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The structure of the title complex, C14H10O4.C13H9N, which was cocrystallized from an ethanol solution containing a 1:1 mixture of diphenic acid and acridine, has been determined. Hydro­gen bonding exists between acid–acid and acid–base as well as acridine π–π interactions. Proton transfer occurs in one of the two carboxyl­ic acid–aromatic nitro­gen interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680101618X/tk6040sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680101618X/tk6040Isup2.hkl
Contains datablock I

CCDC reference: 176023

Key indicators

  • Single-crystal X-ray study
  • T = 295 K
  • Mean [sigma](C-C) = 0.008 Å
  • Disorder in main residue
  • R factor = 0.064
  • wR factor = 0.211
  • Data-to-parameter ratio = 12.2

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
PLAT_301 Alert C Main Residue Disorder ........................ 2.00 Perc. PLAT_745 Alert C D-H Calc 0.83(5), Rep 0.84000 .... Missing s.u. O1 -H01 1.555 1.555 PLAT_745 Alert C D-H Calc 0.86(5), Rep 0.85000 .... Missing s.u. O7 -H03 1.555 1.555 PLAT_745 Alert C D-H Calc 0.84(5), Rep 0.84000 .... Missing s.u. O5 -H02 1.555 1.555 PLAT_746 Alert C H...A Calc 1.75(5), Rep 1.74000 .... Missing s.u. H01 -O4 1.555 1.555 PLAT_746 Alert C H...A Calc 1.74(5), Rep 1.75000 .... Missing s.u. H03 -O3 1.555 1.555 PLAT_746 Alert C H...A Calc 1.86(4), Rep 1.86000 .... Missing s.u. H02 -N1 1.555 2.755 PLAT_748 Alert C D-H..A Calc 177(8), Rep 178.00 .... Missing s.u. O1 -H01 -O4 1.555 1.555 1.555 PLAT_748 Alert C D-H..A Calc 173(5), Rep 173.00 .... Missing s.u. O7 -H03 -O3 1.555 1.555 1.555
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
9 Alert Level C = Please check

Comment top

Diphenic acid (biphenyl-2,2'-dicarboxylic acid), (I), forms infinite zigzag acid chains via R22(8) carboxylic acid pairs (Fronczek et al., 1987). It is of interest since it is potentially a good building block in crystal engineering with organic bases. To date, no organic co-crystal structure involving diphenic acid exists in the Cambridge Structural Database (CONQUEST 1.2, 2001). We report here the first diphenic acid co-crystal structure with acridine as the base.

The asymmetric unit of complex (I) comprises of two acid and two base molecules (Fig. 1). The torsion angles of the two phenyl rings are approximately 72° and 89°, respectively. A two-acid–two-base unit exists (Fig. 2), involving an O1—H01···O4 intramolecular hydrogen bond, an O7—H03···O3 acid–acid interaction and several acid–base intermolecular interactions (Table 2). In one of the two pairs of acid–base contacts, proton transfer occurs from the carboxylic acid group O3—C14—O4 to aromatic N2, evidenced by the O3—C14 and O4—C14 bond distances (Table 1). H02, the proton involved in the other acid–base contact (located from the difference map) remains within the carboxylic group attached to O5. The O6 site was refined with disorder over two distinct positions (O6A & O6B) with equal occupancy, and possible weak hydrogen bonds C40—H40—O6A and C40—H40—O6B are noted. An infinite supramolecular unit is formed along the a axis by packing the two-acid–two-base units via π-π interactions between acridine molecules. Acridine molecular planes are approximately perpendicular to the a axis, with a distance of approximately 3.5 Å between adjacent planes (Fig. 2). The infinite supramolecular units pack assemble via close packing (Fig. 3).

Experimental top

Diphenic acid and acridine were obtained from Aldrich. 28 mg of the acid and 18 mg of the base were dissolved in 15 ml of ethanol. Crystals were obtained by slow evaporation of the ethanol solution at the room temperature.

Refinement top

Owing to large anisotropic displacement parameters, the O6 atom was refined over two distinct positions with equal fixed occupation factors (from refinement).

