Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803007633/na6223sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536803007633/na6223Isup2.hkl |
CCDC reference: 214618
Key indicators
- Single-crystal X-ray study
- T = 293 K
- Mean (C-C) = 0.004 Å
- R factor = 0.051
- wR factor = 0.153
- Data-to-parameter ratio = 18.9
checkCIF results
No syntax errors found ADDSYM reports no extra symmetry
Alert Level B:
PLAT_728 Alert B D-H..A Calc 136.62, Rep 134.00, Dev. 2.62 Deg. C2 -H2 -O4 1.555 1.555 3.655
0 Alert Level A = Potentially serious problem
1 Alert Level B = Potential problem
0 Alert Level C = Please check
Anisole (0.05 mol) was dissolved in 6 ml DMF and kept under ice-cold condition. To this, 1.4 ml POCl3 (0.035 ml) was added dropwise for 15 min with stirring. The reaction mixture was stirred at room temperature for 30 minutes and then at 353–363 K for 15 h. The reaction mixture was finally poured into crushed ice and treated with sodium perchlorate or dilute perchloric acid. The creamy yellow precipitate obtained was filtered, washed with water and dried. This crude product was recrystallized using CHCl3 to give pure vinamidinium perchlorate.
The H atom on N7 was located in a difference Fourier map and refined, while all other H atoms were positioned geometrically and were allowed to ride on their attached atoms. One of the methyl group (C11) was found to be disordered; it was treated as an idealized disordered methyl group, with two positions rotated from each other by 60°, and the site-occupation factors fixed at 0.5.
Data collection: SMART (Siemens, 1996); cell refinement: SAINT; data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ZORTEP (Zsolnai, 1997) and PLUTON (Spek, 1990); software used to prepare material for publication: SHELXL97 and PARST (Nardelli, 1995).
C9H13N2ClO4 | F(000) = 520 |
Mr = 248.66 | Dx = 1.433 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 7.8382 (2) Å | Cell parameters from 3903 reflections |
b = 17.5688 (6) Å | θ = 2.3–28.3° |
c = 9.1123 (2) Å | µ = 0.33 mm−1 |
β = 113.269 (1)° | T = 293 K |
V = 1152.77 (6) Å3 | Prism, pale yellow |
Z = 4 | 0.28 × 0.16 × 0.12 mm |
Siemens SMART CCD area-detector diffractometer | 2854 independent reflections |
Radiation source: fine-focus sealed tube | 1917 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.039 |
ω scans | θmax = 28.3°, θmin = 2.3° |
Absorption correction: multi-scan (SADABS; Siemens, 1996) | h = −10→8 |
Tmin = 0.913, Tmax = 0.961 | k = −15→23 |
7777 measured reflections | l = −11→12 |
