Abstract
In the title compound, C20H14N4, the dihedral angles between the central benzene ring and the pendant benzimidazole ring systems are 46.60 (15) and 47.89 (16)°. The dihedral angle between the benzimidazole ring systems is 85.62 (12)° and the N atoms lie to the same side of the molecule. In the crystal, molecules are linked by C—H⋯N interactions and weak aromatic π–π stacking [shortest centroid–centroid separation = 3.770 (2) Å] is observed.
Related literature
For background to benzimidazole derivatives as ligands in crystal engineering, see: Li et al. (2009 ▶); Vijayan et al. (2006 ▶).
Experimental
Crystal data
C20H14N4
M r = 310.35
Orthorhombic,
a = 9.5458 (19) Å
b = 20.499 (4) Å
c = 7.9283 (16) Å
V = 1551.4 (5) Å3
Z = 4
Mo Kα radiation
μ = 0.08 mm−1
T = 293 K
0.25 × 0.22 × 0.18 mm
Data collection
Rigaku Mercury CCD diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005 ▶) T min = 0.980, T max = 0.985
12744 measured reflections
1479 independent reflections
1298 reflections with I > 2σ(I)
R int = 0.075
Refinement
R[F 2 > 2σ(F 2)] = 0.051
wR(F 2) = 0.104
S = 1.17
1479 reflections
231 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.14 e Å−3
Δρmin = −0.16 e Å−3
Data collection: CrystalClear (Rigaku/MSC, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811031278/hb6340sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811031278/hb6340Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811031278/hb6340Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C1—H1⋯N4i | 0.93 | 2.50 | 3.359 (5) | 153 |
| C6—H6⋯N4ii | 0.93 | 2.56 | 3.447 (5) | 159 |
Symmetry codes: (i)
; (ii)
.
supplementary crystallographic information
Comment
In recent years, benzimidazole has been well used in crystal engineering, because they exhibit a strong networking ability (Vijayan et al., 2006). To our knowledge, the research on benzimidazole ligands bearing rigid spacers is still less developed (Li et al., 2009), and the title compound was well designed for building polymer architecture. We report here the structure and conformation of a rigid benzimidazole derivative, and further explore the ligand coordination. As shown in Fig. 1, the title compound is trans-conformation and tends to trans-coordination. The molecule has no inversion centre because two benzimidazole rings are not coplanar.
Experimental
The ligand 1,4-di(1H-benzimidazol-1-yl)benzene was prepared by a modified method (Li et al., 2009). A mixture of 1,4-dibromophenyl (3.72 g, 12.0 mmol), benzimidazole (4.25 g, 36.0 mmol), CuI (0.38 g, 2.0 mmol), 1,10-phenanthroline (0.72 g, 4.0 mmol), and Cs2CO3 (2.48 g, 18.0 mmol) was suspended in DMF (50 ml) and refluxed for 48 h to afford (I) as off-white powder, yield: 25% (based on 1,4-dibromophenyl), Mp: 291°C. Colourless blocks of (I) were obtained by recrystallizing from a mixed solvent of methanol and water (1:1).
Refinement
C-bound H atoms were positioned geometrically and refined in the riding-model approximation, with C—H = 0.93Å and Uiso(H) = 1.2Ueq. Anomalous dispersion was negligible and Friedel pairs were merged before refinement.
Figures
Fig. 1.
The molecular structure of (I). Displacement ellipsoids are drawn at the 30% probability level and H atoms are shown as small spheres of arbitrary radius.
Fig. 2.
The crystal packing for (I).
