Abstract
In the title compound, C20H20N2O2, the pyrazole ring makes dihedral angles of 15.68 (4) and 83.40 (4)°, respectively, with the tolyl and benzyl rings, respectively.
Related literature
For arelated structure, see: Ge et al. (2007 ▶). For applications of nitrogen-containing heterocyclic compounds in agrochemicals and pharmaceuticals, see: Ge et al. (2009a
▶,b
▶, 2011 ▶).
Experimental
Crystal data
C20H20N2O2
M r = 320.38
Triclinic,
a = 7.666 (4) Å
b = 10.160 (6) Å
c = 11.381 (7) Å
α = 83.991 (9)°
β = 87.466 (9)°
γ = 85.47 (1)°
V = 878.2 (9) Å3
Z = 2
Mo Kα radiation
μ = 0.08 mm−1
T = 298 K
0.21 × 0.16 × 0.12 mm
Data collection
Bruker SMART CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 1997 ▶) T min = 0.984, T max = 0.991
4489 measured reflections
3045 independent reflections
2182 reflections with I > 2σ(I)
R int = 0.032
Refinement
R[F 2 > 2σ(F 2)] = 0.066
wR(F 2) = 0.220
S = 1.06
3045 reflections
217 parameters
H-atom parameters constrained
Δρmax = 0.34 e Å−3
Δρmin = −0.21 e Å−3
Data collection: SMART (Bruker, 1997 ▶); cell refinement: SAINT (Bruker, 1997 ▶); data reduction: SAINT; 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: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811002339/jh2257sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811002339/jh2257Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
supplementary crystallographic information
Comment
Synthesis of nitrogen-containing heterocyclic compounds has been a subject of great interest due to the wide application in agrochemical and pharmaceutical fields (Ge et al.; 2011, 2009a, 2009b). Some pyrazole derivatives which belong to this category have been of interest for their biological activities. Considerable efforts have been devoted to the development of novel pyrazole compounds. We report here the crystal structure of the title compound, (I) (Fig. 1)
Experimental
A mixture of ethyl 3-p-tolyl-1H-pyrazole-5-carboxylate (0.02 mol), benzyl chloride (0.0024 mol) and potassium carbonate (0.02 mol) in acetonitrile (100 ml) was heated to reflux for 10 h. The solvent was removed under reduced pressure and an product was isolated by column chromatography on silica gel (yield 82%). Crystals of (I) suitable for X-ray diffraction were obtained by slow cooling of the refluxed solution of the product in ethyl acetate at room temperature for 2 d.
Refinement
All H atoms were placed in geometrically calculated positions and refined using a riding model with C—H = 0.97 Å (for CH2 groups) and 0.96 Å (for CH3 groups), their isotropic displacement parameters were set to 1.2 times (1.5 times for CH3 groups) the equivalent displacement parameter of their parent atoms.
Figures
Fig. 1.
