The title compound, C
13H
10BrN
3O, was prepared by the reaction of isonicotinohydrazide and 4-bromobenzaldehyde. The dihedral angle between the benzene and pyridine rings is 8.60 (12)°. The crystal packing is stabilized by intermolecular C—H
O and N—H
O hydogen-bonding interactions.
Supporting information
CCDC reference: 712428
Key indicators
- Single-crystal X-ray study
- T = 273 K
- Mean (C-C) = 0.003 Å
- R factor = 0.036
- wR factor = 0.094
- Data-to-parameter ratio = 18.2
checkCIF/PLATON results
No syntax errors found
Alert level B
PLAT057_ALERT_3_B Correction for Absorption Required RT(exp) ... 1.21
Alert level C
ABSTM02_ALERT_3_C The ratio of Tmax/Tmin expected RT(exp) is > 1.10
Absorption corrections should be applied.
Tmin and Tmax expected: 0.459 0.549
RT(exp) = 1.195
Value of measurement temperature given = 273.000
Value of melting point given = 0.000
PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.97
PLAT790_ALERT_4_C Centre of Gravity not Within Unit Cell: Resd. # 1
C13 H10 Br N3 O
0 ALERT level A = In general: serious problem
1 ALERT level B = Potentially serious problem
3 ALERT level C = Check and explain
0 ALERT level G = General alerts; check
0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data
0 ALERT type 2 Indicator that the structure model may be wrong or deficient
3 ALERT type 3 Indicator that the structure quality may be low
1 ALERT type 4 Improvement, methodology, query or suggestion
0 ALERT type 5 Informative message, check
A mixture of the isonicotinohydrazide (0.1 mol), and 4-bromobenzaldehyde (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.
H atoms were fixed geometrically and allowed to ride on their attached atoms,
with N—H = 0.86 Å and C—H = 0.93 Å, and with
Uiso=1.2–Ueq(C,N).
All H atoms were placed in idealized positions and refined with riding
constraints, with N—H = 0.86 Å and C—H = 0.93 Å and with
Uiso(H) = 1.2Ueq(C,N).
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'-(4-Bromobenzylidene)isonicotinohydrazide
top
Crystal data top
C13H10BrN3O | F(000) = 608 |
Mr = 304.15 | Dx = 1.643 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 2167 reflections |
a = 18.715 (9) Å | θ = 3.3–24.3° |
b = 6.517 (3) Å | µ = 3.33 mm−1 |
c = 10.126 (5) Å | T = 273 K |
β = 95.512 (9)° | Block, yellow |
V = 1229.3 (11) Å3 | 0.25 × 0.20 × 0.18 mm |
Z = 4 | |
Data collection top
Bruker SMART CCD area-detector diffractometer | 1914 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.034 |
Graphite monochromator | θmax = 28.4°, θmin = 2.2° |
ϕ and ω scans | h = −18→25 |
7721 measured reflections | k = −7→8 |
2992 independent reflections | l = −13→13 |
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)] = 0.036 | H-atom parameters constrained |
wR(F2) = 0.094 | w = 1/[σ2(Fo2) + (0.0429P)2 + 0.1134P] where P = (Fo2 + 2Fc2)/3 |
S = 1.01 | (Δ/σ)max < 0.001 |
2992 reflections | Δρmax = 0.39 e Å−3 |
164 parameters | Δρmin = −0.55 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: 0.0072 (10) |
Crystal data top
C13H10BrN3O | V = 1229.3 (11) Å3 |
Mr = 304.15 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 18.715 (9) Å | µ = 3.33 mm−1 |
b = 6.517 (3) Å | T = 273 K |
c = 10.126 (5) Å | 0.25 × 0.20 × 0.18 mm |
β = 95.512 (9)° | |
Data collection top
Bruker SMART CCD area-detector diffractometer | 1914 reflections with I > 2σ(I) |
7721 measured reflections | Rint = 0.034 |
