Abstract
In the title compound, C14H12N2, the N⋯N distance is 2.719 (1) Å. The N—C—C—N torsion angle [0.9 (1)°] is close to the ideal value of 0° as expected. Bond lengths and angles are consistent with those observed for [1,10]phenanthroline and coordinated 5,6 dimethyl[1,10]phenanthroline. In the crystal, C—H⋯N hydrogen bonds link the molecules into C(4) chains running parallel to the b axis. Weak π–π interactions between benzene and pyridine rings [centroid–centroid distance = 3.5337 (7) Å] and between benzene rings [centroid–centroid distances = 3.6627 (7) and 3.8391 (7)Å] also occur.
Related literature
For [1,10]phenanthroline and 5,6-dimethyl[1,10]phenanthroline, see: Ton & Bolte (2005 ▶) and Gasque et al. (1999 ▶), respectively. For hydrogen-bond motifs, see: Bernstein et al. (1995 ▶).
Experimental
Crystal data
C14H12N2
M r = 208.26
Monoclinic,
a = 7.1932 (7) Å
b = 10.0572 (10) Å
c = 13.8729 (13) Å
β = 93.673 (5)°
V = 1001.55 (17) Å3
Z = 4
Mo Kα radiation
μ = 0.08 mm−1
T = 100 K
0.11 × 0.10 × 0.09 mm
Data collection
Bruker APEXII CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2009 ▶) T min = 0.991, T max = 0.993
16500 measured reflections
1855 independent reflections
1613 reflections with I > 2σ(I)
R int = 0.022
Refinement
R[F 2 > 2σ(F 2)] = 0.035
wR(F 2) = 0.100
S = 1.06
1855 reflections
171 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.16 e Å−3
Δρmin = −0.20 e Å−3
Data collection: APEX2 (Bruker, 2009 ▶); cell refinement: SAINT (Bruker, 2009 ▶); data reduction: SAINT; program(s) used to solve structure: SIR97 (Altomare, et al. 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-32 (Farrugia, 2012 ▶); software used to prepare material for publication: WinGX (Farrugia, 2012 ▶).
Supplementary Material
Crystal structure: contains datablock(s) srd3013, I. DOI: 10.1107/S1600536813025087/bx2451sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813025087/bx2451Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536813025087/bx2451Isup3.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 |
|---|---|---|---|---|
| C2—H2⋯N1i | 0.945 (14) | 2.439 (13) | 3.3718 (15) | 169.0 (10) |
Symmetry code: (i)
.
Acknowledgments
The author thanks Professor Richard Andersen and Dr DiPasquale for their support. This work was supported by the Director, Office of Science, Office of Basic Energy Sciences, and the Division of Chemical Sciences, Geosciences, and Biosciences of the US Department of Energy under contract No. DE–AC02-05CH11231.
supplementary crystallographic information
1. Comment
5,6-dimethyl-1,10-phenanthroline was obtained from Sigma-Aldrich. The distances and angles are consistent with those observed for [1,10]phenanthroline (Ton & Bolte, 2005) and coordinated 5,6-dimethyl-1,10-phenanthroline (Gasque, et al., 1999). The crystal packing is stabilized by an intermolecular C—H···N hydrogen bond interaction which links the molecules into chains with graph-set notation C(4) (Bernstein, et al., 1995) running parallel to the b axis. Weak intermolecular π-π interactions, involving the benzene rings, and the pyridine rings, respectively with an average plane-to plane separation of 3.5982 (7) Å further stabilize and reinforce the crystal structure.
2. Experimental
Crystals of the title compound, 5,6-dimethyl-1,10-phenanthroline, were obtained by sublimation at 160 °C under dynamic vacuum.
3. Refinement
All non-hydrogen atoms were refined anisotropically. Aromatic hydrogen atoms were located in the Fourier map and refined isotropically. Methyl hydrogen atoms were placed based on the expected geometry of the carbon atoms to which they were attached and refined using a riding model, with C—H distances 0.98 Å and Uiso(H) = 1.5 Ueq(C).
Figures
Fig. 1.
Top view of the structure of 5,6-dimethyl-1,10-phenanthroline, displacement ellipsoids drawn at the 50% probability level.
