organic compounds
†
of 2,5-bis(4-methylpyridin-2-yl)pyrazine chloroform disolvateaInstitute of Physics, University of Neuchâtel, rue Emile-Argand 11, CH-2000 Neuchâtel, Switzerland
*Correspondence e-mail: helen.stoeckli-evans@unine.ch
The heterocyclic molecule in the title solvate, C16H14N4·2CHCl3, possesses inversion symmetry, with the inversion centre situated at the centre of the pyrazine ring. The outer pyridine rings are inclined to the central pyrazine ring by 4.89 (9)°. The compound crystallized as a chloroform disolvate with the solvent molecules linked to the title molecule by C—H⋯N hydrogen bonds. In the crystal, molecules are further linked by π–π interactions involving the pyrazine and pyridine rings of neighbouring molecules [inter-centroid distance = 3.5629 (12) Å; symmetry code: x, y + 1, z + 1].
Keywords: crystal structure; pyrazine; pyridine; bis(2-pyridyl)pyrazine; solvate.
CCDC reference: 1004308
1. Related literature
The title compound is the 4-methylpyridine derivative of the ligand 2,5-bis(pyridin-2-yl)pyrazine (bppz), see: Neels & Stoeckli-Evans (1993); Schmitt (2008). For the synthesis of a number of transition-metal complexes of bppz, especially of copper(II), and for their magnetic properties, see for example: Escuer et al. (1993); Neels et al. (1995); Yuste et al. (2009); Bentama et al. (2012).
2. Experimental
2.1. Crystal data
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2.3. Refinement
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Data collection: X-AREA (Stoe & Cie, 2009); cell X-AREA; data reduction: X-RED32 (Stoe & Cie, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2013 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL2013, PLATON (Spek, 2009) and publCIF (Westrip, 2010).
Supporting information
CCDC reference: 1004308
10.1107/S1600536814009544/wm0002sup1.cif
contains datablocks I, New_Global_Publ_Block. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536814009544/wm0002Isup2.hkl
The title compound was prepared in 3 stages:
Stage 1. Synthesis of methyl-2-pyridine-4-methyl-ketoxime (1): Hydroxylamine hydrochloride (566 mg, 8.14 mmol) in pyridine (5ml) was added to a solution of 2-acetyl-4-methylpyrine (1.0 g, 7.40 mmol) in pyridine (22 ml) with vigorous stirring for 3 h at room temperature. The colourless solution was then poured into iced water. The oxime that precipitated was filtered and then dried under vacuum, yielding 1.33 g of compound (1) as a white powder. MS (ESI) calc. for C8H10N2O [M+H]+ : 150.18; found 151.1.
Stage 2. Synthesis of methyl-p-tosyl-2-actelypyridine oxime (2): Tosyl chloride (2.40 g, 7.32 mmol) was added to a solution of (1) [1.0 g, 6.6 mmol] in pyridine (10 ml) with stirring for 20 h. The orange solution obtained was poured into iced water. A white precipitate was obtained which was filtered, washed with cold water and dried, yielding compound (2) as a white powder [Yield 74%; 523 mg]. MS (ESI) calc. for C15H16N2O3S [M+H]+: 304.36; found 305.1.