All H atoms bonded to C atoms were placed geometrically and refined using a riding model with the Uiso values for each H atom taken as 1.2 Ueq of the carrier atom. The O-bound H01, H02 and H03 were located from difference Fourier maps and were included in the model with the O– H distance restrained to 0.82 +/-0.02 Å. The H2 atom was located from the difference Fourier map and was refined using a riding model with the Uiso value taken as 1.2 Ueq of N2.

Computing details top

Data collection: CAD-4 Software (Enraf-Nonius, 1988); cell refinement: CAD-4 Software (SETANG); data reduction: TEXSAN(Molecular Structure Corporation, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP (Sheldrick, 1993); software used to prepare material for publication: SHELXL97).

Figures top
[Figure 1] Fig. 1. The asymmetric unit of (I) showing displacement ellipsoids at the 30% probability level. H atoms bonded to carbon have been omitted for clarity (Sheldrick, 1993).
[Figure 2] Fig. 2. Projection of the molecular packing of (I) onto the (010) plane showing the acridine molecules stacked along the a axis. (Watkin et al., 1996).
[Figure 3] Fig. 3. Projection onto (100) showing the packing of the infinite supramolecular unit. (Watkin et al., 1996).
Diphenic acid–acridine (1/1) top
Crystal data top
C14H10O4·C14H9O4·C13H9N·C13H10N+Dx = 1.347 Mg m3
Mr = 842.86Melting point: not measured K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 14.461 (3) ÅCell parameters from 25 reflections
b = 15.863 (3) Åθ = 8.0–15.0°
c = 19.166 (3) ŵ = 0.09 mm1
β = 108.98 (2)°T = 295 K
V = 4157.5 (13) Å3Block, yellow
Z = 40.30 × 0.30 × 0.20 mm
F(000) = 1760
Data collection top
Enraf-Nonius CAD-4
diffractometer
Rint = 0.045
Radiation source: fine-focus sealed tubeθmax = 25.0°, θmin = 3.6°
Graphite monochromatorh = 1716
ω/2θ scansk = 018
7509 measured reflectionsl = 022
7275 independent reflections3 standard reflections every 200 reflections
3160 reflections with I > 2σ(I) intensity decay: none
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)] = 0.064Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.211H atoms treated by a mixture of independent and constrained refinement
S = 1.01 w = 1/[σ2(Fo2) + (0.0914P)2]
where P = (Fo2 + 2Fc2)/3
7275 reflections(Δ/σ)max = 0.002
598 parametersΔρmax = 0.23 e Å3
3 restraintsΔρmin = 0.25 e Å3
Crystal data top
C14H10O4·C14H9O4·C13H9N·C13H10N+V = 4157.5 (13) Å3
Mr = 842.86Z = 4
Monoclinic, P21/cMo Kα radiation
a = 14.461 (3) ŵ = 0.09 mm1
b = 15.863 (3) ÅT = 295 K
c = 19.166 (3) Å0.30 × 0.30 × 0.20 mm
β = 108.98 (2)°
Data collection top
Enraf-Nonius CAD-4
diffractometer
Rint = 0.045
7509 measured reflections3 standard reflections every 200 reflections
