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The cation of the title compound, C38H44N10O24+·4NO3, is centrosymmetric. In the crystal structure, cations and anions are linked into a three-dimensional framework by a combination of N—H...O and C—H...O hydrogen bonds and aromatic π–π stacking inter­actions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807020764/lh2376sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807020764/lh2376Isup2.hkl
Contains datablock I

CCDC reference: 651377

Key indicators

  • Single-crystal X-ray study
  • T = 294 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.065
  • wR factor = 0.169
  • Data-to-parameter ratio = 15.0

checkCIF/PLATON results

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Alert level C PLAT244_ALERT_4_C Low 'Solvent' Ueq as Compared to Neighbors for N6 PLAT244_ALERT_4_C Low 'Solvent' Ueq as Compared to Neighbors for N7 PLAT790_ALERT_4_C Centre of Gravity not Within Unit Cell: Resd. # 3 N O3
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 3 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

As part of our continuing studies on the ligands or metal complexes containing multi-benzimidazole groups (Zhang et al., 2005; Li et al., 2005; Qiu et al., 2005), we report here the crystal structure of a related compound, (I), which was obtained unexpectedly by reacting µ2-N,N, N', N'-tetrakis(Benzimidazol-2-ylmethyl)- 3,6- dioxaoctane-1,8-diamine (EGTB) with Fe(NO3).6H2O in H2O solution.

In the aymmetric unit of (I) (Fig. 1), the cation lies across an inversion center in space group of P21/c. The two terminal benzimidazoles rings on one side of the cation are effectively planar with the dihedral angle of only 0.75 (1)°.

All imine N atoms in the benzimidazole groups of are protonated foming a tetracation. Two nitrate anions lie to the inner side of the two end-on benzimidazole groups, forming the four nearly symmetric intra-molecular hydrogen bonds (Table 1). However, the other two anions lie at the outside of the two benzimidazole groups, linking the adjacent cations into a two-dimensional network running parallel the (100) direction. These networks are further joined by the C7–H···O7i (symmetry code as in Table 1) hydrogen bonds, forming a three-dimensional framework (Fig.2). In addition, the supramolecular aggregation is augmented by π-π stacking interactions between the aromatic rings C5—C10 and C13—C18, respectively. The two phenyl rings which lie in the molecules at (x,y,z) and (-x,1 - y,-z), respectively, are almost parallel with the dihedral angle of only 1.36 (1)°, the ring centroid separation of 3.682 (2) Å and the interpalanar spacing of ca 3.404 Å.

Related literature top

We have already published some crystal structures tha are related to the title compound (Zhang et al., 2005; Li et al., 2005; Qiu et al., 2005).

For related literature, see: Hendriks et al. (1982).

Experimental top

All reagents and solvents were used as obtained without further purification. EGTB [EGTB = (µ2-N,N,N',N'- tetrakis(Benzimidazol-2-ylmethyl)-3,6-dioxaoctane-1,8-diamine] was prepared according to literature procedure (Hendriks et al., 1982). The title organic salt was obtained unexpectedly by reacting EGTB with Fe(NO3).6H2O (molar ratio: 1/2). The mixture was stirred for half an hour at 70° and then filtered. The resulting pale-yellow solution was kept in air for one week. Crystals of (I) suitable for single-crystal X-ray diffraction analysis were grown by slow evaporation of the solution at the bottom of the vessel.

Refinement top

All H atoms bonded to carbon atoms were placed in calculated positions with C–H=0.97 Å(methylene) and 0.93 Å(aromatic), Uiso(H) = 1.2Ueq(C). H atoms bonded to imine N atoms were located from the difference maps and the N—H distance were refined freely without any constraints, but their Uiso(H) values were set 1.2 times Ueq of their carrier atoms.

Structure description top

As part of our continuing studies on the ligands or metal complexes containing multi-benzimidazole groups (Zhang et al., 2005; Li et al., 2005; Qiu et al., 2005), we report here the crystal structure of a related compound, (I), which was obtained unexpectedly by reacting µ2-N,N, N', N'-tetrakis(Benzimidazol-2-ylmethyl)- 3,6- dioxaoctane-1,8-diamine (EGTB) with Fe(NO3).6H2O in H2O solution.

In the aymmetric unit of (I) (Fig. 1), the cation lies across an inversion center in space group of P21/c. The two terminal benzimidazoles rings on one side of the cation are effectively planar with the dihedral angle of only 0.75 (1)°.

