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A polymorph of N′-[(4-hy­dr­oxy­phen­yl)methyl­­idene]pyridine-4-carbohydrazide

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aDepartment of Chemistry, Nirmala College Muvattupuzha, Ernakulam, 686661, Kerala, India, bDepartment of Chemistry, Keene, State College, 229 Main Street, Keene, NH03435-2001, USA, and cDepartment of Chemistry, Central University of Kerala, Tejaswini Hills, Periye, Kasaragod 671 320, Kerala, India
*Correspondence e-mail: [email protected]

Edited by M. Weil, Vienna University of Technology, Austria (Received 11 March 2026; accepted 24 March 2026; online 27 March 2026)

The synthesis and single-crystal X-ray diffraction analysis of a polymorphic form of the isoniazid derivative N′-[(4-hy­droxy­phen­yl)methyl­idene]pyridine-4-carbohydrazide, C13H11N3O2, are reported, revealing that both the mol­ecular conformation and the hydrogen-bonding scheme differ in the two polymorphs. The crystal packing of the title polymorph is primarily consolidated by N—H⋯O and O—H⋯N hydrogen-bonding inter­actions, leading to the formation of a supra­molecular layer parallel to (001). The inter­molecular contacts were further qu­anti­fied and analysed using Hirshfeld surface analysis.

3D view (loading...)
[Scheme 3D1]
Chemical scheme
[Scheme 1]

Structure description

N-containing heterocycles constitute a major class of natural products and possess a wide range of applications (Goetz et al., 2015View full citation). They are widely used as starting materials for the synthesis of biologically important compounds. Among them, isoniazid-based scaffolds, which contain nitro­gen heterocycles, have attracted considerable attention in medicinal chemistry due to their diverse biological activities, including anti-carcinogenic, anti-fungal, anti-mycobacterial, analgesic, anti­bacterial, and anti­viral properties (Tom et al., 2020View full citation; Rodrigues et al., 2014View full citation; Mohanram & Meshram, 2014View full citation; Judge et al., 2013View full citation; Hu et al., 2017View full citation; Costa et al., 2024View full citation). Among these, their anti-tubercular activity is particularly significant. As part of our ongoing research in this field, we report here on the synthesis and crystal structure of a polymorph of N′-[(4-hy­droxy­phen­yl)methyl­idene]pyridine-4-carbohydrazide, an isoniazid-derived mol­ecule with potential anti­tubercular activity.

Single-crystal X-ray diffraction analysis of the title compound, C13H11N3O2, revealed that it is dimorphic. The title PA polymorph (Fig. 1[link]) crystallizes in the monoclinic space group P21/c. The previously reported polymorph PB (Deng et al., 2005View full citation) crystallizes in the same space group type but with different unit-cell parameters. The differences between the PA and PB forms can mainly be attributed to crystal-packing effects. An additional monohydrated ortho­rhom­bic form has also been reported (Tai et al., 2007View full citation). The overlay of the two mol­ecules of the polymorphs (Fig. 2[link]) indicates that they possess distinct mol­ecular conformations. PA adopts a slightly twisted conformation compared to the more planar PB form. The dihedral angles between the pyridine ring (C2, C3, C4, N3, C5, C6) and hydrazide moiety (N1, N2, C1, O1, C7) are 36.14 (8)° in PA and 9.59 (8)° in PB. Similarly, the dihedral angles between the hydrazide moiety and phenol ring are 23.97 (8)° in PA and 3.96 (7)° in PB.

[Figure 1]
Figure 1
Mol­ecular structure of polymorph PA with displacement ellipsoids drawn at the 30% probability level.
[Figure 2]
Figure 2
Superimposition of the mol­ecular structures of PA (gold) and PB (blue).

The mol­ecular packing and hydrogen-bonding patterns differ significantly in the two extended structures of PA and PB. The polymorphs exhibit different combinations of hydrogen-bonding donor and acceptor sites, leading to distinct supra­molecular networks. The PA polymorph reported here exhibits two types of classical hydrogen-bonding inter­actions (Table 1[link]). The NH group of the N=NH—C=O moiety is hydrogen-bonded to the O atom of the same moiety of a neighbouring mol­ecule into chains extending parallel to [100]. These chains are connected through O—H⋯N hydrogen-bonding inter­actions involving the phenol OH group and the pyridine N atom, leading to the formation of a supra­molecular layer extending parallel to (001) (Fig. 3[link]). In polymorph PB, the NH group of the N=NH—C=O moiety bonds to the pyridine N atom, and the phenol OH group forms bifurcated hydrogen bonds to the N=NH—C=O moiety and the carbonyl O atom of neighbouring mol­ecules, thus leading to a different supra­molecular arrangement.