7275 independent reflections intensity decay: none
3160 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.0643 restraints
wR(F2) = 0.211H atoms treated by a mixture of independent and constrained refinement
S = 1.01Δρmax = 0.23 e Å3
7275 reflectionsΔρmin = 0.25 e Å3
598 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*/UeqOcc. (<1)
H010.498 (3)0.470 (5)0.208 (3)0.15 (4)*
O10.4420 (3)0.4601 (2)0.1793 (2)0.0636 (10)
O20.3023 (3)0.5244 (2)0.1240 (2)0.0708 (11)
O30.7697 (2)0.5046 (2)0.27410 (16)0.0540 (9)
O40.6161 (3)0.4858 (2)0.26916 (18)0.0632 (10)
C80.6443 (3)0.5338 (3)0.1611 (2)0.0427 (11)
C140.6786 (4)0.5062 (3)0.2403 (2)0.0465 (12)
C20.4360 (3)0.6095 (3)0.1934 (2)0.0444 (11)
C70.5678 (3)0.5905 (3)0.1335 (2)0.0366 (10)
C10.5214 (3)0.6365 (3)0.1817 (2)0.0406 (11)
C110.5836 (4)0.5761 (3)0.0127 (3)0.0524 (13)
H110.56210.58970.03720.063*
C90.6905 (4)0.5006 (3)0.1131 (3)0.0521 (12)
H90.74350.46430.13120.063*
C120.5395 (3)0.6116 (3)0.0589 (2)0.0475 (12)
H120.48950.65060.04010.057*
C60.5609 (4)0.7140 (3)0.2107 (3)0.0551 (13)
H60.61700.73400.20270.066*
C100.6582 (4)0.5213 (3)0.0397 (3)0.0542 (13)
H100.68790.49730.00810.065*
C130.3868 (4)0.5286 (3)0.1622 (3)0.0512 (12)
C30.3930 (4)0.6585 (3)0.2339 (3)0.0603 (14)
H30.33580.64020.24140.072*
C50.5163 (5)0.7615 (3)0.2515 (3)0.0713 (17)
H50.54320.81300.27120.086*
C40.4339 (5)0.7334 (4)0.2630 (3)0.0742 (17)
H40.40510.76550.29100.089*
H030.861 (3)0.544 (3)0.242 (3)0.08 (2)*
O70.9094 (3)0.5653 (2)0.2317 (2)0.0607 (9)
O51.1873 (3)0.5394 (2)0.2677 (2)0.0655 (10)
H021.228 (5)0.531 (5)0.310 (2)0.16 (4)*
O6A1.2233 (10)0.4118 (8)0.2447 (7)0.104 (4)0.50
O6B1.1697 (9)0.4049 (7)0.2685 (7)0.101 (5)0.50
C151.0219 (3)0.5484 (3)0.1355 (2)0.0458 (12)
C211.0477 (3)0.6347 (3)0.1661 (2)0.0439 (11)
C161.0725 (3)0.4755 (3)0.1634 (2)0.0441 (11)
C220.9903 (4)0.6801 (3)0.1990 (2)0.0516 (13)
C261.1275 (4)0.6757 (3)0.1567 (3)0.0573 (13)
H261.16570.64730.13360.069*
C171.0415 (4)0.3984 (3)0.1276 (3)0.0598 (14)
H171.07520.34930.14690.072*
C280.9010 (4)0.6449 (4)0.2125 (3)0.0604 (14)
C190.9100 (4)0.4657 (4)0.0357 (3)0.0704 (16)
H190.85580.46300.00680.084*
C180.9620 (4)0.3943 (4)0.0644 (3)0.0711 (16)
H180.94330.34280.04090.085*
O80.8293 (3)0.6857 (3)0.2072 (3)0.1088 (17)
C200.9394 (4)0.5413 (4)0.0711 (3)0.0634 (15)
H200.90380.58960.05190.076*
C271.1572 (4)0.4702 (3)0.2327 (3)0.0613 (14)
C231.0136 (4)0.7632 (3)0.2208 (3)0.0640 (15)
H230.97390.79330.24150.077*
C241.0940 (5)0.8015 (4)0.2123 (3)0.0741 (17)
H241.10960.85680.22770.089*
C251.1517 (4)0.7566 (4)0.1804 (3)0.0732 (17)
H251.20730.78150.17500.088*
N10.6889 (3)0.0480 (2)0.0941 (2)0.0447 (10)
C410.6445 (3)0.0175 (3)0.0507 (2)0.0432 (11)