2992 independent reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.036 | 0 restraints |
wR(F2) = 0.094 | H-atom parameters constrained |
S = 1.01 | Δρmax = 0.39 e Å−3 |
2992 reflections | Δρmin = −0.55 e Å−3 |
164 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 | |
Br | 0.038461 (17) | 0.64201 (4) | 0.85386 (4) | 0.08031 (18) | |
N3 | 0.25010 (10) | 1.5120 (3) | 0.93706 (17) | 0.0390 (4) | |
N2 | 0.29511 (10) | 1.6713 (3) | 0.90925 (18) | 0.0386 (4) | |
H2A | 0.3079 | 1.6847 | 0.8304 | 0.046* | |
O1 | 0.30311 (10) | 1.7983 (3) | 1.11880 (16) | 0.0529 (4) | |
C7 | 0.10215 (13) | 0.8680 (3) | 0.8543 (3) | 0.0457 (6) | |
C10 | 0.19040 (12) | 1.2072 (3) | 0.8503 (2) | 0.0369 (5) | |
N1 | 0.46415 (11) | 2.2729 (3) | 0.8926 (2) | 0.0545 (6) | |
C4 | 0.36913 (11) | 1.9665 (3) | 0.9610 (2) | 0.0349 (5) | |
C13 | 0.31906 (12) | 1.8058 (3) | 1.0047 (2) | 0.0362 (5) | |
C9 | 0.19163 (13) | 1.0539 (4) | 0.7549 (2) | 0.0446 (6) | |
H9A | 0.2229 | 1.0656 | 0.6893 | 0.054* | |
C12 | 0.23656 (13) | 1.3861 (3) | 0.8414 (2) | 0.0417 (5) | |
H12A | 0.2570 | 1.4094 | 0.7626 | 0.050* | |
C3 | 0.37459 (13) | 2.1531 (3) | 1.0273 (2) | 0.0448 (6) | |
H3B | 0.3471 | 2.1787 | 1.0972 | 0.054* | |
C5 | 0.41305 (13) | 1.9365 (4) | 0.8605 (2) | 0.0455 (6) | |
H5A | 0.4115 | 1.8140 | 0.8133 | 0.055* | |
C11 | 0.14423 (13) | 1.1841 (4) | 0.9499 (2) | 0.0438 (6) | |
H11A | 0.1429 | 1.2844 | 1.0150 | 0.053* | |
C8 | 0.14730 (14) | 0.8850 (3) | 0.7560 (3) | 0.0488 (6) | |
H8A | 0.1480 | 0.7843 | 0.6911 | 0.059* | |
C6 | 0.10088 (13) | 1.0151 (4) | 0.9526 (2) | 0.0473 (6) | |
H6A | 0.0708 | 0.9994 | 1.0199 | 0.057* | |
C2 | 0.42134 (14) | 2.3003 (4) | 0.9882 (3) | 0.0515 (6) | |
H2B | 0.4229 | 2.4263 | 1.0315 | 0.062* | |
C1 | 0.45933 (14) | 2.0919 (4) | 0.8314 (3) | 0.0552 (7) | |
H1B | 0.4891 | 2.0684 | 0.7646 | 0.066* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Br | 0.0729 (3) | 0.04607 (19) | 0.1216 (4) | −0.01855 (14) | 0.0075 (2) | −0.00034 (16) |
N3 | 0.0430 (11) | 0.0399 (10) | 0.0350 (10) | −0.0045 (8) | 0.0083 (8) | 0.0038 (9) |
N2 | 0.0456 (11) | 0.0415 (10) | 0.0301 (10) | −0.0063 (8) | 0.0103 (8) | 0.0034 (8) |
O1 | 0.0674 (12) | 0.0593 (10) | 0.0341 (9) | −0.0110 (9) | 0.0160 (8) | −0.0036 (8) |
C7 | 0.0409 (13) | 0.0333 (12) | 0.0618 (16) | 0.0013 (9) | −0.0016 (12) | 0.0032 (11) |
C10 | 0.0383 (12) | 0.0367 (11) | 0.0352 (12) | 0.0003 (9) | 0.0013 (10) | 0.0032 (10) |
N1 | 0.0568 (14) | 0.0567 (14) | 0.0492 (13) | −0.0143 (11) | 0.0019 (11) | 0.0077 (11) |
C4 | 0.0363 (12) | 0.0387 (12) | 0.0294 (11) | 0.0036 (9) | 0.0022 (9) | 0.0023 (9) |
C13 | 0.0380 (13) | 0.0390 (11) | 0.0321 (12) | 0.0051 (9) | 0.0055 (10) | 0.0024 (10) |
C9 | 0.0509 (14) | 0.0462 (13) | 0.0375 (13) | 0.0051 (11) | 0.0081 (11) | −0.0005 (11) |
C12 | 0.0469 (14) | 0.0440 (13) | 0.0355 (12) | −0.0016 (10) | 0.0102 (11) | 0.0037 (11) |
C3 | 0.0457 (14) | 0.0457 (14) | 0.0437 (13) | 0.0035 (10) | 0.0086 (11) | −0.0041 (11) |
C5 | 0.0482 (14) | 0.0493 (13) | 0.0400 (13) | −0.0052 (11) | 0.0097 (11) | −0.0050 (11) |
C11 | 0.0472 (14) | 0.0443 (13) | 0.0403 (13) | −0.0005 (10) | 0.0060 (11) | −0.0057 (10) |
C8 | 0.0571 (16) | 0.0396 (13) | 0.0487 (15) | 0.0076 (11) | 0.0005 (13) | −0.0090 (11) |
C6 | 0.0431 (14) | 0.0510 (14) | 0.0489 (14) | −0.0025 (11) | 0.0103 (11) | 0.0065 (12) |
C2 | 0.0532 (16) | 0.0402 (13) | 0.0596 (16) | −0.0022 (11) | −0.0029 (14) | −0.0006 (12) |
