supplementary materials
4,4'-Bipyridine-2,3,4,5,6-pentafluorobenzoic acid (1/2)
A solution of 4,4'-bipyridine (2 mmol) in ethanol (5 ml) was added into
2,3,4,5,6-pentafluorobenzoic acid (4 mmol) in ethanol(20 ml). The mixture was
refluxed with stirring for 10 min. The resultant solution was filtered.
Colourless blocks of (I) were formed after a few days of
slow evaporation of the solvent at room temperature.
All H atoms were placed in calculated positions and included in a riding-model
approximation, with C—H = 0.93 Å, O—H = 0.82Å and Uiso(H)=
1.2Ueq(C) or 1.5Ueq(O).
Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SAINT (Bruker, 2001); 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: SHELXL97 (Sheldrick, 2008).
4,4'-Bipyridine–2,3,4,5,6-pentafluorobenzoic acid (1/2)
top
Crystal data top
| C10H8N2·2C7HF5O2 | F(000) = 1160 |
| Mr = 580.34 | Dx = 1.714 Mg m−3 |
| Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -C 2yc | Cell parameters from 187 reflections |
| a = 17.910 (3) Å | θ = 2.2–22.0° |
| b = 10.7016 (19) Å | µ = 0.17 mm−1 |
| c = 13.498 (3) Å | T = 296 K |
| β = 119.631 (3)° | BLOCK, colorless |
| V = 2248.8 (7) Å3 | 0.30 × 0.28 × 0.20 mm |
| Z = 4 | |
Data collection top
Bruker SMART CCD diffractometer | 2695 independent reflections |
| Radiation source: fine-focus sealed tube | 2060 reflections with I > 2σ(I) |
| graphite | Rint = 0.022 |
| ω scans | θmax = 28.2°, θmin = 2.3° |
Absorption correction: multi-scan (SADABS; Bruker, 2001) | h = −23→22 |
| Tmin = 0.946, Tmax = 0.974 | k = −14→11 |
| 6884 measured reflections | l = −17→17 |
Refinement top
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.041 | H-atom parameters constrained |
| wR(F2) = 0.120 | w = 1/[σ2(Fo2) + (0.0524P)2 + 1.397P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.05 | (Δ/σ)max < 0.001 |
| 2695 reflections | Δρmax = 0.25 e Å−3 |
| 183 parameters | Δρmin = −0.18 e Å−3 |
| 0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0039 (7) |
Crystal data top
| C10H8N2·2C7HF5O2 | V = 2248.8 (7) Å3 |
| Mr = 580.34 | Z = 4 |
| Monoclinic, C2/c | Mo Kα radiation |
| a = 17.910 (3) Å | µ = 0.17 mm−1 |
| b = 10.7016 (19) Å | T = 296 K |
| c = 13.498 (3) Å | 0.30 × 0.28 × 0.20 mm |
| β = 119.631 (3)° | |
Data collection top
Bruker SMART CCD diffractometer | 2695 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2001) | 2060 reflections with I > 2σ(I) |
| Tmin = 0.946, Tmax = 0.974 | Rint = 0.022 |
| 6884 measured reflections | θmax = 28.2° |
Refinement top