C360.6100 (3)0.0109 (3)0.0277 (3)0.0463 (12)
C290.6962 (3)0.1226 (3)0.0616 (3)0.0447 (11)
C350.6196 (3)0.0646 (3)0.0587 (3)0.0537 (13)
H350.59740.06980.10980.064*
C340.6616 (3)0.1340 (3)0.0159 (3)0.0475 (12)
C400.6353 (3)0.0946 (3)0.0839 (3)0.0540 (13)
H400.65830.09980.13500.065*
C300.7421 (4)0.1908 (3)0.1083 (3)0.0579 (14)
H300.76480.18440.15930.069*
C370.5678 (4)0.0835 (4)0.0693 (3)0.0618 (14)
H370.54570.08100.12050.074*
C380.5596 (4)0.1562 (4)0.0352 (3)0.0669 (15)
H380.53140.20320.06300.080*
C330.6719 (4)0.2141 (4)0.0451 (3)0.0612 (14)
H330.64850.22270.09590.073*
C390.5931 (4)0.1610 (3)0.0414 (3)0.0671 (15)
H390.58620.21140.06400.081*
C320.7150 (4)0.2776 (3)0.0002 (4)0.0700 (16)
H320.72050.33010.02010.084*
C310.7521 (4)0.2659 (3)0.0766 (4)0.0705 (16)
H310.78400.31020.10650.085*
N20.1773 (3)0.0562 (2)0.0821 (2)0.0458 (10)
H20.19200.03950.12710.055*
C540.1363 (3)0.0001 (3)0.0277 (2)0.0421 (11)
C530.1143 (3)0.0815 (3)0.0456 (3)0.0523 (12)
H530.12860.09780.09450.063*
C420.1963 (3)0.1374 (3)0.0695 (3)0.0489 (12)
C490.1158 (3)0.0250 (3)0.0458 (3)0.0488 (12)
C480.1413 (3)0.1067 (4)0.0602 (3)0.0606 (15)
H480.13240.12290.10860.073*
C470.1795 (3)0.1635 (3)0.0038 (3)0.0555 (13)
C520.0718 (4)0.1360 (3)0.0098 (4)0.0656 (15)
H520.05740.19050.00140.079*
C500.0706 (4)0.0344 (4)0.1013 (3)0.0692 (16)
H500.05560.01920.15060.083*
C460.2036 (4)0.2492 (4)0.0146 (4)0.0782 (18)
H460.19610.26900.06180.094*
C450.2375 (4)0.3014 (4)0.0446 (5)0.0816 (19)
H450.25270.35680.03680.098*
C510.0489 (4)0.1116 (5)0.0843 (4)0.0778 (18)
H510.01860.14960.12170.093*
C430.2324 (4)0.1936 (3)0.1302 (3)0.0612 (14)
H430.24340.17480.17820.073*
C440.2503 (4)0.2746 (4)0.1170 (4)0.0790 (18)
H440.27110.31270.15590.095*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.067 (3)0.045 (2)0.078 (3)0.007 (2)0.022 (2)0.0049 (19)
O20.044 (2)0.092 (3)0.066 (2)0.005 (2)0.0034 (19)0.008 (2)
O30.049 (2)0.071 (2)0.0386 (18)0.0099 (18)0.0089 (16)0.0062 (16)
O40.063 (2)0.077 (3)0.057 (2)0.0105 (19)0.0297 (19)0.0213 (19)
C80.050 (3)0.038 (3)0.038 (3)0.003 (2)0.012 (2)0.004 (2)
C140.060 (3)0.039 (3)0.041 (3)0.017 (2)0.017 (3)0.002 (2)
C20.050 (3)0.047 (3)0.035 (2)0.007 (2)0.012 (2)0.003 (2)
C70.041 (3)0.035 (2)0.033 (2)0.005 (2)0.011 (2)0.000 (2)
C10.045 (3)0.039 (3)0.033 (2)0.005 (2)0.006 (2)0.000 (2)
C110.054 (3)0.071 (3)0.031 (3)0.016 (3)0.013 (2)0.002 (2)
C90.057 (3)0.051 (3)0.049 (3)0.002 (2)0.017 (3)0.007 (2)
C120.049 (3)0.046 (3)0.045 (3)0.006 (2)0.011 (2)0.004 (2)
C60.056 (3)0.050 (3)0.053 (3)0.004 (3)0.009 (3)0.003 (3)
C100.052 (3)0.072 (4)0.043 (3)0.015 (3)0.022 (3)0.011 (3)
C130.058 (3)0.058 (3)0.045 (3)0.001 (3)0.028 (3)0.003 (3)
C30.058 (3)0.072 (4)0.046 (3)0.023 (3)0.010 (3)0.006 (3)
