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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2015 Dec 24;71(Pt 12):o1076–o1077. doi: 10.1107/S2056989015024317

Crystal structure of N,N,N′,N′,N′′,N′′-hexa­methyl­guanidinium cyanate 1.5-hydrate

Ioannis Tiritiris a, Willi Kantlehner a,*
PMCID: PMC4719987  PMID: 26870506

Abstract

The title hydrated salt, C7H18N3 +·OCN.1.5H2O, was synthesized starting from N,N,N′,N′,N′′,N′′-hexa­methyl­guanidinium chloride by a twofold anion-exchange reaction. The asymmetric unit contains two cations, two cyanate anions and three water mol­ecules. One cation shows orientational disorder and two sets of N-atom positions were found related by a 60° rotation, with an occupancy ratio of 0.852 (6):0.148 (6). The C—N bond lengths in both guanidin­ium ions range from 1.329 (2) to 1.358 (10) Å, indicating double-bond character, pointing towards charge delocalization within the NCN planes. Strong O—H⋯N hydrogen bonds between the crystal water mol­ecules and the cyanate ions and strong O—H⋯O hydrogen bonds between the water mol­ecules are present, resulting in a two-dimensional hydrogen bonded network running parallel to the (001) plane. The hexa­methyl­guanidinium ions are packed in between the layers built up by water mol­ecules and cyanate ions.

Keywords: crystal structure, cyanate, hexa­methyl­guanidinium, salt, O—H⋯O hydrogen bonds, O—H⋯N hydrogen bonds

Related literature  

For the synthesis of hexa­substituted guanidinium salts with different anions, see: Kantlehner et al. (1984). For the crystal structure of N,N,N′,N′,N′′,N′′-hexa­methyl­guanidinium chloride, see: Oelkers & Sundermeyer (2011). For the crystal structure of N,N,N′,N′,N′′,N′′-hexa­methyl­guanidinium di­fluoro­tri­methyl­silicate, see: Röschenthaler et al. (2002). For the crystal structure of N,N,N′,N′,N′′,N′′-hexa­methyl­guanidinium tetra­phenyl­borate, see: Frey et al. (1998). For the crystal structure of N,N,N′,N′,N′′,N′′-hexa­methyl­guanidinium fluoride, see: Kolomeitsev et al. (2000). For the crystal structure of N,N,N′,N′,N′′,N′′-hexa­methyl­guanidinium hexa­fluoro­silicate hexa­hydrate, see: Zhang et al. (1999). For the crystal structures of [C(NMe2)3][Mn(CO)5] and [C(NMe2)3][Co(CO)4], see: Petz & Weller (1991). For a neutron diffraction studie of deuterated ammonium cyanate, see: MacLean et al. (2003). For the use of intensity quotients and differences in absolute structure refinement, see: Parsons et al. (2013).graphic file with name e-71-o1076-scheme1.jpg

Experimental  

Crystal data  

  • 2C7H18N3 +·2CNO·3H2O

  • M r = 426.58

  • Monoclinic, Inline graphic

  • a = 8.3245 (5) Å

  • b = 22.536 (2) Å

  • c = 13.2580 (12) Å

  • β = 108.092 (7)°

  • V = 2364.2 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 100 K

  • 0.40 × 0.25 × 0.10 mm

Data collection  

  • Bruker Kappa APEXII DUO diffractometer

  • 19766 measured reflections

  • 5588 independent reflections

  • 5279 reflections with I > 2σ(I)

  • R int = 0.025

  • Standard reflections: 0

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.034

  • wR(F 2) = 0.089

  • S = 1.02

  • 5588 reflections

  • 328 parameters

  • 2 restraints

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

  • Δρmax = 0.40 e Å−3

  • Δρmin = −0.19 e Å−3

Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: DIAMOND (Brandenburg & Putz, 2005); software used to prepare material for publication: SHELXL2014.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S2056989015024317/rz5180sup1.cif

e-71-o1076-sup1.cif (600.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989015024317/rz5180Isup2.hkl

e-71-o1076-Isup2.hkl (306.3KB, hkl)

. DOI: 10.1107/S2056989015024317/rz5180fig1.tif

The structure of the title compound with displacement ellipsoids at the 50% probability level. All hydrogen atoms are omitted for clarity. Only the major component of the disordered cation is shown.

