Abstract
In the title compound, C14H16N4, the six-membered hexahydropyrimidine ring adopts a chair conformation. In the crystal, one of the two pyrimidine N atoms engages in N—H⋯N hydrogen bonding with one of the pyridine N atoms, generating a helical chain running along the c axis. The helical pitch is the length of the c axis.
Related literature
For related structures, see: Song et al. (2010 ▶); Jayaratna & Norman (2010 ▶); Fun & Kia (2008 ▶); Warad et al. (2012 ▶). For competition between cyclization and bisimine formation, see: Locke et al. (2009 ▶). For the use of hexahydropyrimidines as polydentate ligands for the synthesis of transition metal coordination complexes, see: Schmidt et al. (2011 ▶).
Experimental
Crystal data
C14H16N4
M r = 240.31
Monoclinic,
a = 14.2372 (14) Å
b = 8.0302 (8) Å
c = 11.3277 (9) Å
β = 103.075 (8)°
V = 1261.5 (2) Å3
Z = 4
Mo Kα radiation
μ = 0.08 mm−1
T = 293 K
0.3 × 0.2 × 0.15 mm
Data collection
Agilent Xcalibur Eos diffractometer
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011 ▶) T min = 0.98, T max = 0.99
4640 measured reflections
2238 independent reflections
1656 reflections with I > 2σ(I)
R int = 0.023
Refinement
R[F 2 > 2σ(F 2)] = 0.041
wR(F 2) = 0.108
S = 1.05
2238 reflections
171 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.14 e Å−3
Δρmin = −0.15 e Å−3
Data collection: CrysAlis PRO (Agilent, 2011 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶) and ORTEP (Burnett & Johnson, 1996 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536813007459/nk2200sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813007459/nk2200Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536813007459/nk2200Isup3.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 |
|---|---|---|---|---|
| N3—H3⋯N2i | 0.878 (17) | 2.425 (18) | 3.2845 (19) | 166.4 (15) |
Symmetry code: (i)
.
Acknowledgments
The X-ray structural work was done at Hamdi Mango Center for Scientific research at The University of Jordan, Amman 11942, Jordan.
supplementary crystallographic information
Comment
Condensation of 1,3-diamines with 2-dipyridlketone is a well documented reaction for two potential products, hexahydropyrimidine and classical Schiff bases compounds (Warad et al., 2012; Song et al., 2010; Jayaratna & Norman, 2010; Fun & Kia, 2008). Both of these products are extensively utilized as polydentate ligands to synthesize coordination metal complexes. The title compound was obtained during our attempt to synthesize novel ligands in order to study their coordination chemistry.
The pyrimidine ring in the molecule assumes a chair configuration allowing better disposition for H-bonding. The molecular units are connected via hydrogen bonding between one pyrimidine nitrogen atom, N3 and one pyridinic nitrogen atom, N2 in adjacent molecule as shown in Fig. 2. Hydrogen bond values are tabulated.
Experimental
A solution of 2-dipyridlketone (0.25 g, 1.45 mmol) in anhydrous ethanol (20 ml) was mixed with 1,3-propanediamine (0.16 ml, 1.5 mmoL) and allowed to reflux for about four hours. The resulting mixture was concentrated under reduced pressure and the title compound was precipitated by the addition of 40 ml of ice cool distilled water. The precipitate was filtered off, washed three times with 40 ml of distilled water, recrystallized in ethanol and allowed to stand at room temperature. After three days, colourless crystals suitable for single-crystal X-ray data collection were obtained (0.24 g, yield 77%).
Refinement
All nonhydrogen atoms were refined anisotropically. H atoms attached to C were positioned geometrically, with C—H = 0.93 and 0.96 Å for aromatic and methyl H, respectively, and constrained to ride on their parent atoms, with Uiso(H) = 1.2Ueq. The two H atoms attched to the pyrimidinic N atoms were located in a difference Fourier map and refined fully to values of 0.88 (2) Å for the H atom involved in intermolecular H-bonding, and 0.92 (2) Å for the H atom involved in the biforcatd intramolecular hydrogen bonding. Highest difference peak and hole are 0.14 and -0.15 e/Å3 .
