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The title compound, 8,15,28,35-tetra­aza­hepta­cyclo[35.3.1.12,6.117,21.122,26.09,14·029,34]tetraconta-1(41),2,4,6(42),7,9,11,13,15,17,19,21(43),22,24,26(44),27,29,31,33,35,37,39-docosaene-41,42,43,44-tetrol dimeth­yl sulfoxide tetra­solvate, C40H28N4O4·4C2H6OS, adopts a chair-shaped C2h symmetric conformation with crystallographically imposed inversion symmetry. Four intra­molecular hydrogen bonds are observed between phenol O and imine N atoms.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S010827010501022X/av1234sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S010827010501022X/av1234Isup2.hkl
Contains datablock I

CCDC reference: 275538

Comment top

Our ongoing studies of the coordination chemistry of macrocyclic ligands (Kühn et al., 2001) and metal–functional group cooperation (Kövari & Krämer, 1996; Plitt et al., 2004) require the synthesis and modelling of known and novel cyclic compounds. The Schiff base macrocycle in the title compound, (I), attracts attention since it might be considered as a dimeric C—C-coupled form of the well described ligand N,N'-bis(salicylidene)-benzene-1,2-diamine (salphen). Biphenyl-derived Schiff base macrocycle (I) is analogous to the binaphthyl-derived compounds prepared by Brunner & Schiesling (1994) and Zhang et al. (2001). However, Zhang and co-workers describe the formation of a polymer when condensing the biphenyl-derived dicarbaldehyde with 1,2-diaminobenzene in ethanol. We report here the first synthesis of (I), which can be obtained in good yield when acetonitrile is used as solvent. To the best of our knowledge, no structural data have previously been published for (I), nor for its binaphthyl derivative and analogues containing different 1,2-diamino moieties.

The molecular structure of (I) is shown in Fig. 1. The compound crystallizes from dimethyl sulfoxide (DMSO) solution. X-ray diffraction analysis reveals one molecule of (I) and four molecules of DMSO per unit cell. In the crystal structure, the molecule shows a chair-shaped C2h symmetric conformation with crystallographically imposed inversion symmetry [symmetry code: (i) 2 − x, 1 − y, 2 − z]. Selected bond distances and angles (Table 1) are typical and do not differ from those observed for salphen (Bresciani Pahor et al., 1976).

For the phenol rings, the attached O (O2 and O12) and C atoms (C17 and C28i), and for the phenylendiamine rings the attached N atoms (N18 and N27), deviate from the ring planes by only 0.04, 0.14 and 0.07 Å (mean values), respectively. The imino unit C—CN and the phenolic rings are almost coplanar, with interplanar angles of 7.0 (4) and 7.4 (4)°, respectively, whereas on the other side, the imino unit C—NC and the phenylene diamine rings deviate from coplanarity by 47.6 (4) and 54.8 (4)°, respectively. As expected, the biphenylene unit is not planar. The two aromatic rings are twisted relative to each other by an angle of 76.8 (4)° (Fig. 2).

Schiff base macrocycle (I) contains four intramolecular O—H···N hydrogen bonds, between the phenol O atoms and the imino N atoms (Table 2). Notable intermolecular interactions between the molecules of (I) or interactions involving the solvent molecules were not found.

Experimental top

Schiff base macrocycle (I) was prepared using a procedure similar to that described for the analogous binaphthyl derivative (Brunner & Schiesling, 1994; Zhang et al., 2001). 2,2'-Dihydroxybiphenyl-3,3'-dicarbaldehyde (484 mg, 2 mmol) (Yardley & Fletcher, 1976; Zhang et al., 2001) and 1,2-diaminobenzene (216 mg, 2 mmol) were dissolved in dry acetonitrile (20 ml) and refluxed overnight. The precipitate which formed was filtered off, washed with acetonitrile (3 × 1 ml) and dried in vacuo, yielding 70% of a pale yellow solid. 1H NMR (200 MHz, DMSO-d6, δ, p.p.m.): 7.56–7.59 (m, 6H, Har), 8.26 (s, 3H, CHN), 14.47 (s, 3H, OH); IR (KBr, ν, cm−1): 1617 (s), 1582 (m), 1437 (m), 1212 (m), 826 (m), 779 (m), 747 (s). HRMS (ESI+): m/z, calculated for C40H29N4O4 ([M+H]+): 629.2189; found: 629.2188. Elemental analysis (%), calculated for C40H28N4O4·2CH3CN: C 74.35, H 4.82, N 11.82; found: C 74.29, H 4.78, N 11.89. Single crystals were obtained by slow cooling of a saturated solution of (I) in DMSO.