. DOI: 10.1107/S2056989015024317/rz5180fig2.tif

The structure of the orientationally disordered cation. The nitro­gen atoms are disordered between the opaque and dark positions.

c . DOI: 10.1107/S2056989015024317/rz5180fig3.tif

O—H⋯N and O—H⋯O hydrogen bonds (black dashed lines) between anions and water mol­ecules and between the water mol­ecules (view down the c axis).

c . DOI: 10.1107/S2056989015024317/rz5180fig4.tif

View down the c axis of the two-dimensional O—H⋯N and O—H⋯O hydrogen-bonding network (all hydrogen bonds are indicated by black dashed lines).

a . DOI: 10.1107/S2056989015024317/rz5180fig5.tif

Packing of the guanidinium ions in between the layers build up by water mol­ecules and cyanate ions (down the a axis).

CCDC reference: 867308

Additional supporting information: crystallographic information; 3D view; checkCIF report

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

D—H⋯A D—H H⋯A DA D—H⋯A
O3—H31⋯N2 0.78 (3) 2.00 (3) 2.780 (3) 176 (3)
O3—H32⋯O5i 0.86 (4) 2.00 (4) 2.858 (4) 172 (3)
O4—H42⋯O3ii 0.83 (4) 2.04 (4) 2.852 (4) 164 (3)
O4—H41⋯N1ii 0.84 (3) 2.00 (3) 2.833 (3) 173 (3)
O5—H51⋯O2iii 0.85 (3) 1.92 (3) 2.761 (3) 175 (3)
O5—H52⋯O1iv 0.74 (4) 2.10 (4) 2.840 (4) 177 (3)

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

Acknowledgments

The authors thank Dr W. Frey (Institut für Organische Chemie, Universität Stuttgart) for measuring the diffraction data.

supplementary crystallographic information

S1. Comment

The reaction of phosgene with N,N,N',N'-tetramethylurea yields N,N,N',N'-tetramethylchloroformamidinium chloride, which can be transformed by a mixture of dimethylamine and triethylamine into a mixture of N,N,N',N',N'',N''-hexamethylguanidinium chloride and triethylamine hydrochloride. Treating the salt mixture with an aqueous sodium hydroxide solution leads after work up to the pure guanidinium chloride. Conversion of the chloride to the tetrafluoroborate salt occurs by heating it with BF3O(C2H5)2 (Kantlehner et al., 1984). A further anion exchange was possible by reacting N,N,N',N',N'',N''-hexamethylguanidinium tetrafluoroborate with potassium cyanate in water. According to the structure analysis of the title compound, the asymmetric unit contains two N,N,N',N',N'',N''-hexamethylguanidinium (HMG+) ions, two cyanate ions and three water molecules (Fig. 1). One cation (cation I) shows an orientational disorder and two sets of N positions were found related by a 60° rotation, with an occupancy ratio of 0.852 (6):0.148 (6). This leads to the characteristic star-shaped appearance of the HMG+ ion (Fig. 2). The second cation (cation II) is not disordered. Searching for known crystal structures in literature of N,N,N',N',N'',N''-hexamethylguanidinium salts [see, for example: chloride salt (Oelkers & Sundermeyer, 2011), difluorotrimethylsilicate salt (Röschenthaler et al., 2002), tetraphenylborate salt (Frey et al., 1998), fluoride salt (Kolomeitsev et al., 2000), hexafluorosilicate hexahydrate salt (Zhang et al., 1999), [Mn(CO)5] and [Co(CO)4] salts (Petz & Weller, 1991)], it is obvious that in all those compounds the HMG+ ions are orientationally disordered too. In the title salt, the C–N bond lengths of both cations are in a range from 1.329 (2) and 1.358 (10) Å, indicating double bond character. The CN3 units are planar and the N–C–N angles are ranging from 118.0 (7)° to 121.8 (7)°. The positive charge is completely delocalized in the CN3 plane. The N–C bond lengths in the non-disordered guanidinium ion (cation II) are in a typical range from 1.453 (3) to 1.475 (2) Å, characteristic for a N–C single bond. In the disordered one (cation I), some N–C bond lengths deviate from their typical values and appear to be slightly longer [d(N–C) = 1.464 (3) − 1.655 (10) Å]. The N–C and C–O bond lengths in both cyanate ions [d(N–C) = 1.165 (3) and 1.172 (3) Å; d(C–O) = 1.213 (3) and 1.230 (3) Å] are in very good agreement with the data determined from a neutron diffraction study of deuterated ammonium cyanate (ND4OCN) at 14 K [d(N–C) = 1.191 (5) Å and d(C–O) =) 1.215 (5) Å (MacLean et al., 2003)]. Strong O–H···N hydrogen bonds between the crystal water molecules and the cyanate ions [d(H···N) = 2.00 (3) Å (Tab. 1)] and strong O–H···O hydrogen bonds between the water molecules are present [d(H···O) = 1.92 (3) − 2.10 (4) Å (Tab. 1)] (Fig. 3), resulting in a two-dimensional hydrogen bonded network parallel to the (0 0 1) plane (Fig. 4). Additionally, C–H···N and C–H···O interactions between the H atoms of the guanidinium –N(CH3)2 groups and the cyanate ions are present [d(H···N) = 2.52 – 2.61 Å; d(H···O) = 2.46 – 2.60 Å]. The hexamethylguanidinium ions are packed in between the layers build up by water molecules and cyanate ions (Fig. 5).