C50.077 (4)0.052 (3)0.068 (4)0.007 (3)0.001 (3)0.020 (3)
C40.069 (4)0.083 (5)0.060 (4)0.029 (4)0.006 (3)0.021 (3)
O70.054 (2)0.069 (3)0.058 (2)0.006 (2)0.0176 (19)0.0089 (19)
O50.073 (3)0.054 (2)0.052 (2)0.010 (2)0.004 (2)0.004 (2)
O6A0.125 (11)0.067 (8)0.083 (8)0.037 (8)0.017 (7)0.015 (6)
O6B0.118 (11)0.047 (6)0.084 (8)0.025 (7)0.040 (7)0.035 (6)
C150.040 (3)0.063 (3)0.035 (3)0.001 (2)0.013 (2)0.006 (2)
C210.043 (3)0.049 (3)0.034 (2)0.008 (2)0.005 (2)0.009 (2)
C160.043 (3)0.049 (3)0.039 (3)0.002 (2)0.011 (2)0.004 (2)
C220.055 (3)0.049 (3)0.045 (3)0.008 (3)0.009 (3)0.008 (2)
C260.048 (3)0.060 (4)0.061 (3)0.007 (3)0.014 (3)0.011 (3)
C170.068 (4)0.053 (3)0.056 (3)0.003 (3)0.015 (3)0.006 (3)
C280.070 (4)0.064 (4)0.049 (3)0.016 (3)0.020 (3)0.002 (3)
C190.048 (3)0.093 (5)0.062 (4)0.000 (3)0.007 (3)0.025 (4)
C180.070 (4)0.077 (4)0.067 (4)0.022 (3)0.023 (3)0.029 (3)
O80.094 (3)0.081 (3)0.177 (5)0.035 (3)0.079 (3)0.014 (3)
C200.051 (3)0.076 (4)0.061 (3)0.016 (3)0.015 (3)0.010 (3)
C270.082 (4)0.043 (3)0.049 (3)0.002 (3)0.007 (3)0.003 (3)
C230.080 (4)0.047 (3)0.056 (3)0.009 (3)0.009 (3)0.006 (3)
C240.092 (5)0.045 (3)0.072 (4)0.004 (3)0.009 (4)0.007 (3)
C250.066 (4)0.062 (4)0.081 (4)0.006 (3)0.010 (3)0.030 (3)
N10.041 (2)0.047 (2)0.045 (2)0.0024 (19)0.0120 (19)0.0049 (19)
C410.030 (2)0.052 (3)0.047 (3)0.006 (2)0.011 (2)0.005 (2)
C360.031 (2)0.055 (3)0.048 (3)0.002 (2)0.006 (2)0.006 (3)
C290.037 (3)0.046 (3)0.051 (3)0.003 (2)0.015 (2)0.000 (2)
C350.039 (3)0.069 (4)0.046 (3)0.004 (3)0.003 (2)0.001 (3)
C340.030 (2)0.055 (3)0.054 (3)0.009 (2)0.010 (2)0.007 (3)
C400.050 (3)0.058 (3)0.055 (3)0.015 (3)0.018 (3)0.003 (3)
C300.063 (3)0.051 (3)0.057 (3)0.001 (3)0.016 (3)0.003 (3)
C370.051 (3)0.076 (4)0.054 (3)0.000 (3)0.010 (3)0.009 (3)
C380.052 (3)0.070 (4)0.075 (4)0.019 (3)0.015 (3)0.026 (3)
C330.053 (3)0.071 (4)0.058 (3)0.014 (3)0.015 (3)0.021 (3)
C390.055 (3)0.058 (4)0.083 (4)0.016 (3)0.015 (3)0.003 (3)
C320.068 (4)0.046 (3)0.096 (5)0.010 (3)0.027 (4)0.020 (3)
C310.073 (4)0.044 (3)0.092 (5)0.000 (3)0.024 (4)0.003 (3)
N20.048 (2)0.048 (2)0.042 (2)0.0013 (19)0.0162 (19)0.0055 (19)
C540.032 (2)0.053 (3)0.039 (3)0.008 (2)0.008 (2)0.000 (2)
C530.046 (3)0.050 (3)0.057 (3)0.007 (2)0.011 (3)0.000 (3)
C420.037 (3)0.049 (3)0.061 (3)0.003 (2)0.016 (2)0.013 (3)
C490.031 (2)0.073 (4)0.043 (3)0.002 (2)0.012 (2)0.005 (3)
C480.044 (3)0.093 (4)0.044 (3)0.013 (3)0.013 (3)0.027 (3)
C470.037 (3)0.061 (3)0.067 (4)0.008 (3)0.014 (3)0.018 (3)
C520.046 (3)0.053 (3)0.098 (5)0.000 (3)0.024 (3)0.014 (3)
C500.049 (3)0.106 (5)0.055 (3)0.010 (4)0.019 (3)0.014 (4)
C460.061 (4)0.079 (4)0.094 (5)0.014 (4)0.025 (4)0.038 (4)
C450.055 (4)0.059 (4)0.122 (6)0.001 (3)0.018 (4)0.023 (4)