Crystal data
| C20H14N4 | Dx = 1.329 Mg m−3 |
| Mr = 310.35 | Melting point: 564 K |
| Orthorhombic, Pna21 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2c -2n | Cell parameters from 13068 reflections |
| a = 9.5458 (19) Å | θ = 3.3–27.6° |
| b = 20.499 (4) Å | µ = 0.08 mm−1 |
| c = 7.9283 (16) Å | T = 293 K |
| V = 1551.4 (5) Å3 | Block, colorless |
| Z = 4 | 0.25 × 0.22 × 0.18 mm |
| F(000) = 648 |
Data collection
| Rigaku Mercury CCD diffractometer | 1479 independent reflections |
| Radiation source: fine-focus sealed tube | 1298 reflections with I > 2σ(I) |
| graphite | Rint = 0.075 |
| Detector resolution: 9 pixels mm-1 | θmax = 25.0°, θmin = 3.5° |
| ω scans | h = −11→11 |
| Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005) | k = −24→24 |
| Tmin = 0.980, Tmax = 0.985 | l = −9→9 |
| 12744 measured reflections |
Refinement
| 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) = 0.104 | H-atom parameters constrained |
| S = 1.17 | w = 1/[σ2(Fo2) + (0.0488P)2 + 0.1271P] where P = (Fo2 + 2Fc2)/3 |
| 1479 reflections | (Δ/σ)max < 0.001 |
| 231 parameters | Δρmax = 0.14 e Å−3 |
| 1 restraint | Δρmin = −0.16 e Å−3 |
| 0 constraints |
Special details
| 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)
| x | y | z | Uiso*/Ueq | ||
| N1 | 0.2140 (3) | 0.55131 (15) | 0.6320 (4) | 0.0462 (8) | |
| N2 | 0.4461 (3) | 0.53457 (14) | 0.6010 (4) | 0.0411 (8) | |
| N3 | 0.9643 (3) | 0.40659 (14) | 0.6681 (4) | 0.0383 (7) | |
| N4 | 1.1632 (3) | 0.37523 (15) | 0.7980 (4) | 0.0479 (9) | |
| C1 | 0.3178 (4) | 0.51125 (18) | 0.6527 (5) | 0.0452 (9) | |
| H1 | 0.3065 | 0.4699 | 0.6993 | 0.043 (10)* | |
| C2 | 0.2750 (3) | 0.60700 (16) | 0.5602 (4) | 0.0361 (8) | |
| C3 | 0.2141 (4) | 0.66544 (17) | 0.5108 (5) | 0.0427 (9) | |
| H3 | 0.1189 | 0.6729 | 0.5263 | 0.036 (9)* | |
| C4 | 0.2986 (4) | 0.71179 (17) | 0.4385 (5) | 0.0421 (9) | |
| H4 | 0.2598 | 0.7513 | 0.4047 | 0.063 (13)* | |
| C5 | 0.4412 (4) | 0.70086 (17) | 0.4146 (5) | 0.0442 (10) | |
| H5 | 0.4948 | 0.7331 | 0.3629 | 0.046 (11)* | |
| C6 | 0.5059 (4) | 0.64388 (17) | 0.4649 (5) | 0.0431 (9) | |
| H6 | 0.6014 | 0.6371 | 0.4499 | 0.045 (10)* | |
| C7 | 0.4197 (3) | 0.59693 (16) | 0.5399 (5) | 0.0364 (8) | |
| C8 | 0.5788 (3) | 0.50222 (17) | 0.6151 (4) | 0.0379 (9) | |
| C9 | 0.5905 (4) | 0.43768 (17) | 0.5667 (5) | 0.0419 (9) | |
| H9 | 0.5134 | 0.4158 | 0.5226 | 0.058 (12)* | |
| C10 | 0.7177 (3) | 0.40549 (17) | 0.5842 (5) | 0.0408 (9) | |
| H10 | 0.7256 | 0.3618 | 0.5539 | 0.037 (9)* | |
| C11 | 0.8327 (3) | 0.43899 (17) | 0.6469 (5) | 0.0366 (8) | |
| C12 | 0.8204 (4) | 0.50358 (17) | 0.6927 (5) | 0.0421 (9) | |
| H12 | 0.8982 | 0.5260 | 0.7330 | 0.047 (11)* | |
