Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807049057/ez2099sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807049057/ez2099Isup2.hkl |
CCDC reference: 667356
Key indicators
- Single-crystal X-ray study
- T = 297 K
- Mean (C-C) = 0.003 Å
- R factor = 0.051
- wR factor = 0.132
- Data-to-parameter ratio = 12.9
checkCIF/PLATON results
No syntax errors found
Alert level B PLAT738_ALERT_1_B D-H..A Calc 152.1(2), Rep 152.0(10) ...... 5.00 su-Ra N1 -H1 -O1 1.555 1.555 1.555
Alert level C PLAT244_ALERT_4_C Low 'Solvent' Ueq as Compared to Neighbors for Cl1 PLAT420_ALERT_2_C D-H Without Acceptor N2 - H2A ... ?
Alert level G PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 3
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check
The title compound was obtained by decomposition of [FeL(ClO4)2(H2O)2](ClO4), L = 4-(3-aminoacridine-6-imino)pentane-2-one, in 70% HClO4 solution (Rus et al., 2001). Slow evaporation of the mother liquor at room temperature deposited the product as yellow crystals.
All hydrogen atoms were placed in calculated positions using a riding model, with C—H = 0.93–0.97 Å and Uiso= 1.2Ueq(C) for aryl H. The H atoms bonded to N1 and N2 were found in a difference map and refined with a restrained N—H distance of 0.86 (2), 0.85 (2) and 0.87 (2) Å, respectively.
Nitrogen containing heterocycles, along with aromatic amines, are valuable candidates for building supramolecular architectures (Berceanu et al., 2002 and Diop et al., 2002). The structural investigation of acridinium-3,6-diamine perchlorate, (C13H12N3)+(ClO4)- (I), is a result of our constant interest in this field. The asymmetric unit of the title compound consists of two independent halves of each molecular ion. The remainder of the molecules are generated by twofold axes through atoms C7 and N1 for (C13H12N3)+ and the Cl1 atom, bisecting the O—Cl—O angles, for (ClO4)- (Fig. 1). All metric data for the organic unit are consistent with the corresponding values found in homologous derivatives [cf. (C13H13N3)Cl2·2H2O; (C13H12N3)2(SO4)·3.5H2O and C13H11N3·H2O: C—C = 1.32—1.45 Å, C—N = 1.33—1.39 Å, C—N—C = 118—123° (Obendorf et al., 1974; Jones & Neidle, 1975 and Achari & Neidle, 1976)]. The perchlorate unit is essentially tetrahedral.
The molecules associate in the solid state into a two-dimensional network via N—H···O and C—H···O hydrogen bonding (Fig. 2). Thus, each perchlorate unit links three organic units, which in turn is connected to three other perchlorates through the NH2 group interacting with the O2 atoms from two ClO4- cations (Table 1).
The two-dimensional layers along the (112) plane are stacked in the third dimension due to off-set π-π interactions between organic molecules facing in alternating directions [distances between centroids: Cg1—Cg1vi = 3.69 Å, Cg2—Cg2iii = 3.72 Å, Cg1i—Cg1iii = 3.69 Å, symmetry codes: (i) -x + 2, y, -z + 1/2; (iii) 2 - x, -y, -z; (iv) x, -y, z - 1/2; distance between the planes of two interacting cations 3.35 Å] (Fig. 3).
All these interactions lead to the formation of a three-dimensional supramolecular architecture built up by interlocking layers (Fig. 4).
For similar structures, see: Obendorf et al. (1974); Jones & Neidle (1975); Achari & Neidle (1976). For related literature, see: Berceanu et al. (2002); Diop et al. (2002). For synthesis, see: Rus et al. (2001).
Data collection: SMART (Bruker, 2000); cell refinement: SAINT-Plus (Bruker, 2000); data reduction: SAINT-Plus (Bruker, 2000); program(s) used to solve structure: SHELXTL (Bruker, 2001); program(s) used to refine structure: SHELXTL (Bruker, 2001); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2007).