Stage 3. Synthesis of 2,5-bis(4-methyl-2-yl)-pyrazine: Potassium tert-butoxide (516 mg, 4.60 mmol) was added in small portions to a solution of (2) [1.0 g, 3.286 mmol] in dry ethanol (15 ml). The mixture was stirred at room temperature for 20 h. The precipitate of potassium p-toluenesulfonate that formed was filtered off and washed with ether. The filtrate and the washed fractions were collected. This process was repeated until no further precipitation occurred. An aqueous solution of hydrogen peroxide (30%, 4 ml) was then added to the assembled filtrates and washed fractions. When the
had stopped, the mixture was placed in a refrigerator over night yielding the title compound. It was filtered off and washed with water/methanol (1/1, v/v) and dried (yield 5%, 43 mg). MS (ESI) calc. for C16H14N4 [M+H]+: 262.31, found 263.13. The colourless rod-like crystals used for X-ray were obtained by slow evaporation of a solution in chloroform.Data collection: X-AREA (Stoe & Cie, 2009); cell
X-AREA (Stoe & Cie, 2009); data reduction: X-RED32 (Stoe & Cie, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2013 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL2013 (Sheldrick, 2008), PLATON (Spek, 2009) and publCIF (Westrip, 2010).C16H14N4·2CHCl3 | F(000) = 1016 |
Mr = 501.05 | Dx = 1.546 Mg m−3 |
Monoclinic, I2/a | Mo Kα radiation, λ = 0.71073 Å |
a = 16.4498 (17) Å | Cell parameters from 12496 reflections |
b = 6.0691 (4) Å | θ = 1.5–25.6° |
c = 21.605 (3) Å | µ = 0.81 mm−1 |
β = 93.885 (9)° | T = 173 K |
V = 2152.0 (4) Å3 | Rod, colourless |
Z = 4 | 0.45 × 0.29 × 0.23 mm |
Stoe IPDS 2 diffractometer | 1902 independent reflections |
Radiation source: fine-focus sealed tube | 1676 reflections with I > 2σ(I) |
Plane graphite monochromator | Rint = 0.066 |
ϕ + ω scans | θmax = 25.2°, θmin = 1.9° |
Absorption correction: multi-scan (MULscanABS in PLATON; Spek, 2009) | h = −19→19 |
Tmin = 0.567, Tmax = 1.000 | k = −7→7 |
9566 measured reflections | l = −25→25 |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-atom parameters constrained |
R[F2 > 2σ(F2)] = 0.040 | w = 1/[σ2(Fo2) + (0.0725P)2 + 0.8241P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.112 | (Δ/σ)max = 0.002 |
S = 1.06 | Δρmax = 0.31 e Å−3 |
1902 reflections | Δρmin = −0.30 e Å−3 |
129 parameters | Extinction correction: SHELXL2013 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.0064 (11) |
C16H14N4·2CHCl3 | V = 2152.0 (4) Å3 |
Mr = 501.05 | Z = 4 |
Monoclinic, I2/a | Mo Kα radiation |
a = 16.4498 (17) Å | µ = 0.81 mm−1 |
