Related literature
For general background, see: Cimerman et al. (1997
). For bond-length data, see: Chiu et al. (1998
).
Experimental
Crystal data
C12H11N3O2 Mr = 229.24 Tetragonal, I 41 /a a = 17.313 (3) Å c = 15.749 (5) Å V = 4720.5 (18) Å3 Z = 16 Mo Kα radiation μ = 0.09 mm−1 T = 293 (2) K 0.25 × 0.20 × 0.19 mm
|
Data collection
Bruker SMART CCD area-detector diffractometer Absorption correction: none 14901 measured reflections 2911 independent reflections 2151 reflections with I > 2σ(I) Rint = 0.028
|
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A | N2—H2A⋯O1i | 0.86 | 2.18 | 2.9083 (19) | 143 | N2—H2A⋯N3i | 0.86 | 2.58 | 3.3255 (19) | 146 | Symmetry code: (i) . | |
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.
Supporting information
A mixture of the isonicotinohydrazide (0.1 mol), and 5-methylfuran-2-carbaldehyde (0.1 mol) was stirred in refluxing ethanol (20 mL) for 4 h to afford the title compound (0.082 mol, yield 82%). Single crystals suitable for X-ray measurements were obtained by recrystallization from ethanol at room temperature.
All H atoms were fixed geometrically and allowed to ride on their attached atoms, with C—H distances in the range 0.93-0.97 Å and N—H = 0.86 Å, and with Uiso=1.2–1.5Ueq(N,C).
Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT (Bruker, 1997); 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 (Sheldrick, 2008).
N'-[(5-Methylfuran-2-yl)methylene]isonicotinohydrazide
top Crystal data top C12H11N3O2 | Dx = 1.290 Mg m−3 |
Mr = 229.24 | Mo Kα radiation, λ = 0.71073 Å |
Tetragonal, I41/a | Cell parameters from 4665 reflections |
Hall symbol: -I 4ad | θ = 2.9–27.2° |
a = 17.313 (3) Å | µ = 0.09 mm−1 |
c = 15.749 (5) Å | T = 273 K |
V = 4720.5 (18) Å3 | Block, yellow |
Z = 16 | 0.25 × 0.20 × 0.19 mm |
F(000) = 1920 | |
Data collection top Bruker SMART CCD area-detector diffractometer | 2151 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.028 |
Graphite monochromator | θmax = 28.3°, θmin = 1.8° |
ϕ and ω scans | h = −16→23 |
14901 measured reflections | k = −22→22 |
2911 independent reflections | l = −20→20 |
Refinement top Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.041 | H-atom parameters constrained |
wR(F2) = 0.117 | w = 1/[σ2(Fo2) + (0.0456P)2 + 2.257P] where P = (Fo2 + 2Fc2)/3 |
S = 1.04 | (Δ/σ)max < 0.001 |
2911 reflections | Δρmax = 0.17 e Å−3 |
155 parameters | Δρmin = −0.14 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0031 (3) |
Crystal data top C12H11N3O2 | Z = 16 |
Mr = 229.24 | Mo Kα radiation |
Tetragonal, I41/a | µ = 0.09 mm−1 |
a = 17.313 (3) Å | T = 273 K |
c = 15.749 (5) Å | 0.25 × 0.20 × 0.19 mm |
V = 4720.5 (18) Å3 | |
Data collection top Bruker SMART CCD area-detector diffractometer | 2151 reflections with I > 2σ(I) |
14901 measured reflections | Rint = 0.028 |
2911 independent reflections | |
Refinement top R[F2 > 2σ(F2)] = 0.041 | 0 restraints |
wR(F2) = 0.117 | H-atom parameters constrained |
S = 1.04 | Δρmax = 0.17 e Å−3 |
2911 reflections | Δρmin = −0.14 e Å−3 |
155 parameters | |
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 | |
O2 | 0.58347 (5) | 0.51303 (5) | 0.10958 (6) | 0.0482 (3) | |
N3 | 0.72302 (6) | 0.49350 (7) | 0.03623 (7) | 0.0427 (3) | |
C12 | 0.67464 (8) | 0.53721 (7) | −0.00223 (9) | 0.0423 (3) | |
H12A | 0.6866 | 0.5578 | −0.0552 | 0.051* | |
N2 | 0.79076 (6) | 0.47620 (7) | −0.00603 (7) | 0.0443 (3) | |