| C13 | 0.6930 (4) | 0.53532 (18) | 0.6794 (5) | 0.0455 (10) | |
| H13 | 0.6843 | 0.5786 | 0.7130 | 0.037 (10)* | |
| C14 | 1.0470 (4) | 0.40901 (19) | 0.8087 (5) | 0.0443 (9) | |
| H14 | 1.0229 | 0.4329 | 0.9042 | 0.046 (11)* | |
| C15 | 1.0353 (3) | 0.36720 (16) | 0.5527 (5) | 0.0391 (9) | |
| C16 | 1.0063 (4) | 0.3484 (2) | 0.3891 (6) | 0.0523 (11) | |
| H16 | 0.9241 | 0.3610 | 0.3355 | 0.064 (13)* | |
| C17 | 1.1043 (4) | 0.3103 (2) | 0.3088 (6) | 0.0662 (12) | |
| H17 | 1.0880 | 0.2971 | 0.1983 | 0.086 (16)* | |
| C18 | 1.2279 (5) | 0.2907 (2) | 0.3899 (6) | 0.0650 (13) | |
| H18 | 1.2914 | 0.2644 | 0.3325 | 0.055 (12)* | |
| C19 | 1.2571 (4) | 0.30983 (19) | 0.5533 (6) | 0.0525 (10) | |
| H19 | 1.3397 | 0.2973 | 0.6065 | 0.065 (13)* | |
| C20 | 1.1584 (4) | 0.34847 (17) | 0.6357 (5) | 0.0423 (9) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| N1 | 0.0327 (17) | 0.0505 (18) | 0.056 (2) | 0.0003 (15) | 0.0048 (16) | 0.0058 (17) |
| N2 | 0.0318 (16) | 0.0426 (18) | 0.049 (2) | 0.0027 (13) | 0.0035 (15) | 0.0057 (15) |
| N3 | 0.0292 (15) | 0.0410 (16) | 0.0448 (18) | 0.0019 (13) | −0.0052 (14) | 0.0046 (16) |
| N4 | 0.040 (2) | 0.058 (2) | 0.046 (2) | 0.0025 (16) | −0.0089 (16) | 0.0052 (18) |
| C1 | 0.041 (2) | 0.038 (2) | 0.057 (2) | −0.0039 (17) | 0.010 (2) | 0.009 (2) |
| C2 | 0.0285 (17) | 0.0417 (19) | 0.038 (2) | −0.0029 (16) | 0.0033 (17) | −0.0012 (17) |
| C3 | 0.034 (2) | 0.047 (2) | 0.047 (2) | 0.0072 (17) | 0.0010 (17) | −0.0050 (19) |
| C4 | 0.039 (2) | 0.0353 (18) | 0.052 (2) | 0.0059 (17) | 0.0013 (19) | 0.0000 (19) |
| C5 | 0.044 (2) | 0.038 (2) | 0.051 (2) | −0.0019 (18) | 0.0041 (19) | 0.003 (2) |
| C6 | 0.031 (2) | 0.047 (2) | 0.052 (2) | −0.0003 (17) | 0.0011 (19) | −0.0041 (19) |
| C7 | 0.0305 (18) | 0.0354 (19) | 0.043 (2) | 0.0001 (15) | 0.0014 (17) | −0.0035 (19) |
| C8 | 0.0363 (19) | 0.041 (2) | 0.036 (2) | 0.0057 (15) | 0.0021 (16) | 0.0033 (17) |
| C9 | 0.0316 (19) | 0.042 (2) | 0.052 (2) | −0.0021 (16) | −0.0049 (18) | 0.0017 (19) |
| C10 | 0.039 (2) | 0.038 (2) | 0.046 (2) | 0.0017 (17) | −0.0042 (17) | −0.0015 (18) |
| C11 | 0.0318 (19) | 0.044 (2) | 0.0339 (19) | 0.0024 (15) | −0.0022 (17) | 0.0042 (18) |
| C12 | 0.034 (2) | 0.043 (2) | 0.049 (2) | −0.0014 (17) | −0.0066 (17) | −0.0030 (19) |
| C13 | 0.044 (2) | 0.039 (2) | 0.054 (3) | 0.0039 (17) | −0.0021 (19) | −0.0105 (19) |
| C14 | 0.039 (2) | 0.053 (2) | 0.041 (2) | −0.0013 (19) | −0.0063 (19) | 0.001 (2) |
| C15 | 0.0338 (19) | 0.0346 (18) | 0.049 (2) | 0.0030 (15) | −0.0013 (18) | 0.0040 (18) |
| C16 | 0.048 (2) | 0.061 (3) | 0.048 (2) | 0.013 (2) | −0.013 (2) | −0.007 (2) |
| C17 | 0.064 (3) | 0.079 (3) | 0.056 (3) | 0.024 (2) | −0.004 (2) | −0.015 (3) |