C13H12N3+·ClO4− | F(000) = 640 |
Mr = 309.71 | Dx = 1.538 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -C 2yc | Cell parameters from 2203 reflections |
a = 15.122 (3) Å | θ = 2.8–26.3° |
b = 13.477 (3) Å | µ = 0.31 mm−1 |
c = 6.6922 (13) Å | T = 297 K |
β = 101.21 (3)° | Block, yellow |
V = 1337.8 (5) Å3 | 0.33 × 0.29 × 0.19 mm |
Z = 4 |
Bruker SMART APEX CCD area-detector diffractometer | 1378 independent reflections |
Radiation source: fine-focus sealed tube | 1271 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.034 |
φ and ω scans | θmax = 26.4°, θmin = 2.0° |
Absorption correction: multi-scan (SHELXTL; Bruker, 2001) | h = −18→18 |
Tmin = 0.906, Tmax = 0.934 | k = −16→16 |
7044 measured reflections | l = −8→8 |
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)] = 0.051 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.132 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.12 | w = 1/[σ2(Fo2) + (0.0551P)2 + 1.4184P] where P = (Fo2 + 2Fc2)/3 |
1378 reflections | (Δ/σ)max = 0.002 |
107 parameters | Δρmax = 0.29 e Å−3 |
3 restraints | Δρmin = −0.26 e Å−3 |
C13H12N3+·ClO4− | V = 1337.8 (5) Å3 |
Mr = 309.71 | Z = 4 |
Monoclinic, C2/c | Mo Kα radiation |
a = 15.122 (3) Å | µ = 0.31 mm−1 |
b = 13.477 (3) Å | T = 297 K |
c = 6.6922 (13) Å | 0.33 × 0.29 × 0.19 mm |
β = 101.21 (3)° |
Bruker SMART APEX CCD area-detector diffractometer | 1378 independent reflections |
Absorption correction: multi-scan (SHELXTL; Bruker, 2001) | 1271 reflections with I > 2σ(I) |
Tmin = 0.906, Tmax = 0.934 | Rint = 0.034 |
7044 measured reflections |
R[F2 > 2σ(F2)] = 0.051 | 3 restraints |
wR(F2) = 0.132 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.12 | Δρmax = 0.29 e Å−3 |
1378 reflections | Δρmin = −0.26 e Å−3 |
107 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 | ||
O1 | 1.07618 (16) | 0.26928 (18) | 0.3309 (4) | 0.0941 (8) | |
Cl1 | 1.0000 | 0.32862 (5) | 0.2500 | 0.0515 (3) | |
O2 | 0.98003 (15) | 0.3883 (2) | 0.4083 (4) | 0.1039 (10) | |
H2B | 0.6281 (14) | 0.013 (2) | 0.088 (4) | 0.068 (9)* | |
H2A | 0.6775 (19) | 0.1098 (13) | 0.086 (4) | 0.058 (8)* | |
H1 | 1.0000 | 0.1045 (14) | 0.2500 | 0.038 (8)* | |
C1 | 0.91822 (13) | −0.00693 (16) | 0.2142 (3) | 0.0332 (5) | |
C2 | 0.83806 (13) | 0.04662 (16) | 0.1780 (3) | 0.0369 (5) | |
H2 | 0.8394 | 0.1156 | 0.1765 | 0.044* | |
C3 | 0.75599 (14) | −0.00306 (18) | 0.1442 (3) | 0.0409 (5) | |
C4 | 0.75544 (16) | −0.10858 (19) | 0.1491 (3) | 0.0482 (6) | |
H4 | 0.7007 | −0.1421 | 0.1291 | 0.058* | |
C5 | 0.83282 (16) | −0.16078 (18) | 0.1823 (3) | 0.0472 (6) | |
H5 | 0.8305 | −0.2297 | 0.1832 | 0.057* | |
C6 | 0.91832 (14) | −0.11245 (16) | 0.2160 (3) | 0.0379 (5) | |
C7 | 1.0000 | −0.1620 (2) | 0.2500 | 0.0422 (7) | |
H7 | 1.0000 | −0.2310 | 0.2500 | 0.051* | |
N1 | 1.0000 | 0.04076 (17) | 0.2500 | 0.0334 (5) | |
N2 | 0.67680 (14) | 0.04645 (19) | 0.1091 (3) | 0.0555 (6) |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0980 (17) | 0.0749 (15) | 0.1176 (19) | 0.0489 (13) | 0.0411 (14) | 0.0333 (13) |
Cl1 | 0.0437 (5) | 0.0335 (4) | 0.0787 (6) | 0.000 | 0.0151 (4) | 0.000 |