C510.055 (4)0.096 (5)0.075 (5)0.002 (4)0.012 (3)0.040 (4)
C430.057 (3)0.056 (4)0.065 (4)0.004 (3)0.012 (3)0.004 (3)
C440.064 (4)0.059 (4)0.102 (5)0.004 (3)0.010 (4)0.002 (4)
Geometric parameters (Å, º) top
O1—C131.325 (6)C24—C251.382 (8)
O1—H010.84 (5)C24—H240.9300
O2—C131.205 (6)C25—H250.9300
O3—C141.265 (5)N1—C411.355 (5)
O4—C141.246 (5)N1—C291.357 (5)
C8—C71.391 (6)C41—C401.405 (6)
C8—C91.404 (6)C41—C361.424 (6)
C8—C141.500 (6)C36—C351.364 (6)
C2—C31.381 (6)C36—C371.420 (7)
C2—C11.393 (6)C29—C341.417 (6)
C2—C131.495 (6)C29—C301.423 (6)
C7—C121.393 (6)C35—C341.389 (6)
C7—C11.497 (6)C35—H350.9300
C1—C61.393 (6)C34—C331.415 (7)
C11—C101.351 (7)C40—C391.350 (7)
C11—C121.369 (6)C40—H400.9300
C11—H110.9300C30—C311.366 (7)
C9—C101.371 (6)C30—H300.9300
C9—H90.9300C37—C381.349 (7)
C12—H120.9300C37—H370.9300
C6—C51.385 (7)C38—C391.390 (7)
C6—H60.9300C38—H380.9300
C10—H100.9300C33—C321.340 (7)
C3—C41.364 (7)C33—H330.9300
C3—H30.9300C39—H390.9300
C5—C41.356 (8)C32—C311.406 (7)
C5—H50.9300C32—H320.9300
C4—H40.9300C31—H310.9300
O7—C281.308 (6)N2—C541.354 (5)
O7—H030.85 (5)N2—C421.355 (6)
O5—C271.287 (6)N2—H20.8600
O5—H020.84 (5)C54—C491.400 (6)
O6A—C271.297 (12)C54—C531.400 (6)
O6B—C271.223 (11)C53—C521.350 (7)
C15—C161.381 (6)C53—H530.9300
C15—C201.415 (6)C42—C471.408 (7)
C15—C211.489 (6)C42—C431.423 (7)
C21—C261.385 (6)C49—C481.399 (7)
C21—C221.394 (6)C49—C501.411 (7)
C16—C171.402 (6)C48—C471.377 (7)
C16—C271.487 (7)C48—H480.9300
C22—C231.392 (7)C47—C461.436 (8)
C22—C281.505 (7)C52—C511.412 (8)
C26—C251.369 (7)C52—H520.9300
C26—H260.9300C50—C511.330 (8)
C17—C181.373 (7)C50—H500.9300
C17—H170.9300C46—C451.360 (8)
C28—O81.199 (6)C46—H460.9300
C19—C181.371 (7)C45—C441.406 (8)
C19—C201.375 (7)C45—H450.9300
C19—H190.9300C51—H510.9300
C18—H180.9300C43—C441.352 (7)
C20—H200.9300C43—H430.9300
C23—C241.367 (7)C44—H440.9300
C23—H230.9300
C13—O1—H01113 (5)C25—C24—H24120.5
C7—C8—C9118.8 (4)C26—C25—C24120.2 (5)
C7—C8—C14122.3 (4)C26—C25—H25119.9
C9—C8—C14118.9 (4)C24—C25—H25119.9
O4—C14—O3123.6 (4)C41—N1—C29118.6 (4)
O4—C14—C8118.4 (4)N1—C41—C40119.0 (4)
O3—C14—C8118.0 (4)N1—C41—C36121.7 (4)
C3—C2—C1120.2 (5)C40—C41—C36119.3 (4)
C3—C2—C13117.7 (4)C35—C36—C37123.6 (5)
C1—C2—C13122.1 (4)C35—C36—C41118.2 (4)
C8—C7—C12118.6 (4)C37—C36—C41118.2 (5)
C8—C7—C1122.7 (4)N1—C29—C34122.6 (4)
C12—C7—C1118.4 (4)N1—C29—C30117.6 (4)
C2—C1—C6118.5 (4)C34—C29—C30119.8 (4)
C2—C1—C7123.3 (4)C36—C35—C34121.8 (5)
C6—C1—C7117.9 (4)C36—C35—H35119.1
C10—C11—C12120.0 (4)C34—C35—H35119.1
C10—C11—H11120.0C35—C34—C33124.1 (5)
C12—C11—H11120.0C35—C34—C29117.1 (4)
C10—C9—C8120.5 (5)C33—C34—C29118.9 (5)
C10—C9—H9119.8C39—C40—C41119.8 (5)
C8—C9—H9119.8C39—C40—H40120.1