Crystal data
| C14H12N2 | F(000) = 440 |
| Mr = 208.26 | SHELXL-97 |
| Monoclinic, P21/c | Dx = 1.381 Mg m−3 |
| Hall symbol: -P 2ybc | Mo Kα radiation, λ = 0.71073 Å |
| a = 7.1932 (7) Å | Cell parameters from 9819 reflections |
| b = 10.0572 (10) Å | θ = 2.5–25.4° |
| c = 13.8729 (13) Å | µ = 0.08 mm−1 |
| β = 93.673 (5)° | T = 100 K |
| V = 1001.55 (17) Å3 | Block, colourless |
| Z = 4 | 0.11 × 0.10 × 0.09 mm |
Data collection
| Bruker APEXII CCD diffractometer | 1855 independent reflections |
| Radiation source: microfocus sealed tube | 1613 reflections with I > 2σ(I) |
| QUAZAR multilayer mirrors monochromator | Rint = 0.022 |
| Detector resolution: 8.366 pixels mm-1 | θmax = 25.5°, θmin = 2.5° |
| φ and ω scans | h = −8→8 |
| Absorption correction: multi-scan (SADABS; Bruker, 2009) | k = −12→12 |
| Tmin = 0.991, Tmax = 0.993 | l = −16→16 |
| 16500 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)] = 0.035 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.100 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.06 | w = 1/[σ2(Fo2) + (0.0576P)2 + 0.2458P] where P = (Fo2 + 2Fc2)/3 |
| 1855 reflections | (Δ/σ)max < 0.001 |
| 171 parameters | Δρmax = 0.16 e Å−3 |
| 0 restraints | Δρmin = −0.20 e Å−3 |
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 | ||
| C1 | 0.42701 (15) | 0.02490 (12) | 0.23673 (8) | 0.0163 (3) | |
| C2 | 0.42141 (15) | 0.15376 (12) | 0.19967 (8) | 0.0169 (3) | |
| C3 | 0.35250 (15) | 0.17126 (12) | 0.10622 (8) | 0.0155 (3) | |
| C4 | 0.29281 (14) | 0.06112 (11) | 0.04921 (8) | 0.0133 (3) | |
| C5 | 0.22138 (14) | 0.07469 (11) | −0.05047 (8) | 0.0140 (3) | |
| C6 | 0.17602 (14) | −0.03576 (11) | −0.10406 (8) | 0.0140 (3) | |
| C7 | 0.19526 (14) | −0.16667 (11) | −0.06034 (8) | 0.0136 (3) | |
| C8 | 0.15222 (15) | −0.28403 (12) | −0.11278 (8) | 0.0168 (3) | |
| C9 | 0.17425 (16) | −0.40516 (12) | −0.06876 (8) | 0.0192 (3) | |
| C10 | 0.24086 (16) | −0.40937 (12) | 0.02795 (9) | 0.0193 (3) | |
| C11 | 0.26123 (14) | −0.18229 (11) | 0.03706 (8) | 0.0132 (3) | |
| C12 | 0.31061 (14) | −0.06488 (11) | 0.09349 (8) | 0.0128 (3) | |
| C13 | 0.20306 (16) | 0.21432 (12) | −0.08965 (8) | 0.0182 (3) | |
| H13A | 0.3273 | 0.2519 | −0.0961 | 0.027* | |
| H13B | 0.1353 | 0.2692 | −0.0452 | 0.027* | |
| H13C | 0.1347 | 0.2125 | −0.1530 | 0.027* | |
| C14 | 0.10570 (15) | −0.03036 (12) | −0.20896 (8) | 0.0188 (3) | |
| H14A | −0.0264 | −0.0549 | −0.2148 | 0.028* | |
| H14B | 0.1771 | −0.0926 | −0.2464 | 0.028* | |
| H14C | 0.1207 | 0.0600 | −0.2337 | 0.028* | |