O2 | 0.0599 (13) | 0.1064 (18) | 0.137 (2) | 0.0192 (12) | −0.0019 (13) | −0.0666 (17) |
C1 | 0.0377 (11) | 0.0405 (11) | 0.0216 (9) | −0.0026 (8) | 0.0062 (7) | −0.0006 (7) |
C2 | 0.0388 (11) | 0.0419 (11) | 0.0298 (10) | −0.0013 (9) | 0.0062 (8) | 0.0004 (8) |
C3 | 0.0384 (11) | 0.0574 (13) | 0.0266 (10) | −0.0039 (9) | 0.0058 (8) | −0.0011 (9) |
C4 | 0.0441 (13) | 0.0592 (14) | 0.0411 (12) | −0.0167 (11) | 0.0075 (10) | −0.0032 (11) |
C5 | 0.0547 (14) | 0.0437 (12) | 0.0434 (12) | −0.0121 (10) | 0.0100 (10) | −0.0017 (10) |
C6 | 0.0442 (12) | 0.0394 (11) | 0.0297 (10) | −0.0043 (9) | 0.0061 (8) | 0.0001 (8) |
C7 | 0.0581 (19) | 0.0339 (15) | 0.0350 (15) | 0.000 | 0.0097 (13) | 0.000 |
N1 | 0.0374 (13) | 0.0303 (12) | 0.0327 (12) | 0.000 | 0.0072 (9) | 0.000 |
N2 | 0.0354 (11) | 0.0683 (16) | 0.0608 (13) | −0.0036 (10) | 0.0045 (9) | 0.0007 (11) |
O1—Cl1 | 1.420 (2) | C4—C5 | 1.346 (3) |
Cl1—O2i | 1.409 (2) | C4—H4 | 0.9300 |
Cl1—O2 | 1.409 (2) | C5—C6 | 1.426 (3) |
Cl1—O1i | 1.420 (2) | C5—H5 | 0.9300 |
C1—N1 | 1.373 (2) | C6—C7 | 1.384 (3) |
C1—C2 | 1.391 (3) | C7—C6i | 1.384 (3) |
C1—C6 | 1.422 (3) | C7—H7 | 0.9300 |
C2—C3 | 1.389 (3) | N1—C1i | 1.373 (2) |
C2—H2 | 0.9300 | N1—H1 | 0.859 (18) |
C3—N2 | 1.351 (3) | N2—H2B | 0.849 (17) |
C3—C4 | 1.423 (3) | N2—H2A | 0.868 (17) |
Cl1—O1—H1 | 96.4 (2) | C5—C4—H4 | 119.4 |
O2i—Cl1—O2 | 110.4 (3) | C3—C4—H4 | 119.4 |
O2i—Cl1—O1 | 109.37 (14) | C4—C5—C6 | 121.3 (2) |
O2—Cl1—O1 | 108.13 (15) | C4—C5—H5 | 119.3 |
O2i—Cl1—O1i | 108.13 (15) | C6—C5—H5 | 119.3 |
O2—Cl1—O1i | 109.37 (14) | C7—C6—C1 | 118.9 (2) |
O1—Cl1—O1i | 111.5 (2) | C7—C6—C5 | 123.9 (2) |
N1—C1—C2 | 120.83 (19) | C1—C6—C5 | 117.1 (2) |
N1—C1—C6 | 117.86 (19) | C6—C7—C6i | 122.3 (3) |
C2—C1—C6 | 121.31 (18) | C6—C7—H7 | 118.9 |
C3—C2—C1 | 119.9 (2) | C6i—C7—H7 | 118.9 |
C3—C2—H2 | 120.0 | C1i—N1—C1 | 124.2 (2) |
C1—C2—H2 | 120.0 | C1i—N1—H1 | 117.92 (12) |
N2—C3—C2 | 121.6 (2) | C1—N1—H1 | 117.91 (12) |
N2—C3—C4 | 119.3 (2) | C3—N2—H2B | 119 (2) |
C2—C3—C4 | 119.1 (2) | C3—N2—H2A | 118.4 (19) |
C5—C4—C3 | 121.2 (2) | H2B—N2—H2A | 122 (3) |
H1—O1—Cl1—O2i | −119.52 (15) | N1—C1—C6—C7 | −1.1 (2) |
H1—O1—Cl1—O2 | 120.25 (15) | C2—C1—C6—C7 | 179.14 (15) |
H1—O1—Cl1—O1i | 0.001 (1) | N1—C1—C6—C5 | 178.86 (15) |
N1—C1—C2—C3 | −179.32 (15) | C2—C1—C6—C5 | −0.9 (3) |
C6—C1—C2—C3 | 0.4 (3) | C4—C5—C6—C7 | −179.71 (18) |
C1—C2—C3—N2 | 179.85 (19) | C4—C5—C6—C1 | 0.3 (3) |
C1—C2—C3—C4 | 0.6 (3) | C1—C6—C7—C6i | 0.55 (12) |
N2—C3—C4—C5 | 179.6 (2) | C5—C6—C7—C6i | −179.4 (2) |
C2—C3—C4—C5 | −1.2 (3) | C2—C1—N1—C1i | −179.68 (19) |
C3—C4—C5—C6 | 0.7 (3) | C6—C1—N1—C1i | 0.55 (12) |
Symmetry code: (i) −x+2, y, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1 | 0.86 (2) | 2.51 (2) | 3.296 (3) | 152 (1) |
N1—H1···O1i | 0.86 (2) | 2.51 (2) | 3.296 (3) | 152 (1) |
C2—H2···O1i | 0.93 | 2.44 | 3.274 (3) | 150 |
N2—H2B···O2ii | 0.85 (2) | 2.35 (3) | 3.174 (3) | 164 (2) |
Symmetry codes: (i) −x+2, y, −z+1/2; (ii) −x+3/2, y−1/2, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C13H12N3+·ClO4− |
