Abstract
In the title compound, CH6N3 +·C5H8NO4 −, there are two independent cations and two independent anions in the asymmetric unit. In the crystal structure, cations and anions are linked by intermolecular N—H⋯O hydrogen bonds into a three-dimensional network.
Related literature
For an early report of salts formed from amino acids and guanidines, see: Armstrong (1956 ▶).
Experimental
Crystal data
CH6N3 +·C5H8NO4 −
M r = 206.21
Monoclinic,
a = 8.7793 (7) Å
b = 10.8729 (10) Å
c = 10.0801 (9) Å
β = 104.552 (1)°
V = 931.34 (14) Å3
Z = 4
Mo Kα radiation
μ = 0.12 mm−1
T = 150 K
0.42 × 0.26 × 0.20 mm
Data collection
Bruker SMART APEX diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.950, T max = 0.976
5501 measured reflections
2220 independent reflections
2087 reflections with I > 2σ(I)
R int = 0.021
Refinement
R[F 2 > 2σ(F 2)] = 0.031
wR(F 2) = 0.081
S = 1.06
2220 reflections
255 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.30 e Å−3
Δρmin = −0.23 e Å−3
Data collection: SMART (Bruker, 1997 ▶); cell refinement: SAINT (Bruker, 1997 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810036354/lh5125sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810036354/lh5125Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1A⋯O8 | 0.91 | 1.89 | 2.795 (2) | 179 |
| N1—H1B⋯O4i | 0.91 | 1.84 | 2.738 (2) | 170 |
| N1—H1C⋯O2i | 0.91 | 2.13 | 3.017 (2) | 165 |
| N2—H2A⋯O2ii | 0.91 | 2.09 | 2.998 (2) | 173 |
| N2—H2B⋯O7iii | 0.91 | 2.16 | 2.740 (2) | 120 |
| N2—H2C⋯O5iii | 0.91 | 1.92 | 2.817 (3) | 170 |
| N3—H3A⋯O2i | 0.88 | 2.08 | 2.900 (3) | 154 |
| N3—H3B⋯O3 | 0.88 | 2.08 | 2.841 (3) | 145 |
| N4—H4A⋯O3iv | 0.88 | 1.95 | 2.826 (2) | 173 |
| N4—H4B⋯O1i | 0.88 | 2.22 | 3.095 (2) | 170 |
| N5—H5A⋯O4iv | 0.88 | 1.96 | 2.831 (2) | 172 |
| N5—H5B⋯O6 | 0.88 | 2.35 | 3.092 (3) | 142 |
| N6—H6A⋯O6 | 0.88 | 2.04 | 2.897 (2) | 165 |
| N6—H6B⋯O8v | 0.88 | 1.97 | 2.824 (2) | 164 |
| N7—H7A⋯O5 | 0.88 | 2.00 | 2.851 (2) | 163 |
| N7—H7B⋯O8vi | 0.88 | 2.02 | 2.775 (3) | 143 |
| N8—H8A⋯O7v | 0.88 | 2.08 | 2.954 (3) | 170 |
| N8—H8B⋯O1vi | 0.88 | 2.23 | 2.953 (3) | 140 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
; (v)
; (vi)
.
Acknowledgments
This work was supported by NSFC (project No. 20772210) and the Scientific Research Foundation for Returned Overseas Chinese Scholars, State Education Ministry. The authors acknowledge Dr Deng Xuebin for collecting the data at the Testing Center, College of Chemistry, Beijing Normal University.
supplementary crystallographic information
Comment
To better understand the formation of complex salts between a guanidine compounds and amino acids we carried out the crystal structure determination of the title compound. The asymmetric unit of the title compound is shown in Fig. 1. There are two independent cations and two indpendent anions in the asymmetric unit. In the crystal structure, cations and anions are linked by intramolecular N—H···O hydrogen bonds into a three-dimensional network (see Fig. 2).
Experimental
L-Glutamic acid (1.47 g.) and guanidine carbonate (0.90 g) were suspended in 10 ml of water. When the evolution of CO2 had ceased the solution was diluted with 20 ml of acetone, and evaporated to a clear syrup. The syrup was dissolved in 30 ml of absolute methanol to yield a clear solution, and was allowed to stand overnight at room temperature. This solution was then placed in a fume hood for another day, whereupon the crystals of the title compound were collected and dried.