| N1 | 0.37466 (12) | −0.08243 (9) | 0.18696 (7) | 0.0150 (2) | |
| N2 | 0.28440 (13) | −0.30292 (9) | 0.08056 (7) | 0.0163 (3) | |
| H1 | 0.4752 (17) | 0.0073 (13) | 0.3036 (9) | 0.019 (3)* | |
| H2 | 0.4698 (17) | 0.2240 (14) | 0.2390 (9) | 0.020 (3)* | |
| H3 | 0.3500 (18) | 0.2604 (15) | 0.0801 (9) | 0.023 (3)* | |
| H8 | 0.1103 (18) | −0.2799 (14) | −0.1809 (10) | 0.026 (3)* | |
| H9 | 0.1465 (17) | −0.4866 (14) | −0.1012 (9) | 0.022 (3)* | |
| H10 | 0.2560 (18) | −0.4966 (14) | 0.0606 (9) | 0.024 (3)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0132 (5) | 0.0220 (7) | 0.0137 (6) | −0.0005 (4) | 0.0003 (4) | −0.0018 (5) |
| C2 | 0.0141 (6) | 0.0184 (6) | 0.0183 (6) | −0.0024 (4) | 0.0026 (4) | −0.0061 (5) |
| C3 | 0.0146 (6) | 0.0130 (6) | 0.0194 (6) | 0.0002 (4) | 0.0043 (4) | 0.0005 (5) |
| C4 | 0.0086 (5) | 0.0157 (6) | 0.0160 (6) | 0.0004 (4) | 0.0031 (4) | 0.0004 (5) |
| C5 | 0.0095 (5) | 0.0160 (6) | 0.0167 (6) | 0.0014 (4) | 0.0030 (4) | 0.0034 (5) |
| C6 | 0.0098 (5) | 0.0184 (6) | 0.0141 (6) | 0.0011 (4) | 0.0023 (4) | 0.0007 (5) |
| C7 | 0.0093 (5) | 0.0169 (6) | 0.0149 (6) | 0.0007 (4) | 0.0020 (4) | −0.0005 (5) |
| C8 | 0.0154 (6) | 0.0210 (7) | 0.0142 (6) | −0.0015 (5) | 0.0008 (4) | −0.0024 (5) |
| C9 | 0.0201 (6) | 0.0157 (6) | 0.0217 (6) | −0.0018 (5) | 0.0014 (5) | −0.0045 (5) |
| C10 | 0.0209 (6) | 0.0126 (6) | 0.0241 (7) | 0.0004 (5) | 0.0001 (5) | 0.0012 (5) |
| C11 | 0.0101 (5) | 0.0145 (6) | 0.0151 (6) | 0.0005 (4) | 0.0026 (4) | 0.0012 (5) |
| C12 | 0.0091 (5) | 0.0165 (6) | 0.0130 (6) | 0.0004 (4) | 0.0019 (4) | 0.0013 (4) |
| C13 | 0.0197 (6) | 0.0169 (7) | 0.0177 (6) | 0.0004 (5) | 0.0000 (5) | 0.0029 (5) |
| C14 | 0.0192 (6) | 0.0218 (7) | 0.0150 (6) | 0.0019 (5) | −0.0014 (4) | 0.0023 (5) |
| N1 | 0.0138 (5) | 0.0180 (5) | 0.0131 (5) | 0.0002 (4) | −0.0002 (4) | 0.0002 (4) |
| N2 | 0.0172 (5) | 0.0135 (5) | 0.0178 (5) | −0.0001 (4) | −0.0003 (4) | 0.0013 (4) |
Geometric parameters (Å, º)
| C1—N1 | 1.3230 (15) | C8—C9 | 1.3673 (17) |
| C1—C2 | 1.3939 (17) | C8—H8 | 0.975 (14) |
| C1—H1 | 0.985 (13) | C9—C10 | 1.3960 (17) |
| C2—C3 | 1.3695 (16) | C9—H9 | 0.950 (14) |
| C2—H2 | 0.945 (14) | C10—N2 | 1.3220 (15) |
| C3—C4 | 1.4118 (16) | C10—H10 | 0.990 (14) |
| C3—H3 | 0.967 (15) | C11—N2 | 1.3605 (14) |
| C4—C12 | 1.4105 (16) | C11—C12 | 1.4483 (15) |
| C4—C5 | 1.4505 (16) | C12—N1 | 1.3595 (14) |
| C5—C6 | 1.3645 (16) | C13—H13A | 0.9800 |
| C5—C13 | 1.5085 (15) | C13—H13B | 0.9800 |
| C6—C7 | 1.4525 (16) | C13—H13C | 0.9800 |
| C6—C14 | 1.5108 (15) | C14—H14A | 0.9800 |