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)] = 0.051 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.153 | w = 1/[σ2(Fo2) + (0.0752P)2 + 0.2933P] where P = (Fo2 + 2Fc2)/3 |
S = 1.02 | (Δ/σ)max = 0.001 |
2854 reflections | Δρmax = 0.34 e Å−3 |
151 parameters | Δρmin = −0.22 e Å−3 |
0 restraints | Extinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.007 (2) |
C9H13N2ClO4 | V = 1152.77 (6) Å3 |
Mr = 248.66 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 7.8382 (2) Å | µ = 0.33 mm−1 |
b = 17.5688 (6) Å | T = 293 K |
c = 9.1123 (2) Å | 0.28 × 0.16 × 0.12 mm |
β = 113.269 (1)° |
Siemens SMART CCD area-detector diffractometer | 2854 independent reflections |
Absorption correction: multi-scan (SADABS; Siemens, 1996) | 1917 reflections with I > 2σ(I) |
Tmin = 0.913, Tmax = 0.961 | Rint = 0.039 |
7777 measured reflections |
R[F2 > 2σ(F2)] = 0.051 | 0 restraints |
wR(F2) = 0.153 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.02 | Δρmax = 0.34 e Å−3 |
2854 reflections | Δρmin = −0.22 e Å−3 |
151 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Cl1 | 0.75658 (8) | 0.09207 (4) | 0.40685 (6) | 0.0505 (2) | |
O1 | 0.6675 (5) | 0.16311 (15) | 0.3667 (4) | 0.1206 (11) | |
O2 | 0.9502 (3) | 0.10162 (17) | 0.4825 (3) | 0.1099 (10) | |
O3 | 0.6889 (4) | 0.04966 (17) | 0.5051 (3) | 0.1095 (10) | |
O4 | 0.7132 (3) | 0.04853 (13) | 0.2645 (2) | 0.0815 (7) | |
C1 | 0.1972 (3) | 0.04931 (12) | 0.0399 (3) | 0.0407 (5) | |
C2 | 0.1093 (3) | 0.08289 (14) | −0.1084 (3) | 0.0490 (6) | |
H2 | 0.1057 | 0.0581 | −0.1997 | 0.059* | |
C3 | 0.0268 (4) | 0.15331 (15) | −0.1204 (3) | 0.0581 (7) | |
H3 | −0.0322 | 0.1757 | −0.2202 | 0.070* | |
C4 | 0.0309 (4) | 0.19080 (14) | 0.0139 (4) | 0.0634 (7) | |
H4 | −0.0216 | 0.2389 | 0.0056 | 0.076* | |
C5 | 0.1141 (4) | 0.15589 (17) | 0.1606 (4) | 0.0689 (8) | |
H5 | 0.1141 | 0.1802 | 0.2513 | 0.083* | |
C6 | 0.1973 (4) | 0.08558 (15) | 0.1753 (3) | 0.0590 (7) | |
H6 | 0.2530 | 0.0626 | 0.2749 | 0.071* | |
N7 | 0.2839 (3) | −0.02239 (11) | 0.0462 (2) | 0.0410 (4) | |
C8 | 0.3865 (3) | −0.05880 (13) | 0.1778 (3) | 0.0435 (5) | |
H8 | 0.4032 | −0.0355 | 0.2742 | 0.052* | |
N9 | 0.4664 (3) | −0.12399 (11) | 0.1854 (2) | 0.0460 (5) | |
C10 | 0.5844 (5) | −0.1561 (2) | 0.3408 (3) | 0.0789 (10) | |
H10A | 0.7117 | −0.1552 | 0.3526 | 0.118* | |
H10B | 0.5476 | −0.2077 | 0.3473 | 0.118* | |
H10C | 0.5714 | −0.1265 | 0.4243 | 0.118* | |
C11 | 0.4510 (4) | −0.16781 (15) | 0.0437 (3) | 0.0565 (6) | |
H11A | 0.5201 | −0.2143 | 0.0764 | 0.085* | 0.50 |
H11B | 0.5000 | −0.1384 | −0.0196 | 0.085* | 0.50 |
H11C | 0.3229 | −0.1794 | −0.0184 | 0.085* | 0.50 |
H11D | 0.3752 | −0.1404 | −0.0508 | 0.085* | 0.50 |
H11E | 0.3953 | −0.2163 | 0.0452 | 0.085* | 0.50 |