Mr | 309.71 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 297 |
a, b, c (Å) | 15.122 (3), 13.477 (3), 6.6922 (13) |
β (°) | 101.21 (3) |
V (Å3) | 1337.8 (5) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.31 |
Crystal size (mm) | 0.33 × 0.29 × 0.19 |
Data collection | |
Diffractometer | Bruker SMART APEX CCD area-detector |
Absorption correction | Multi-scan (SHELXTL; Bruker, 2001) |
Tmin, Tmax | 0.906, 0.934 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 7044, 1378, 1271 |
Rint | 0.034 |
(sin θ/λ)max (Å−1) | 0.625 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.051, 0.132, 1.12 |
No. of reflections | 1378 |
No. of parameters | 107 |
No. of restraints | 3 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.29, −0.26 |
Computer programs: SMART (Bruker, 2000), SAINT-Plus (Bruker, 2000), SHELXTL (Bruker, 2001), DIAMOND (Brandenburg, 2006), publCIF (Westrip, 2007).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1 | 0.86 (2) | 2.51 (2) | 3.296 (3) | 152 (1) |
N1—H1···O1i | 0.86 (2) | 2.51 (2) | 3.296 (3) | 152 (1) |
C2—H2···O1i | 0.93 | 2.44 | 3.274 (3) | 150 |
N2—H2B···O2ii | 0.85 (2) | 2.35 (3) | 3.174 (3) | 164 (2) |
Symmetry codes: (i) −x+2, y, −z+1/2; (ii) −x+3/2, y−1/2, −z+1/2. |
Nitrogen containing heterocycles, along with aromatic amines, are valuable candidates for building supramolecular architectures (Berceanu et al., 2002 and Diop et al., 2002). The structural investigation of acridinium-3,6-diamine perchlorate, (C13H12N3)+(ClO4)- (I), is a result of our constant interest in this field. The asymmetric unit of the title compound consists of two independent halves of each molecular ion. The remainder of the molecules are generated by twofold axes through atoms C7 and N1 for (C13H12N3)+ and the Cl1 atom, bisecting the O—Cl—O angles, for (ClO4)- (Fig. 1). All metric data for the organic unit are consistent with the corresponding values found in homologous derivatives [cf. (C13H13N3)Cl2·2H2O; (C13H12N3)2(SO4)·3.5H2O and C13H11N3·H2O: C—C = 1.32—1.45 Å, C—N = 1.33—1.39 Å, C—N—C = 118—123° (Obendorf et al., 1974; Jones & Neidle, 1975 and Achari & Neidle, 1976)]. The perchlorate unit is essentially tetrahedral.
The molecules associate in the solid state into a two-dimensional network via N—H···O and C—H···O hydrogen bonding (Fig. 2). Thus, each perchlorate unit links three organic units, which in turn is connected to three other perchlorates through the NH2 group interacting with the O2 atoms from two ClO4- cations (Table 1).
The two-dimensional layers along the (112) plane are stacked in the third dimension due to off-set π-π interactions between organic molecules facing in alternating directions [distances between centroids: Cg1—Cg1vi = 3.69 Å, Cg2—Cg2iii = 3.72 Å, Cg1i—Cg1iii = 3.69 Å, symmetry codes: (i) -x + 2, y, -z + 1/2; (iii) 2 - x, -y, -z; (iv) x, -y, z - 1/2; distance between the planes of two interacting cations 3.35 Å] (Fig. 3).
All these interactions lead to the formation of a three-dimensional supramolecular architecture built up by interlocking layers (Fig. 4).