Figures
Fig. 1.
An ORTEP (Burnett & Johnson, 1996) view of the title compound. Displacement ellipsoids are drawn at the 30% probability level. H atoms are represented as small spheres of arbitrary radii.
Fig. 2.
View approximately down b axis showing helical chains extending along c axis formed by intermolecular N—H···N hydrogen bonds joining one pyrimidinic nitrogen, N3, and one pyridinic nitrogen, N2 in adjacent molecule.
Crystal data
| C14H16N4 | F(000) = 512 |
| Mr = 240.31 | Dx = 1.265 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 1403 reflections |
| a = 14.2372 (14) Å | θ = 3.1–29.1° |
| b = 8.0302 (8) Å | µ = 0.08 mm−1 |
| c = 11.3277 (9) Å | T = 293 K |
| β = 103.075 (8)° | Parallelpiped, colourless |
| V = 1261.5 (2) Å3 | 0.3 × 0.2 × 0.15 mm |
| Z = 4 |
Data collection
| Agilent Xcalibur Eos diffractometer | 2238 independent reflections |
| Radiation source: Enhance (Mo) X-ray Source | 1656 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.023 |
| Detector resolution: 16.0534 pixels mm-1 | θmax = 25.0°, θmin = 3.1° |
| ω scans | h = −16→15 |
| Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) | k = −9→9 |
| Tmin = 0.98, Tmax = 0.99 | l = −13→13 |
| 4640 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)] = 0.041 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.108 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0446P)2 + 0.061P] where P = (Fo2 + 2Fc2)/3 |
| 2238 reflections | (Δ/σ)max < 0.001 |
| 171 parameters | Δρmax = 0.14 e Å−3 |
| 0 restraints | Δρmin = −0.15 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 | ||
| N3 | 0.79810 (10) | 0.13990 (18) | 0.07018 (11) | 0.0369 (4) | |
| N2 | 0.79269 (10) | 0.05042 (18) | −0.24206 (10) | 0.0406 (4) | |
| N4 | 0.82606 (10) | 0.32537 (17) | −0.08565 (12) | 0.0377 (4) | |
| C14 | 0.76709 (11) | 0.18825 (19) | −0.05728 (12) | 0.0315 (4) | |
| C10 | 0.76853 (11) | 0.03058 (19) | −0.13524 (12) | 0.0306 (4) | |
| C5 | 0.66284 (12) | 0.2490 (2) | −0.08265 (13) | 0.0356 (4) | |
| C11 | 0.90172 (13) | 0.1041 (2) | 0.10491 (14) | 0.0456 (5) | |
| H11A | 0.9148 | 0.0036 | 0.0640 | 0.055* | |
| H11B | 0.9198 | 0.0835 | 0.1915 | 0.055* | |
| C9 | 0.74371 (12) | −0.1230 (2) | −0.09704 (14) | 0.0412 (4) | |
| H9A | 0.7238 | −0.1323 | −0.0246 | 0.049* | |
| N1 | 0.63469 (11) | 0.3400 (2) | −0.18294 (12) | 0.0511 (4) | |