All imine N atoms in the benzimidazole groups of are protonated foming a tetracation. Two nitrate anions lie to the inner side of the two end-on benzimidazole groups, forming the four nearly symmetric intra-molecular hydrogen bonds (Table 1). However, the other two anions lie at the outside of the two benzimidazole groups, linking the adjacent cations into a two-dimensional network running parallel the (100) direction. These networks are further joined by the C7–H···O7i (symmetry code as in Table 1) hydrogen bonds, forming a three-dimensional framework (Fig.2). In addition, the supramolecular aggregation is augmented by π-π stacking interactions between the aromatic rings C5—C10 and C13—C18, respectively. The two phenyl rings which lie in the molecules at (x,y,z) and (-x,1 - y,-z), respectively, are almost parallel with the dihedral angle of only 1.36 (1)°, the ring centroid separation of 3.682 (2) Å and the interpalanar spacing of ca 3.404 Å.

We have already published some crystal structures tha are related to the title compound (Zhang et al., 2005; Li et al., 2005; Qiu et al., 2005).

For related literature, see: Hendriks et al. (1982).

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SAINT-Plus (Bruker, 2001); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: PLATON.

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level. Hydrogen bonds are shown as dashed lines. Atoms marked with suffix 'a' are related by the symmetry operator (1 - x, 1 - y, 1 - z).
[Figure 2] Fig. 2. Part of the crystal structure of (I), showing the formation of the three-dimensional network. Hydrogen bonding are shown as dashed lines. For the sake of clarity, H atoms not involved in the motif have been omitted.
2,2',2'',2'''-[N,N,N',N'-(3,6-Dioxaoctane-1,8- diyldinitrilo)tetramethylene]tetrakis(benzimidazolium) tetranitrate top
Crystal data top
C38H44N10O24+·4(NO3)F(000) = 964
Mr = 920.87Dx = 1.439 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 2223 reflections
a = 8.4296 (6) Åθ = 2.4–19.9°
b = 17.6744 (12) ŵ = 0.11 mm1
c = 14.279 (1) ÅT = 294 K
β = 92.421 (1)°Block, colourless
V = 2125.5 (3) Å30.20 × 0.12 × 0.10 mm
Z = 2
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
4642 independent reflections
Radiation source: fine focus sealed Siemens Mo tube2655 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.067
0.3° wide ω exposures scansθmax = 27.0°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2001)
h = 1010
Tmin = 0.975, Tmax = 0.989k = 1922
23482 measured reflectionsl = 1818
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.065Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.169H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0744P)2 + 0.3238P]
where P = (Fo2 + 2Fc2)/3
4642 reflections(Δ/σ)max < 0.001
310 parametersΔρmax = 0.29 e Å3
0 restraintsΔρmin = 0.19 e Å3
Crystal data top
C38H44N10O24+·4(NO3)V = 2125.5 (3) Å3
Mr = 920.87Z = 2
Monoclinic, P21/cMo Kα radiation
a = 8.4296 (6) ŵ = 0.11 mm1
b = 17.6744 (12) ÅT = 294 K
c = 14.279 (1) Å0.20 × 0.12 × 0.10 mm
β = 92.421 (1)°
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
4642 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2001)
2655 reflections with I > 2σ(I)
Tmin = 0.975, Tmax = 0.989Rint = 0.067
23482 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0650 restraints
wR(F2) = 0.169H atoms treated by a mixture of independent and constrained refinement
S = 1.03Δρmax = 0.29 e Å3
4642 reflectionsΔρmin = 0.19 e Å3
310 parameters
Special details top