b = 6.0691 (4) Å | T = 173 K |
c = 21.605 (3) Å | 0.45 × 0.29 × 0.23 mm |
β = 93.885 (9)° |
Stoe IPDS 2 diffractometer | 1902 independent reflections |
Absorption correction: multi-scan (MULscanABS in PLATON; Spek, 2009) | 1676 reflections with I > 2σ(I) |
Tmin = 0.567, Tmax = 1.000 | Rint = 0.066 |
9566 measured reflections |
R[F2 > 2σ(F2)] = 0.040 | 0 restraints |
wR(F2) = 0.112 | H-atom parameters constrained |
S = 1.06 | Δρmax = 0.31 e Å−3 |
1902 reflections | Δρmin = −0.30 e Å−3 |
129 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
N1 | 0.72397 (10) | 0.6344 (3) | 0.19653 (8) | 0.0368 (4) | |
N2 | 0.89303 (10) | 0.2947 (3) | 0.25318 (8) | 0.0394 (4) | |
C1 | 0.68638 (12) | 0.8157 (3) | 0.21400 (9) | 0.0374 (4) | |
H1 | 0.6406 | 0.8677 | 0.1890 | 0.045* | |
C2 | 0.78878 (11) | 0.5676 (3) | 0.23260 (8) | 0.0328 (4) | |
C3 | 0.83238 (11) | 0.3674 (3) | 0.21341 (9) | 0.0328 (4) | |
C4 | 0.93307 (13) | 0.1154 (3) | 0.23585 (10) | 0.0418 (5) | |
H4 | 0.9771 | 0.0635 | 0.2627 | 0.050* | |
C5 | 0.91455 (13) | 0.0006 (3) | 0.18141 (10) | 0.0401 (5) | |
H5 | 0.9446 | −0.1274 | 0.1720 | 0.048* | |
C6 | 0.85181 (12) | 0.0739 (3) | 0.14075 (9) | 0.0376 (5) | |
C7 | 0.81112 (11) | 0.2637 (3) | 0.15755 (9) | 0.0378 (5) | |
H7 | 0.7685 | 0.3224 | 0.1305 | 0.045* | |
C8 | 0.82828 (15) | −0.0466 (4) | 0.08138 (11) | 0.0510 (6) | |
H8A | 0.7910 | −0.1672 | 0.0898 | 0.077* | |
H8B | 0.8772 | −0.1066 | 0.0642 | 0.077* | |
H8C | 0.8012 | 0.0556 | 0.0515 | 0.077* | |
Cl1 | 0.50499 (4) | 0.55130 (10) | 0.09961 (3) | 0.0569 (2) | |
Cl2 | 0.65296 (4) | 0.52518 (12) | 0.03495 (3) | 0.0617 (3) | |
Cl3 | 0.57200 (4) | 0.12697 (10) | 0.06982 (3) | 0.0582 (2) | |
C10 | 0.59461 (13) | 0.4006 (3) | 0.09061 (10) | 0.0416 (5) | |
H10 | 0.6275 | 0.3999 | 0.1312 | 0.050* |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1 | 0.0398 (9) | 0.0332 (9) | 0.0377 (9) | −0.0008 (7) | 0.0045 (7) | −0.0041 (7) |
N2 | 0.0429 (9) | 0.0351 (9) | 0.0405 (9) | 0.0005 (7) | 0.0053 (7) | −0.0032 (7) |
C1 | 0.0404 (10) | 0.0333 (10) | 0.0385 (10) | −0.0002 (8) | 0.0035 (8) | −0.0027 (8) |
C2 | 0.0356 (10) | 0.0294 (10) | 0.0340 (10) | −0.0039 (8) | 0.0075 (7) | 0.0008 (8) |
C3 | 0.0343 (9) | 0.0290 (9) | 0.0358 (10) | −0.0042 (7) | 0.0090 (7) | −0.0001 (7) |
C4 | 0.0467 (11) | 0.0374 (11) | 0.0417 (11) | 0.0052 (9) | 0.0054 (8) | −0.0004 (8) |
C5 | 0.0460 (11) | 0.0326 (10) | 0.0433 (11) | 0.0022 (8) | 0.0140 (9) | −0.0003 (8) |
C6 | 0.0424 (10) | 0.0343 (10) | 0.0377 (10) | −0.0038 (8) | 0.0136 (8) | −0.0047 (8) |