| R[F2 > 2σ(F2)] = 0.041 | H-atom parameters constrained |
| wR(F2) = 0.120 | Δρmax = 0.25 e Å−3 |
| S = 1.05 | Δρmin = −0.18 e Å−3 |
| 2695 reflections | Absolute structure: ? |
| 183 parameters | Flack parameter: ? |
| 0 restraints | Rogers parameter: ? |
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| | x | y | z | Uiso*/Ueq | |
| C10 | 0.49615 (12) | 0.70420 (16) | 0.63825 (14) | 0.0565 (4) | |
| H10 | 0.5208 | 0.6330 | 0.6818 | 0.068* | |
| C12 | 0.44977 (12) | 0.91468 (15) | 0.61897 (14) | 0.0541 (4) | |
| H12 | 0.4429 | 0.9890 | 0.6493 | 0.065* | |
| C13 | 0.42370 (13) | 0.90600 (16) | 0.50439 (14) | 0.0578 (5) | |
| H13 | 0.3984 | 0.9755 | 0.4584 | 0.069* | |
| C9 | 0.46907 (12) | 0.70404 (16) | 0.52338 (15) | 0.0574 (4) | |
| H9 | 0.4762 | 0.6316 | 0.4910 | 0.069* | |
| C11 | 0.48637 (10) | 0.81117 (13) | 0.68843 (12) | 0.0430 (3) | |
| N1 | 0.43312 (9) | 0.80276 (13) | 0.45658 (11) | 0.0516 (4) | |
| F1 | 0.31878 (9) | 0.41200 (10) | 0.13362 (9) | 0.0756 (4) | |
| F5 | 0.38044 (8) | 0.81354 (10) | 0.04501 (10) | 0.0727 (4) | |
| F2 | 0.24519 (9) | 0.35110 (11) | −0.08528 (10) | 0.0807 (4) | |
| O2 | 0.38410 (9) | 0.76706 (11) | 0.24230 (10) | 0.0624 (4) | |
| H2 | 0.4019 | 0.7781 | 0.3105 | 0.094* | |
| F4 | 0.30691 (9) | 0.74859 (12) | −0.17270 (10) | 0.0802 (4) | |
| F3 | 0.23514 (9) | 0.51811 (12) | −0.24105 (8) | 0.0766 (4) | |
| C2 | 0.35217 (10) | 0.61682 (14) | 0.09940 (12) | 0.0442 (3) | |
| C3 | 0.31759 (11) | 0.49867 (15) | 0.06163 (13) | 0.0490 (4) | |
| O1 | 0.42833 (13) | 0.57290 (14) | 0.29718 (11) | 0.0921 (6) | |
| C7 | 0.34739 (11) | 0.69832 (14) | 0.01702 (14) | 0.0475 (4) | |
| C4 | 0.27894 (12) | 0.46524 (15) | −0.05187 (14) | 0.0529 (4) | |
| C5 | 0.27456 (11) | 0.54934 (17) | −0.13111 (13) | 0.0524 (4) | |
| C1 | 0.39257 (11) | 0.65043 (16) | 0.22420 (13) | 0.0512 (4) | |
| C6 | 0.30987 (12) | 0.66596 (16) | −0.09672 (14) | 0.0527 (4) | |
Atomic displacement parameters (Å2) top| | U11 | U22 | U33 | U12 | U13 | U23 |
| C10 | 0.0778 (12) | 0.0382 (8) | 0.0439 (9) | 0.0111 (8) | 0.0227 (8) | 0.0021 (6) |
| C12 | 0.0787 (11) | 0.0355 (8) | 0.0413 (8) | 0.0068 (8) | 0.0244 (8) | −0.0005 (6) |
| C13 | 0.0836 (12) | 0.0384 (8) | 0.0409 (8) | 0.0075 (8) | 0.0229 (8) | 0.0029 (7) |
| C9 | 0.0754 (11) | 0.0435 (9) | 0.0466 (9) | 0.0083 (8) | 0.0250 (8) | −0.0065 (7) |
| C11 | 0.0513 (8) | 0.0341 (7) | 0.0379 (8) | −0.0014 (6) | 0.0177 (6) | −0.0004 (6) |
| N1 | 0.0633 (8) | 0.0464 (8) | 0.0388 (7) | 0.0000 (6) | 0.0205 (6) | −0.0036 (5) |