Refinement top

Hydroxyl H atoms were refined isotropically (H1 and H12 at O2 and O12). All other H atoms were included in the structural model at geometrically calculated positions, with C—H distances in the range 0.95–0.98 Ån and refined riding on their parent C atom, with Uiso(H) = 1.0, 1.2 or 1.5Ueq(C). Please check added text. Two solvent molecules of DMSO were found in the asymmetric unit. One of these is exactly located, while the other one was found in two alternative orientations (93:7 occupancy). Both instances of this disordered DMSO molecule, as well as the proper DMSO molecule, were constrained to have similar chemically equivalent distances and angles.

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SMART; data reduction: SHELXTL (Bruker, 2001); program(s) used to solve structure: SHELXTL; program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. The structure of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level and H atoms are shown as spheres of arbitrary size. DMSO molecules and aromatic H atoms have been omitted for clarity. Atoms without labels or marked with a superscript `i' are at the symmetry position (2 − x, 1 − y, 2 − z).
[Figure 2] Fig. 2. An alternative view of (I), revealing the chair conformation.
8,15,28,35- tetraazaheptacyclo[35.3.1.12,6.117,21.122,26.09,14·O29,34]tetraconta- 37,38,39,40-tetrol dimethyl sulfoxide tetrasolvate top
Crystal data top
C40H28N4O4·4C2H6OSZ = 1
Mr = 941.18F(000) = 496
Triclinic, P1Dx = 1.313 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 10.4876 (6) ÅCell parameters from 1790 reflections
b = 11.2572 (7) Åθ = 1.9–27.5°
c = 12.4998 (8) ŵ = 0.26 mm1
α = 99.603 (1)°T = 200 K
β = 110.874 (2)°Polyhedron, yellow
γ = 112.700 (2)°0.12 × 0.10 × 0.08 mm
V = 1190.15 (13) Å3
Data collection top
Bruker SMART CCD area-detector
diffractometer
4343 independent reflections
Radiation source: normal-focus sealed tube2489 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.064
ϕ and ω scansθmax = 25.3°, θmin = 1.9°
Absorption correction: multi-scan
(SADABS; Bruker, 1997)
h = 1212
Tmin = 0.886, Tmax = 0.980k = 1313
10638 measured reflectionsl = 1515
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)] = 0.049Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.112H atoms treated by a mixture of independent and constrained refinement
S = 0.99 w = 1/[σ2(Fo2) + (0.0446P)2 + 0.0226P]
where P = (Fo2 + 2Fc2)/3
4343 reflections(Δ/σ)max = 0.001
315 parametersΔρmax = 0.19 e Å3
36 restraintsΔρmin = 0.29 e Å3
Crystal data top
C40H28N4O4·4C2H6OSγ = 112.700 (2)°
Mr = 941.18V = 1190.15 (13) Å3
Triclinic, P1Z = 1