S2. Experimental

To a solution of 10 g (0.043 mol) N,N,N',N',N'',N''-hexamethylguanidinium tetrafluoroborate in water, 3.51 g (0.043 mol) potassium cyanate in 20 ml water was added. The solution was kept for twelve hours at 273 K and the precipitated potassium tetrafluoroborate was removed by filtration. After removing of the water, the residue was redissolved in acetonitrile and the solution was filtered again to remove the insoluble residue. The title compound crystallized from a saturated acetonitrile solution after several days at 273 K, forming colorless single crystals. Yield: 7.05 g (88%).

S3. Refinement

The O-bound H atoms of the water molecules were located in a difference Fourier map and were refined freely [O—H = 0.74 (4) − 0.86 (4) Å]. The atoms N6, N7 and N8 of one cation are disordered over two sets of sites (N6A, N7A and N8A; N6B, N7B and N8B) with refined occupancies of 0.862 (6):0.138 (6), 0.852 (6):0.148 (6) and 0.852 (6):0.148 (6). The title compound crystallizes in the non-centrosymmetric space group Cc; however, in the absence of significant anomalous scattering effects, the determined Flack parameter x = 0.2 (3) (Parsons et al., 2013) is essentially meaningless. The hydrogen atoms of the methyl groups were allowed to rotate with a fixed angle around the C–N bonds to best fit the experimental electron density, with Uiso(H) set to 1.5 Ueq(C) and d(C—H) = 0.98 Å.

Figures

Fig. 1.

Fig. 1.

The structure of the title compound with displacement ellipsoids at the 50% probability level. All hydrogen atoms are omitted for clarity. Only the major component of the disordered cation is shown.

Fig. 2.

Fig. 2.

The structure of the orientationally disordered cation. The nitrogen atoms are disordered between the opaque and dark positions.

Fig. 3.

Fig. 3.

O—H···N and O—H···O hydrogen bonds (black dashed lines) between anions and water molecules and between the water molecules (view down the c axis).

Fig. 4.

Fig. 4.

View down the c axis of the two-dimensional O—H···N and O—H···O hydrogen-bonding network (all hydrogen bonds are indicated by black dashed lines).

Fig. 5.

Fig. 5.

Packing of the guanidinium ions in between the layers build up by water molecules and cyanate ions (down the a axis).

Crystal data

2C7H18N3+·2CNO·3H2O F(000) = 936
Mr = 426.58 Dx = 1.199 Mg m3
Monoclinic, Cc Mo Kα radiation, λ = 0.71073 Å
a = 8.3245 (5) Å Cell parameters from 19766 reflections
b = 22.536 (2) Å θ = 1.8–28.4°
c = 13.2580 (12) Å µ = 0.09 mm1
β = 108.092 (7)° T = 100 K
V = 2364.2 (3) Å3 Block, colorless
Z = 4 0.40 × 0.25 × 0.10 mm

Data collection

Bruker Kappa APEXII DUO diffractometer 5279 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.025
Triumph monochromator θmax = 28.4°, θmin = 1.8°
φ scans, and ω scans h = −11→11
19766 measured reflections k = −29→30
5588 independent reflections l = −17→17