H2A | 0.7980 | 0.4901 | −0.0578 | 0.053* | |
C8 | 0.60143 (8) | 0.55421 (7) | 0.03726 (8) | 0.0417 (3) | |
O1 | 0.83833 (7) | 0.42110 (8) | 0.11302 (7) | 0.0750 (4) | |
C4 | 0.91448 (8) | 0.41092 (8) | −0.01179 (8) | 0.0442 (3) | |
C11 | 0.84487 (8) | 0.43670 (9) | 0.03721 (8) | 0.0460 (3) | |
C9 | 0.51105 (8) | 0.53616 (9) | 0.13450 (10) | 0.0513 (4) | |
C7 | 0.54259 (8) | 0.60254 (8) | 0.01805 (10) | 0.0505 (4) | |
H7A | 0.5402 | 0.6366 | −0.0276 | 0.061* | |
C3 | 0.91374 (8) | 0.39635 (10) | −0.09860 (9) | 0.0531 (4) | |
H3B | 0.8696 | 0.4056 | −0.1307 | 0.064* | |
N1 | 1.04629 (8) | 0.35518 (10) | −0.09513 (9) | 0.0736 (5) | |
C5 | 0.98256 (9) | 0.39741 (11) | 0.03194 (10) | 0.0640 (5) | |
H5A | 0.9853 | 0.4061 | 0.0901 | 0.077* | |
C2 | 0.98006 (9) | 0.36780 (11) | −0.13609 (10) | 0.0650 (5) | |
H2B | 0.9784 | 0.3566 | −0.1938 | 0.078* | |
C6 | 0.48512 (9) | 0.59116 (9) | 0.08124 (11) | 0.0561 (4) | |
H6A | 0.4382 | 0.6170 | 0.0851 | 0.067* | |
C1 | 1.04634 (10) | 0.37078 (13) | −0.01203 (12) | 0.0758 (6) | |
H1B | 1.0920 | 0.3633 | 0.0180 | 0.091* | |
C10 | 0.47813 (11) | 0.49172 (12) | 0.20700 (12) | 0.0760 (6) | |
H10A | 0.4277 | 0.5113 | 0.2203 | 0.114* | |
H10B | 0.5112 | 0.4971 | 0.2556 | 0.114* | |
H10C | 0.4743 | 0.4382 | 0.1918 | 0.114* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O2 | 0.0471 (5) | 0.0516 (6) | 0.0459 (6) | 0.0050 (4) | 0.0087 (4) | 0.0080 (4) |
N3 | 0.0440 (6) | 0.0466 (6) | 0.0374 (6) | 0.0030 (5) | 0.0080 (5) | 0.0042 (5) |
C12 | 0.0482 (7) | 0.0410 (7) | 0.0377 (7) | −0.0013 (5) | 0.0043 (5) | 0.0035 (5) |
N2 | 0.0455 (6) | 0.0564 (7) | 0.0309 (5) | 0.0060 (5) | 0.0089 (4) | 0.0086 (5) |
C8 | 0.0469 (7) | 0.0390 (7) | 0.0393 (7) | −0.0019 (5) | 0.0027 (5) | 0.0022 (5) |
O1 | 0.0740 (8) | 0.1156 (10) | 0.0355 (6) | 0.0391 (7) | 0.0150 (5) | 0.0225 (6) |
C4 | 0.0432 (7) | 0.0547 (8) | 0.0346 (7) | 0.0036 (6) | 0.0027 (5) | 0.0012 (6) |
C11 | 0.0493 (8) | 0.0564 (8) | 0.0324 (7) | 0.0078 (6) | 0.0065 (5) | 0.0053 (6) |
C9 | 0.0462 (8) | 0.0537 (8) | 0.0540 (9) | 0.0000 (6) | 0.0107 (6) | −0.0028 (7) |
C7 | 0.0529 (8) | 0.0440 (7) | 0.0545 (9) | 0.0040 (6) | 0.0006 (6) | 0.0051 (6) |
C3 | 0.0429 (7) | 0.0785 (10) | 0.0379 (7) | 0.0050 (7) | −0.0012 (6) | −0.0047 (7) |
N1 | 0.0497 (8) | 0.1162 (13) | 0.0550 (8) | 0.0166 (8) | 0.0024 (6) | −0.0196 (8) |
C5 | 0.0577 (9) | 0.0961 (13) | 0.0381 (8) | 0.0182 (9) | −0.0062 (7) | −0.0109 (8) |
C2 | 0.0546 (9) | 0.1006 (13) | 0.0399 (8) | 0.0090 (9) | 0.0034 (7) | −0.0151 (8) |
C6 | 0.0468 (8) | 0.0544 (9) | 0.0672 (10) | 0.0085 (6) | 0.0047 (7) | −0.0014 (7) |
C1 | 0.0483 (9) | 0.1212 (16) | 0.0579 (10) | 0.0220 (10) | −0.0099 (7) | −0.0188 (10) |
C10 | 0.0718 (12) | 0.0839 (13) | 0.0722 (12) | 0.0022 (9) | 0.0292 (9) | 0.0134 (10) |
Geometric parameters (Å, º) top O2—C9 | 1.3735 (16) | C7—C6 | 1.421 (2) |
O2—C8 | 1.3793 (16) | C7—H7A | 0.9300 |
N3—C12 | 1.2812 (17) | C3—C2 | 1.383 (2) |
N3—N2 | 1.3813 (15) | C3—H3B | 0.9300 |
C12—C8 | 1.4421 (18) | N1—C2 | 1.334 (2) |
C12—H12A | 0.9300 | N1—C1 | 1.336 (2) |
N2—C11 | 1.3450 (17) | C5—C1 | 1.383 (2) |
N2—H2A | 0.8600 | C5—H5A | 0.9300 |
C8—C7 | 1.3526 (19) | C2—H2B | 0.9300 |
O1—C11 | 1.2293 (16) | C6—H6A | 0.9300 |
C4—C5 | 1.385 (2) | C1—H1B | 0.9300 |
C4—C3 | 1.3904 (19) | C10—H10A | 0.9600 |
C4—C11 | 1.4990 (18) | C10—H10B | 0.9600 |