H11F | 0.5725 | −0.1753 | 0.0440 | 0.085* | 0.50 |
H7 | 0.273 (4) | −0.0405 (17) | −0.040 (4) | 0.070 (9)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.0600 (4) | 0.0554 (4) | 0.0369 (3) | −0.0038 (3) | 0.0200 (2) | −0.0073 (2) |
O1 | 0.142 (2) | 0.0674 (17) | 0.136 (2) | 0.0303 (16) | 0.0374 (19) | −0.0123 (16) |
O2 | 0.0655 (15) | 0.136 (3) | 0.105 (2) | −0.0195 (14) | 0.0092 (13) | 0.0016 (17) |
O3 | 0.147 (2) | 0.133 (2) | 0.0808 (16) | −0.0242 (19) | 0.0795 (18) | 0.0046 (15) |
O4 | 0.1266 (19) | 0.0787 (15) | 0.0445 (10) | −0.0073 (13) | 0.0397 (12) | −0.0125 (10) |
C1 | 0.0397 (11) | 0.0372 (11) | 0.0452 (11) | −0.0039 (9) | 0.0168 (9) | −0.0001 (9) |
C2 | 0.0534 (13) | 0.0489 (14) | 0.0467 (12) | −0.0012 (11) | 0.0220 (11) | 0.0059 (10) |
C3 | 0.0562 (15) | 0.0509 (14) | 0.0653 (16) | 0.0022 (12) | 0.0222 (12) | 0.0179 (13) |
C4 | 0.0560 (15) | 0.0378 (13) | 0.095 (2) | 0.0047 (11) | 0.0284 (15) | 0.0025 (14) |
C5 | 0.0795 (19) | 0.0547 (16) | 0.0687 (18) | 0.0066 (14) | 0.0253 (15) | −0.0154 (14) |
C6 | 0.0707 (17) | 0.0539 (16) | 0.0448 (13) | 0.0096 (13) | 0.0149 (12) | −0.0020 (11) |
N7 | 0.0484 (10) | 0.0391 (10) | 0.0352 (9) | −0.0001 (8) | 0.0163 (8) | 0.0000 (8) |
C8 | 0.0513 (13) | 0.0445 (13) | 0.0383 (11) | −0.0006 (10) | 0.0216 (10) | 0.0015 (9) |
N9 | 0.0516 (11) | 0.0445 (11) | 0.0448 (10) | 0.0055 (9) | 0.0221 (8) | 0.0074 (8) |
C10 | 0.101 (2) | 0.081 (2) | 0.0570 (17) | 0.0360 (19) | 0.0327 (17) | 0.0253 (15) |
C11 | 0.0649 (16) | 0.0470 (14) | 0.0608 (15) | 0.0006 (12) | 0.0283 (13) | −0.0049 (11) |
Cl1—O1 | 1.406 (3) | N7—C8 | 1.316 (3) |
Cl1—O2 | 1.407 (2) | N7—H7 | 0.82 (3) |
Cl1—O3 | 1.419 (2) | C8—N9 | 1.294 (3) |
Cl1—O4 | 1.426 (2) | C8—H8 | 0.9300 |
C1—C2 | 1.383 (3) | N9—C10 | 1.465 (3) |
C1—C6 | 1.388 (3) | N9—C11 | 1.466 (3) |
C1—N7 | 1.422 (3) | C10—H10A | 0.9600 |
C2—C3 | 1.380 (3) | C10—H10B | 0.9600 |
C2—H2 | 0.9300 | C10—H10C | 0.9600 |
C3—C4 | 1.379 (4) | C11—H11A | 0.9600 |
C3—H3 | 0.9300 | C11—H11B | 0.9600 |
C4—C5 | 1.378 (4) | C11—H11C | 0.9600 |
C4—H4 | 0.9300 | C11—H11D | 0.9600 |
C5—C6 | 1.378 (4) | C11—H11E | 0.9600 |
C5—H5 | 0.9300 | C11—H11F | 0.9600 |
C6—H6 | 0.9300 | ||
O1—Cl1—O2 | 110.5 (2) | C8—N9—C10 | 120.0 (2) |
O1—Cl1—O3 | 111.1 (2) | C8—N9—C11 | 123.2 (2) |
O2—Cl1—O3 | 110.7 (2) | C10—N9—C11 | 116.7 (2) |
O1—Cl1—O4 | 108.9 (2) | N9—C10—H10A | 109.5 |
O2—Cl1—O4 | 109.5 (2) | N9—C10—H10B | 109.5 |
O3—Cl1—O4 | 106.1 (2) | H10A—C10—H10B | 109.5 |
C2—C1—C6 | 119.8 (2) | N9—C10—H10C | 109.5 |
C2—C1—N7 | 117.6 (2) | H10A—C10—H10C | 109.5 |
C6—C1—N7 | 122.6 (2) | H10B—C10—H10C | 109.5 |