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.034 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.089 H atoms treated by a mixture of independent and constrained refinement
S = 1.02 w = 1/[σ2(Fo2) + (0.0493P)2 + 0.9721P] where P = (Fo2 + 2Fc2)/3
5588 reflections (Δ/σ)max < 0.001
328 parameters Δρmax = 0.40 e Å3
2 restraints Δρmin = −0.19 e Å3

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 Occ. (<1)
O1 0.3316 (2) 0.36058 (8) 0.23689 (17) 0.0409 (4)
C1 0.2204 (3) 0.32390 (9) 0.22404 (19) 0.0269 (4)
N1 0.1126 (3) 0.28850 (9) 0.2104 (2) 0.0397 (5)
C2 0.4331 (2) 0.02149 (8) 0.32420 (15) 0.0181 (4)
O2 0.5548 (2) −0.00567 (8) 0.38261 (13) 0.0316 (4)
N2 0.3167 (2) 0.04653 (9) 0.26863 (17) 0.0300 (4)
C3 0.1363 (2) 0.09910 (8) 0.52739 (14) 0.0150 (3)
N3 0.2570 (2) 0.05814 (7) 0.54024 (13) 0.0194 (3)
N4 −0.0178 (2) 0.08430 (7) 0.52842 (14) 0.0200 (3)
N5 0.1730 (2) 0.15661 (7) 0.51504 (14) 0.0206 (3)
C4 0.0955 (3) 0.20481 (9) 0.55702 (18) 0.0258 (4)
H4A 0.0156 0.2262 0.4982 0.039*
H4B 0.1835 0.2322 0.5974 0.039*
H4C 0.0355 0.1885 0.6037 0.039*
C5 0.2881 (3) 0.17368 (10) 0.45722 (18) 0.0245 (4)
H5A 0.3885 0.1925 0.5060 0.037*
H5B 0.2316 0.2017 0.4008 0.037*
H5C 0.3221 0.1383 0.4258 0.037*
C6 0.2163 (3) −0.00338 (8) 0.50317 (16) 0.0208 (4)
H6A 0.2274 −0.0294 0.5642 0.031*
H6B 0.2943 −0.0165 0.4655 0.031*
H6C 0.1001 −0.0052 0.4551 0.031*
C7 0.4348 (2) 0.07080 (9) 0.59433 (16) 0.0198 (4)
H7A 0.4983 0.0686 0.5433 0.030*
H7B 0.4799 0.0416 0.6508 0.030*
H7C 0.4458 0.1107 0.6251 0.030*
C8 −0.0467 (3) 0.03409 (10) 0.59113 (17) 0.0243 (4)
H8A −0.0926 0.0005 0.5440 0.036*
H8B −0.1274 0.0458 0.6279 0.036*
H8C 0.0604 0.0225 0.6434 0.036*
C9 −0.1698 (2) 0.11617 (9) 0.46464 (17) 0.0216 (4)
H9A −0.2186 0.1382 0.5118 0.032*
H9B −0.2528 0.0876 0.4229 0.032*
H9C −0.1391 0.1439 0.4167 0.032*
N6A 0.3149 (2) 0.16312 (8) 0.08657 (15) 0.0176 (5) 0.862 (6)
N7A 0.2872 (2) 0.16823 (8) −0.09169 (15) 0.0176 (5) 0.852 (6)
N8A 0.5332 (2) 0.13023 (8) 0.02745 (15) 0.0165 (5) 0.852 (6)
N6B 0.4372 (13) 0.1485 (5) −0.0765 (8) 0.011 (3) 0.138 (6)
N7B 0.2238 (14) 0.1787 (5) −0.0095 (9) 0.017 (3) 0.148 (6)
N8B 0.4759 (12) 0.1399 (4) 0.1027 (7) 0.011 (3) 0.148 (6)
C10 0.3786 (2) 0.15393 (7) 0.00727 (15) 0.0140 (3)
C11 0.1322 (3) 0.15698 (9) 0.0706 (2) 0.0257 (4)
H11A 0.0761 0.1414 −0.0007 0.038*
H11B 0.0846 0.1959 0.0784 0.038*
H11C 0.1146 0.1295 0.1236 0.038*
C12 0.4256 (3) 0.18015 (10) 0.19285 (17) 0.0286 (5)
H12A 0.5401 0.1874 0.1900 0.043*
H12B 0.4282 0.1480 0.2431 0.043*
H12C 0.3818 0.2163 0.2160 0.043*
C13 0.6009 (2) 0.08765 (9) 0.11404 (17) 0.0218 (4)
H13A 0.5138 0.0783 0.1471 0.033*
H13B 0.6992 0.1050 0.1672 0.033*
H13C 0.6349 0.0513 0.0857 0.033*
C14 0.6438 (3) 0.14659 (10) −0.0358 (2) 0.0318 (5)
H14A 0.5891 0.1775 −0.0868 0.048*
H14B 0.6643 0.1116 −0.0740 0.048*
H14C 0.7516 0.1615 0.0113 0.048*
C15 0.2985 (3) 0.13442 (10) −0.18353 (16) 0.0274 (4)
H15A 0.3685 0.0991 −0.1591 0.041*
H15B 0.3495 0.1592 −0.2261 0.041*