Refinement
In the absence of significant anomalous dispersion effects Friedel pairs were merged. The absolute configuation is known from the starting material. H atoms were placed in calculated positions (C—H = 0.99 or 1.00 Å, N—H = 0.88 or 0.91 Å) and were refined as riding, with Uiso(H) = 1.2Ueq(C,N) or 1.5eq(N) for –NH3 groups.
Figures
Fig. 1.
The asymmetric unit of the title compound with displacement ellipsoids drawn at the 30% probability level.
Fig. 2.
Part of the crystal structure of the title compound with hydrogen bonds shown as dashed lines.
Crystal data
| CH6N3+·C5H8NO4− | F(000) = 440 |
| Mr = 206.21 | Dx = 1.471 Mg m−3 |
| Monoclinic, P21 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2yb | Cell parameters from 2748 reflections |
| a = 8.7793 (7) Å | θ = 2.4–27.5° |
| b = 10.8729 (10) Å | µ = 0.12 mm−1 |
| c = 10.0801 (9) Å | T = 150 K |
| β = 104.552 (1)° | Prism, colourless |
| V = 931.34 (14) Å3 | 0.42 × 0.26 × 0.20 mm |
| Z = 4 |
Data collection
| Bruker SMART APEX diffractometer | 2220 independent reflections |
| Radiation source: fine-focus sealed tube | 2087 reflections with I > 2σ(I) |
| graphite | Rint = 0.021 |
| φ and ω scans | θmax = 27.5°, θmin = 2.4° |
| Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −11→10 |
| Tmin = 0.950, Tmax = 0.976 | k = −14→9 |
| 5501 measured reflections | l = −8→13 |
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)] = 0.031 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.081 | H-atom parameters constrained |
| S = 1.06 | w = 1/[σ2(Fo2) + (0.044P)2 + 0.2149P] where P = (Fo2 + 2Fc2)/3 |
| 2220 reflections | (Δ/σ)max < 0.001 |
| 255 parameters | Δρmax = 0.30 e Å−3 |
| 1 restraint | Δρmin = −0.22 e Å−3 |
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 | ||
| C1 | 0.3633 (2) | 0.4498 (2) | −0.1328 (2) | 0.0157 (4) | |
| C2 | 0.4808 (2) | 0.5516 (2) | −0.06507 (19) | 0.0152 (4) | |
| H2 | 0.5234 | 0.5892 | −0.1389 | 0.018* | |
| C3 | 0.6207 (2) | 0.5030 (2) | 0.0442 (2) | 0.0175 (4) | |
| H3C | 0.6924 | 0.5723 | 0.0803 | 0.021* | |
| H3D | 0.6793 | 0.4434 | 0.0016 | 0.021* | |
| C4 | 0.5727 (2) | 0.4405 (2) | 0.1632 (2) | 0.0185 (4) | |
| H4C | 0.4937 | 0.3761 | 0.1264 | 0.022* | |
| H4D | 0.5227 | 0.5020 | 0.2111 | 0.022* | |
| C5 | 0.7121 (2) | 0.3823 (2) | 0.2661 (2) | 0.0161 (4) | |
| C6 | 0.6284 (3) | 0.5883 (2) | 0.6253 (2) | 0.0170 (4) | |
| C7 | 0.5001 (2) | 0.5088 (2) | 0.5315 (2) | 0.0142 (4) | |
| H7 | 0.5153 | 0.5159 | 0.4368 | 0.017* | |