a = 10.4876 (6) ÅMo Kα radiation
b = 11.2572 (7) ŵ = 0.26 mm1
c = 12.4998 (8) ÅT = 200 K
α = 99.603 (1)°0.12 × 0.10 × 0.08 mm
β = 110.874 (2)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
4343 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 1997)
2489 reflections with I > 2σ(I)
Tmin = 0.886, Tmax = 0.980Rint = 0.064
10638 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.04936 restraints
wR(F2) = 0.112H atoms treated by a mixture of independent and constrained refinement
S = 0.99Δρmax = 0.19 e Å3
4343 reflectionsΔρmin = 0.29 e Å3
315 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. The used restraints constrain all chemically equivalent bonds and angles in the two solvent DMSO molecules, one of them occurring in two instances, to be similar.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
C10.8732 (3)0.0938 (3)0.8449 (2)0.0265 (7)
C20.7859 (3)0.1544 (3)0.7926 (2)0.0268 (7)
O20.8601 (2)0.27820 (19)0.78267 (18)0.0331 (5)
H20.781 (4)0.302 (3)0.744 (3)0.076 (12)*
C30.6228 (3)0.0874 (3)0.7487 (2)0.0273 (7)
C40.5513 (4)0.0374 (3)0.7635 (3)0.0342 (8)
H40.44180.08240.73490.041*
C50.6361 (4)0.0960 (3)0.8182 (3)0.0380 (8)
H50.58670.18000.82970.046*
C60.7962 (4)0.0309 (3)0.8569 (2)0.0341 (8)
H60.85450.07330.89260.041*
C111.0434 (3)0.1578 (3)0.8825 (2)0.0282 (7)
C121.1523 (3)0.2704 (3)0.9918 (2)0.0266 (7)
O121.0988 (2)0.3194 (2)1.06285 (19)0.0322 (5)
H121.181 (4)0.382 (4)1.135 (3)0.081 (13)*
C131.3126 (3)0.3282 (3)1.0279 (3)0.0276 (7)
C141.3625 (4)0.2722 (3)0.9525 (3)0.0363 (8)
H141.47060.31140.97550.044*
C151.2571 (4)0.1615 (3)0.8458 (3)0.0410 (8)
H151.29170.12410.79520.049*
C161.0996 (3)0.1050 (3)0.8130 (3)0.0335 (8)
H161.02740.02700.74010.040*
C171.4276 (3)0.4326 (3)1.1471 (3)0.0298 (7)
H171.53490.46221.17130.036*
N181.3894 (3)0.4864 (2)1.2211 (2)0.0286 (6)
C211.5059 (3)0.5707 (3)1.3436 (3)0.0275 (7)
C221.6028 (3)0.5273 (3)1.4127 (3)0.0314 (7)
H221.59600.44251.37650.038*
C231.7091 (3)0.6061 (3)1.5339 (3)0.0340 (8)
H231.77410.57481.58090.041*
C241.7207 (3)0.7300 (3)1.5864 (3)0.0361 (8)
H241.79340.78401.66980.043*
C251.6269 (3)0.7756 (3)1.5180 (3)0.0354 (8)
H251.63680.86191.55450.043*
C261.5180 (3)0.6969 (3)1.3965 (3)0.0275 (7)
N271.4145 (3)0.7378 (2)1.3249 (2)0.0294 (6)
C281.4728 (3)0.8565 (3)1.3150 (2)0.0299 (7)
H281.58300.90991.35080.036*
S10.93529 (10)0.25776 (9)0.45586 (8)0.0379 (3)0.933 (3)
O110.8233 (7)0.1130 (5)0.3751 (3)0.0559 (13)0.933 (3)
C311.0499 (5)0.2568 (6)0.6001 (4)0.0532 (14)0.933 (3)
H31A0.98120.20530.63130.080*0.933 (3)
H31B1.11980.35160.65800.080*0.933 (3)
H31C1.11170.21300.59040.080*0.933 (3)
C320.8283 (6)0.3265 (5)0.5022 (6)0.0588 (15)0.933 (3)