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) top
xyzUiso*/Ueq
C10.2091 (3)0.53564 (19)0.38291 (19)0.0604 (8)
H1A0.22690.58950.37590.072*
H1B0.13980.52840.43470.072*
C20.1299 (3)0.50482 (16)0.29426 (18)0.0481 (7)
H2A0.12470.45020.30060.058*
H2B0.02140.52330.29110.058*
C30.2078 (3)0.60132 (15)0.1804 (2)0.0516 (7)
H3A0.27770.60790.12870.062*
H3B0.25320.62870.23390.062*
C40.0490 (3)0.63386 (16)0.15382 (17)0.0439 (6)
C50.2006 (3)0.64709 (15)0.10256 (16)0.0402 (6)
C60.3564 (3)0.63661 (16)0.06912 (18)0.0482 (7)
H60.39760.58870.05620.058*
C70.4458 (3)0.70087 (19)0.05621 (18)0.0538 (8)
H70.55050.69640.03370.065*
C80.3840 (3)0.77308 (17)0.07599 (19)0.0550 (8)
H80.44910.81520.06700.066*
C90.2306 (3)0.78310 (16)0.10818 (18)0.0510 (7)
H90.18920.83100.12050.061*
C100.1396 (3)0.71858 (15)0.12152 (17)0.0420 (6)
C110.3475 (3)0.48165 (16)0.1873 (2)0.0505 (7)
H11A0.42230.49070.23950.061*
H11B0.39320.50130.13100.061*
C120.3205 (3)0.39871 (16)0.17669 (17)0.0453 (7)
C130.2109 (3)0.28778 (17)0.14316 (17)0.0481 (7)
C140.1108 (4)0.22818 (18)0.11782 (19)0.0564 (8)
H140.00650.23610.09640.068*
C150.1746 (4)0.15673 (19)0.1262 (2)0.0666 (9)
H150.11200.11530.10880.080*
C160.3291 (5)0.1445 (2)0.1598 (2)0.0759 (10)
H160.36640.09510.16570.091*
C170.4284 (4)0.2034 (2)0.1844 (2)0.0676 (9)
H170.53240.19520.20630.081*
C180.3663 (3)0.27573 (17)0.17529 (18)0.0508 (7)
C190.4248 (3)0.52156 (19)0.49117 (19)0.0605 (8)
H19A0.35200.51130.54040.073*
H19B0.44680.57540.49070.073*
N10.1992 (2)0.52134 (12)0.20352 (14)0.0427 (5)
N20.0788 (2)0.59601 (14)0.12376 (15)0.0450 (6)
H20.084 (3)0.5449 (17)0.1178 (18)0.054*
N30.0169 (3)0.70765 (14)0.15369 (15)0.0465 (6)
H30.085 (3)0.7437 (16)0.1678 (18)0.056*
N40.4296 (3)0.34628 (16)0.19490 (16)0.0548 (7)
H40.516 (4)0.3587 (17)0.218 (2)0.066*
N50.1875 (3)0.36534 (14)0.14572 (15)0.0456 (6)
H50.106 (3)0.3912 (16)0.1281 (19)0.055*
N60.7793 (3)0.37255 (17)0.32131 (19)0.0621 (7)
O10.3557 (2)0.49900 (11)0.40309 (12)0.0566 (5)
O20.6974 (3)0.42656 (14)0.29412 (17)0.0876 (8)
O30.8884 (3)0.37929 (14)0.38036 (19)0.0902 (8)
O40.7453 (3)0.30882 (15)0.28733 (18)0.0908 (8)
N70.2022 (3)0.41060 (15)0.06511 (16)0.0546 (6)
O50.3230 (2)0.44713 (13)0.04530 (17)0.0787 (7)
O60.0836 (2)0.44321 (12)0.10178 (17)0.0766 (7)
O70.1903 (3)0.34285 (14)0.0487 (2)0.0942 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0578 (18)0.075 (2)0.0474 (17)0.0142 (16)0.0083 (13)0.0031 (15)
C20.0402 (14)0.0546 (18)0.0488 (16)0.0041 (13)0.0059 (12)0.0025 (13)
C30.0405 (14)0.0479 (18)0.0652 (18)0.0094 (12)0.0127 (13)0.0071 (14)
C40.0427 (14)0.0443 (18)0.0442 (15)0.0071 (12)0.0053 (11)0.0033 (12)
C50.0433 (14)0.0412 (16)0.0360 (13)0.0016 (12)0.0003 (11)0.0054 (11)
C60.0455 (14)0.0530 (18)0.0455 (15)0.0055 (13)0.0057 (12)0.0012 (13)
C70.0441 (15)0.070 (2)0.0469 (16)0.0052 (15)0.0040 (12)0.0087 (14)
C80.0589 (18)0.055 (2)0.0504 (17)0.0157 (15)0.0009 (14)0.0098 (14)
C90.0621 (18)0.0461 (18)0.0447 (16)0.0003 (14)0.0032 (13)0.0003 (13)