H15C 0.1849 0.1223 −0.2268 0.041*
C16 0.1731 (3) 0.22027 (9) −0.1124 (2) 0.0296 (5)
H16A 0.1823 0.2404 −0.0453 0.044*
H16B 0.0563 0.2071 −0.1455 0.044*
H16C 0.2051 0.2478 −0.1602 0.044*
O3 0.0041 (2) 0.08290 (7) 0.28078 (13) 0.0251 (3)
H31 0.090 (4) 0.0710 (12) 0.277 (2) 0.025 (7)*
H32 −0.055 (4) 0.0523 (16) 0.285 (3) 0.044 (9)*
O4 0.8891 (2) 0.20268 (8) 0.24797 (15) 0.0327 (4)
H41 0.962 (4) 0.2257 (13) 0.237 (2) 0.027 (7)*
H42 0.934 (5) 0.1695 (18) 0.250 (3) 0.054 (10)*
O5 0.8322 (2) 0.02166 (9) 0.81332 (15) 0.0330 (4)
H51 0.747 (4) 0.0190 (13) 0.835 (2) 0.031 (7)*
H52 0.833 (4) 0.0529 (16) 0.795 (3) 0.039 (9)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0293 (9) 0.0276 (8) 0.0665 (13) −0.0008 (7) 0.0161 (9) 0.0045 (8)
C1 0.0280 (10) 0.0187 (9) 0.0352 (12) 0.0088 (8) 0.0114 (9) 0.0042 (8)
N1 0.0375 (11) 0.0197 (9) 0.0630 (15) −0.0025 (8) 0.0172 (11) −0.0015 (9)
C2 0.0195 (9) 0.0180 (8) 0.0223 (9) −0.0058 (7) 0.0147 (7) −0.0039 (7)
O2 0.0260 (8) 0.0351 (9) 0.0356 (9) 0.0022 (7) 0.0123 (7) 0.0047 (7)
N2 0.0277 (9) 0.0340 (10) 0.0329 (10) 0.0041 (8) 0.0162 (8) 0.0065 (8)
C3 0.0180 (8) 0.0153 (8) 0.0111 (8) −0.0003 (6) 0.0038 (6) −0.0008 (6)
N3 0.0186 (8) 0.0171 (7) 0.0222 (8) −0.0009 (6) 0.0061 (6) −0.0008 (6)
N4 0.0209 (8) 0.0191 (8) 0.0218 (8) −0.0010 (6) 0.0090 (6) 0.0019 (6)
N5 0.0226 (8) 0.0166 (7) 0.0230 (8) −0.0009 (6) 0.0080 (6) 0.0006 (6)
C4 0.0331 (11) 0.0153 (9) 0.0274 (10) 0.0048 (7) 0.0069 (8) −0.0030 (8)
C5 0.0249 (10) 0.0244 (10) 0.0262 (10) −0.0068 (8) 0.0108 (8) 0.0029 (8)
C6 0.0278 (10) 0.0142 (8) 0.0219 (9) 0.0022 (7) 0.0102 (7) −0.0001 (7)
C7 0.0154 (8) 0.0209 (9) 0.0218 (9) −0.0004 (7) 0.0039 (7) −0.0006 (7)
C8 0.0252 (10) 0.0275 (10) 0.0247 (10) −0.0029 (8) 0.0142 (8) 0.0060 (8)
C9 0.0178 (9) 0.0231 (9) 0.0246 (10) 0.0021 (7) 0.0073 (7) −0.0004 (8)
N6A 0.0164 (10) 0.0201 (9) 0.0175 (10) −0.0003 (7) 0.0068 (7) −0.0014 (7)
N7A 0.0198 (9) 0.0179 (10) 0.0149 (9) 0.0020 (7) 0.0050 (7) 0.0007 (7)
N8A 0.0145 (9) 0.0168 (9) 0.0181 (9) 0.0002 (7) 0.0050 (7) −0.0002 (7)
N6B 0.013 (5) 0.017 (6) 0.006 (5) −0.001 (4) 0.006 (4) −0.001 (4)
N7B 0.016 (5) 0.016 (5) 0.024 (6) 0.006 (4) 0.014 (4) 0.005 (4)
N8B 0.016 (5) 0.012 (5) 0.003 (4) 0.000 (4) 0.003 (3) −0.001 (3)
C10 0.0148 (7) 0.0102 (7) 0.0163 (8) −0.0019 (6) 0.0038 (6) −0.0013 (6)
C11 0.0200 (9) 0.0248 (10) 0.0379 (12) 0.0004 (8) 0.0173 (9) −0.0008 (9)
C12 0.0421 (13) 0.0267 (11) 0.0163 (9) −0.0055 (9) 0.0084 (9) −0.0055 (8)
C13 0.0167 (8) 0.0183 (9) 0.0267 (10) 0.0021 (7) 0.0011 (7) 0.0037 (8)
C14 0.0263 (11) 0.0293 (11) 0.0492 (14) −0.0076 (9) 0.0251 (10) −0.0115 (10)
C15 0.0394 (12) 0.0268 (10) 0.0144 (9) −0.0007 (9) 0.0060 (8) −0.0044 (8)
C16 0.0240 (10) 0.0211 (9) 0.0356 (12) 0.0016 (8) −0.0026 (9) 0.0095 (9)
O3 0.0214 (7) 0.0235 (7) 0.0314 (8) 0.0013 (6) 0.0097 (6) 0.0028 (6)
O4 0.0283 (8) 0.0272 (8) 0.0483 (10) 0.0062 (7) 0.0200 (7) 0.0074 (7)
O5 0.0313 (9) 0.0332 (9) 0.0414 (10) 0.0117 (7) 0.0211 (8) 0.0132 (8)