C9—C6 | 1.346 (2) | C10—H10C | 0.9600 |
C9—C10 | 1.490 (2) | | |
| | | |
C9—O2—C8 | 106.92 (11) | C2—C3—C4 | 118.50 (14) |
C12—N3—N2 | 117.08 (11) | C2—C3—H3B | 120.7 |
N3—C12—C8 | 119.42 (12) | C4—C3—H3B | 120.7 |
N3—C12—H12A | 120.3 | C2—N1—C1 | 116.18 (14) |
C8—C12—H12A | 120.3 | C1—C5—C4 | 119.14 (14) |
C11—N2—N3 | 117.23 (11) | C1—C5—H5A | 120.4 |
C11—N2—H2A | 121.4 | C4—C5—H5A | 120.4 |
N3—N2—H2A | 121.4 | N1—C2—C3 | 124.47 (14) |
C7—C8—O2 | 109.55 (12) | N1—C2—H2B | 117.8 |
C7—C8—C12 | 133.77 (13) | C3—C2—H2B | 117.8 |
O2—C8—C12 | 116.66 (11) | C9—C6—C7 | 107.52 (13) |
C5—C4—C3 | 117.78 (13) | C9—C6—H6A | 126.2 |
C5—C4—C11 | 118.59 (12) | C7—C6—H6A | 126.2 |
C3—C4—C11 | 123.56 (12) | N1—C1—C5 | 123.88 (15) |
O1—C11—N2 | 122.64 (12) | N1—C1—H1B | 118.1 |
O1—C11—C4 | 120.56 (13) | C5—C1—H1B | 118.1 |
N2—C11—C4 | 116.79 (11) | C9—C10—H10A | 109.5 |
C6—C9—O2 | 109.43 (13) | C9—C10—H10B | 109.5 |
C6—C9—C10 | 135.66 (15) | H10A—C10—H10B | 109.5 |
O2—C9—C10 | 114.68 (14) | C9—C10—H10C | 109.5 |
C8—C7—C6 | 106.55 (13) | H10A—C10—H10C | 109.5 |
C8—C7—H7A | 126.7 | H10B—C10—H10C | 109.5 |
C6—C7—H7A | 126.7 | | |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···O1i | 0.86 | 2.18 | 2.9083 (19) | 143 |
N2—H2A···N3i | 0.86 | 2.58 | 3.3255 (19) | 146 |
Symmetry code: (i) −y+5/4, x−1/4, z−1/4. |
Experimental details
Crystal data |
Chemical formula | C12H11N3O2 |
Mr | 229.24 |
Crystal system, space group | Tetragonal, I41/a |
Temperature (K) | 273 |
a, c (Å) | 17.313 (3), 15.749 (5) |
V (Å3) | 4720.5 (18) |
Z | 16 |
Radiation type | Mo Kα |
µ (mm−1) | 0.09 |
Crystal size (mm) | 0.25 × 0.20 × 0.19 |
|
Data collection |
Diffractometer | Bruker SMART CCD area-detector diffractometer |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 14901, 2911, 2151 |
Rint | 0.028 |
(sin θ/λ)max (Å−1) | 0.667 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.041, 0.117, 1.04 |
No. of reflections | 2911 |
No. of parameters | 155 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.17, −0.14 |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···O1i | 0.86 | 2.18 | 2.9083 (19) | 143 |
N2—H2A···N3i | 0.86 | 2.58 | 3.3255 (19) | 146 |
Symmetry code: (i) −y+5/4, x−1/4, z−1/4. |
References
Bruker (1997). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Chiu, P., Chen, B. & Cheng, K. F. (1998). Tetrahedron Lett. 39, 9229–9232. Web of Science CSD CrossRef CAS Google Scholar
Cimerman, Z., Galic, N. & Bosner, B. (1997). Anal. Chim. Acta, 343, 145–153. CrossRef CAS Web of Science Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
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ISSN: 2056-9890
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Schiff bases have received considerable attention in the literature. They are attractive from several points of view, such as the possibility of analytical application (Cimerman et al., 1997). As part of our search for new schiff base compounds we synthesized the title compound (I), and describe its structure here.
In the title compound (I) (Fig. 1), the C12—N3 bond length of 1.2812 (17)Å is comparable with C—N double bond [1.284 (2) Å] reported (Chiu et al., 1998). The pyridine ring (N1/C1–C5) makes a dihedral angle of 46.90 (9)°, with the plane of the furan ring (O2/C6–C9).
The crsytal packing is stabilized by intermolecular N—H···O, N—H···N hydrogen bonds (Table 1, Fig. 2).