C100.0459 (14)0.0434 (17)0.0364 (14)0.0002 (12)0.0033 (11)0.0027 (11)
C110.0367 (14)0.062 (2)0.0527 (17)0.0006 (13)0.0044 (12)0.0033 (14)
C120.0409 (14)0.0554 (19)0.0395 (14)0.0031 (13)0.0007 (11)0.0018 (13)
C130.0538 (16)0.055 (2)0.0356 (14)0.0063 (14)0.0035 (12)0.0021 (13)
C140.0645 (18)0.058 (2)0.0470 (16)0.0045 (16)0.0040 (14)0.0006 (14)
C150.092 (2)0.052 (2)0.0566 (19)0.0009 (18)0.0123 (17)0.0033 (15)
C160.111 (3)0.059 (2)0.058 (2)0.021 (2)0.005 (2)0.0032 (17)
C170.075 (2)0.072 (2)0.0546 (19)0.0264 (19)0.0056 (16)0.0036 (17)
C180.0571 (17)0.056 (2)0.0393 (15)0.0119 (15)0.0001 (12)0.0011 (13)
C190.0645 (19)0.070 (2)0.0456 (17)0.0011 (15)0.0152 (14)0.0014 (14)
N10.0360 (11)0.0454 (14)0.0460 (13)0.0016 (10)0.0062 (9)0.0050 (10)
N20.0433 (12)0.0399 (13)0.0507 (13)0.0031 (11)0.0087 (10)0.0027 (11)
N30.0482 (13)0.0407 (15)0.0499 (13)0.0080 (10)0.0078 (10)0.0014 (11)
N40.0441 (13)0.0697 (18)0.0498 (14)0.0114 (13)0.0078 (11)0.0008 (12)
N50.0409 (12)0.0483 (16)0.0469 (13)0.0074 (11)0.0052 (10)0.0007 (11)
N60.0457 (14)0.066 (2)0.0738 (18)0.0063 (14)0.0011 (13)0.0094 (15)
O10.0544 (11)0.0675 (14)0.0464 (11)0.0091 (10)0.0150 (9)0.0071 (9)
O20.0809 (16)0.0818 (18)0.0986 (18)0.0335 (14)0.0129 (14)0.0038 (14)
O30.0605 (14)0.0913 (19)0.116 (2)0.0012 (13)0.0352 (14)0.0062 (15)
O40.0764 (16)0.0726 (18)0.121 (2)0.0040 (14)0.0302 (15)0.0099 (15)
N70.0473 (14)0.0551 (17)0.0602 (15)0.0020 (12)0.0134 (11)0.0018 (12)
O50.0533 (12)0.0746 (16)0.1052 (18)0.0111 (11)0.0310 (12)0.0085 (13)
O60.0480 (12)0.0495 (13)0.129 (2)0.0029 (10)0.0305 (12)0.0134 (12)
O70.0891 (17)0.0481 (15)0.141 (2)0.0016 (13)0.0459 (16)0.0181 (15)
Geometric parameters (Å, º) top
C1—O11.414 (3)C12—N41.323 (3)
C1—C21.508 (4)C12—N51.326 (3)
C1—H1A0.9700C13—N51.386 (4)
C1—H1B0.9700C13—C181.386 (4)
C2—N11.473 (3)C13—C141.388 (4)
C2—H2A0.9700C14—C151.376 (4)
C2—H2B0.9700C14—H140.9300
C3—N11.454 (3)C15—C161.385 (5)
C3—C41.491 (3)C15—H150.9300
C3—H3A0.9700C16—C171.374 (5)
C3—H3B0.9700C16—H160.9300
C4—N21.324 (3)C17—C181.385 (4)
C4—N31.332 (3)C17—H170.9300
C5—C101.387 (4)C18—N41.380 (4)
C5—C61.391 (3)C19—O11.421 (3)
C5—N21.391 (3)C19—C19i1.491 (6)
C6—C71.371 (4)C19—H19A0.9700
C6—H60.9300C19—H19B0.9700
C7—C81.403 (4)N2—H20.91 (3)
C7—H70.9300N3—H30.87 (3)
C8—C91.366 (4)N4—H40.82 (3)
C8—H80.9300N5—H50.86 (3)
C9—C101.383 (4)N6—O31.227 (3)
C9—H90.9300N6—O21.231 (3)
C10—N31.392 (3)N6—O41.255 (3)
C11—N11.460 (3)N7—O71.225 (3)
C11—C121.490 (4)N7—O51.228 (3)
C11—H11A0.9700N7—O61.249 (3)
C11—H11B0.9700
O1—C1—C2111.0 (2)C18—C13—C14121.7 (3)
O1—C1—H1A109.4C15—C14—C13116.3 (3)
C2—C1—H1A109.4C15—C14—H14121.9
O1—C1—H1B109.4C13—C14—H14121.9
C2—C1—H1B109.4C14—C15—C16122.1 (3)
H1A—C1—H1B108.0C14—C15—H15118.9
N1—C2—C1119.3 (2)C16—C15—H15118.9
N1—C2—H2A107.5C17—C16—C15121.6 (3)
C1—C2—H2A107.5C17—C16—H16119.2
N1—C2—H2B107.5C15—C16—H16119.2
C1—C2—H2B107.5C16—C17—C18116.9 (3)
H2A—C2—H2B107.0C16—C17—H17121.6
N1—C3—C4112.3 (2)C18—C17—H17121.6
N1—C3—H3A109.1N4—C18—C17132.3 (3)
C4—C3—H3A109.1N4—C18—C13106.3 (2)