The molecular structure of (I), showing displacement ellipsoids drawn at the 50% probability level.
Crystal data
| C20H20N2O2 | Z = 2 |
| Mr = 320.38 | F(000) = 340 |
| Triclinic, P1 | Dx = 1.212 Mg m−3 |
| a = 7.666 (4) Å | Mo Kα radiation, λ = 0.71073 Å |
| b = 10.160 (6) Å | Cell parameters from 1778 reflections |
| c = 11.381 (7) Å | θ = 2.6–24.2° |
| α = 83.991 (9)° | µ = 0.08 mm−1 |
| β = 87.466 (9)° | T = 298 K |
| γ = 85.47 (1)° | BLOCK, white |
| V = 878.2 (9) Å3 | 0.21 × 0.16 × 0.12 mm |
Data collection
| Bruker SMART CCD area-detector diffractometer | 3045 independent reflections |
| Radiation source: fine-focus sealed tube | 2182 reflections with I > 2σ(I) |
| graphite | Rint = 0.032 |
| phi and ω scans | θmax = 25.1°, θmin = 1.8° |
| Absorption correction: multi-scan (SADABS; Bruker, 1997) | h = −9→8 |
| Tmin = 0.984, Tmax = 0.991 | k = −12→9 |
| 4489 measured reflections | l = −13→13 |
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)] = 0.066 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.220 | H-atom parameters constrained |
| S = 1.06 | w = 1/[σ2(Fo2) + (0.1348P)2 + 0.1525P] where P = (Fo2 + 2Fc2)/3 |
| 3045 reflections | (Δ/σ)max < 0.001 |
| 217 parameters | Δρmax = 0.34 e Å−3 |
| 0 restraints | Δρmin = −0.21 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 | ||
| O1 | 0.3059 (3) | 0.5585 (2) | 0.70282 (17) | 0.0826 (7) | |
| O2 | 0.2483 (3) | 0.6693 (2) | 0.86211 (17) | 0.0703 (6) | |
| N1 | 0.3539 (3) | 0.3185 (2) | 0.86746 (18) | 0.0548 (6) | |
| N2 | 0.3537 (3) | 0.2290 (2) | 0.96361 (19) | 0.0569 (6) | |
| C1 | 0.1960 (6) | 0.9004 (4) | 0.8654 (3) | 0.0955 (11) | |
| H1A | 0.1004 | 0.8824 | 0.9206 | 0.143* | |
| H1B | 0.1698 | 0.9836 | 0.8191 | 0.143* | |
| H1C | 0.3006 | 0.9049 | 0.9077 | 0.143* | |
| C2 | 0.2227 (5) | 0.7932 (3) | 0.7865 (3) | 0.0764 (9) | |
| H2A | 0.1213 | 0.7919 | 0.7387 | 0.092* | |
| H2B | 0.3246 | 0.8065 | 0.7342 | 0.092* | |
| C3 | 0.2870 (3) | 0.5601 (3) | 0.8081 (2) | 0.0597 (7) | |
| C4 | 0.3021 (3) | 0.4439 (3) | 0.8954 (2) | 0.0528 (6) | |
| C5 | 0.2658 (3) | 0.4323 (3) | 1.0152 (2) | 0.0551 (7) | |
| H5 | 0.2268 | 0.5002 | 1.0609 | 0.066* | |
| C6 | 0.2990 (3) | 0.2986 (3) | 1.0543 (2) | 0.0517 (6) | |
| C7 | 0.2828 (3) | 0.2321 (3) | 1.1751 (2) | 0.0523 (6) | |
| C8 | 0.2692 (4) | 0.3059 (3) | 1.2712 (2) | 0.0625 (7) | |
| H8 | 0.2707 | 0.3978 | 1.2586 | 0.075* | |
| C9 | 0.2535 (4) | 0.2459 (3) | 1.3851 (2) | 0.0669 (8) | |
| H9 | 0.2442 | 0.2982 | 1.4478 | 0.080* | |
| C10 | 0.2512 (4) | 0.1096 (3) | 1.4083 (2) | 0.0616 (7) | |
| C11 | 0.2643 (4) | 0.0367 (3) | 1.3121 (3) | 0.0717 (8) | |
| H11 | 0.2620 | −0.0551 | 1.3247 | 0.086* | |
| C12 | 0.2806 (4) | 0.0958 (3) | 1.1980 (2) | 0.0648 (8) | |