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1⋯O1i 0.86 2.34 3.1452 (15) 156
O2—H2⋯N3ii 0.82 1.96 2.7356 (16) 159
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation.
[Figure 3]
Figure 3
Formation of supra­molecular (001) layers in the crystal structure of PA. Hydrogen bonds are shown as dotted lines.

To visualize and qu­antify the contributions of inter­molecular inter­actions in the supra­molecular assembly of the title compound, a Hirshfeld surface (HS) analysis (Spackman & Jayatilaka, 2009View full citation) was performed using CrystalExplorer (Spackman et al., 2021View full citation). The Hirshfeld surface mapped over dnorm is shown in Fig. 4[link], where prominent deep-red spots correspond to significant inter­molecular contacts. These spots appear around atoms N3, N1, O1 and O2, indicating that these atoms participate in the inter­molecular hydrogen bonds, as discussed above. The associated two-dimensional fingerprint plots provide qu­anti­tative insight into the various non-covalent inter­actions contributing to the crystal packing. The H⋯H, C⋯H, N⋯H and O⋯H, inter­actions dominate the packing, collectively accounting for approximately 95% of the total Hirshfeld surface area (Fig. 5[link]).

[Figure 4]
Figure 4
The Hirshfeld surface of PA mapped over dnorm.
[Figure 5]
Figure 5
The two-dimensional fingerprint plots for PA for different contact types.

Synthesis and crystallization

A mixture of p-hy­droxy­benzaldehyde (1 mmol) and isonicotinic hydrazide (1 mmol) was refluxed in methanol (20 ml) at 343 K for 30 min. After completion of the reaction, the mixture was allowed to cool to room temperature. Colourless crystals suitable for X-ray diffraction were obtained by slow evaporation of the solution at room temperature.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link].

Table 2
Experimental details

Crystal data
Chemical formula C13H11N3O2
Mr 241.25
Crystal system, space group Monoclinic, P21/c
Temperature (K) 293
a, b, c (Å) 5.36340 (13), 14.4462 (4), 14.6619 (4)
β (°) 91.229 (3)
V3) 1135.75 (5)
Z 4
Radiation type Cu Kα
μ (mm−1) 0.81
Crystal size (mm) 0.42 × 0.33 × 0.29
 
Data collection
Diffractometer Rigaku Oxford Diffraction Gemini Eos
Absorption correction Multi-scan (CrysAlis PRO; Rigaku OD, 2015View full citation)
Tmin, Tmax 0.858, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 7898, 2185, 1901
Rint 0.027
(sin θ/λ)max−1) 0.624
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.039, 0.112, 1.05
No. of reflections 2185
No. of parameters 164
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.22, −0.25
Computer programs: CrysAlis PRO (Rigaku OD, 2015View full citation), SHELXT (Sheldrick, 2015aView full citation), SHELXL (Sheldrick, 2015bView full citation), ORTEP-3 for Windows (Farrugia, 2012View full citation), Mercury (Macrae et al., 2020View full citation) and publCIF (Westrip, 2010View full citation).