| C6 | 0.79561 (13) | −0.0872 (2) | −0.30852 (15) | 0.0506 (5) | |
| H6A | 0.8117 | −0.0751 | −0.3832 | 0.061* | |
| C13 | 0.92964 (13) | 0.2875 (2) | −0.05846 (14) | 0.0474 (5) | |
| H13A | 0.9651 | 0.3833 | −0.0774 | 0.057* | |
| H13B | 0.9417 | 0.1947 | −0.1078 | 0.057* | |
| C12 | 0.96337 (13) | 0.2441 (3) | 0.07420 (15) | 0.0532 (5) | |
| H12A | 0.9582 | 0.3410 | 0.1235 | 0.064* | |
| H12B | 1.0304 | 0.2098 | 0.0911 | 0.064* | |
| C1 | 0.54414 (16) | 0.3966 (3) | −0.20904 (18) | 0.0639 (6) | |
| H1A | 0.5240 | 0.4598 | −0.2790 | 0.077* | |
| C7 | 0.77636 (14) | −0.2439 (2) | −0.27331 (15) | 0.0520 (5) | |
| H7A | 0.7821 | −0.3359 | −0.3210 | 0.062* | |
| C4 | 0.60138 (14) | 0.2111 (3) | −0.00797 (16) | 0.0539 (5) | |
| H4A | 0.6222 | 0.1458 | 0.0608 | 0.065* | |
| C8 | 0.74829 (13) | −0.2622 (2) | −0.16589 (15) | 0.0503 (5) | |
| H8A | 0.7327 | −0.3666 | −0.1403 | 0.060* | |
| C2 | 0.47951 (15) | 0.3674 (3) | −0.13943 (19) | 0.0647 (6) | |
| H2A | 0.4174 | 0.4109 | −0.1607 | 0.078* | |
| C3 | 0.50821 (15) | 0.2726 (3) | −0.03762 (19) | 0.0685 (6) | |
| H3A | 0.4655 | 0.2496 | 0.0114 | 0.082* | |
| H4 | 0.8042 (12) | 0.352 (2) | −0.1662 (16) | 0.052 (5)* | |
| H3 | 0.7859 (12) | 0.224 (2) | 0.1143 (14) | 0.050 (5)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| N3 | 0.0487 (9) | 0.0332 (8) | 0.0296 (7) | 0.0036 (7) | 0.0108 (6) | −0.0032 (6) |
| N2 | 0.0533 (10) | 0.0376 (9) | 0.0329 (7) | −0.0027 (7) | 0.0141 (6) | −0.0042 (6) |
| N4 | 0.0455 (9) | 0.0288 (8) | 0.0398 (8) | −0.0039 (7) | 0.0120 (6) | −0.0006 (6) |
| C14 | 0.0390 (10) | 0.0265 (9) | 0.0301 (8) | 0.0004 (7) | 0.0102 (6) | −0.0010 (6) |
| C10 | 0.0353 (9) | 0.0274 (9) | 0.0286 (7) | 0.0023 (7) | 0.0059 (6) | −0.0010 (6) |
| C5 | 0.0408 (10) | 0.0297 (9) | 0.0368 (9) | −0.0001 (7) | 0.0099 (7) | −0.0050 (7) |
| C11 | 0.0493 (12) | 0.0495 (11) | 0.0348 (9) | 0.0080 (9) | 0.0030 (7) | −0.0025 (8) |
| C9 | 0.0557 (12) | 0.0320 (10) | 0.0350 (9) | −0.0030 (8) | 0.0087 (7) | 0.0008 (7) |
| N1 | 0.0506 (10) | 0.0521 (10) | 0.0490 (9) | 0.0117 (8) | 0.0078 (7) | 0.0072 (7) |
| C6 | 0.0613 (13) | 0.0550 (13) | 0.0374 (9) | 0.0009 (10) | 0.0154 (8) | −0.0131 (9) |
| C13 | 0.0426 (11) | 0.0482 (12) | 0.0529 (10) | −0.0101 (9) | 0.0139 (8) | −0.0064 (8) |
| C12 | 0.0451 (12) | 0.0599 (14) | 0.0512 (10) | −0.0036 (10) | 0.0039 (8) | −0.0127 (9) |