| F1 | 0.1289 (11) | 0.0458 (6) | 0.0587 (6) | −0.0090 (6) | 0.0515 (7) | 0.0036 (5) |
| F5 | 0.1063 (9) | 0.0427 (6) | 0.0662 (7) | −0.0179 (6) | 0.0403 (7) | −0.0041 (5) |
| F2 | 0.1197 (10) | 0.0498 (6) | 0.0704 (7) | −0.0246 (7) | 0.0454 (7) | −0.0210 (5) |
| O2 | 0.0914 (9) | 0.0431 (6) | 0.0387 (6) | 0.0117 (6) | 0.0214 (6) | −0.0040 (5) |
| F4 | 0.1189 (10) | 0.0679 (8) | 0.0561 (6) | 0.0000 (7) | 0.0450 (7) | 0.0184 (6) |
| F3 | 0.1011 (9) | 0.0798 (8) | 0.0386 (5) | −0.0019 (7) | 0.0268 (6) | −0.0116 (5) |
| C2 | 0.0529 (8) | 0.0380 (7) | 0.0384 (7) | 0.0070 (6) | 0.0200 (7) | −0.0006 (6) |
| C3 | 0.0690 (10) | 0.0380 (8) | 0.0429 (8) | 0.0035 (7) | 0.0298 (8) | 0.0024 (6) |
| O1 | 0.1500 (15) | 0.0554 (8) | 0.0406 (7) | 0.0404 (9) | 0.0239 (8) | 0.0032 (6) |
| C7 | 0.0571 (9) | 0.0352 (7) | 0.0473 (8) | 0.0003 (7) | 0.0236 (7) | −0.0007 (6) |
| C4 | 0.0691 (11) | 0.0394 (8) | 0.0505 (9) | −0.0048 (7) | 0.0298 (8) | −0.0087 (7) |
| C5 | 0.0616 (10) | 0.0552 (10) | 0.0365 (8) | 0.0046 (8) | 0.0213 (7) | −0.0049 (7) |
| C1 | 0.0627 (10) | 0.0439 (9) | 0.0390 (8) | 0.0103 (7) | 0.0190 (7) | −0.0018 (6) |
| C6 | 0.0677 (10) | 0.0478 (9) | 0.0440 (8) | 0.0054 (8) | 0.0287 (8) | 0.0088 (7) |
Geometric parameters (Å, °) top
| C10—C9 | 1.377 (2) | F2—C4 | 1.3383 (19) |
| C10—C11 | 1.385 (2) | O2—C1 | 1.295 (2) |
| C10—H10 | 0.9300 | O2—H2 | 0.8200 |
| C12—C13 | 1.380 (2) | F4—C6 | 1.3352 (19) |
| C12—C11 | 1.389 (2) | F3—C5 | 1.3328 (18) |
| C12—H12 | 0.9300 | C2—C7 | 1.382 (2) |
| C13—N1 | 1.332 (2) | C2—C3 | 1.389 (2) |
| C13—H13 | 0.9300 | C2—C1 | 1.512 (2) |
| C9—N1 | 1.330 (2) | C3—C4 | 1.380 (2) |
| C9—H9 | 0.9300 | O1—C1 | 1.202 (2) |
| C11—C11i | 1.483 (3) | C7—C6 | 1.381 (2) |
| F1—C3 | 1.3358 (18) | C4—C5 | 1.370 (2) |
| F5—C7 | 1.3388 (18) | C5—C6 | 1.372 (3) |
| | | |
| C9—C10—C11 | 119.51 (15) | C3—C2—C1 | 120.42 (14) |
| C9—C10—H10 | 120.2 | F1—C3—C4 | 116.50 (15) |
| C11—C10—H10 | 120.2 | F1—C3—C2 | 121.41 (14) |
| C13—C12—C11 | 119.23 (15) | C4—C3—C2 | 122.08 (15) |
| C13—C12—H12 | 120.4 | F5—C7—C6 | 116.66 (14) |
| C11—C12—H12 | 120.4 | F5—C7—C2 | 120.75 (14) |
| N1—C13—C12 | 123.04 (15) | C6—C7—C2 | 122.59 (15) |
| N1—C13—H13 | 118.5 | F2—C4—C5 | 119.63 (15) |
| C12—C13—H13 | 118.5 | F2—C4—C3 | 120.38 (15) |
| N1—C9—C10 | 123.05 (16) | C5—C4—C3 | 119.99 (16) |
| N1—C9—H9 | 118.5 | F3—C5—C4 | 119.92 (16) |
| C10—C9—H9 | 118.5 | F3—C5—C6 | 120.44 (16) |
| C10—C11—C12 | 117.44 (14) | C4—C5—C6 | 119.63 (15) |
| C10—C11—C11i | 119.81 (10) | O1—C1—O2 | 125.12 (15) |