N1—C3—H3B109.1C17—C18—C13121.4 (3)
C4—C3—H3B109.1O1—C19—C19i108.7 (3)
H3A—C3—H3B107.9O1—C19—H19A110.0
N2—C4—N3109.4 (2)C19i—C19—H19A110.0
N2—C4—C3126.6 (3)O1—C19—H19B110.0
N3—C4—C3124.0 (2)C19i—C19—H19B110.0
C10—C5—C6121.7 (2)H19A—C19—H19B108.3
C10—C5—N2106.5 (2)C3—N1—C11112.3 (2)
C6—C5—N2131.8 (2)C3—N1—C2114.7 (2)
C7—C6—C5116.2 (3)C11—N1—C2114.7 (2)
C7—C6—H6121.9C4—N2—C5109.0 (2)
C5—C6—H6121.9C4—N2—H2124.5 (17)
C6—C7—C8121.9 (3)C5—N2—H2126.5 (17)
C6—C7—H7119.0C4—N3—C10109.0 (2)
C8—C7—H7119.0C4—N3—H3125.6 (18)
C9—C8—C7121.6 (3)C10—N3—H3125.2 (18)
C9—C8—H8119.2C12—N4—C18109.5 (2)
C7—C8—H8119.2C12—N4—H4119 (2)
C8—C9—C10116.8 (3)C18—N4—H4131 (2)
C8—C9—H9121.6C12—N5—C13109.3 (2)
C10—C9—H9121.6C12—N5—H5121.4 (19)
C9—C10—C5121.7 (2)C13—N5—H5129.3 (19)
C9—C10—N3132.2 (3)O3—N6—O2122.4 (3)
C5—C10—N3106.1 (2)O3—N6—O4120.3 (3)
N1—C11—C12111.2 (2)O2—N6—O4117.3 (3)
N1—C11—H11A109.4C1—O1—C19112.0 (2)
C12—C11—H11A109.4N6—O2—H495.9 (8)
N1—C11—H11B109.4N6—O4—H489.8 (8)
C12—C11—H11B109.4O7—N7—O5122.9 (2)
H11A—C11—H11B108.0O7—N7—O6117.4 (2)
N4—C12—N5108.9 (3)O5—N7—O6119.6 (3)
N4—C12—C11124.6 (2)N7—O6—H2120.4 (9)
N5—C12—C11126.5 (2)N7—O6—H5121.3 (8)
N5—C13—C18106.1 (2)H2—O6—H5117.9 (12)
N5—C13—C14132.2 (3)
O1—C1—C2—N169.8 (3)C12—C11—N1—C267.7 (3)
N1—C3—C4—N221.2 (4)C1—C2—N1—C360.6 (3)
N1—C3—C4—N3161.5 (2)C1—C2—N1—C1171.7 (3)
C10—C5—C6—C70.1 (4)N3—C4—N2—C50.2 (3)
N2—C5—C6—C7179.7 (3)C3—C4—N2—C5177.4 (3)
C5—C6—C7—C80.3 (4)C10—C5—N2—C40.0 (3)
C6—C7—C8—C90.8 (4)C6—C5—N2—C4179.9 (3)
C7—C8—C9—C100.8 (4)N2—C4—N3—C100.3 (3)
C8—C9—C10—C50.4 (4)C3—C4—N3—C10177.4 (2)
C8—C9—C10—N3179.2 (3)C9—C10—N3—C4179.9 (3)
C6—C5—C10—C90.0 (4)C5—C10—N3—C40.3 (3)
N2—C5—C10—C9179.9 (2)N5—C12—N4—C180.0 (3)
C6—C5—C10—N3179.7 (2)C11—C12—N4—C18178.4 (2)
N2—C5—C10—N30.1 (3)C17—C18—N4—C12178.0 (3)
N1—C11—C12—N4154.4 (2)C13—C18—N4—C120.3 (3)
N1—C11—C12—N527.5 (4)N4—C12—N5—C130.3 (3)
N5—C13—C14—C15178.5 (3)C11—C12—N5—C13178.1 (2)
C18—C13—C14—C150.1 (4)C18—C13—N5—C120.5 (3)
C13—C14—C15—C161.2 (4)C14—C13—N5—C12179.0 (3)
C14—C15—C16—C171.6 (5)C2—C1—O1—C19174.0 (2)
C15—C16—C17—C180.8 (5)C19i—C19—O1—C1177.9 (3)
C16—C17—C18—N4178.5 (3)O3—N6—O2—H4169.1 (8)
C16—C17—C18—C130.3 (4)O4—N6—O2—H49.7 (8)
N5—C13—C18—N40.5 (3)O3—N6—O4—H4169.7 (8)
C14—C13—C18—N4179.2 (2)O2—N6—O4—H49.1 (8)
N5—C13—C18—C17178.1 (2)O7—N7—O6—H2173.8 (10)
C14—C13—C18—C170.7 (4)O5—N7—O6—H24.6 (10)
C4—C3—N1—C11153.5 (2)O7—N7—O6—H51.3 (10)
C4—C3—N1—C273.1 (3)O5—N7—O6—H5177.1 (10)
C12—C11—N1—C3158.9 (2)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C14—H14···O70.932.583.364 (4)142
C11—H11A···O10.972.433.094 (3)125
C6—H6···O50.932.593.379 (4)143
N4—H4···O40.82 (3)2.31 (3)2.995 (3)142 (3)
N4—H4···O20.82 (3)2.20 (3)2.975 (4)160 (3)
N5—H5···O60.86 (3)1.87 (3)2.719 (3)174 (3)
N2—H2···O60.91 (3)1.81 (3)2.719 (3)177 (3)
C7—H7···O7ii0.932.533.443 (4)166
N3—H3···O4iii0.87 (3)1.93 (3)2.789 (3)169 (3)
N3—H3···O3iii0.87 (3)2.51 (3)3.180 (3)134 (2)
Symmetry codes: (ii) x1, y+1, z; (iii) x+1, y+1/2, z+1/2.

