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In the crystal structure of the title compound, C12H10N4, the pyridine ring makes a dihedral angle of 1.12 (9)° with the mean plane of the complete almost planar and crystallographically centrosymmetric molecule. There are stacks of parallel molecules along the a-axis direction, with alternate stacks having a herring-bone arrangement relative to each other and an interplanar spacing of 3.551 Å.
Supporting information
CCDC reference: 146108
Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 1997); program(s) used to refine structure: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 1990).
Crystal data top
C12H10N4 | F(000) = 220 |
Mr = 210.24 | Dx = 1.293 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 3.8515 (3) Å | Cell parameters from 2605 reflections |
b = 11.0201 (8) Å | θ = 2.5–28.3° |
c = 12.7303 (9) Å | µ = 0.08 mm−1 |
β = 92.312 (2)° | T = 293 K |
V = 539.88 (7) Å3 | Block, orange |
Z = 2 | 0.38 × 0.36 × 0.32 mm |
Data collection top
Siemens SMART CCD area-detector diffractometer | 1065 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.031 |
Graphite monochromator | θmax = 28.4°, θmin = 2.5° |
Detector resolution: 8.33 pixels mm-1 | h = −5→5 |
ω scans | k = −14→7 |
3584 measured reflections | l = −16→16 |
1325 independent reflections | |
Refinement top
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)] = 0.067 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.110 | All H-atom parameters refined |
S = 1.25 | w = 1/[σ2(Fo2) + (0.0958P)2 + 0.1438P] where P = (Fo2 + 2Fc2)/3 |
1325 reflections | (Δ/σ)max < 0.001 |
93 parameters | Δρmax = 0.31 e Å−3 |
0 restraints | Δρmin = −0.20 e Å−3 |
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 | |
N1 | 0.0922 (6) | 0.8462 (2) | 0.08500 (15) | 0.0580 (6) | |
N2 | 0.4664 (5) | 1.00082 (15) | 0.44528 (12) | 0.0453 (5) | |
C1 | 0.2637 (5) | 0.88327 (16) | 0.29857 (14) | 0.0380 (5) | |
C2 | 0.3255 (6) | 0.97260 (19) | 0.22425 (15) | 0.0429 (5) | |
C3 | 0.2348 (6) | 0.9499 (2) | 0.12006 (17) | 0.0524 (6) | |
C4 | 0.0341 (7) | 0.7614 (2) | 0.15670 (19) | 0.0547 (6) | |
C5 | 0.1144 (6) | 0.77541 (19) | 0.26308 (17) | 0.0473 (5) | |
C6 | 0.3510 (5) | 0.90013 (18) | 0.41100 (15) | 0.0416 (5) | |
H2 | 0.436 (7) | 1.049 (3) | 0.244 (2) | 0.064 (8)* | |
H3 | 0.276 (7) | 1.011 (3) | 0.067 (2) | 0.061 (7)* | |
H4 | −0.077 (8) | 0.687 (3) | 0.129 (2) | 0.073 (8)* | |
H5 | 0.062 (7) | 0.708 (3) | 0.312 (2) | 0.063 (7)* | |
H6 | 0.318 (6) | 0.833 (2) | 0.457 (2) | 0.056 (7)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
N1 | 0.0709 (13) | 0.0645 (13) | 0.0383 (9) | 0.0023 (10) | −0.0024 (8) | −0.0116 (8) |
N2 | 0.0617 (11) | 0.0423 (9) | 0.0312 (9) | −0.0022 (7) | −0.0073 (7) | 0.0017 (6) |
C1 | 0.0408 (10) | 0.0379 (9) | 0.0352 (9) | 0.0026 (7) | 0.0002 (7) | −0.0025 (7) |
C2 | 0.0510 (11) | 0.0404 (10) | 0.0373 (10) | −0.0011 (8) | −0.0003 (8) | −0.0008 (7) |
C3 | 0.0658 (14) | 0.0554 (13) | 0.0362 (10) | 0.0042 (10) | 0.0020 (9) | 0.0025 (9) |
C4 | 0.0627 (14) | 0.0516 (12) | 0.0497 (12) | −0.0048 (10) | −0.0007 (10) | −0.0166 (10) |
C5 | 0.0575 (13) | 0.0392 (10) | 0.0453 (11) | −0.0029 (8) | 0.0028 (9) | −0.0051 (8) |
C6 | 0.0522 (11) | 0.0375 (9) | 0.0350 (9) | −0.0016 (8) | −0.0009 (7) | 0.0021 (7) |
Geometric parameters (Å, º) top
N1—C4 | 1.332 (3) | C2—C3 | 1.381 (3) |
N1—C3 | 1.337 (3) | C2—H2 | 0.97 (3) |
N2—C6 | 1.266 (3) | C3—H3 | 0.97 (3) |
N2—N2i | 1.407 (3) | C4—C5 | 1.386 (3) |
C1—C5 | 1.388 (3) | C4—H4 | 0.98 (3) |
C1—C2 | 1.393 (3) | C5—H5 | 0.99 (3) |
C1—C6 | 1.469 (3) | C6—H6 | 0.95 (3) |
| | | |
C4—N1—C3 | 116.7 (2) | C2—C3—H3 | 119.9 (17) |
C6—N2—N2i | 112.2 (2) | N1—C4—C5 | 123.7 (2) |
C5—C1—C2 | 117.64 (18) | N1—C4—H4 | 114.9 (18) |
C5—C1—C6 | 120.08 (17) | C5—C4—H4 | 121.4 (18) |
C2—C1—C6 | 122.28 (17) | C4—C5—C1 | 119.2 (2) |
C3—C2—C1 | 118.75 (19) | C4—C5—H5 | 119.0 (16) |
C3—C2—H2 | 119.9 (17) | C1—C5—H5 | 121.8 (16) |
C1—C2—H2 | 121.3 (17) | N2—C6—C1 | 120.67 (17) |
N1—C3—C2 | 124.1 (2) | N2—C6—H6 | 121.4 (16) |
N1—C3—H3 | 116.1 (17) | C1—C6—H6 | 117.9 (16) |
| | | |
C5—C1—C2—C3 | 0.3 (3) | C2—C1—C5—C4 | 0.0 (3) |
C6—C1—C2—C3 | −179.78 (19) | C6—C1—C5—C4 | −179.98 (19) |
C4—N1—C3—C2 | 0.5 (4) | N2i—N2—C6—C1 | 179.84 (19) |
C1—C2—C3—N1 | −0.5 (4) | C5—C1—C6—N2 | −175.41 (19) |
C3—N1—C4—C5 | −0.3 (4) | C2—C1—C6—N2 | 4.6 (3) |
N1—C4—C5—C1 | 0.0 (4) | | |
Symmetry code: (i) −x+1, −y+2, −z+1. |
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