H32A0.75910.33780.43250.088*0.933 (3)
H32B0.90090.41610.56830.088*0.933 (3)
H32C0.76610.26340.53130.088*0.933 (3)
S20.84997 (10)0.35728 (8)0.17968 (7)0.0406 (3)
O210.7445 (3)0.3809 (2)0.2251 (2)0.0598 (7)
C410.7608 (4)0.1772 (3)0.1046 (3)0.0626 (11)
H41A0.76240.13150.16490.094*
H41B0.81800.15760.06330.094*
H41C0.65260.14290.04410.094*
C420.8245 (4)0.4064 (3)0.0499 (3)0.0434 (9)
H42A0.71430.35410.01110.065*
H42B0.88750.38730.01470.065*
H42C0.85760.50500.07390.065*
S1B0.862 (2)0.1692 (17)0.5114 (15)0.075 (7)*0.067 (3)
O11B0.811 (11)0.094 (10)0.381 (3)0.075 (7)*0.067 (3)
C31B1.067 (4)0.231 (10)0.586 (9)0.075 (7)*0.067 (3)
H31D1.10530.25960.67490.112*0.067 (3)
H31E1.11990.31020.56550.112*0.067 (3)
H31F1.08970.15800.55930.112*0.067 (3)
C32B0.867 (11)0.330 (5)0.515 (11)0.075 (7)*0.067 (3)
H32D0.80430.32270.43180.112*0.067 (3)
H32E0.97490.40160.54620.112*0.067 (3)
H32F0.82440.35310.56820.112*0.067 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0310 (18)0.0276 (17)0.0193 (15)0.0153 (15)0.0099 (14)0.0060 (13)
C20.0324 (18)0.0201 (16)0.0255 (16)0.0104 (14)0.0148 (15)0.0053 (13)
O20.0298 (13)0.0299 (12)0.0435 (13)0.0155 (10)0.0170 (11)0.0190 (10)
C30.0310 (18)0.0246 (17)0.0222 (16)0.0130 (15)0.0099 (14)0.0056 (13)
C40.0304 (18)0.0284 (18)0.0322 (18)0.0080 (15)0.0112 (15)0.0077 (15)
C50.040 (2)0.0226 (17)0.0389 (19)0.0075 (16)0.0135 (17)0.0124 (15)
C60.043 (2)0.0285 (17)0.0259 (17)0.0188 (16)0.0098 (16)0.0077 (14)
C110.0342 (19)0.0268 (17)0.0266 (16)0.0175 (15)0.0136 (15)0.0104 (14)
C120.0335 (19)0.0242 (16)0.0297 (17)0.0185 (15)0.0163 (15)0.0118 (14)
O120.0276 (13)0.0360 (12)0.0294 (12)0.0162 (11)0.0130 (11)0.0020 (10)
C130.0291 (18)0.0282 (17)0.0307 (17)0.0179 (15)0.0132 (15)0.0138 (14)
C140.0320 (19)0.045 (2)0.041 (2)0.0229 (17)0.0201 (17)0.0172 (17)
C150.046 (2)0.053 (2)0.0363 (19)0.0322 (19)0.0239 (18)0.0123 (17)
C160.039 (2)0.0335 (18)0.0277 (17)0.0207 (16)0.0125 (16)0.0084 (14)
C170.0265 (18)0.0297 (17)0.0371 (18)0.0157 (15)0.0148 (16)0.0153 (15)
N180.0268 (14)0.0291 (14)0.0291 (14)0.0156 (12)0.0110 (12)0.0075 (12)
C210.0229 (17)0.0270 (17)0.0327 (18)0.0119 (14)0.0134 (15)0.0102 (14)
C220.0283 (18)0.0319 (17)0.0361 (18)0.0168 (15)0.0148 (16)0.0118 (15)
C230.0224 (17)0.044 (2)0.0348 (19)0.0179 (15)0.0105 (15)0.0135 (16)
C240.0296 (19)0.039 (2)0.0285 (17)0.0133 (16)0.0075 (15)0.0078 (15)
C250.036 (2)0.0321 (18)0.0347 (19)0.0162 (16)0.0148 (17)0.0069 (15)
C260.0214 (17)0.0303 (17)0.0346 (18)0.0142 (14)0.0143 (15)0.0124 (15)
N270.0279 (15)0.0258 (14)0.0339 (15)0.0147 (12)0.0133 (12)0.0072 (12)
C280.0280 (18)0.0312 (18)0.0260 (16)0.0133 (15)0.0123 (14)0.0028 (14)