C3—C2—C1 | 119.8 (2) | N9—C11—H11A | 109.5 |
C3—C2—H2 | 120.1 | N9—C11—H11B | 109.5 |
C1—C2—H2 | 120.1 | H11A—C11—H11B | 109.5 |
C2—C3—C4 | 120.8 (2) | N9—C11—H11C | 109.5 |
C2—C3—H3 | 119.6 | H11A—C11—H11C | 109.5 |
C4—C3—H3 | 119.6 | H11B—C11—H11C | 109.5 |
C5—C4—C3 | 119.0 (2) | N9—C11—H11D | 109.5 |
C5—C4—H4 | 120.5 | H11A—C11—H11D | 141.1 |
C3—C4—H4 | 120.5 | H11B—C11—H11D | 56.3 |
C4—C5—C6 | 121.1 (3) | H11C—C11—H11D | 56.3 |
C4—C5—H5 | 119.4 | N9—C11—H11E | 109.5 |
C6—C5—H5 | 119.4 | H11A—C11—H11E | 56.3 |
C5—C6—C1 | 119.4 (2) | H11B—C11—H11E | 141.1 |
C5—C6—H6 | 120.3 | H11C—C11—H11E | 56.3 |
C1—C6—H6 | 120.3 | H11D—C11—H11E | 109.5 |
C8—N7—C1 | 125.3 (2) | N9—C11—H11F | 109.5 |
C8—N7—H7 | 119 (2) | H11A—C11—H11F | 56.3 |
C1—N7—H7 | 116 (2) | H11B—C11—H11F | 56.3 |
N9—C8—N7 | 126.0 (2) | H11C—C11—H11F | 141.1 |
N9—C8—H8 | 117.0 | H11D—C11—H11F | 109.5 |
N7—C8—H8 | 117.0 | H11E—C11—H11F | 109.5 |
C6—C1—C2—C3 | 1.9 (4) | N7—C1—C6—C5 | 178.5 (2) |
N7—C1—C2—C3 | −178.5 (2) | C2—C1—N7—C8 | 173.9 (2) |
C1—C2—C3—C4 | 0.0 (4) | C6—C1—N7—C8 | −6.5 (4) |
C2—C3—C4—C5 | −1.9 (4) | C1—N7—C8—N9 | −179.9 (2) |
C3—C4—C5—C6 | 1.9 (4) | N7—C8—N9—C10 | 177.0 (2) |
C4—C5—C6—C1 | 0.0 (4) | N7—C8—N9—C11 | −0.7 (4) |
C2—C1—C6—C5 | −1.9 (4) |
D—H···A | D—H | H···A | D···A | D—H···A |
C11—H11D···N7 | 0.96 | 2.47 | 2.875 (3) | 105 |
N7—H7···O4i | 0.82 (3) | 2.09 (3) | 2.877 (3) | 160 (3) |
C2—H2···O4i | 0.93 | 2.56 | 3.295 (3) | 134 |
C11—H11D···O4i | 0.96 | 2.41 | 3.329 (3) | 160 |
C8—H8···O3ii | 0.93 | 2.40 | 3.174 (4) | 140 |
C11—H11E···O1iii | 0.96 | 2.38 | 3.310 (4) | 162 |
Symmetry codes: (i) −x+1, −y, −z; (ii) −x+1, −y, −z+1; (iii) −x+1, y−1/2, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C9H13N2ClO4 |
Mr | 248.66 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 293 |
a, b, c (Å) | 7.8382 (2), 17.5688 (6), 9.1123 (2) |
β (°) | 113.269 (1) |
V (Å3) | 1152.77 (6) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.33 |
Crystal size (mm) | 0.28 × 0.16 × 0.12 |
Data collection | |
Diffractometer | Siemens SMART CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Siemens, 1996) |
Tmin, Tmax | 0.913, 0.961 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 7777, 2854, 1917 |
Rint | 0.039 |
(sin θ/λ)max (Å−1) | 0.667 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.051, 0.153, 1.02 |
No. of reflections | 2854 |
No. of parameters | 151 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.34, −0.22 |
Computer programs: SMART (Siemens, 1996), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ZORTEP (Zsolnai, 1997) and PLUTON (Spek, 1990), SHELXL97 and PARST (Nardelli, 1995).