| C18 | 0.057 (3) | 0.068 (3) | 0.070 (3) | 0.024 (2) | 0.003 (2) | −0.010 (3) |
| C19 | 0.042 (2) | 0.056 (2) | 0.060 (3) | 0.011 (2) | −0.005 (2) | 0.006 (2) |
| C20 | 0.037 (2) | 0.041 (2) | 0.049 (2) | 0.0012 (16) | −0.0034 (19) | 0.005 (2) |
Geometric parameters (Å, °)
| N1—C1 | 1.298 (5) | C8—C13 | 1.381 (5) |
| N1—C2 | 1.402 (4) | C8—C9 | 1.382 (5) |
| N2—C1 | 1.377 (4) | C9—C10 | 1.389 (5) |
| N2—C7 | 1.390 (4) | C9—H9 | 0.9300 |
| N2—C8 | 1.434 (4) | C10—C11 | 1.387 (5) |
| N3—C14 | 1.367 (4) | C10—H10 | 0.9301 |
| N3—C15 | 1.396 (5) | C11—C12 | 1.378 (5) |
| N3—C11 | 1.431 (4) | C12—C13 | 1.384 (5) |
| N4—C14 | 1.310 (4) | C12—H12 | 0.9299 |
| N4—C20 | 1.400 (5) | C13—H13 | 0.9301 |
| C1—H1 | 0.9301 | C14—H14 | 0.9299 |
| C2—C3 | 1.388 (5) | C15—C16 | 1.381 (6) |
| C2—C7 | 1.406 (4) | C15—C20 | 1.400 (5) |
| C3—C4 | 1.372 (5) | C16—C17 | 1.374 (6) |
| C3—H3 | 0.9300 | C16—H16 | 0.9299 |
| C4—C5 | 1.393 (5) | C17—C18 | 1.402 (6) |
| C4—H4 | 0.9299 | C17—H17 | 0.9300 |
| C5—C6 | 1.380 (5) | C18—C19 | 1.382 (6) |
| C5—H5 | 0.9301 | C18—H18 | 0.9300 |
| C6—C7 | 1.399 (5) | C19—C20 | 1.394 (5) |
| C6—H6 | 0.9300 | C19—H19 | 0.9301 |
| C1—N1—C2 | 104.4 (3) | C10—C9—H9 | 120.0 |
| C1—N2—C7 | 105.2 (3) | C11—C10—C9 | 119.5 (3) |
| C1—N2—C8 | 127.0 (3) | C11—C10—H10 | 120.3 |
| C7—N2—C8 | 127.8 (3) | C9—C10—H10 | 120.2 |
| C14—N3—C15 | 106.0 (3) | C12—C11—C10 | 120.2 (3) |
| C14—N3—C11 | 125.8 (3) | C12—C11—N3 | 119.3 (3) |
| C15—N3—C11 | 128.2 (3) | C10—C11—N3 | 120.5 (3) |
| C14—N4—C20 | 103.8 (3) | C11—C12—C13 | 120.4 (3) |
| N1—C1—N2 | 115.0 (3) | C11—C12—H12 | 119.8 |
| N1—C1—H1 | 122.5 | C13—C12—H12 | 119.8 |
| N2—C1—H1 | 122.5 | C8—C13—C12 | 119.4 (3) |
| C3—C2—N1 | 130.0 (3) | C8—C13—H13 | 120.3 |
| C3—C2—C7 | 120.4 (3) | C12—C13—H13 | 120.3 |
| N1—C2—C7 | 109.6 (3) | N4—C14—N3 | 114.6 (4) |
| C4—C3—C2 | 118.0 (3) | N4—C14—H14 | 122.7 |
| C4—C3—H3 | 121.0 | N3—C14—H14 | 122.7 |
| C2—C3—H3 | 120.9 | C16—C15—N3 | 132.8 (3) |
| C3—C4—C5 | 121.3 (3) | C16—C15—C20 | 122.2 (4) |
| C3—C4—H4 | 119.3 | N3—C15—C20 | 104.9 (3) |
| C5—C4—H4 | 119.4 | C17—C16—C15 | 117.2 (4) |
| C6—C5—C4 | 122.3 (4) | C17—C16—H16 | 121.4 |
| C6—C5—H5 | 118.9 | C15—C16—H16 | 121.4 |
| C4—C5—H5 | 118.9 | C16—C17—C18 | 121.5 (5) |
| C5—C6—C7 | 116.2 (3) | C16—C17—H17 | 119.2 |
| C5—C6—H6 | 121.9 | C18—C17—H17 | 119.3 |
| C7—C6—H6 | 121.9 | C19—C18—C17 | 121.2 (4) |
| N2—C7—C6 | 132.4 (3) | C19—C18—H18 | 119.4 |
| N2—C7—C2 | 105.9 (3) | C17—C18—H18 | 119.4 |
| C6—C7—C2 | 121.7 (3) | C18—C19—C20 | 117.7 (4) |
| C13—C8—C9 | 120.6 (3) | C18—C19—H19 | 121.2 |
| C13—C8—N2 | 119.9 (3) | C20—C19—H19 | 121.1 |