S10.0304 (6)0.0462 (6)0.0326 (5)0.0155 (5)0.0130 (4)0.0148 (4)
O110.0488 (19)0.044 (2)0.0483 (16)0.0185 (18)0.0108 (14)0.0073 (15)
C310.046 (3)0.078 (3)0.041 (3)0.035 (2)0.017 (2)0.027 (2)
C320.066 (4)0.067 (3)0.044 (3)0.046 (3)0.016 (3)0.006 (2)
S20.0440 (5)0.0432 (5)0.0349 (5)0.0250 (4)0.0160 (4)0.0096 (4)
O210.0831 (19)0.0752 (18)0.0555 (15)0.0557 (16)0.0474 (15)0.0233 (13)
C410.100 (3)0.040 (2)0.066 (3)0.032 (2)0.057 (2)0.0220 (19)
C420.042 (2)0.046 (2)0.051 (2)0.0234 (17)0.0255 (18)0.0219 (17)
Geometric parameters (Å, º) top
C1—C61.388 (4)C24—C251.378 (4)
C1—C21.391 (4)C24—H240.9500
C1—C111.491 (4)C25—C261.390 (4)
C2—O21.362 (3)C25—H250.9500
C2—C31.412 (4)C26—N271.422 (3)
O2—N27i2.626 (3)N27—C281.286 (3)
O2—H20.96 (3)C28—C3i1.458 (4)
C3—C41.393 (4)C28—H280.9500
C3—C28i1.458 (4)S1—O111.477 (5)
C4—C51.366 (4)S1—C311.780 (5)
C4—H40.9500S1—C321.782 (5)
C5—C61.393 (4)C31—H31A0.9800
C5—H50.9500C31—H31B0.9800
C6—H60.9500C31—H31C0.9800
C11—C161.385 (4)C32—H32A0.9800
C11—C121.404 (4)C32—H32B0.9800
C12—O121.356 (3)C32—H32C0.9800
C12—C131.404 (4)S2—O211.497 (2)
O12—N182.603 (3)S2—C421.765 (3)
O12—H120.90 (4)S2—C411.772 (3)
C13—C141.403 (4)C41—H41A0.9800
C13—C171.448 (4)C41—H41B0.9800
C14—C151.373 (4)C41—H41C0.9800
C14—H140.9500C42—H42A0.9800
C15—C161.386 (4)C42—H42B0.9800
C15—H150.9500C42—H42C0.9800
C16—H160.9500S1B—O11B1.497 (18)
C17—N181.284 (3)S1B—C32B1.781 (16)
C17—H170.9500S1B—C31B1.782 (16)
N18—C211.423 (3)C31B—H31D0.9800
C21—C221.384 (4)C31B—H31E0.9800
C21—C261.400 (4)C31B—H31F0.9800
C22—C231.381 (4)C32B—H32D0.9800
C22—H220.9500C32B—H32E0.9800
C23—C241.378 (4)C32B—H32F0.9800
C23—H230.9500
C6—C1—C2118.1 (3)C23—C22—H22119.7
C6—C1—C11120.8 (3)C21—C22—H22119.7
C2—C1—C11121.0 (3)C24—C23—C22119.9 (3)
O2—C2—C1118.8 (3)C24—C23—H23120.0
O2—C2—C3120.6 (3)C22—C23—H23120.0
C1—C2—C3120.5 (3)C25—C24—C23120.0 (3)
C2—O2—N27i87.30 (16)C25—C24—H24120.0
C2—O2—H2107 (2)C23—C24—H24120.0
C4—C3—C2119.1 (3)C24—C25—C26120.8 (3)
C4—C3—C28i119.4 (3)C24—C25—H25119.6
C2—C3—C28i121.5 (3)C26—C25—H25119.6
C5—C4—C3121.1 (3)C25—C26—C21119.0 (3)
C5—C4—H4119.5C25—C26—N27122.3 (3)
C3—C4—H4119.5C21—C26—N27118.7 (2)
C4—C5—C6119.0 (3)C28—N27—C26118.4 (2)
C4—C5—H5120.5N27—C28—C3i122.9 (3)
C6—C5—H5120.5N27—C28—H28118.6
C1—C6—C5122.2 (3)C3i—C28—H28118.6
C1—C6—H6118.9O11—S1—C31107.4 (3)
C5—C6—H6118.9O11—S1—C32106.7 (3)
C16—C11—C12117.8 (3)C31—S1—C3297.9 (2)
C16—C11—C1121.1 (3)O21—S2—C42107.22 (14)
C12—C11—C1121.1 (3)O21—S2—C41106.48 (16)
O12—C12—C13121.0 (2)C42—S2—C4198.27 (16)
O12—C12—C11118.3 (3)S2—C41—H41A109.5
C13—C12—C11120.7 (3)S2—C41—H41B109.5
C12—O12—N1886.96 (16)H41A—C41—H41B109.5