| C12—C11—C11i | 122.74 (10) | O1—C1—C2 | 121.09 (15) |
| C9—N1—C13 | 117.73 (14) | O2—C1—C2 | 113.78 (14) |
| C1—O2—H2 | 109.5 | F4—C6—C5 | 120.39 (15) |
| C7—C2—C3 | 116.11 (14) | F4—C6—C7 | 120.03 (16) |
| C7—C2—C1 | 123.47 (15) | C5—C6—C7 | 119.57 (15) |
| Symmetry codes: (i) −x+1, y, −z+3/2. |
Hydrogen-bond geometry (Å, °) top
| D—H···A | D—H | H···A | D···A | D—H···A |
| O2—H2···N1 | 0.82 | 1.78 | 2.602 (2) | 176 |
| C9—H9···O1 | 0.93 | 2.40 | 3.102 (2) | 132 |
| C10—H10···O1ii | 0.93 | 2.35 | 3.196 (2) | 152 |
| C12—H12···F5iii | 0.93 | 2.48 | 3.126 (2) | 127 |
| C13—H13···F5iii | 0.93 | 2.63 | 3.214 (2) | 121 |
| Symmetry codes: (ii) −x+1, −y+1, −z+1; (iii) x, −y+2, z+1/2. |
Table 1
Hydrogen-bond geometry (Å, °) top
| D—H···A | D—H | H···A | D···A | D—H···A |
| O2—H2···N1 | 0.82 | 1.78 | 2.602 (2) | 176 |
| C9—H9···O1 | 0.93 | 2.40 | 3.102 (2) | 132 |
| C10—H10···O1i | 0.93 | 2.35 | 3.196 (2) | 152 |
| C12—H12···F5ii | 0.93 | 2.48 | 3.126 (2) | 127 |
| C13—H13···F5ii | 0.93 | 2.63 | 3.214 (2) | 121 |
| Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) x, −y+2, z+1/2. |
This work was supported by the Project of the Provincial Key Laboratory of
Liaoning Province, China (No. 2008S104), the Project for Innovation Teams of
Liaoning Province, China (No. 2007 T052) and the Doctoral Start-up Project of
Liaoning University.
Bruker (2001). SMART, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.
Chopra, D. & Row, T. N. G. (2008). CrystEngComm, 10, 54–67.
Choudhury, A. R. & Row, T. N. G. (2004). Cryst. Growth Des. 4, 47–52 .
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.
Weak interactions involving fluorine is of great interest and importance in producing new suppramolecular assemblies. Fluorine can provide C—H···F, N—H···F hydrogen bonds (e.g. Chopra & Row, 2008) as well as C—F···F and C—F···π interactions (e.g. Choudhury & Row, 2004). in crystal engineering. Fluorine derivatives have generated a wide variety of crystal structures. The title molecular complex is composed of 4,4'-bipyridine and 2,3,4,5,6-pentafluorobenzoic acid with the molar ratio of 1:2 to form a basic unit. The components are linked by O—H···N hdrogen bond (O2···N1 2.602 (2) Å, O2—H2···N1 176 °) (Fig. 1). C9—H9···O1 weak hydrogen bond further strengthen the connection (Table 1). Intermolecular C10—H10···O1(symmery code: -x + 1, -y + 1, -z + 1), C12—H12···F5, C13—H13···F5 (symmery code: x, -y + 2, z + 1/2) hydrogen bonds and F1···F3 [2.859 (2) Å, symmery code: x, -y, -1/2 + z] interaction link these units further.