C7 | 0.0388 (10) | 0.0381 (11) | 0.0372 (10) | −0.0011 (8) | 0.0077 (8) | −0.0025 (8) |
C8 | 0.0578 (13) | 0.0499 (13) | 0.0460 (12) | 0.0046 (10) | 0.0076 (10) | −0.0152 (10) |
Cl1 | 0.0557 (4) | 0.0538 (4) | 0.0613 (4) | 0.0130 (3) | 0.0040 (3) | −0.0024 (3) |
Cl2 | 0.0589 (4) | 0.0759 (5) | 0.0507 (4) | −0.0204 (3) | 0.0069 (3) | 0.0140 (3) |
Cl3 | 0.0758 (5) | 0.0417 (4) | 0.0594 (4) | −0.0037 (3) | 0.0207 (3) | −0.0062 (2) |
C10 | 0.0449 (11) | 0.0426 (11) | 0.0376 (11) | −0.0012 (9) | 0.0041 (8) | 0.0024 (9) |
N1—C1 | 1.329 (3) | C5—H5 | 0.9500 |
N1—C2 | 1.340 (3) | C6—C7 | 1.393 (3) |
N2—C4 | 1.339 (3) | C6—C8 | 1.504 (3) |
N2—C3 | 1.346 (3) | C7—H7 | 0.9500 |
C1—C2i | 1.391 (3) | C8—H8A | 0.9800 |
C1—H1 | 0.9500 | C8—H8B | 0.9800 |
C2—C1i | 1.391 (3) | C8—H8C | 0.9800 |
C2—C3 | 1.484 (3) | Cl1—C10 | 1.757 (2) |
C3—C7 | 1.385 (3) | Cl2—C10 | 1.760 (2) |
C4—C5 | 1.383 (3) | Cl3—C10 | 1.753 (2) |
C4—H4 | 0.9500 | C10—H10 | 1.0000 |
C5—C6 | 1.383 (3) | ||
C1—N1—C2 | 116.90 (17) | C5—C6—C8 | 121.56 (19) |
C4—N2—C3 | 116.44 (17) | C7—C6—C8 | 121.58 (19) |
N1—C1—C2i | 122.74 (18) | C3—C7—C6 | 120.36 (18) |
N1—C1—H1 | 118.6 | C3—C7—H7 | 119.8 |
C2i—C1—H1 | 118.6 | C6—C7—H7 | 119.8 |
N1—C2—C1i | 120.36 (17) | C6—C8—H8A | 109.5 |
N1—C2—C3 | 117.77 (16) | C6—C8—H8B | 109.5 |
C1i—C2—C3 | 121.87 (17) | H8A—C8—H8B | 109.5 |
N2—C3—C7 | 122.68 (17) | C6—C8—H8C | 109.5 |
N2—C3—C2 | 116.19 (16) | H8A—C8—H8C | 109.5 |
C7—C3—C2 | 121.13 (17) | H8B—C8—H8C | 109.5 |
N2—C4—C5 | 124.3 (2) | Cl3—C10—Cl1 | 110.88 (12) |
N2—C4—H4 | 117.9 | Cl3—C10—Cl2 | 110.37 (12) |
C5—C4—H4 | 117.9 | Cl1—C10—Cl2 | 110.64 (12) |
C6—C5—C4 | 119.35 (19) | Cl3—C10—H10 | 108.3 |
C6—C5—H5 | 120.3 | Cl1—C10—H10 | 108.3 |
C4—C5—H5 | 120.3 | Cl2—C10—H10 | 108.3 |
C5—C6—C7 | 116.86 (18) | ||
C2—N1—C1—C2i | −0.8 (3) | C3—N2—C4—C5 | −1.7 (3) |
C1—N1—C2—C1i | 0.7 (3) | N2—C4—C5—C6 | 1.2 (3) |
C1—N1—C2—C3 | −179.12 (16) | C4—C5—C6—C7 | 0.6 (3) |
C4—N2—C3—C7 | 0.5 (3) | C4—C5—C6—C8 | −179.05 (19) |
C4—N2—C3—C2 | −179.40 (16) | N2—C3—C7—C6 | 1.2 (3) |
N1—C2—C3—N2 | −174.82 (17) | C2—C3—C7—C6 | −178.94 (16) |
C1i—C2—C3—N2 | 5.3 (3) | C5—C6—C7—C3 | −1.7 (3) |
N1—C2—C3—C7 | 5.3 (3) | C8—C6—C7—C3 | 177.96 (19) |
C1i—C2—C3—C7 | −174.56 (18) |
Symmetry code: (i) −x+3/2, −y+3/2, −z+1/2. |
Footnotes
†This work is part of the PhD thesis (Neuchâtel, 2008) of LS.
Acknowledgements
This work was supported by the Swiss National Science Foundation and the University of Neuchâtel.
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