| C8 | 0.3304 (2) | 0.5466 (2) | 0.52340 (19) | 0.0164 (4) | |
| H8C | 0.3259 | 0.6367 | 0.5357 | 0.020* | |
| H8D | 0.2954 | 0.5067 | 0.5990 | 0.020* | |
| C9 | 0.2181 (2) | 0.5106 (2) | 0.3863 (2) | 0.0171 (4) | |
| H9A | 0.2379 | 0.4240 | 0.3655 | 0.020* | |
| H9B | 0.1083 | 0.5165 | 0.3946 | 0.020* | |
| C10 | 0.2368 (2) | 0.5920 (2) | 0.2679 (2) | 0.0156 (4) | |
| C11 | 0.9131 (2) | 0.7443 (2) | 0.4492 (2) | 0.0176 (4) | |
| C12 | 0.9193 (3) | 0.7368 (2) | 0.9641 (2) | 0.0179 (4) | |
| N1 | 0.3944 (2) | 0.65067 (18) | −0.01100 (17) | 0.0155 (4) | |
| H1A | 0.3351 | 0.6164 | 0.0415 | 0.023* | |
| H1B | 0.3307 | 0.6918 | −0.0823 | 0.023* | |
| H1C | 0.4648 | 0.7040 | 0.0407 | 0.023* | |
| N2 | 0.5301 (2) | 0.37747 (18) | 0.57395 (19) | 0.0183 (4) | |
| H2A | 0.4960 | 0.3633 | 0.6507 | 0.027* | |
| H2B | 0.6351 | 0.3617 | 0.5918 | 0.027* | |
| H2C | 0.4774 | 0.3275 | 0.5052 | 0.027* | |
| N3 | 0.7857 (2) | 0.6972 (2) | 0.3634 (2) | 0.0240 (4) | |
| H3A | 0.7411 | 0.7361 | 0.2870 | 0.029* | |
| H3B | 0.7461 | 0.6272 | 0.3832 | 0.029* | |
| N4 | 0.9733 (2) | 0.84922 (19) | 0.42024 (19) | 0.0204 (4) | |
| H4A | 1.0578 | 0.8797 | 0.4770 | 0.024* | |
| H4B | 0.9288 | 0.8887 | 0.3441 | 0.024* | |
| N5 | 0.9797 (2) | 0.68433 (19) | 0.5639 (2) | 0.0215 (4) | |
| H5A | 1.0643 | 0.7145 | 0.6209 | 0.026* | |
| H5B | 0.9394 | 0.6144 | 0.5829 | 0.026* | |
| N6 | 0.9603 (2) | 0.62410 (19) | 0.9389 (2) | 0.0242 (4) | |
| H6A | 0.9036 | 0.5832 | 0.8682 | 0.029* | |
| H6B | 1.0442 | 0.5899 | 0.9926 | 0.029* | |
| N7 | 0.7924 (2) | 0.78798 (19) | 0.88260 (19) | 0.0222 (4) | |
| H7A | 0.7361 | 0.7467 | 0.8121 | 0.027* | |
| H7B | 0.7648 | 0.8631 | 0.8991 | 0.027* | |
| N8 | 1.0012 (2) | 0.8000 (2) | 1.0716 (2) | 0.0248 (5) | |
| H8A | 1.0844 | 0.7668 | 1.1274 | 0.030* | |
| H8B | 0.9721 | 0.8751 | 1.0868 | 0.030* | |
| O1 | 0.22034 (18) | 0.47085 (14) | −0.15334 (15) | 0.0197 (3) | |
| O2 | 0.42560 (19) | 0.35290 (15) | −0.16612 (15) | 0.0206 (3) | |
| O3 | 0.76473 (19) | 0.43703 (16) | 0.37806 (16) | 0.0221 (4) | |
| O4 | 0.76678 (19) | 0.28334 (16) | 0.23297 (16) | 0.0236 (4) | |
| O5 | 0.6030 (2) | 0.70163 (15) | 0.62702 (17) | 0.0234 (4) | |
| O6 | 0.75073 (18) | 0.53379 (16) | 0.68837 (16) | 0.0225 (4) | |
| O7 | 0.2657 (2) | 0.70271 (16) | 0.28796 (17) | 0.0277 (4) | |
| O8 | 0.21550 (17) | 0.54149 (15) | 0.15054 (14) | 0.0184 (3) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0218 (10) | 0.0148 (10) | 0.0098 (9) | −0.0013 (8) | 0.0027 (8) | 0.0026 (8) |