Structural data


Computing details top

N'-[(4-Hydroxyphenyl)methylidene]pyridine-4-carbohydrazide top
Crystal data top
C13H11N3O2F(000) = 504
Mr = 241.25Dx = 1.411 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54184 Å
a = 5.36340 (13) ÅCell parameters from 3210 reflections
b = 14.4462 (4) Åθ = 4.3–71.3°
c = 14.6619 (4) ŵ = 0.81 mm1
β = 91.229 (3)°T = 293 K
V = 1135.75 (5) Å3Block, pale yellow
Z = 40.42 × 0.33 × 0.29 mm
Data collection top
Rigaku Oxford Diffraction Gemini Eos
diffractometer
1901 reflections with I > 2σ(I)
Radiation source: Enhance (Cu) X-ray SourceRint = 0.027
ω scansθmax = 74.3°, θmin = 4.3°
Absorption correction: multi-scan
(CrysAlisPro; Rigaku OD, 2015)
h = 65
Tmin = 0.858, Tmax = 1.000k = 1717
7898 measured reflectionsl = 1718
2185 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039H-atom parameters constrained
wR(F2) = 0.112 w = 1/[σ2(Fo2) + (0.0635P)2 + 0.3435P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
2185 reflectionsΔρmax = 0.22 e Å3
164 parametersΔρmin = 0.25 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.4746 (3)0.44240 (9)0.39335 (9)0.0229 (3)
C20.5399 (2)0.34115 (9)0.39757 (9)0.0211 (3)
C30.7526 (2)0.30837 (9)0.43964 (9)0.0235 (3)
H30.8631800.3485850.4690940.028*
C40.7997 (3)0.21405 (10)0.43747 (10)0.0252 (3)
H40.9437070.1926480.4669900.030*
C50.4466 (3)0.18484 (10)0.35751 (10)0.0269 (3)
H50.3379400.1430610.3292770.032*
C60.3834 (2)0.27780 (10)0.35686 (9)0.0246 (3)
H60.2351130.2971530.3288770.029*
C70.8580 (3)0.63450 (9)0.36248 (9)0.0236 (3)
H70.9966670.5985990.3494560.028*
C80.8798 (2)0.73497 (9)0.35866 (9)0.0218 (3)
C90.6961 (2)0.79454 (10)0.39373 (9)0.0237 (3)
H90.5547510.7697270.4200740.028*
C100.7254 (3)0.88975 (10)0.38910 (10)0.0262 (3)
H100.6052710.9288030.4129080.031*
C110.9400 (3)0.92725 (10)0.34775 (10)0.0252 (3)
C121.1243 (3)0.86858 (10)0.31337 (10)0.0250 (3)
H121.2651310.8934090.2866670.030*
C131.0954 (3)0.77356 (10)0.31942 (10)0.0240 (3)
H131.2187140.7346880.2975310.029*
N10.6758 (2)0.49791 (8)0.38618 (8)0.0244 (3)
H10.8215560.4734190.3833140.029*
N20.6528 (2)0.59354 (8)0.38331 (8)0.0252 (3)
N30.6540 (2)0.15252 (8)0.39630 (8)0.0265 (3)
O10.25700 (19)0.46875 (7)0.39380 (8)0.0327 (3)
O20.9794 (2)1.01946 (7)0.34003 (9)0.0354 (3)
H20.8583661.0476000.3590960.053*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0241 (7)0.0206 (7)0.0240 (7)0.0022 (5)0.0011 (5)0.0009 (5)
C20.0210 (7)0.0194 (7)0.0230 (7)0.0008 (5)0.0024 (5)0.0005 (5)
C30.0216 (7)0.0219 (7)0.0268 (7)0.0018 (5)0.0013 (5)0.0003 (5)
C40.0217 (7)0.0237 (7)0.0301 (7)0.0009 (5)0.0008 (6)0.0024 (6)
C50.0259 (7)0.0232 (7)0.0315 (8)0.0046 (6)0.0012 (6)0.0026 (6)
C60.0198 (7)0.0258 (7)0.0280 (7)0.0008 (5)0.0018 (5)0.0008 (5)
C70.0246 (7)0.0200 (7)0.0259 (7)0.0038 (5)0.0027 (5)0.0017 (5)
C80.0230 (7)0.0188 (7)0.0233 (7)0.0017 (5)0.0049 (5)0.0001 (5)