C12—O12—H12108 (2)S2—C41—H41C109.5
C14—C13—C12118.9 (3)H41A—C41—H41C109.5
C14—C13—C17119.1 (3)H41B—C41—H41C109.5
C12—C13—C17121.6 (3)S2—C42—H42A109.5
C15—C14—C13120.9 (3)S2—C42—H42B109.5
C15—C14—H14119.6H42A—C42—H42B109.5
C13—C14—H14119.5S2—C42—H42C109.5
C14—C15—C16119.1 (3)H42A—C42—H42C109.5
C14—C15—H15120.4H42B—C42—H42C109.5
C16—C15—H15120.4O11B—S1B—C32B105 (2)
C11—C16—C15122.5 (3)O11B—S1B—C31B105 (2)
C11—C16—H16118.8C32B—S1B—C31B98.0 (19)
C15—C16—H16118.8S1B—C31B—H31D109.5
N18—C17—C13122.2 (3)S1B—C31B—H31E109.5
N18—C17—H17118.9H31D—C31B—H31E109.5
C13—C17—H17118.9S1B—C31B—H31F109.5
C17—N18—C21118.7 (2)H31D—C31B—H31F109.5
C17—N18—H1298.7 (12)H31E—C31B—H31F109.5
C21—N18—H12139.8 (11)S1B—C32B—H32D109.5
C17—N18—O1288.05 (17)S1B—C32B—H32E109.5
C21—N18—O12150.31 (19)H32D—C32B—H32E109.5
C22—C21—C26119.6 (3)S1B—C32B—H32F109.5
C22—C21—N18121.1 (3)H32D—C32B—H32F109.5
C26—C21—N18119.3 (2)H32E—C32B—H32F109.5
C23—C22—C21120.6 (3)
C6—C1—C2—O2178.6 (2)C12—C11—C16—C152.0 (4)
C11—C1—C2—O23.9 (4)C1—C11—C16—C15179.5 (3)
C6—C1—C2—C32.5 (4)C14—C15—C16—C111.5 (5)
C11—C1—C2—C3175.0 (2)C14—C13—C17—N18179.0 (3)
C1—C2—O2—N27i178.3 (2)C12—C13—C17—N186.5 (4)
C3—C2—O2—N27i0.6 (2)C13—C17—N18—C21169.6 (2)
O2—C2—C3—C4178.3 (2)C13—C17—N18—H125.1 (12)
C1—C2—C3—C42.8 (4)C13—C17—N18—O123.2 (3)
O2—C2—C3—C28i3.8 (4)C12—O12—N18—C170.1 (2)
C1—C2—C3—C28i175.1 (2)C12—O12—N18—C21155.6 (4)
C2—C3—C4—C50.7 (4)C12—O12—N18—H12170 (6)
C28i—C3—C4—C5177.3 (3)C17—N18—C21—C2248.8 (4)
C3—C4—C5—C61.6 (4)H12—N18—C21—C22107.0 (18)
C2—C1—C6—C50.2 (4)O12—N18—C21—C22103.0 (4)
C11—C1—C6—C5177.4 (3)C17—N18—C21—C26134.1 (3)
C4—C5—C6—C11.9 (4)H12—N18—C21—C2670.1 (18)
C6—C1—C11—C1673.5 (4)O12—N18—C21—C2674.2 (5)
C2—C1—C11—C16104.0 (3)C26—C21—C22—C231.2 (4)
C6—C1—C11—C12104.0 (3)N18—C21—C22—C23176.0 (3)
C2—C1—C11—C1278.5 (3)C21—C22—C23—C240.8 (4)
C16—C11—C12—O12177.4 (2)C22—C23—C24—C250.3 (4)
C1—C11—C12—O120.1 (4)C23—C24—C25—C261.1 (5)
C16—C11—C12—C131.0 (4)C24—C25—C26—C210.7 (4)
C1—C11—C12—C13178.6 (3)C24—C25—C26—N27177.1 (3)
C13—C12—O12—N183.0 (3)C22—C21—C26—C250.4 (4)
C11—C12—O12—N18175.4 (2)N18—C21—C26—C25176.8 (3)
O12—C12—C13—C14178.8 (2)C22—C21—C26—N27178.3 (2)
C11—C12—C13—C140.4 (4)N18—C21—C26—N271.1 (4)
O12—C12—C13—C176.2 (4)C25—C26—N27—C2855.7 (4)
C11—C12—C13—C17172.2 (2)C21—C26—N27—C28126.5 (3)
C12—C13—C14—C150.9 (4)C26—N27—C28—C3i175.5 (2)
C17—C13—C14—C15171.8 (3)C2—C3—C28i—N27i6.8 (4)
C13—C14—C15—C160.0 (4)
Symmetry code: (i) x+2, y+1, z+2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H2···N27i0.96 (3)1.75 (4)2.626 (3)150 (2)
O12—H12···N180.90 (4)1.80 (4)2.603 (3)147 (2)
Symmetry code: (i) x+2, y+1, z+2.