| C2 | 0.0177 (9) | 0.0146 (10) | 0.0126 (8) | −0.0017 (8) | 0.0025 (7) | −0.0002 (8) |
| C3 | 0.0153 (9) | 0.0193 (10) | 0.0165 (10) | 0.0003 (9) | 0.0013 (8) | −0.0003 (8) |
| C4 | 0.0159 (10) | 0.0222 (12) | 0.0161 (10) | 0.0029 (9) | 0.0017 (8) | −0.0005 (9) |
| C5 | 0.0153 (9) | 0.0163 (10) | 0.0158 (10) | 0.0001 (8) | 0.0024 (8) | 0.0010 (8) |
| C6 | 0.0180 (10) | 0.0187 (11) | 0.0135 (9) | −0.0030 (9) | 0.0024 (8) | 0.0002 (8) |
| C7 | 0.0177 (9) | 0.0134 (10) | 0.0110 (9) | 0.0014 (8) | 0.0023 (7) | 0.0009 (8) |
| C8 | 0.0167 (9) | 0.0203 (10) | 0.0115 (9) | 0.0013 (8) | 0.0024 (7) | 0.0006 (8) |
| C9 | 0.0166 (9) | 0.0184 (10) | 0.0151 (9) | −0.0024 (8) | 0.0021 (7) | 0.0000 (8) |
| C10 | 0.0126 (9) | 0.0167 (10) | 0.0155 (10) | 0.0014 (8) | −0.0005 (7) | 0.0014 (8) |
| C11 | 0.0169 (10) | 0.0180 (11) | 0.0182 (10) | 0.0029 (8) | 0.0048 (8) | −0.0029 (8) |
| C12 | 0.0186 (10) | 0.0176 (11) | 0.0169 (10) | 0.0009 (8) | 0.0035 (8) | 0.0015 (8) |
| N1 | 0.0186 (8) | 0.0142 (8) | 0.0122 (8) | −0.0007 (7) | 0.0008 (6) | 0.0010 (7) |
| N2 | 0.0202 (9) | 0.0136 (9) | 0.0184 (9) | 0.0008 (7) | −0.0003 (7) | −0.0010 (7) |
| N3 | 0.0246 (10) | 0.0203 (10) | 0.0214 (9) | −0.0026 (8) | −0.0052 (8) | 0.0023 (8) |
| N4 | 0.0205 (9) | 0.0211 (10) | 0.0172 (9) | −0.0025 (8) | 0.0001 (7) | 0.0001 (8) |
| N5 | 0.0189 (9) | 0.0211 (10) | 0.0206 (9) | −0.0030 (8) | −0.0024 (7) | 0.0020 (8) |
| N6 | 0.0237 (10) | 0.0209 (11) | 0.0233 (10) | 0.0065 (8) | −0.0028 (8) | −0.0031 (8) |
| N7 | 0.0240 (10) | 0.0171 (9) | 0.0209 (9) | 0.0043 (8) | −0.0032 (8) | −0.0035 (8) |
| N8 | 0.0284 (10) | 0.0203 (11) | 0.0195 (9) | 0.0056 (8) | −0.0057 (8) | −0.0024 (8) |
| O1 | 0.0183 (7) | 0.0212 (9) | 0.0175 (7) | −0.0006 (6) | 0.0010 (6) | −0.0013 (6) |
| O2 | 0.0253 (8) | 0.0183 (8) | 0.0167 (8) | 0.0026 (7) | 0.0024 (6) | −0.0035 (6) |
| O3 | 0.0235 (8) | 0.0218 (9) | 0.0171 (8) | 0.0053 (7) | −0.0020 (6) | −0.0046 (7) |
| O4 | 0.0253 (8) | 0.0208 (8) | 0.0199 (8) | 0.0068 (7) | −0.0032 (6) | −0.0048 (7) |
| O5 | 0.0280 (9) | 0.0137 (8) | 0.0232 (8) | −0.0024 (7) | −0.0033 (7) | 0.0003 (6) |
| O6 | 0.0191 (8) | 0.0201 (9) | 0.0234 (8) | 0.0000 (7) | −0.0035 (6) | −0.0009 (7) |
| O7 | 0.0405 (10) | 0.0178 (8) | 0.0195 (8) | −0.0069 (8) | −0.0025 (7) | 0.0026 (7) |
| O8 | 0.0220 (7) | 0.0185 (8) | 0.0143 (7) | 0.0015 (6) | 0.0039 (6) | 0.0016 (6) |
Geometric parameters (Å, °)