| C9—C8—N2 | 119.5 (3) | C19—C20—N4 | 129.2 (3) |
| C8—C9—C10 | 119.8 (3) | C19—C20—C15 | 120.2 (4) |
| C8—C9—H9 | 120.1 | N4—C20—C15 | 110.6 (3) |
| C2—N1—C1—N2 | −0.1 (4) | C14—N3—C11—C12 | 46.4 (5) |
| C7—N2—C1—N1 | −0.1 (5) | C15—N3—C11—C12 | −133.0 (4) |
| C8—N2—C1—N1 | 177.2 (4) | C14—N3—C11—C10 | −132.3 (4) |
| C1—N1—C2—C3 | 179.9 (4) | C15—N3—C11—C10 | 48.3 (5) |
| C1—N1—C2—C7 | 0.2 (4) | C10—C11—C12—C13 | 1.1 (6) |
| N1—C2—C3—C4 | −178.1 (4) | N3—C11—C12—C13 | −177.6 (4) |
| C7—C2—C3—C4 | 1.5 (5) | C9—C8—C13—C12 | 0.9 (6) |
| C2—C3—C4—C5 | 0.2 (6) | N2—C8—C13—C12 | 179.9 (3) |
| C3—C4—C5—C6 | −1.4 (6) | C11—C12—C13—C8 | −1.8 (6) |
| C4—C5—C6—C7 | 0.8 (6) | C20—N4—C14—N3 | 0.6 (4) |
| C1—N2—C7—C6 | −177.3 (4) | C15—N3—C14—N4 | −0.5 (4) |
| C8—N2—C7—C6 | 5.4 (7) | C11—N3—C14—N4 | −179.9 (3) |
| C1—N2—C7—C2 | 0.2 (4) | C14—N3—C15—C16 | −178.0 (4) |
| C8—N2—C7—C2 | −177.1 (3) | C11—N3—C15—C16 | 1.4 (6) |
| C5—C6—C7—N2 | 178.1 (4) | C14—N3—C15—C20 | 0.1 (4) |
| C5—C6—C7—C2 | 1.0 (6) | C11—N3—C15—C20 | 179.6 (3) |
| C3—C2—C7—N2 | 180.0 (3) | N3—C15—C16—C17 | 177.6 (4) |
| N1—C2—C7—N2 | −0.3 (4) | C20—C15—C16—C17 | −0.3 (6) |
| C3—C2—C7—C6 | −2.2 (6) | C15—C16—C17—C18 | 0.6 (7) |
| N1—C2—C7—C6 | 177.6 (4) | C16—C17—C18—C19 | −1.0 (7) |
| C1—N2—C8—C13 | −131.9 (4) | C17—C18—C19—C20 | 1.0 (6) |
| C7—N2—C8—C13 | 44.8 (5) | C18—C19—C20—N4 | −178.6 (4) |
| C1—N2—C8—C9 | 47.1 (5) | C18—C19—C20—C15 | −0.6 (5) |
| C7—N2—C8—C9 | −136.2 (4) | C14—N4—C20—C19 | 177.6 (4) |
| C13—C8—C9—C10 | 0.7 (6) | C14—N4—C20—C15 | −0.5 (4) |
| N2—C8—C9—C10 | −178.3 (3) | C16—C15—C20—C19 | 0.3 (5) |
| C8—C9—C10—C11 | −1.4 (6) | N3—C15—C20—C19 | −178.1 (3) |
| C9—C10—C11—C12 | 0.5 (5) | C16—C15—C20—N4 | 178.6 (4) |
| C9—C10—C11—N3 | 179.2 (3) | N3—C15—C20—N4 | 0.3 (4) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C1—H1···N4i | 0.93 | 2.50 | 3.359 (5) | 153 |
| C6—H6···N4ii | 0.93 | 2.56 | 3.447 (5) | 159 |
Symmetry codes: (i) x−1, y, z; (ii) −x+2, −y+1, z−1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB6340).
References
- Li, Z. X., Xu, Y., Zuo, Y., Li, L., Pan, Q., Hu, T. L. & Bu, X. H. (2009). Cryst. Growth Des. 9, 3904–3909.
- Rigaku/MSC (2005). CrystalClear Rigaku/MSC Inc., The Woodlands, Texas, USA.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Vijayan, N., Bhagavannarayana, G., Balamurugan, N., Babu, R. R., Maurya, K. K., Gopalakrishnan, R. & Ramasamy, P. (2006). J. Cryst. Growth, 293, 318–323.
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811031278/hb6340sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811031278/hb6340Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811031278/hb6340Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