C1 | 0.0541 (16) | 0.0706 (18) | 0.0428 (14) | −0.0117 (13) | 0.0139 (12) | 0.0010 (13) |
Geometric parameters (Å, º) top
Br—C7 | 1.894 (2) | C4—C13 | 1.500 (3) |
N3—C12 | 1.276 (3) | C9—C8 | 1.379 (3) |
N3—N2 | 1.383 (2) | C9—H9A | 0.9300 |
N2—C13 | 1.349 (3) | C12—H12A | 0.9300 |
N2—H2A | 0.8600 | C3—C2 | 1.382 (3) |
O1—C13 | 1.222 (3) | C3—H3B | 0.9300 |
C7—C8 | 1.371 (4) | C5—C1 | 1.382 (3) |
C7—C6 | 1.384 (3) | C5—H5A | 0.9300 |
C10—C9 | 1.391 (3) | C11—C6 | 1.370 (3) |
C10—C11 | 1.398 (3) | C11—H11A | 0.9300 |
C10—C12 | 1.459 (3) | C8—H8A | 0.9300 |
N1—C2 | 1.326 (3) | C6—H6A | 0.9300 |
N1—C1 | 1.331 (3) | C2—H2B | 0.9300 |
C4—C5 | 1.382 (3) | C1—H1B | 0.9300 |
C4—C3 | 1.388 (3) | | |
| | | |
C12—N3—N2 | 114.10 (18) | C10—C12—H12A | 118.6 |
C13—N2—N3 | 120.59 (18) | C4—C3—C2 | 119.3 (2) |
C13—N2—H2A | 119.7 | C4—C3—H3B | 120.4 |
N3—N2—H2A | 119.7 | C2—C3—H3B | 120.4 |
C8—C7—C6 | 121.4 (2) | C4—C5—C1 | 118.9 (2) |
C8—C7—Br | 119.52 (19) | C4—C5—H5A | 120.6 |
C6—C7—Br | 119.09 (19) | C1—C5—H5A | 120.6 |
C9—C10—C11 | 118.4 (2) | C6—C11—C10 | 120.6 (2) |
C9—C10—C12 | 118.8 (2) | C6—C11—H11A | 119.7 |
C11—C10—C12 | 122.8 (2) | C10—C11—H11A | 119.7 |
C2—N1—C1 | 116.1 (2) | C7—C8—C9 | 118.9 (2) |
C5—C4—C3 | 117.3 (2) | C7—C8—H8A | 120.5 |
C5—C4—C13 | 123.5 (2) | C9—C8—H8A | 120.5 |
C3—C4—C13 | 119.2 (2) | C11—C6—C7 | 119.5 (2) |
O1—C13—N2 | 123.8 (2) | C11—C6—H6A | 120.3 |
O1—C13—C4 | 121.6 (2) | C7—C6—H6A | 120.3 |
N2—C13—C4 | 114.59 (18) | N1—C2—C3 | 124.0 (2) |
C8—C9—C10 | 121.2 (2) | N1—C2—H2B | 118.0 |
C8—C9—H9A | 119.4 | C3—C2—H2B | 118.0 |
C10—C9—H9A | 119.4 | N1—C1—C5 | 124.4 (2) |
N3—C12—C10 | 122.9 (2) | N1—C1—H1B | 117.8 |
N3—C12—H12A | 118.6 | C5—C1—H1B | 117.8 |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···O1i | 0.86 | 2.14 | 2.966 (3) | 161 |
C12—H12A···O1i | 0.93 | 2.60 | 3.377 (3) | 142 |
Symmetry code: (i) x, −y+7/2, z−1/2. |
Experimental details
Crystal data |
Chemical formula | C13H10BrN3O |
Mr | 304.15 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 273 |
a, b, c (Å) | 18.715 (9), 6.517 (3), 10.126 (5) |
β (°) | 95.512 (9) |
V (Å3) | 1229.3 (11) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 3.33 |
Crystal size (mm) | 0.25 × 0.20 × 0.18 |
|
Data collection |
Diffractometer | Bruker SMART CCD area-detector diffractometer |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 7721, 2992, 1914 |
Rint | 0.034 |
(sin θ/λ)max (Å−1) | 0.669 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.036, 0.094, 1.01 |
No. of reflections | 2992 |
No. of parameters | 164 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.39, −0.55 |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···O1i | 0.86 | 2.14 | 2.966 (3) | 161 |
C12—H12A···O1i | 0.93 | 2.60 | 3.377 (3) | 142 |
Symmetry code: (i) x, −y+7/2, z−1/2. |
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 herein we report the crstal structure of (I).
In (I) (Fig. 1),
As seen in Fig. 1, the C12—N3 bond length of 1.276 (3)Å is comparable with C—N double bond [1.284 (2) Å] reported (Chiu et al., 1998). In the title molecule, the benzene ring (C6–C10) is essentialy planar with a maximum deviation of 0.009 (2) Å for C6 and C9, while the pyridine ring is planar, with a maximum deviation of 0.012 (2) Å for C3. The dihedral angle between the benzene and pyridine rings is 8.60 (12)°.
The crystal packing is stabilized by intermolecular C—H···O and N—H···O hydogen-bonding interactions.