| C7—C8 | 1.4104 (15) | C14—H14B | 0.9800 |
| C7—C11 | 1.4118 (15) | C14—H14C | 0.9800 |
| N1—C1—C2 | 124.44 (10) | C8—C9—H9 | 122.8 (8) |
| N1—C1—H1 | 114.6 (8) | C10—C9—H9 | 118.6 (8) |
| C2—C1—H1 | 121.0 (7) | N2—C10—C9 | 124.10 (11) |
| C3—C2—C1 | 117.96 (10) | N2—C10—H10 | 116.7 (8) |
| C3—C2—H2 | 123.3 (8) | C9—C10—H10 | 119.2 (8) |
| C1—C2—H2 | 118.7 (8) | N2—C11—C7 | 123.22 (10) |
| C2—C3—C4 | 120.54 (11) | N2—C11—C12 | 117.93 (10) |
| C2—C3—H3 | 118.1 (8) | C7—C11—C12 | 118.84 (10) |
| C4—C3—H3 | 121.3 (8) | N1—C12—C4 | 123.21 (10) |
| C12—C4—C3 | 116.43 (10) | N1—C12—C11 | 117.78 (10) |
| C12—C4—C5 | 121.10 (10) | C4—C12—C11 | 119.00 (10) |
| C3—C4—C5 | 122.46 (10) | C5—C13—H13A | 109.5 |
| C6—C5—C4 | 120.03 (10) | C5—C13—H13B | 109.5 |
| C6—C5—C13 | 123.31 (10) | H13A—C13—H13B | 109.5 |
| C4—C5—C13 | 116.65 (10) | C5—C13—H13C | 109.5 |
| C5—C6—C7 | 119.83 (10) | H13A—C13—H13C | 109.5 |
| C5—C6—C14 | 123.31 (10) | H13B—C13—H13C | 109.5 |
| C7—C6—C14 | 116.87 (10) | C6—C14—H14A | 109.5 |
| C8—C7—C11 | 116.73 (10) | C6—C14—H14B | 109.5 |
| C8—C7—C6 | 122.09 (10) | H14A—C14—H14B | 109.5 |
| C11—C7—C6 | 121.17 (10) | C6—C14—H14C | 109.5 |
| C9—C8—C7 | 119.99 (10) | H14A—C14—H14C | 109.5 |
| C9—C8—H8 | 119.4 (8) | H14B—C14—H14C | 109.5 |
| C7—C8—H8 | 120.6 (8) | C1—N1—C12 | 117.36 (9) |
| C8—C9—C10 | 118.62 (11) | C10—N2—C11 | 117.34 (10) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C2—H2···N1i | 0.945 (14) | 2.439 (13) | 3.3718 (15) | 169.0 (10) |
Symmetry code: (i) −x+1, y+1/2, −z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BX2451).
References
- Altomare, A., Burla, M. C., Camalli, M., Cascarano, G. L., Giacovazzo, C., Guagliardi, A., Moliterni, A. G. G., Polidori, G. & Spagna, R. (1999). J. Appl. Cryst. 32, 115–119.
- Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl. 34, 1555–1573.
- Bruker (2009). APEX2, SAINT and SADABS Bruker AXS Inc. Madison, Wisconsin, USA.
- Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.
- Gasque, L., Moreno-Esparza, R., Mollins, E., Briansó-Penalva, J. L., Ruiz-Ramírez, L. & Medina-Dickinson, G. (1999). Acta Cryst. C55, 158–160.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Ton, Q. C. & Bolte, M. (2005). Acta Cryst. E61, o1406–o1407.
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) srd3013, I. DOI: 10.1107/S1600536813025087/bx2451sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813025087/bx2451Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536813025087/bx2451Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