| H12 | 0.2903 | 0.0433 | 1.1355 | 0.078* | |
| C13 | 0.2361 (5) | 0.0423 (4) | 1.5327 (3) | 0.0880 (10) | |
| H13A | 0.2140 | −0.0490 | 1.5301 | 0.132* | |
| H13B | 0.1414 | 0.0861 | 1.5752 | 0.132* | |
| H13C | 0.3434 | 0.0471 | 1.5719 | 0.132* | |
| C14 | 0.4189 (3) | 0.2742 (3) | 0.7545 (2) | 0.0608 (7) | |
| H14A | 0.3443 | 0.3163 | 0.6925 | 0.073* | |
| H14B | 0.4110 | 0.1791 | 0.7574 | 0.073* | |
| C15 | 0.6048 (3) | 0.3050 (2) | 0.7234 (2) | 0.0485 (6) | |
| C16 | 0.6535 (4) | 0.3469 (3) | 0.6073 (2) | 0.0596 (7) | |
| H16 | 0.5692 | 0.3606 | 0.5501 | 0.071* | |
| C17 | 0.8246 (4) | 0.3682 (3) | 0.5762 (3) | 0.0730 (9) | |
| H17 | 0.8563 | 0.3945 | 0.4979 | 0.088* | |
| C18 | 0.9483 (4) | 0.3509 (4) | 0.6601 (3) | 0.0766 (9) | |
| H18 | 1.0637 | 0.3675 | 0.6390 | 0.092* | |
| C19 | 0.9039 (4) | 0.3090 (3) | 0.7758 (3) | 0.0692 (8) | |
| H19 | 0.9892 | 0.2966 | 0.8324 | 0.083* | |
| C20 | 0.7326 (3) | 0.2855 (3) | 0.8074 (2) | 0.0555 (7) | |
| H20 | 0.7025 | 0.2566 | 0.8853 | 0.067* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.1089 (17) | 0.0879 (17) | 0.0500 (12) | −0.0083 (13) | −0.0052 (10) | −0.0005 (11) |
| O2 | 0.0972 (15) | 0.0575 (12) | 0.0542 (11) | −0.0067 (10) | −0.0058 (9) | 0.0058 (9) |
| N1 | 0.0577 (12) | 0.0589 (14) | 0.0494 (12) | −0.0112 (10) | 0.0018 (9) | −0.0093 (10) |
| N2 | 0.0608 (13) | 0.0548 (13) | 0.0561 (13) | −0.0100 (10) | 0.0022 (10) | −0.0083 (10) |
| C1 | 0.131 (3) | 0.061 (2) | 0.091 (2) | −0.0049 (19) | −0.015 (2) | 0.0112 (18) |
| C2 | 0.091 (2) | 0.065 (2) | 0.0695 (19) | −0.0083 (16) | −0.0136 (16) | 0.0169 (16) |
| C3 | 0.0604 (16) | 0.0674 (18) | 0.0520 (16) | −0.0112 (13) | −0.0059 (11) | −0.0031 (13) |
| C4 | 0.0542 (14) | 0.0551 (16) | 0.0501 (14) | −0.0110 (11) | −0.0027 (11) | −0.0037 (12) |
| C5 | 0.0643 (16) | 0.0517 (15) | 0.0500 (14) | −0.0065 (12) | 0.0008 (11) | −0.0082 (11) |
| C6 | 0.0545 (14) | 0.0512 (15) | 0.0509 (14) | −0.0089 (11) | 0.0025 (11) | −0.0098 (11) |
| C7 | 0.0545 (14) | 0.0491 (15) | 0.0531 (14) | −0.0051 (11) | 0.0026 (11) | −0.0056 (11) |
| C8 | 0.0851 (19) | 0.0470 (15) | 0.0561 (16) | −0.0106 (13) | 0.0011 (13) | −0.0061 (12) |
| C9 | 0.089 (2) | 0.0595 (18) | 0.0530 (16) | −0.0082 (15) | 0.0023 (14) | −0.0104 (13) |
| C10 | 0.0716 (17) | 0.0582 (17) | 0.0534 (15) | −0.0028 (13) | 0.0007 (12) | −0.0007 (12) |
| C11 | 0.103 (2) | 0.0443 (16) | 0.0660 (18) | −0.0029 (14) | 0.0045 (16) | −0.0023 (13) |
| C12 | 0.091 (2) | 0.0462 (15) | 0.0567 (16) | −0.0007 (13) | 0.0029 (14) | −0.0081 (12) |
| C13 | 0.123 (3) | 0.079 (2) | 0.0594 (19) | −0.008 (2) | −0.0044 (18) | 0.0073 (16) |
| C14 | 0.0632 (16) | 0.0726 (19) | 0.0512 (14) | −0.0156 (13) | −0.0016 (12) | −0.0198 (13) |