| C1—O1 | 1.241 (3) | C10—O7 | 1.237 (3) |
| C1—O2 | 1.271 (3) | C10—O8 | 1.275 (3) |
| C1—C2 | 1.549 (3) | C11—N4 | 1.321 (3) |
| C2—N1 | 1.497 (3) | C11—N5 | 1.328 (3) |
| C2—C3 | 1.524 (3) | C11—N3 | 1.332 (3) |
| C2—H2 | 1.0000 | C12—N6 | 1.319 (3) |
| C3—C4 | 1.527 (3) | C12—N7 | 1.329 (3) |
| C3—H3C | 0.9900 | C12—N8 | 1.331 (3) |
| C3—H3D | 0.9900 | N1—H1A | 0.9100 |
| C4—C5 | 1.529 (3) | N1—H1B | 0.9100 |
| C4—H4C | 0.9900 | N1—H1C | 0.9100 |
| C4—H4D | 0.9900 | N2—H2A | 0.9100 |
| C5—O4 | 1.257 (3) | N2—H2B | 0.9100 |
| C5—O3 | 1.257 (3) | N2—H2C | 0.9100 |
| C6—O6 | 1.251 (3) | N3—H3A | 0.8800 |
| C6—O5 | 1.253 (3) | N3—H3B | 0.8800 |
| C6—C7 | 1.541 (3) | N4—H4A | 0.8800 |
| C7—N2 | 1.495 (3) | N4—H4B | 0.8800 |
| C7—C8 | 1.528 (3) | N5—H5A | 0.8800 |
| C7—H7 | 1.0000 | N5—H5B | 0.8800 |
| C8—C9 | 1.533 (3) | N6—H6A | 0.8800 |
| C8—H8C | 0.9900 | N6—H6B | 0.8800 |
| C8—H8D | 0.9900 | N7—H7A | 0.8800 |
| C9—C10 | 1.527 (3) | N7—H7B | 0.8800 |
| C9—H9A | 0.9900 | N8—H8A | 0.8800 |
| C9—H9B | 0.9900 | N8—H8B | 0.8800 |
| O1—C1—O2 | 126.4 (2) | C10—C9—H9B | 109.1 |
| O1—C1—C2 | 118.4 (2) | C8—C9—H9B | 109.1 |
| O2—C1—C2 | 115.21 (18) | H9A—C9—H9B | 107.8 |
| N1—C2—C3 | 112.11 (16) | O7—C10—O8 | 123.2 (2) |
| N1—C2—C1 | 109.42 (16) | O7—C10—C9 | 119.6 (2) |
| C3—C2—C1 | 113.44 (18) | O8—C10—C9 | 117.14 (19) |
| N1—C2—H2 | 107.2 | N4—C11—N5 | 120.2 (2) |
| C3—C2—H2 | 107.2 | N4—C11—N3 | 120.4 (2) |
| C1—C2—H2 | 107.2 | N5—C11—N3 | 119.4 (2) |
| C2—C3—C4 | 112.99 (17) | N6—C12—N7 | 119.7 (2) |
| C2—C3—H3C | 109.0 | N6—C12—N8 | 121.3 (2) |
| C4—C3—H3C | 109.0 | N7—C12—N8 | 119.0 (2) |
| C2—C3—H3D | 109.0 | C2—N1—H1A | 109.5 |
| C4—C3—H3D | 109.0 | C2—N1—H1B | 109.5 |
| H3C—C3—H3D | 107.8 | H1A—N1—H1B | 109.5 |
| C3—C4—C5 | 112.67 (17) | C2—N1—H1C | 109.5 |
| C3—C4—H4C | 109.1 | H1A—N1—H1C | 109.5 |
| C5—C4—H4C | 109.1 | H1B—N1—H1C | 109.5 |
| C3—C4—H4D | 109.1 | C7—N2—H2A | 109.5 |
| C5—C4—H4D | 109.1 | C7—N2—H2B | 109.5 |
| H4C—C4—H4D | 107.8 | H2A—N2—H2B | 109.5 |
| O4—C5—O3 | 124.40 (19) | C7—N2—H2C | 109.5 |
| O4—C5—C4 | 117.95 (18) | H2A—N2—H2C | 109.5 |
| O3—C5—C4 | 117.6 (2) | H2B—N2—H2C | 109.5 |
| O6—C6—O5 | 126.2 (2) | C11—N3—H3A | 120.0 |
| O6—C6—C7 | 116.6 (2) | C11—N3—H3B | 120.0 |
| O5—C6—C7 | 117.06 (19) | H3A—N3—H3B | 120.0 |
| N2—C7—C8 | 111.79 (18) | C11—N4—H4A | 120.0 |
| N2—C7—C6 | 108.12 (16) | C11—N4—H4B | 120.0 |
| C8—C7—C6 | 115.78 (18) | H4A—N4—H4B | 120.0 |
| N2—C7—H7 | 106.9 | C11—N5—H5A | 120.0 |