C11—C12—C7121.4 (4)C41—C40—H40120.1
C11—C12—H12119.3C31—C30—C29118.5 (5)
C7—C12—H12119.3C31—C30—H30120.7
C5—C6—C1119.9 (5)C29—C30—H30120.7
C5—C6—H6120.0C38—C37—C36120.7 (5)
C1—C6—H6120.0C38—C37—H37119.6
C11—C10—C9120.7 (5)C36—C37—H37119.6
C11—C10—H10119.7C37—C38—C39120.2 (5)
C9—C10—H10119.7C37—C38—H38119.9
O2—C13—O1121.1 (5)C39—C38—H38119.9
O2—C13—C2123.2 (5)C32—C33—C34120.5 (5)
O1—C13—C2115.8 (4)C32—C33—H33119.7
C4—C3—C2120.3 (5)C34—C33—H33119.7
C4—C3—H3119.8C40—C39—C38121.8 (5)
C2—C3—H3119.8C40—C39—H39119.1
C4—C5—C6120.6 (5)C38—C39—H39119.1
C4—C5—H5119.7C33—C32—C31120.8 (5)
C6—C5—H5119.7C33—C32—H32119.6
C5—C4—C3120.5 (5)C31—C32—H32119.6
C5—C4—H4119.8C30—C31—C32121.5 (5)
C3—C4—H4119.8C30—C31—H31119.3
C28—O7—H03116 (4)C32—C31—H31119.3
C27—O5—H02112 (6)C54—N2—C42123.5 (4)
C16—C15—C20117.5 (4)C54—N2—H2118.2
C16—C15—C21125.8 (4)C42—N2—H2118.2
C20—C15—C21116.7 (4)N2—C54—C49119.0 (4)
C26—C21—C22117.4 (5)N2—C54—C53119.8 (4)
C26—C21—C15119.6 (4)C49—C54—C53121.2 (5)
C22—C21—C15122.8 (4)C52—C53—C54118.7 (5)
C15—C16—C17119.7 (4)C52—C53—H53120.7
C15—C16—C27124.9 (4)C54—C53—H53120.7
C17—C16—C27115.3 (4)N2—C42—C47118.6 (5)
C23—C22—C21120.2 (5)N2—C42—C43119.4 (4)
C23—C22—C28115.9 (5)C47—C42—C43122.0 (5)
C21—C22—C28123.8 (5)C48—C49—C54118.6 (5)
C25—C26—C21122.1 (5)C48—C49—C50123.8 (5)
C25—C26—H26118.9C54—C49—C50117.6 (5)
C21—C26—H26118.9C47—C48—C49121.0 (4)
C18—C17—C16121.1 (5)C47—C48—H48119.5
C18—C17—H17119.5C49—C48—H48119.5
C16—C17—H17119.5C48—C47—C42119.1 (5)
O8—C28—O7122.9 (5)C48—C47—C46124.1 (5)
O8—C28—C22123.5 (5)C42—C47—C46116.8 (5)
O7—C28—C22113.6 (5)C53—C52—C51121.0 (5)
C18—C19—C20118.7 (5)C53—C52—H52119.5
C18—C19—H19120.6C51—C52—H52119.5
C20—C19—H19120.6C51—C50—C49121.2 (6)
C19—C18—C17120.5 (5)C51—C50—H50119.4
C19—C18—H18119.8C49—C50—H50119.4
C17—C18—H18119.8C45—C46—C47119.7 (6)
C19—C20—C15122.5 (5)C45—C46—H46120.1
C19—C20—H20118.7C47—C46—H46120.1
C15—C20—H20118.7C46—C45—C44122.3 (6)
O6B—C27—O5117.8 (7)C46—C45—H45118.8
O6B—C27—O6A47.9 (6)C44—C45—H45118.8
O5—C27—O6A114.3 (8)C50—C51—C52120.3 (5)
O6B—C27—C16118.5 (7)C50—C51—H51119.9
O5—C27—C16117.3 (5)C52—C51—H51119.9
O6A—C27—C16123.0 (7)C44—C43—C42118.9 (5)
C24—C23—C22121.1 (5)C44—C43—H43120.5
C24—C23—H23119.4C42—C43—H43120.5
C22—C23—H23119.4C43—C44—C45120.1 (6)
C23—C24—C25118.9 (5)C43—C44—H44120.0
C23—C24—H24120.5C45—C44—H44120.0
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H01···O40.841.742.578 (6)178
O7—H03···O30.851.752.596 (5)173
O5—H02···N1i0.841.862.675 (5)162
C40—H40···O6Aii0.932.393.258 (14)155
C40—H40···O6Bii0.932.573.282 (12)133
N2—H2···O3iii0.861.882.734 (5)177
Symmetry codes: (i) x+2, y+1/2, z+1/2; (ii) x+2, y1/2, z+1/2; (iii) x+1, y1/2, z+1/2.

