parameters from 1570 reflections
b = 8.1650 (8) Å θ = 2.5–28.8°
c = 9.5595 (9) Å µ = 0.13 mm1
α = 88.013 (2)° T = 293 K
β = 84.647 (2)° Parallelepiped, colourless
γ = 88.093 (2)° 0.23 × 0.18 × 0.12 mm
V = 552.68 (9) Å3

Data collection

Siemens SMART CCD diffractometer 1545 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.028
Graphite monochromator θmax = 28.3°, θmin = 2.1°
ω scans h = −9→9
5533 measured reflections k = −10→10
2719 independent reflections l = −12→12

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.047 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.142 w = 1/[σ2(Fo2) + (0.0791P)2] where P = (Fo2 + 2Fc2)/3
S = 0.97 (Δ/σ)max < 0.001
2719 reflections Δρmax = 0.30 e Å3
173 parameters Δρmin = −0.26 e Å3
3 restraints Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.010 (4)

Special details

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)

x y z Uiso*/Ueq
N3 0.3081 (2) 1.0330 (2) 0.36672 (15) 0.0308 (4)
N1 0.4064 (2) 0.8895 (2) 0.16163 (15) 0.0323 (4)
H1 0.4894 0.8279 0.1160 0.039*
O1 0.62741 (19) 0.68205 (18) −0.02657 (14) 0.0385 (4)
O3 0.6682 (2) 0.2996 (2) 0.25900 (15) 0.0456 (4)
O2 0.8071 (2) 0.6984 (2) 0.14806 (15) 0.0480 (5)
O4 0.3997 (2) 0.44613 (19) 0.26505 (14) 0.0431 (4)
C7 0.5535 (3) 0.3930 (3) 0.3191 (2) 0.0309 (5)
C1 0.2450 (3) 0.9365 (2) 0.10469 (19) 0.0284 (4)
N2 0.1121 (2) 1.0287 (2) 0.17327 (15) 0.0305 (4)
C2 0.1488 (3) 1.0729 (2) 0.30373 (18) 0.0281 (4)
C6 0.5839 (3) 0.4567 (3) 0.46117 (19) 0.0339 (5)
H6A 0.6871 0.5321 0.4491 0.041*
H6B 0.6233 0.3651 0.5200 0.041*
N4 0.2251 (2) 0.8874 (2) −0.02317 (16) 0.0370 (4)
H3 0.1250 0.9151 −0.0632 0.044*
H2 0.3123 0.8277 −0.0664 0.044*
N6 0.5975 (2) 0.8950 (2) 0.34112 (18) 0.0402 (5)
H6 0.6226 0.9242 0.4228 0.048*
H7 0.6778 0.8356 0.2909 0.048*
C3 0.4365 (3) 0.9412 (2) 0.29314 (19) 0.0301 (5)
C4 0.7771 (3) 0.6435 (2) 0.0324 (2) 0.0308 (5)
N5 0.0177 (2) 1.1639 (2) 0.37353 (17) 0.0396 (5)
H5 0.0347 1.1959 0.4561 0.048*
H4 −0.0848 1.1912 0.3365 0.048*
O1W 0.0343 (3) 0.6661 (3) 0.36216 (18) 0.0637 (6)
H1W 0.126 (4) 0.591 (3) 0.353 (3) 0.097*
H2W −0.024 (4) 0.667 (4) 0.288 (2) 0.097*
H12 0.385 (4) 0.393 (3) 0.171 (2) 0.097*
C5 0.9192 (3) 0.5292 (3) −0.04228 (19) 0.0306 (5)
H5A 0.9717 0.5841 −0.1280 0.037*
H5B 0.8543 0.4341 −0.0690 0.037*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N3 0.0277 (9) 0.0441 (10) 0.0218 (8) 0.0109 (8) −0.0092 (7) −0.0101 (7)
N1 0.0283 (9) 0.0444 (10) 0.0248 (8) 0.0147 (8) −0.0070 (7) −0.0131 (7)
O1 0.0295 (8) 0.0537 (10) 0.0344 (8) 0.0173 (7) −0.0150 (6) −0.0151 (7)
O3 0.0392 (9) 0.0659 (11) 0.0337 (8) 0.0230 (8) −0.0151 (7) −0.0236 (7)
O2 0.0455 (9) 0.0664 (11) 0.0351 (8) 0.0258 (8) −0.0193 (7) −0.0285 (8)
O4 0.0381 (9) 0.0635 (11) 0.0303 (8) 0.0209 (7) −0.0178 (6) −0.0191 (7)
C7 0.0278 (10) 0.0395 (12) 0.0261 (9) 0.0081 (9) −0.0067 (8) −0.0069 (8)
C1 0.0269 (10) 0.0366 (11) 0.0222 (9) 0.0051 (8) −0.0061 (8) −0.0061 (8)
N2 0.0281 (9) 0.0428 (10) 0.0217 (8) 0.0076 (7) −0.0085 (7) −0.0097 (7)
C2 0.0250 (10) 0.0386 (11) 0.0215 (9) 0.0063 (8) −0.0062 (8) −0.0067 (8)
C6 0.0296 (11) 0.0479 (13) 0.0257 (10) 0.0076 (9) −0.0106 (8) −0.0085 (9)
N4 0.0332 (9) 0.0548 (12) 0.0245 (8) 0.0131 (8) −0.0107 (7) −0.0169 (8)
N6 0.0330 (10) 0.0596 (12) 0.0295 (9) 0.0231 (9) −0.0130 (7) −0.0173 (8)
C3 0.0301 (10) 0.0372 (12) 0.0243 (9) 0.0055 (9) −0.0095 (8) −0.0070 (8)
C4 0.0282 (10) 0.0357 (11) 0.0294 (10) 0.0105 (9) −0.0083 (8) −0.0083 (8)
N5 0.0322 (9) 0.0630 (13) 0.0255 (8) 0.0174 (9) −0.0127 (7) −0.0182 (8)
O1W 0.0646 (12) 0.0902 (15) 0.0408 (9) 0.0294 (10) −0.0287 (8) −0.0315 (9)
C5 0.0299 (10) 0.0388 (12) 0.0243 (9) 0.0108 (9) −0.0087 (8) −0.0104 (8)