| C1 | 0.0583 (14) | 0.0653 (15) | 0.0618 (12) | 0.0154 (11) | −0.0001 (10) | 0.0046 (10) |
| C7 | 0.0639 (13) | 0.0400 (12) | 0.0462 (10) | 0.0107 (10) | 0.0004 (9) | −0.0178 (9) |
| C4 | 0.0487 (12) | 0.0639 (14) | 0.0528 (11) | 0.0017 (10) | 0.0190 (9) | 0.0024 (9) |
| C8 | 0.0639 (13) | 0.0279 (10) | 0.0518 (11) | −0.0024 (9) | −0.0024 (9) | −0.0018 (8) |
| C2 | 0.0448 (13) | 0.0705 (16) | 0.0731 (14) | 0.0124 (11) | 0.0012 (10) | −0.0182 (12) |
| C3 | 0.0452 (13) | 0.0887 (18) | 0.0779 (15) | 0.0000 (12) | 0.0269 (10) | −0.0126 (13) |
Geometric parameters (Å, º)
| N3—C14 | 1.4635 (18) | N1—C1 | 1.336 (2) |
| N3—C11 | 1.467 (2) | C6—C7 | 1.367 (3) |
| N3—H3 | 0.878 (17) | C6—H6A | 0.9300 |
| N2—C10 | 1.3401 (18) | C13—C12 | 1.511 (2) |
| N2—C6 | 1.343 (2) | C13—H13A | 0.9700 |
| N4—C14 | 1.4638 (19) | C13—H13B | 0.9700 |
| N4—C13 | 1.468 (2) | C12—H12A | 0.9700 |
| N4—H4 | 0.921 (17) | C12—H12B | 0.9700 |
| C14—C5 | 1.527 (2) | C1—C2 | 1.361 (3) |
| C14—C10 | 1.546 (2) | C1—H1A | 0.9300 |
| C10—C9 | 1.379 (2) | C7—C8 | 1.372 (2) |
| C5—N1 | 1.334 (2) | C7—H7A | 0.9300 |
| C5—C4 | 1.381 (2) | C4—C3 | 1.384 (3) |
| C11—C12 | 1.514 (2) | C4—H4A | 0.9300 |
| C11—H11A | 0.9700 | C8—H8A | 0.9300 |
| C11—H11B | 0.9700 | C2—C3 | 1.365 (3) |
| C9—C8 | 1.373 (2) | C2—H2A | 0.9300 |
| C9—H9A | 0.9300 | C3—H3A | 0.9300 |
| C14—N3—C11 | 112.16 (12) | C7—C6—H6A | 118.0 |
| C14—N3—H3 | 107.7 (11) | N4—C13—C12 | 109.54 (14) |
| C11—N3—H3 | 108.3 (11) | N4—C13—H13A | 109.8 |
| C10—N2—C6 | 117.07 (15) | C12—C13—H13A | 109.8 |
| C14—N4—C13 | 113.39 (13) | N4—C13—H13B | 109.8 |
| C14—N4—H4 | 108.1 (11) | C12—C13—H13B | 109.8 |
| C13—N4—H4 | 110.8 (11) | H13A—C13—H13B | 108.2 |
| N3—C14—N4 | 110.86 (12) | C13—C12—C11 | 109.23 (14) |
| N3—C14—C5 | 109.51 (12) | C13—C12—H12A | 109.8 |
| N4—C14—C5 | 107.45 (13) | C11—C12—H12A | 109.8 |
| N3—C14—C10 | 107.83 (12) | C13—C12—H12B | 109.8 |
| N4—C14—C10 | 114.09 (12) | C11—C12—H12B | 109.8 |
| C5—C14—C10 | 106.97 (12) | H12A—C12—H12B | 108.3 |
| N2—C10—C9 | 121.72 (14) | N1—C1—C2 | 123.9 (2) |
| N2—C10—C14 | 117.23 (13) | N1—C1—H1A | 118.0 |
| C9—C10—C14 | 121.03 (13) | C2—C1—H1A | 118.0 |
| N1—C5—C4 | 122.15 (17) | C6—C7—C8 | 118.39 (16) |
| N1—C5—C14 | 115.30 (14) | C6—C7—H7A | 120.8 |
| C4—C5—C14 | 122.55 (15) | C8—C7—H7A | 120.8 |