Geometric parameters (Å, º)

O1—C1 1.213 (3) N8A—C10 1.341 (3)
C1—N1 1.172 (3) N8A—C13 1.468 (3)
C2—N2 1.165 (3) N8A—C14 1.472 (3)
C2—O2 1.230 (3) N6B—C10 1.350 (10)
C3—N4 1.329 (2) N6B—C15 1.558 (10)
C3—N3 1.336 (2) N6B—C14 1.635 (11)
C3—N5 1.353 (2) N7B—C10 1.358 (10)
N3—C7 1.459 (2) N7B—C11 1.566 (11)
N3—C6 1.475 (2) N7B—C16 1.600 (11)
N4—C8 1.468 (3) N8B—C10 1.311 (9)
N4—C9 1.472 (3) N8B—C13 1.548 (10)
N5—C5 1.453 (3) N8B—C12 1.655 (10)
N5—C4 1.459 (3) C11—H11A 0.9800
C4—H4A 0.9800 C11—H11B 0.9800
C4—H4B 0.9800 C11—H11C 0.9800
C4—H4C 0.9800 C12—H12A 0.9800
C5—H5A 0.9800 C12—H12B 0.9800
C5—H5B 0.9800 C12—H12C 0.9800
C5—H5C 0.9800 C13—H13A 0.9800
C6—H6A 0.9800 C13—H13B 0.9800
C6—H6B 0.9800 C13—H13C 0.9800
C6—H6C 0.9800 C14—H14A 0.9800
C7—H7A 0.9800 C14—H14B 0.9800
C7—H7B 0.9800 C14—H14C 0.9800
C7—H7C 0.9800 C15—H15A 0.9800
C8—H8A 0.9800 C15—H15B 0.9800
C8—H8B 0.9800 C15—H15C 0.9800
C8—H8C 0.9800 C16—H16A 0.9800
C9—H9A 0.9800 C16—H16B 0.9800
C9—H9B 0.9800 C16—H16C 0.9800
C9—H9C 0.9800 O3—H31 0.78 (3)
N6A—C10 1.333 (3) O3—H32 0.86 (4)
N6A—C12 1.475 (3) O4—H41 0.84 (3)
N6A—C11 1.475 (3) O4—H42 0.83 (4)
N7A—C10 1.336 (3) O5—H51 0.85 (3)
N7A—C15 1.464 (3) O5—H52 0.74 (4)
N7A—C16 1.480 (3)
N1—C1—O1 179.2 (3) C10—N8A—C14 121.18 (18)
N2—C2—O2 179.1 (2) C13—N8A—C14 116.95 (18)
N4—C3—N3 121.01 (16) C10—N6B—C15 114.4 (7)
N4—C3—N5 119.77 (17) C10—N6B—C14 110.0 (7)
N3—C3—N5 119.21 (17) C15—N6B—C14 134.5 (7)
C3—N3—C7 122.40 (16) C10—N7B—C11 113.4 (7)
C3—N3—C6 121.41 (16) C10—N7B—C16 111.5 (7)
C7—N3—C6 116.15 (16) C11—N7B—C16 135.0 (7)
C3—N4—C8 121.87 (17) C10—N8B—C13 118.2 (7)
C3—N4—C9 122.10 (16) C10—N8B—C12 110.3 (6)
C8—N4—C9 116.01 (16) C13—N8B—C12 131.3 (6)
C3—N5—C5 121.89 (17) N6A—C10—N7A 119.49 (18)
C3—N5—C4 121.58 (18) N6A—C10—N8A 119.80 (18)
C5—N5—C4 116.52 (17) N7A—C10—N8A 120.72 (18)
N5—C4—H4A 109.5 N8B—C10—N6B 120.0 (6)
N5—C4—H4B 109.5 N8B—C10—N7B 121.8 (7)
H4A—C4—H4B 109.5 N6B—C10—N7B 118.0 (7)
N5—C4—H4C 109.5 N6A—C11—H11A 109.5
H4A—C4—H4C 109.5 N6A—C11—H11B 109.5
H4B—C4—H4C 109.5 H11A—C11—H11B 109.5
N5—C5—H5A 109.5 N6A—C11—H11C 109.5
N5—C5—H5B 109.5 H11A—C11—H11C 109.5
H5A—C5—H5B 109.5 H11B—C11—H11C 109.5
N5—C5—H5C 109.5 N6A—C12—H12A 109.5
H5A—C5—H5C 109.5 N6A—C12—H12B 109.5
H5B—C5—H5C 109.5 H12A—C12—H12B 109.5
N3—C6—H6A 109.5 N6A—C12—H12C 109.5
N3—C6—H6B 109.5 H12A—C12—H12C 109.5