Geometric parameters (Å, º)

N3—C3 1.328 (2) C6—H6A 0.9700
N3—C2 1.358 (2) C6—H6B 0.9700
N1—C1 1.356 (2) N4—H3 0.8600
N1—C3 1.378 (2) N4—H2 0.8600
N1—H1 0.8600 N6—C3 1.313 (2)
O1—C4 1.277 (2) N6—H6 0.8600
O3—C7 1.217 (2) N6—H7 0.8600
O2—C4 1.246 (2) C4—C5 1.500 (3)
O4—C7 1.309 (2) N5—H5 0.8600
O4—H12 1.023 (17) N5—H4 0.8600
C7—C6 1.507 (3) O1W—H1W 0.882 (17)
C1—N4 1.321 (2) O1W—H2W 0.856 (18)
C1—N2 1.328 (2) C5—C5ii 1.522 (3)
N2—C2 1.361 (2) C5—H5A 0.9700
C2—N5 1.319 (2) C5—H5B 0.9700
C6—C6i 1.514 (4)
C3—N3—C2 115.93 (15) C1—N4—H2 120.0
C1—N1—C3 119.48 (16) H3—N4—H2 120.0
C1—N1—H1 120.3 C3—N6—H6 120.0
C3—N1—H1 120.3 C3—N6—H7 120.0
C7—O4—H12 111.6 (17) H6—N6—H7 120.0
O3—C7—O4 122.87 (17) N6—C3—N3 122.22 (17)
O3—C7—C6 121.05 (18) N6—C3—N1 116.61 (17)
O4—C7—C6 116.07 (17) N3—C3—N1 121.17 (17)
N4—C1—N2 120.96 (17) O2—C4—O1 121.88 (17)
N4—C1—N1 117.14 (17) O2—C4—C5 120.22 (17)
N2—C1—N1 121.90 (16) O1—C4—C5 117.90 (16)
C1—N2—C2 115.70 (16) C2—N5—H5 120.0
N5—C2—N3 117.76 (16) C2—N5—H4 120.0
N5—C2—N2 116.44 (16) H5—N5—H4 120.0
N3—C2—N2 125.80 (17) H1W—O1W—H2W 107 (3)
C7—C6—C6i 116.3 (2) C4—C5—C5ii 115.00 (19)
C7—C6—H6A 108.2 C4—C5—H5A 108.5
C6i—C6—H6A 108.2 C5ii—C5—H5A 108.5
C7—C6—H6B 108.2 C4—C5—H5B 108.5
C6i—C6—H6B 108.2 C5ii—C5—H5B 108.5
H6A—C6—H6B 107.4 H5A—C5—H5B 107.5
C1—N4—H3 120.0

Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+2, −y+1, −z.

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N4—H3···N2iii 0.86 2.10 2.959 (2) 176
N1—H1···O1 0.86 2.01 2.844 (2) 164
N5—H4···O3iv 0.86 2.13 2.976 (2) 170
N6—H6···N3v 0.86 2.16 3.015 (2) 173
N1—H1···O2 0.86 2.50 3.199 (2) 138
N4—H2···O3vi 0.86 2.14 2.799 (2) 134
N4—H2···O1 0.86 2.56 3.268 (2) 141
N6—H7···O2 0.86 1.94 2.782 (2) 166
N5—H5···O1Wvii 0.86 2.11 2.912 (2) 154
O1W—H1W···O4 0.88 (2) 2.35 (2) 3.195 (2) 162 (3)
O1W—H2W···O2viii 0.86 (2) 1.89 (2) 2.726 (2) 167 (3)
O4—H12···O1vi 1.02 (2) 1.55 (2) 2.5673 (19) 177 (3)

Symmetry codes: (iii) −x, −y+2, −z; (iv) x−1, y+1, z; (v) −x+1, −y+2, −z+1; (vi) −x+1, −y+1, −z; (vii) −x, −y+2, −z+1; (viii) x−1, y, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CV5324).

References

  1. Dowty, E. (2006). ATOMS Shape Software, Kingsport, Tennessee, USA.
  2. Froschauer, B. & Weil, M. (2012). Acta Cryst. E68, o2553–o2554. [DOI] [PMC free article] [PubMed]
  3. Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453–457.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Siemens (1996). SMART and SAINT Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.
  6. Weinstabl, A., Binder, W. H., Gruber, H. & Kantner, W. (2001). J. Appl. Polym. Sci. 81, 1654–1661.
  7. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812033387/cv5324sup1.cif

e-68-o2555-sup1.cif (21KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812033387/cv5324Isup2.hkl

e-68-o2555-Isup2.hkl (133.5KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812033387/cv5324Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

RESOURCES