Experimental details

Crystal data
Chemical formulaC40H28N4O4·4C2H6OS
Mr941.18
Crystal system, space groupTriclinic, P1
Temperature (K)200
a, b, c (Å)10.4876 (6), 11.2572 (7), 12.4998 (8)
α, β, γ (°)99.603 (1), 110.874 (2), 112.700 (2)
V3)1190.15 (13)
Z1
Radiation typeMo Kα
µ (mm1)0.26
Crystal size (mm)0.12 × 0.10 × 0.08
Data collection
DiffractometerBruker SMART CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 1997)
Tmin, Tmax0.886, 0.980
No. of measured, independent and
observed [I > 2σ(I)] reflections
10638, 4343, 2489
Rint0.064
(sin θ/λ)max1)0.602
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.049, 0.112, 0.99
No. of reflections4343
No. of parameters315
No. of restraints36
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.19, 0.29

Computer programs: SMART (Bruker, 2001), SMART, SHELXTL (Bruker, 2001), SHELXTL.

Selected geometric parameters (Å, º) top
C2—O21.362 (3)C26—N271.422 (3)
C2—C31.412 (4)N27—C281.286 (3)
C3—C28i1.458 (4)
O2—C2—C3120.6 (3)C21—C26—N27118.7 (2)
C2—O2—H2107 (2)C28—N27—C26118.4 (2)
C2—C3—C28i121.5 (3)N27—C28—C3i122.9 (3)
O2—C2—C3—C28i3.8 (4)C25—C26—N27—C2855.7 (4)
C2—C1—C11—C1278.5 (3)C21—C26—N27—C28126.5 (3)
O12—C12—C13—C176.2 (4)C26—N27—C28—C3i175.5 (2)
C12—C13—C17—N186.5 (4)C2—C3—C28i—N27i6.8 (4)
Symmetry code: (i) x+2, y+1, z+2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H2···N27i0.96 (3)1.75 (4)2.626 (3)150 (2)
O12—H12···N180.90 (4)1.80 (4)2.603 (3)147 (2)
Symmetry code: (i) x+2, y+1, z+2.
 

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