H6A—C6—H6B 109.5 H12B—C12—H12C 109.5
N3—C6—H6C 109.5 N8A—C13—H13A 109.5
H6A—C6—H6C 109.5 N8A—C13—H13B 109.5
H6B—C6—H6C 109.5 H13A—C13—H13B 109.5
N3—C7—H7A 109.5 N8A—C13—H13C 109.5
N3—C7—H7B 109.5 H13A—C13—H13C 109.5
H7A—C7—H7B 109.5 H13B—C13—H13C 109.5
N3—C7—H7C 109.5 N8A—C14—H14A 109.5
H7A—C7—H7C 109.5 N8A—C14—H14B 109.5
H7B—C7—H7C 109.5 H14A—C14—H14B 109.5
N4—C8—H8A 109.5 N8A—C14—H14C 109.5
N4—C8—H8B 109.5 H14A—C14—H14C 109.5
H8A—C8—H8B 109.5 H14B—C14—H14C 109.5
N4—C8—H8C 109.5 N7A—C15—H15A 109.5
H8A—C8—H8C 109.5 N7A—C15—H15B 109.5
H8B—C8—H8C 109.5 H15A—C15—H15B 109.5
N4—C9—H9A 109.5 N7A—C15—H15C 109.5
N4—C9—H9B 109.5 H15A—C15—H15C 109.5
H9A—C9—H9B 109.5 H15B—C15—H15C 109.5
N4—C9—H9C 109.5 N7A—C16—H16A 109.5
H9A—C9—H9C 109.5 N7A—C16—H16B 109.5
H9B—C9—H9C 109.5 H16A—C16—H16B 109.5
C10—N6A—C12 120.70 (18) N7A—C16—H16C 109.5
C10—N6A—C11 121.16 (18) H16A—C16—H16C 109.5
C12—N6A—C11 118.14 (19) H16B—C16—H16C 109.5
C10—N7A—C15 121.83 (18) H31—O3—H32 106 (3)
C10—N7A—C16 120.70 (19) H41—O4—H42 102 (3)
C15—N7A—C16 117.45 (18) H51—O5—H52 105 (3)
C10—N8A—C13 121.86 (18)
N4—C3—N3—C7 −146.45 (19) C12—N6A—C10—N8A 34.3 (3)
N5—C3—N3—C7 32.4 (3) C11—N6A—C10—N8A −146.11 (19)
N4—C3—N3—C6 31.5 (3) C15—N7A—C10—N6A −147.2 (2)
N5—C3—N3—C6 −149.64 (18) C16—N7A—C10—N6A 34.4 (3)
N3—C3—N4—C8 30.4 (3) C15—N7A—C10—N8A 32.5 (3)
N5—C3—N4—C8 −148.39 (19) C16—N7A—C10—N8A −145.9 (2)
N3—C3—N4—C9 −147.87 (18) C13—N8A—C10—N6A 31.7 (3)
N5—C3—N4—C9 33.3 (3) C14—N8A—C10—N6A −147.48 (19)
N4—C3—N5—C5 −145.34 (19) C13—N8A—C10—N7A −148.04 (19)
N3—C3—N5—C5 35.8 (3) C14—N8A—C10—N7A 32.8 (3)
N4—C3—N5—C4 33.1 (3) C15—N6B—C10—N8B 150.1 (7)
N3—C3—N5—C4 −145.71 (19) C14—N6B—C10—N8B −19.7 (10)
C13—N8B—C10—N6B −34.6 (10) C15—N6B—C10—N7B −35.3 (10)
C12—N8B—C10—N6B 150.7 (6) C14—N6B—C10—N7B 154.9 (6)
C13—N8B—C10—N7B 151.0 (7) C11—N7B—C10—N8B −32.9 (10)
C12—N8B—C10—N7B −23.7 (9) C16—N7B—C10—N8B 150.9 (7)
C12—N6A—C10—N7A −146.0 (2) C11—N7B—C10—N6B 152.6 (7)
C11—N6A—C10—N7A 33.6 (3) C16—N7B—C10—N6B −23.6 (10)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
O3—H31···N2 0.78 (3) 2.00 (3) 2.780 (3) 176 (3)
O3—H32···O5i 0.86 (4) 2.00 (4) 2.858 (4) 172 (3)
O4—H42···O3ii 0.83 (4) 2.04 (4) 2.852 (4) 164 (3)
O4—H41···N1ii 0.84 (3) 2.00 (3) 2.833 (3) 173 (3)
O5—H51···O2iii 0.85 (3) 1.92 (3) 2.761 (3) 175 (3)
O5—H52···O1iv 0.74 (4) 2.10 (4) 2.840 (4) 177 (3)