Experimental details

Crystal data
Chemical formulaC14H10O4·C14H9O4·C13H9N·C13H10N+
Mr842.86
Crystal system, space groupMonoclinic, P21/c
Temperature (K)295
a, b, c (Å)14.461 (3), 15.863 (3), 19.166 (3)
β (°) 108.98 (2)
V3)4157.5 (13)
Z4
Radiation typeMo Kα
µ (mm1)0.09
Crystal size (mm)0.30 × 0.30 × 0.20
Data collection
DiffractometerEnraf-Nonius CAD-4
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
7509, 7275, 3160
Rint0.045
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.064, 0.211, 1.01
No. of reflections7275
No. of parameters598
No. of restraints3
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.23, 0.25

Computer programs: CAD-4 Software (Enraf-Nonius, 1988), CAD-4 Software (SETANG), TEXSAN(Molecular Structure Corporation, 1995), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), XP (Sheldrick, 1993), SHELXL97).

Selected bond lengths (Å) top
O1—C131.325 (6)O5—C271.287 (6)
O2—C131.205 (6)O6A—C271.297 (12)
O3—C141.265 (5)O6B—C271.223 (11)
O4—C141.246 (5)C28—O81.199 (6)
O7—C281.308 (6)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H01···O40.841.742.578 (6)178
O7—H03···O30.851.752.596 (5)173
O5—H02···N1i0.841.862.675 (5)162
C40—H40···O6Aii0.932.393.258 (14)155
C40—H40···O6Bii0.932.573.282 (12)133
N2—H2···O3iii0.861.882.734 (5)177
Symmetry codes: (i) x+2, y+1/2, z+1/2; (ii) x+2, y1/2, z+1/2; (iii) x+1, y1/2, z+1/2.
 

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