Experimental details

Crystal data
Chemical formulaC38H44N10O24+·4(NO3)
Mr920.87
Crystal system, space groupMonoclinic, P21/c
Temperature (K)294
a, b, c (Å)8.4296 (6), 17.6744 (12), 14.279 (1)
β (°) 92.421 (1)
V3)2125.5 (3)
Z2
Radiation typeMo Kα
µ (mm1)0.11
Crystal size (mm)0.20 × 0.12 × 0.10
Data collection
DiffractometerBruker SMART APEX CCD area-detector
Absorption correctionMulti-scan
(SADABS; Sheldrick, 2001)
Tmin, Tmax0.975, 0.989
No. of measured, independent and
observed [I > 2σ(I)] reflections
23482, 4642, 2655
Rint0.067
(sin θ/λ)max1)0.639
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.065, 0.169, 1.03
No. of reflections4642
No. of parameters310
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.29, 0.19

Computer programs: SMART (Bruker, 2001), SAINT-Plus (Bruker, 2001), SAINT-Plus, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2003), PLATON.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C14—H14···O70.932.583.364 (4)141.7
C11—H11A···O10.972.433.094 (3)125.4
C6—H6···O50.932.593.379 (4)143.4
N4—H4···O40.82 (3)2.31 (3)2.995 (3)142 (3)
N4—H4···O20.82 (3)2.20 (3)2.975 (4)160 (3)
N5—H5···O60.86 (3)1.87 (3)2.719 (3)174 (3)
N2—H2···O60.91 (3)1.81 (3)2.719 (3)177 (3)
C7—H7···O7i0.932.533.443 (4)166.1
N3—H3···O4ii0.87 (3)1.93 (3)2.789 (3)169 (3)
N3—H3···O3ii0.87 (3)2.51 (3)3.180 (3)134 (2)
Symmetry codes: (i) x1, y+1, z; (ii) x+1, y+1/2, z+1/2.
 

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