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

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: RZ5180).

References

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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/S2056989015024317/rz5180sup1.cif

e-71-o1076-sup1.cif (600.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989015024317/rz5180Isup2.hkl

e-71-o1076-Isup2.hkl (306.3KB, hkl)

. DOI: 10.1107/S2056989015024317/rz5180fig1.tif

The structure of the title compound with displacement ellipsoids at the 50% probability level. All hydrogen atoms are omitted for clarity. Only the major component of the disordered cation is shown.

. DOI: 10.1107/S2056989015024317/rz5180fig2.tif

The structure of the orientationally disordered cation. The nitro­gen atoms are disordered between the opaque and dark positions.

c . DOI: 10.1107/S2056989015024317/rz5180fig3.tif

O—H⋯N and O—H⋯O hydrogen bonds (black dashed lines) between anions and water mol­ecules and between the water mol­ecules (view down the c axis).

c . DOI: 10.1107/S2056989015024317/rz5180fig4.tif

View down the c axis of the two-dimensional O—H⋯N and O—H⋯O hydrogen-bonding network (all hydrogen bonds are indicated by black dashed lines).

a . DOI: 10.1107/S2056989015024317/rz5180fig5.tif

Packing of the guanidinium ions in between the layers build up by water mol­ecules and cyanate ions (down the a axis).

CCDC reference: 867308

Additional supporting information: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Crystallographic Communications are provided here courtesy of International Union of Crystallography

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