C90.0203 (6)0.0212 (7)0.0295 (7)0.0009 (5)0.0006 (5)0.0004 (5)
C100.0215 (7)0.0238 (7)0.0334 (7)0.0039 (5)0.0011 (6)0.0028 (6)
C110.0261 (7)0.0186 (7)0.0308 (7)0.0002 (5)0.0040 (6)0.0008 (5)
C120.0207 (6)0.0254 (7)0.0290 (7)0.0022 (5)0.0018 (5)0.0017 (6)
C130.0211 (7)0.0237 (7)0.0273 (7)0.0049 (5)0.0008 (5)0.0027 (5)
N10.0238 (6)0.0153 (6)0.0340 (7)0.0029 (4)0.0011 (5)0.0004 (5)
N20.0285 (6)0.0166 (6)0.0306 (6)0.0017 (5)0.0021 (5)0.0013 (5)
N30.0269 (6)0.0195 (6)0.0332 (7)0.0003 (5)0.0028 (5)0.0004 (5)
O10.0240 (5)0.0257 (5)0.0484 (7)0.0053 (4)0.0031 (4)0.0013 (5)
O20.0307 (6)0.0174 (5)0.0583 (8)0.0003 (4)0.0063 (5)0.0003 (5)
Geometric parameters (Å, º) top
C1—O11.2279 (18)C7—H70.9300
C1—N11.3501 (18)C8—C91.4132 (19)
C1—C21.5049 (18)C8—C131.417 (2)
C2—C31.3696 (19)C9—C101.3862 (19)
C2—C61.3701 (19)C9—H90.9300
C3—C41.3862 (19)C10—C111.420 (2)
C3—H30.9300C10—H100.9300
C4—N31.3212 (18)C11—O21.3538 (17)
C4—H40.9300C11—C121.404 (2)
C5—N31.3234 (18)C12—C131.3844 (19)
C5—C61.385 (2)C12—H120.9300
C5—H50.9300C13—H130.9300
C6—H60.9300N1—N21.3875 (16)
C7—N21.2916 (19)N1—H10.8600
C7—C81.4573 (18)O2—H20.8200
O1—C1—N1125.28 (12)C13—C8—C7118.31 (12)
O1—C1—C2121.43 (12)C10—C9—C8120.38 (13)
N1—C1—C2113.26 (12)C10—C9—H9119.8
C3—C2—C6117.50 (13)C8—C9—H9119.8
C3—C2—C1123.05 (12)C9—C10—C11119.56 (13)
C6—C2—C1119.44 (12)C9—C10—H10120.2
C2—C3—C4118.69 (13)C11—C10—H10120.2
C2—C3—H3120.7O2—C11—C12116.86 (13)
C4—C3—H3120.7O2—C11—C10122.71 (13)
N3—C4—C3124.43 (13)C12—C11—C10120.43 (13)
N3—C4—H4117.8C13—C12—C11119.66 (13)
C3—C4—H4117.8C13—C12—H12120.2
N3—C5—C6123.26 (13)C11—C12—H12120.2
N3—C5—H5118.4C12—C13—C8120.64 (13)
C6—C5—H5118.4C12—C13—H13119.7
C2—C6—C5119.81 (13)C8—C13—H13119.7
C2—C6—H6120.1C1—N1—N2121.55 (11)
C5—C6—H6120.1C1—N1—H1119.2
N2—C7—C8122.33 (12)N2—N1—H1119.2
N2—C7—H7118.8C7—N2—N1112.82 (11)
C8—C7—H7118.8C4—N3—C5116.27 (12)
C9—C8—C13119.31 (13)C11—O2—H2109.5
C9—C8—C7122.37 (13)
O1—C1—C2—C3147.48 (14)C8—C9—C10—C110.8 (2)
N1—C1—C2—C334.59 (18)C9—C10—C11—O2179.30 (13)
O1—C1—C2—C633.4 (2)C9—C10—C11—C121.3 (2)
N1—C1—C2—C6144.56 (13)O2—C11—C12—C13179.82 (13)
C6—C2—C3—C41.1 (2)C10—C11—C12—C130.4 (2)
C1—C2—C3—C4178.08 (13)C11—C12—C13—C81.0 (2)
C2—C3—C4—N30.8 (2)C9—C8—C13—C121.50 (19)
C3—C2—C6—C51.6 (2)C7—C8—C13—C12179.42 (12)
C1—C2—C6—C5177.62 (13)O1—C1—N1—N23.5 (2)
N3—C5—C6—C20.2 (2)C2—C1—N1—N2178.65 (11)
N2—C7—C8—C912.3 (2)C8—C7—N2—N1177.78 (11)
N2—C7—C8—C13168.67 (13)C1—N1—N2—C7170.07 (12)
C13—C8—C9—C100.57 (19)C3—C4—N3—C52.1 (2)
C7—C8—C9—C10179.61 (12)C6—C5—N3—C41.6 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O1i0.862.343.1452 (15)156
O2—H2···N3ii0.821.962.7356 (16)159
Symmetry codes: (i) x+1, y, z; (ii) x, y+1, z.
 

Footnotes

Deceased.

Acknowledgements

The NSF–MRI program (grant No. CHE-1039027) is acknowledged for funds to purchase the Rigaku X-ray diffractometer.

References

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