| C15 | 0.0543 (14) | 0.0459 (14) | 0.0472 (13) | −0.0054 (10) | −0.0033 (10) | −0.0120 (10) |
| C16 | 0.0669 (17) | 0.0637 (17) | 0.0481 (14) | −0.0030 (13) | −0.0076 (12) | −0.0048 (12) |
| C17 | 0.0712 (19) | 0.087 (2) | 0.0594 (17) | −0.0095 (16) | 0.0107 (14) | −0.0026 (15) |
| C18 | 0.0563 (17) | 0.092 (2) | 0.081 (2) | −0.0046 (15) | 0.0081 (15) | −0.0122 (18) |
| C19 | 0.0549 (16) | 0.084 (2) | 0.0699 (18) | 0.0027 (14) | −0.0142 (13) | −0.0154 (16) |
| C20 | 0.0669 (16) | 0.0551 (15) | 0.0456 (13) | −0.0038 (12) | −0.0063 (11) | −0.0096 (11) |
Geometric parameters (Å, °)
| O1—C3 | 1.202 (3) | C9—H9 | 0.9300 |
| O2—C3 | 1.332 (3) | C10—C11 | 1.381 (4) |
| O2—C2 | 1.453 (3) | C10—C13 | 1.510 (4) |
| N1—N2 | 1.348 (3) | C11—C12 | 1.376 (4) |
| N1—C4 | 1.369 (3) | C11—H11 | 0.9300 |
| N1—C14 | 1.461 (3) | C12—H12 | 0.9300 |
| N2—C6 | 1.345 (3) | C13—H13A | 0.9600 |
| C1—C2 | 1.480 (5) | C13—H13B | 0.9600 |
| C1—H1A | 0.9600 | C13—H13C | 0.9600 |
| C1—H1B | 0.9600 | C14—C15 | 1.502 (3) |
| C1—H1C | 0.9600 | C14—H14A | 0.9700 |
| C2—H2A | 0.9700 | C14—H14B | 0.9700 |
| C2—H2B | 0.9700 | C15—C20 | 1.388 (4) |
| C3—C4 | 1.463 (4) | C15—C16 | 1.389 (4) |
| C4—C5 | 1.374 (3) | C16—C17 | 1.372 (4) |
| C5—C6 | 1.392 (4) | C16—H16 | 0.9300 |
| C5—H5 | 0.9300 | C17—C18 | 1.364 (4) |
| C6—C7 | 1.471 (4) | C17—H17 | 0.9300 |
| C7—C12 | 1.384 (4) | C18—C19 | 1.377 (4) |
| C7—C8 | 1.386 (4) | C18—H18 | 0.9300 |
| C8—C9 | 1.378 (4) | C19—C20 | 1.379 (4) |
| C8—H8 | 0.9300 | C19—H19 | 0.9300 |
| C9—C10 | 1.384 (4) | C20—H20 | 0.9300 |
| C3—O2—C2 | 116.6 (2) | C11—C10—C13 | 121.0 (3) |
| N2—N1—C4 | 111.8 (2) | C9—C10—C13 | 122.1 (3) |
| N2—N1—C14 | 118.5 (2) | C12—C11—C10 | 122.0 (3) |
| C4—N1—C14 | 129.5 (2) | C12—C11—H11 | 119.0 |
| C6—N2—N1 | 105.3 (2) | C10—C11—H11 | 119.0 |
| C2—C1—H1A | 109.5 | C11—C12—C7 | 121.0 (3) |
| C2—C1—H1B | 109.5 | C11—C12—H12 | 119.5 |
| H1A—C1—H1B | 109.5 | C7—C12—H12 | 119.5 |
| C2—C1—H1C | 109.5 | C10—C13—H13A | 109.5 |
| H1A—C1—H1C | 109.5 | C10—C13—H13B | 109.5 |
| H1B—C1—H1C | 109.5 | H13A—C13—H13B | 109.5 |
| O2—C2—C1 | 106.8 (3) | C10—C13—H13C | 109.5 |
| O2—C2—H2A | 110.4 | H13A—C13—H13C | 109.5 |
| C1—C2—H2A | 110.4 | H13B—C13—H13C | 109.5 |
| O2—C2—H2B | 110.4 | N1—C14—C15 | 113.41 (19) |
| C1—C2—H2B | 110.4 | N1—C14—H14A | 108.9 |
| H2A—C2—H2B | 108.6 | C15—C14—H14A | 108.9 |
| O1—C3—O2 | 124.5 (3) | N1—C14—H14B | 108.9 |
| O1—C3—C4 | 125.5 (3) | C15—C14—H14B | 108.9 |
| O2—C3—C4 | 110.0 (2) | H14A—C14—H14B | 107.7 |
| N1—C4—C5 | 106.1 (2) | C20—C15—C16 | 118.7 (2) |
| N1—C4—C3 | 123.6 (2) | C20—C15—C14 | 121.2 (2) |
| C5—C4—C3 | 130.3 (3) | C16—C15—C14 | 119.9 (2) |
| C4—C5—C6 | 106.2 (2) | C17—C16—C15 | 120.7 (2) |