| C8—C7—H7 | 106.9 | C11—N5—H5B | 120.0 |
| C6—C7—H7 | 106.9 | H5A—N5—H5B | 120.0 |
| C7—C8—C9 | 112.17 (17) | C12—N6—H6A | 120.0 |
| C7—C8—H8C | 109.2 | C12—N6—H6B | 120.0 |
| C9—C8—H8C | 109.2 | H6A—N6—H6B | 120.0 |
| C7—C8—H8D | 109.2 | C12—N7—H7A | 120.0 |
| C9—C8—H8D | 109.2 | C12—N7—H7B | 120.0 |
| H8C—C8—H8D | 107.9 | H7A—N7—H7B | 120.0 |
| C10—C9—C8 | 112.69 (17) | C12—N8—H8A | 120.0 |
| C10—C9—H9A | 109.1 | C12—N8—H8B | 120.0 |
| C8—C9—H9A | 109.1 | H8A—N8—H8B | 120.0 |
| O1—C1—C2—N1 | 11.3 (3) | O6—C6—C7—N2 | 18.9 (3) |
| O2—C1—C2—N1 | −170.89 (17) | O5—C6—C7—N2 | −163.9 (2) |
| O1—C1—C2—C3 | 137.29 (19) | O6—C6—C7—C8 | 145.18 (19) |
| O2—C1—C2—C3 | −44.9 (2) | O5—C6—C7—C8 | −37.6 (3) |
| N1—C2—C3—C4 | 63.7 (2) | N2—C7—C8—C9 | −83.4 (2) |
| C1—C2—C3—C4 | −60.8 (2) | C6—C7—C8—C9 | 152.21 (18) |
| C2—C3—C4—C5 | 174.99 (19) | C7—C8—C9—C10 | −73.5 (2) |
| C3—C4—C5—O4 | −75.2 (3) | C8—C9—C10—O7 | −36.4 (3) |
| C3—C4—C5—O3 | 104.4 (2) | C8—C9—C10—O8 | 146.12 (19) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···O8 | 0.91 | 1.89 | 2.795 (2) | 179 |
| N1—H1B···O4i | 0.91 | 1.84 | 2.738 (2) | 170 |
| N1—H1C···O2i | 0.91 | 2.13 | 3.017 (2) | 165 |
| N2—H2A···O2ii | 0.91 | 2.09 | 2.998 (2) | 173 |
| N2—H2B···O7iii | 0.91 | 2.16 | 2.740 (2) | 120 |
| N2—H2C···O5iii | 0.91 | 1.92 | 2.817 (3) | 170 |
| N3—H3A···O2i | 0.88 | 2.08 | 2.900 (3) | 154 |
| N3—H3B···O3 | 0.88 | 2.08 | 2.841 (3) | 145 |
| N4—H4A···O3iv | 0.88 | 1.95 | 2.826 (2) | 173 |
| N4—H4B···O1i | 0.88 | 2.22 | 3.095 (2) | 170 |
| N5—H5A···O4iv | 0.88 | 1.96 | 2.831 (2) | 172 |
| N5—H5B···O6 | 0.88 | 2.35 | 3.092 (3) | 142 |
| N6—H6A···O6 | 0.88 | 2.04 | 2.897 (2) | 165 |
| N6—H6B···O8v | 0.88 | 1.97 | 2.824 (2) | 164 |
| N7—H7A···O5 | 0.88 | 2.00 | 2.851 (2) | 163 |
| N7—H7B···O8vi | 0.88 | 2.02 | 2.775 (3) | 143 |
| N8—H8A···O7v | 0.88 | 2.08 | 2.954 (3) | 170 |
| N8—H8B···O1vi | 0.88 | 2.23 | 2.953 (3) | 140 |
Symmetry codes: (i) −x+1, y+1/2, −z; (ii) x, y, z+1; (iii) −x+1, y−1/2, −z+1; (iv) −x+2, y+1/2, −z+1; (v) x+1, y, z+1; (vi) −x+1, y+1/2, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH5125).
References
- Armstrong, M. D. (1956). J. Org. Chem.21, 503–505.
- Bruker (1997). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.
- Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810036354/lh5125sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810036354/lh5125Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