Cl1—O1 | 1.406 (3) | N7—C8 | 1.316 (3) |
Cl1—O2 | 1.407 (2) | C8—N9 | 1.294 (3) |
Cl1—O3 | 1.419 (2) | N9—C10 | 1.465 (3) |
Cl1—O4 | 1.426 (2) | N9—C11 | 1.466 (3) |
C1—N7 | 1.422 (3) | ||
C2—C1—N7 | 117.6 (2) | C8—N9—C10 | 120.0 (2) |
C6—C1—N7 | 122.6 (2) | C8—N9—C11 | 123.2 (2) |
C8—N7—C1 | 125.3 (2) | C10—N9—C11 | 116.7 (2) |
N9—C8—N7 | 126.0 (2) | ||
C2—C1—N7—C8 | 173.9 (2) | N7—C8—N9—C10 | 177.0 (2) |
C6—C1—N7—C8 | −6.5 (4) | N7—C8—N9—C11 | −0.7 (4) |
C1—N7—C8—N9 | −179.9 (2) |
D—H···A | D—H | H···A | D···A | D—H···A |
C11—H11D···N7 | 0.96 | 2.47 | 2.875 (3) | 105 |
N7—H7···O4i | 0.82 (3) | 2.09 (3) | 2.877 (3) | 160 (3) |
C2—H2···O4i | 0.93 | 2.56 | 3.295 (3) | 134 |
C11—H11D···O4i | 0.96 | 2.41 | 3.329 (3) | 160 |
C8—H8···O3ii | 0.93 | 2.40 | 3.174 (4) | 140 |
C11—H11E···O1iii | 0.96 | 2.38 | 3.310 (4) | 162 |
Symmetry codes: (i) −x+1, −y, −z; (ii) −x+1, −y, −z+1; (iii) −x+1, y−1/2, −z+1/2. |
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There are considerable interests in the chemistry and structure of iminium salts, because of their importances in organic synthesis (Boehme & Viehe, 1976). The chromophore of visual pigments contain polyunsaturated iminium salts (Uhl & Abrahamson, 1981; Brige, 1981). The iminium salts exhibit optical properties and the position of the counterion plays in determining the optical properties of iminium cation (Arnaboldi et al., 1979).
The cation of the title compound, (I), is nearly planar and the dihedral angle between the phenyl ring and the Schiff base chain is 7.7 (1)°. The protonation occurs at N9, the positive charge is delocalized between N9 and N7 atoms, as evidenced from the N7—C8 [1.316 (3) Å] and C8═N9 [1.294 (3) Å]. This is confirmed by the planarity of the atoms C1, N7, C8, N9, C10 and C11 [maximum deviation is 0.031 (4) Å for C10]. The perchlorate anion accepts five hydrogen bonds from three different formamidinium cations using three O atoms. One of the perchlorate O atoms (O4) acts as an acceptor in three hydrogen bonds and this O atom is also characterized by an extended bond of 1.426 (2) Å. The cations and anions are linked through N7—H7···O4i and C8—H8···O3ii hydrogen bonds and form a ring, which is further reinforced by two C2—H2···O4i and C11—H11D···O4i hydrogen bonds. The centrosymmetrically related rings are linked via C11—H11E···O1iii interactions and form a staircase, which runs parallel to b axis (see Table 2 for symmetry codes).