| C4—C5—H5 | 126.9 | C17—C16—H16 | 119.7 |
| C6—C5—H5 | 126.9 | C15—C16—H16 | 119.7 |
| N2—C6—C5 | 110.6 (2) | C18—C17—C16 | 119.9 (3) |
| N2—C6—C7 | 120.6 (2) | C18—C17—H17 | 120.0 |
| C5—C6—C7 | 128.8 (2) | C16—C17—H17 | 120.0 |
| C12—C7—C8 | 117.3 (2) | C17—C18—C19 | 120.6 (3) |
| C12—C7—C6 | 122.4 (2) | C17—C18—H18 | 119.7 |
| C8—C7—C6 | 120.2 (2) | C19—C18—H18 | 119.7 |
| C9—C8—C7 | 121.3 (3) | C18—C19—C20 | 119.7 (3) |
| C9—C8—H8 | 119.4 | C18—C19—H19 | 120.1 |
| C7—C8—H8 | 119.4 | C20—C19—H19 | 120.1 |
| C8—C9—C10 | 121.5 (3) | C19—C20—C15 | 120.3 (2) |
| C8—C9—H9 | 119.3 | C19—C20—H20 | 119.9 |
| C10—C9—H9 | 119.3 | C15—C20—H20 | 119.9 |
| C11—C10—C9 | 116.9 (3) | ||
| C4—N1—N2—C6 | 0.6 (3) | C12—C7—C8—C9 | −0.2 (4) |
| C14—N1—N2—C6 | 176.1 (2) | C6—C7—C8—C9 | 179.8 (2) |
| C3—O2—C2—C1 | −175.4 (3) | C7—C8—C9—C10 | 0.2 (5) |
| C2—O2—C3—O1 | 1.8 (4) | C8—C9—C10—C11 | −0.4 (5) |
| C2—O2—C3—C4 | −177.9 (2) | C8—C9—C10—C13 | 179.3 (3) |
| N2—N1—C4—C5 | −0.6 (3) | C9—C10—C11—C12 | 0.6 (5) |
| C14—N1—C4—C5 | −175.4 (2) | C13—C10—C11—C12 | −179.1 (3) |
| N2—N1—C4—C3 | −178.8 (2) | C10—C11—C12—C7 | −0.7 (5) |
| C14—N1—C4—C3 | 6.4 (4) | C8—C7—C12—C11 | 0.4 (4) |
| O1—C3—C4—N1 | 5.4 (4) | C6—C7—C12—C11 | −179.6 (3) |
| O2—C3—C4—N1 | −174.9 (2) | N2—N1—C14—C15 | −99.0 (3) |
| O1—C3—C4—C5 | −172.3 (3) | C4—N1—C14—C15 | 75.5 (3) |
| O2—C3—C4—C5 | 7.4 (4) | N1—C14—C15—C20 | 42.9 (4) |
| N1—C4—C5—C6 | 0.4 (3) | N1—C14—C15—C16 | −140.7 (3) |
| C3—C4—C5—C6 | 178.4 (2) | C20—C15—C16—C17 | 0.2 (4) |
| N1—N2—C6—C5 | −0.4 (3) | C14—C15—C16—C17 | −176.3 (3) |
| N1—N2—C6—C7 | −179.9 (2) | C15—C16—C17—C18 | −1.3 (5) |
| C4—C5—C6—N2 | 0.0 (3) | C16—C17—C18—C19 | 1.5 (5) |
| C4—C5—C6—C7 | 179.5 (2) | C17—C18—C19—C20 | −0.6 (5) |
| N2—C6—C7—C12 | −16.0 (4) | C18—C19—C20—C15 | −0.5 (4) |
| C5—C6—C7—C12 | 164.6 (3) | C16—C15—C20—C19 | 0.7 (4) |
| N2—C6—C7—C8 | 164.0 (2) | C14—C15—C20—C19 | 177.2 (2) |
| C5—C6—C7—C8 | −15.4 (4) |
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: JH2257).
References
- Bruker (1997). SMART, SAINT and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
- Ge, Y.-Q., Dong, W.-L., Xia, Y., Wei, F. & Zhao, B.-X. (2007). Acta Cryst. E63, o1313–o1314.
- Ge, Y. Q., Jia, J., Li, Y., Yin, L. & Wang, J. W. (2009a). Heterocycles, 42, 197–206.
- Ge, Y. Q., Jia, J., Yang, H., Tao, X. T. & Wang, J. W. (2011). Dyes Pigm. 88, 344–349.
- Ge, Y. Q., Jia, J., Yang, H., Zhao, G. L., Zhan, F. X. & Wang, J. W. (2009b). Heterocycles, 72, 725–736.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811002339/jh2257sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811002339/jh2257Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