| N3—C11—C12 | 113.15 (15) | C5—C4—C3 | 118.56 (19) |
| N3—C11—H11A | 108.9 | C5—C4—H4A | 120.7 |
| C12—C11—H11A | 108.9 | C3—C4—H4A | 120.7 |
| N3—C11—H11B | 108.9 | C7—C8—C9 | 118.52 (17) |
| C12—C11—H11B | 108.9 | C7—C8—H8A | 120.7 |
| H11A—C11—H11B | 107.8 | C9—C8—H8A | 120.7 |
| C8—C9—C10 | 120.09 (15) | C1—C2—C3 | 118.3 (2) |
| C8—C9—H9A | 120.0 | C1—C2—H2A | 120.9 |
| C10—C9—H9A | 120.0 | C3—C2—H2A | 120.9 |
| C5—N1—C1 | 117.65 (17) | C2—C3—C4 | 119.4 (2) |
| N2—C6—C7 | 124.09 (16) | C2—C3—H3A | 120.3 |
| N2—C6—H6A | 118.0 | C4—C3—H3A | 120.3 |
| C11—N3—C14—N4 | −53.05 (17) | C10—C14—C5—C4 | 97.46 (17) |
| C11—N3—C14—C5 | −171.44 (13) | C14—N3—C11—C12 | 53.15 (17) |
| C11—N3—C14—C10 | 72.50 (16) | N2—C10—C9—C8 | 3.5 (2) |
| C13—N4—C14—N3 | 56.96 (16) | C14—C10—C9—C8 | −178.02 (15) |
| C13—N4—C14—C5 | 176.59 (11) | C4—C5—N1—C1 | 0.9 (3) |
| C13—N4—C14—C10 | −65.00 (16) | C14—C5—N1—C1 | −179.79 (15) |
| C6—N2—C10—C9 | −2.7 (2) | C10—N2—C6—C7 | −0.5 (3) |
| C6—N2—C10—C14 | 178.80 (14) | C14—N4—C13—C12 | −58.22 (17) |
| N3—C14—C10—N2 | −145.84 (13) | N4—C13—C12—C11 | 54.63 (19) |
| N4—C14—C10—N2 | −22.22 (19) | N3—C11—C12—C13 | −53.6 (2) |
| C5—C14—C10—N2 | 96.46 (16) | C5—N1—C1—C2 | 0.2 (3) |
| N3—C14—C10—C9 | 35.63 (19) | N2—C6—C7—C8 | 2.9 (3) |
| N4—C14—C10—C9 | 159.24 (14) | N1—C5—C4—C3 | −1.2 (3) |
| C5—C14—C10—C9 | −82.08 (17) | C14—C5—C4—C3 | 179.54 (16) |
| N3—C14—C5—N1 | 161.53 (13) | C6—C7—C8—C9 | −2.0 (3) |
| N4—C14—C5—N1 | 41.03 (17) | C10—C9—C8—C7 | −1.0 (2) |
| C10—C14—C5—N1 | −81.87 (16) | N1—C1—C2—C3 | −1.0 (3) |
| N3—C14—C5—C4 | −19.1 (2) | C1—C2—C3—C4 | 0.6 (3) |
| N4—C14—C5—C4 | −139.63 (16) | C5—C4—C3—C2 | 0.4 (3) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N3—H3···N2i | 0.878 (17) | 2.425 (18) | 3.2845 (19) | 166.4 (15) |
| N4—H4···N1 | 0.921 (17) | 2.379 (17) | 2.701 (2) | 100.3 (12) |
| N4—H4···N2 | 0.921 (17) | 2.564 (17) | 2.8034 (19) | 95.3 (12) |
Symmetry code: (i) x, −y+1/2, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NK2200).
References
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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/S1600536813007459/nk2200sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813007459/nk2200Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536813007459/nk2200Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


